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Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


1

Influence of Liquid Water Content and Temperature on the Form and Growth of Branched Planar Snow Crystals in a Cloud  

Science Journals Connector (OSTI)

How liquid water content (LWC) and temperature affect the growth of branched planar snow crystals is poorly understood. To address this issue, a vertical supercooled cloud tunnel was used to grow 167 individual snow crystals for 10 min under ...

Tsuneya Takahashi

2014-11-01T23:59:59.000Z

2

Cloud fraction, liquid and ice water contents derived from long-term radar, lidar, and microwave radiometer data are systematically compared to models to quantify and  

E-Print Network (OSTI)

Cloud fraction, liquid and ice water contents derived from long-term radar, lidar, and microwave a systematic evaluation of clouds in forecast models. Clouds and their associated microphysical processes for end users of weather forecasts, who may be interested not only in cloud cover, but in other variables

Hogan, Robin

3

ARM - Measurement - Liquid water content  

NLE Websites -- All DOE Office Websites (Extended Search)

MicrowaveImager (SSMI): Satellite 14 SSMI15 : Special Sensor MicrowaveImager (SSMI): Satellite 15 Datastreams ECMWFDIAG : European Centre for Medium Range Weather Forecasts...

4

Analysis of soil and water for TATB content  

SciTech Connect

A reverse-phase liquid chromatography (HPLC) method was developed for the analysis of TATB in soil samples. The soil samples were extracted with dimethylformamide (DMF). The extract was analyzed to determine the TATB content in the soil. The detection limit using this procedure was 2 parts/million (ppm) for TATB in the soil. An organic free sample of water was saturated with TATB. The water was filtered through a 0.2-{mu} filter, then injected into both a reverse-phase and normal-phase liquid chromatograph system. No peaks were detected. Therefore, the solubility of TATB in water is less than the detection limits of the chromatograph methods.

Schaffer, C.L.

1992-11-01T23:59:59.000Z

5

Core-softened Fluids, Water-like Anomalies and the Liquid-Liquid Critical Points  

E-Print Network (OSTI)

. INTRODUCTION Water is characterized by well-known thermodynamic and kinetic liquid-state anomalies; for examplePREPRINT Core-softened Fluids, Water-like Anomalies and the Liquid-Liquid Critical Points Evy simulations are used to examine the relationship between water-like anoma- lies and the liquid-liquid critical

Barbosa, Marcia C. B.

6

Absorption Spectra and Photolysis of Methyl Peroxide in Liquid and Frozen Water  

E-Print Network (OSTI)

, University of California, Irvine, California 92697, United States Department of Physical Chemistry with low temperatures, in the presence of clouds with a high liquid-water content and large solar zenith

Nizkorodov, Sergey

7

Accurate measurement of the through-plane water content of proton-exchange  

NLE Websites -- All DOE Office Websites (Extended Search)

Accurate measurement of the through-plane water content of proton-exchange Accurate measurement of the through-plane water content of proton-exchange membranes using neutron radiography Title Accurate measurement of the through-plane water content of proton-exchange membranes using neutron radiography Publication Type Journal Article Year of Publication 2012 Authors Hussey, Daniel S., Dusan Spernjak, Adam Z. Weber, Rangachary Mukundan, Joseph Fairweather, Eric L. Brosha, John Davey, Jacob S. Spendelow, David L. Jacobson, and Rodney L. Borup Journal Journal of Applied Physics Volume 112 Issue 10 Pagination 104906 Date Published 2012 ISSN 00218979 Keywords electrolyte fuel-cells, in-situ, liquid water, microchannel plate detectors, model, nafion, polymer electrolytes, schroeders-paradox, transport, x-ray-scattering Abstract The water sorption of proton-exchange membranes (PEMs) was measured in situ using high-resolution neutron imaging in small-scale fuel cell test sections. A detailed characterization of the measurement uncertainties and corrections associated with the technique is presented. An image-processing procedure resolved a previously reported discrepancy between the measured and predicted membrane water content. With high-resolution neutron-imaging detectors, the water distributions across N1140 and N117 Nafion membranes are resolved in vapor-sorption experiments and during fuel cell and hydrogen-pump operation. The measured in situ water content of a restricted membrane at 80 degrees C is shown to agree with ex situ gravimetric measurements of free-swelling membranes over a water activity range of 0.5 to 1.0 including at liquid equilibration. Schroeder's paradox was verified by in situ water-content measurements which go from a high value at supersaturated or liquid conditions to a lower one with fully saturated vapor. At open circuit and during fuel cell operation, the measured water content indicates that the membrane is operating between the vapor-and liquid-equilibrated states.

8

Isotope and Temperature Effects in Liquid Water Probed by Soft...  

NLE Websites -- All DOE Office Websites (Extended Search)

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print The geometric structure of liquid water has been investigated in detail by many techniques, but many...

9

Phase effects for electrons in liquid water and water vapor  

SciTech Connect

The objective of these studies is to compare transport, energy loss, and other phenomena for electrons in water in the liquid and vapor phases. Understanding the differences and similarities is an interesting physics problem in its own right. It is also important for applying the relatively large body of experimental data available for the vapor to the liquid, which is of greater relevance in radiobiology. This paper presents a summary of results from a series of collaborative studies carried out by the authors at Oak Ridge National Laboratory (ORNL) and the Gesellschaft fuer Strahlen- und Umweltforschung (GSF). 14 figs.

Turner, J.E.; Paretzke, H.G.; Wright, H.A.; Hamm, R.N.; Ritchie, R.H.

1988-01-01T23:59:59.000Z

10

Water Content in Biodiesel, Diesel, and Biodiesel–Diesel Blends  

Science Journals Connector (OSTI)

Water Content in Biodiesel, Diesel, and Biodiesel–Diesel Blends ... In what concerns road transportation, biodiesel is being considered a good alternative to conventional diesels. ...

Patricia Bogalhos Lucente Fregolente; Leonardo Vasconcelos Fregolente; Maria Regina Wolf Maciel

2012-05-17T23:59:59.000Z

11

NATURAL RADIONUCLIDES MEASUREMENTS IN DRINKING WATER BY LIQUID SCINTILLATION COUNTING. METHODS AND RESULTS  

E-Print Network (OSTI)

to dose evaluation, namely gross alpha and beta activity, uranium and radium isotopes content. For tritium activity and uranium isotope concentration have been measured. A Quantulus-Wallac scintillation counter hasNATURAL RADIONUCLIDES MEASUREMENTS IN DRINKING WATER BY LIQUID SCINTILLATION COUNTING. METHODS

12

Soil-Water Characteristic Curve Modeling at Low Water Content: Empirical and Semi-Empirical Approaches  

E-Print Network (OSTI)

Soil-Water Characteristic Curve Modeling at Low Water Content: Empirical and Semi model, the Modified Kovacs (MK) model for the determination of soil-water characteristic curve at the low water contents of two horizons of a soil from Burkina Faso. Combining terms from capillary state

Paris-Sud XI, Université de

13

Energetics of Hydrogen Bond Network Rearrangements in Liquid Water  

NLE Websites -- All DOE Office Websites (Extended Search)

Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Print Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Print The unique chemical and physical properties of liquid water are thought to result from the highly directional hydrogen bonding (H-bonding) network structure and its associated dynamics. However, despite intense experimental and theoretical scrutiny, a complete description of this structure has been elusive. Recently, with the help of their novel liquid microjet apparatus, a University of California, Berkeley, group derived a new energy criterion for H-bonds based on experimental data. With this new criterion based on analysis of the temperature dependence of the x-ray absorption spectra of normal and supercooled liquid water, they concluded that the traditional structural model of water is valid.

14

Energetics of Hydrogen Bond Network Rearrangements in Liquid Water  

NLE Websites -- All DOE Office Websites (Extended Search)

Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Print Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Print The unique chemical and physical properties of liquid water are thought to result from the highly directional hydrogen bonding (H-bonding) network structure and its associated dynamics. However, despite intense experimental and theoretical scrutiny, a complete description of this structure has been elusive. Recently, with the help of their novel liquid microjet apparatus, a University of California, Berkeley, group derived a new energy criterion for H-bonds based on experimental data. With this new criterion based on analysis of the temperature dependence of the x-ray absorption spectra of normal and supercooled liquid water, they concluded that the traditional structural model of water is valid.

15

Energetics of Hydrogen Bond Network Rearrangements in Liquid Water  

NLE Websites -- All DOE Office Websites (Extended Search)

Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Print Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Print The unique chemical and physical properties of liquid water are thought to result from the highly directional hydrogen bonding (H-bonding) network structure and its associated dynamics. However, despite intense experimental and theoretical scrutiny, a complete description of this structure has been elusive. Recently, with the help of their novel liquid microjet apparatus, a University of California, Berkeley, group derived a new energy criterion for H-bonds based on experimental data. With this new criterion based on analysis of the temperature dependence of the x-ray absorption spectra of normal and supercooled liquid water, they concluded that the traditional structural model of water is valid.

16

CONTENTS  

NLE Websites -- All DOE Office Websites (Extended Search)

CONTENTS CONTENTS Introduction ........................................................................................................3 ON THE HORIZON: Promising Research Efforts Currently Underway A Smarter Charge .........................................................................................4 Unlocking Fire Ice .........................................................................................5 CRISP Crunches Cyber Threats ....................................................................6 Gel Zeroes in on Cancer ...............................................................................7 Liquid Solvent: A Solid Solution for CO 2 .....................................................8 Real-time Grid Stability ................................................................................9

17

Interferometric tomography of fuel cells for monitoring membrane water content  

E-Print Network (OSTI)

We have developed a system that uses two 1D interferometric phase projections for reconstruction of 2D water content changes over time in situ in a proton exchange membrane (PEM) fuel cell system. By modifying the filtered ...

Waller, Laura

18

Water content and morphology of sodium chloride aerosol particles  

E-Print Network (OSTI)

to explain the H2O content. The model in which the NaCl particles contain pockets of aqueous NaCl solution was found to be most consistent with the spectroscopic observations. The relevance of salt particle morphology and water content to atmospheric aerosol...

Weis, David D.; Ewing, George E.

1999-09-20T23:59:59.000Z

19

Water an Unusual Liquid; LCLS Provides New Insights | Stanford Synchrotron  

NLE Websites -- All DOE Office Websites (Extended Search)

Water an Unusual Liquid; LCLS Provides New Insights Water an Unusual Liquid; LCLS Provides New Insights Wednesday, November 13, 2013 - 3:00pm SLAC, Redtail Hawk Conference Room 108A Anders Nilsson, SUNCAT The anomalous physical properties of water are responsible for sustaining much of life on earth; for example, water displays a higher heat capacity than common liquids and expands upon freezing. Some of these anomalous physical properties become dramatically enhanced upon supercooling below the freezing point. In particular, extrapolations of the thermal expansion coefficient, isothermal compressibility, heat capacity and correlation length can all be fitted with a power law divergence with the same apparent singularity temperature of about 228 K. Experiments on pure bulk water below about ~240 K have so far been difficult: water crystallization occurs

20

Recent content in Water Power Forum | OpenEI Community  

Open Energy Info (EERE)

Recent content in Water Power Forum Recent content in Water Power Forum Home Name Post date sort icon Type OpenEI launches new Water Power Gateway and Community Forum Graham7781 28 Mar 2013 - 15:16 Blog entry Global Marine Renewable Energy Conference (GMREC) Kch 3 Apr 2013 - 14:26 Event MHK Cost Breakdown Structure Draft Kch 9 Apr 2013 - 13:30 Document MHK LCOE Reporting Guidance Draft Ocop 18 Apr 2013 - 13:41 Document Comments on MHK Cost Reduction Pathway White Papers Alison.labonte 26 Nov 2013 - 11:43 Question 2013 projects and funding Vanessa.gregory 13 Dec 2013 - 09:12 Question Hi Vanessa-I connected wit... NickL 13 Dec 2013 - 14:38 Answer Groups Menu You must login in order to post into this group. Recent content Hi Vanessa-I connected wit... 2013 projects and funding

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


21

Extraction of ethanol from water with liquid propylene  

SciTech Connect

To separate EtOH from water by distillation requires 40 to 50 times the minimum Gibbs free energy of mixing. Also, EtOH forms an azeotrope with water, limiting the EtOH purity to 92%. These considerations have prompted investigations of solvent extraction. This paper describes the use of liquid propylene as solvent. The process application is also described. (DLC)

Victor, J.G.

1983-01-01T23:59:59.000Z

22

ARM - Evaluation Product - MWR Retrievals of Cloud Liquid Water and Water  

NLE Websites -- All DOE Office Websites (Extended Search)

ProductsMWR Retrievals of Cloud Liquid Water and ProductsMWR Retrievals of Cloud Liquid Water and Water Vapor Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Evaluation Product : MWR Retrievals of Cloud Liquid Water and Water Vapor 2005.02.01 - 2011.04.25 Site(s) FKB GRW HFE NIM PYE SBS General Description A new algorithm is being developed for the ARM Program to derive liquid water path (LWP) and precipitable water vapor (PWV) from the 2-channel (23.8 and 31.4 GHz) microwave radiometers (MWRs) deployed at ARM climate research facilities. This algorithm utilizes the "monoRTM" radiative transfer model (http://rtweb.aer.com), a combination of both an advanced statistical and physical-iterative retrieval, and brightness temperature offsets applied before the retrieval is performed. This allows perhaps the

23

Estimating the lunar mantle water budget from phosphates: Complications associated with silicate-liquid-immiscibility  

Science Journals Connector (OSTI)

Abstract The discovery of water within the lunar mantle has broad implications for the formation of the Earth–Moon system, differentiation of the Moon, and the magmatic evolution of lunar basalts, as well as the highland rocks. Recently, there has been considerable interest in using combined water abundances and H-isotope systematics of lunar apatites from mare basalts to quantify the origin and extent of water within the Moon’s mantle. However, the petrologic and geochemical conditions that govern apatite crystallization are not well-constrained, especially for high-FeO basaltic melts that crystallize at fO2 values below the iron–wüstite buffer. Apatites are typically located within the late-stage interstitial regions. In this contribution, we present detailed textural descriptions of late-stage inter-cumulus, residual-liquid pockets (i.e., mesostasis pockets), in order to understand the petrogenesis of lunar apatite. Results from five mare basalts demonstrate that the majority of the residual liquids in mesostasis regions have undergone silicate-liquid immiscibility (SLI) splitting into Si–K-rich (felsic) and Fe-rich (Fe-basaltic) conjugate liquids. We demonstrate the complexity of these residual liquids by documenting a wide range of water contents for apatites in several mesostasis pockets within a single mare basalt, a complexity common to many basalts. These data illustrate that individual apatite-hosting mesostasis pockets behave as independent sub-systems, even within a single rock. Furthermore, we present water concentrations for another phosphate phase, merrillite, indicating additional uncertainties during considerations of water partitioning into apatite. Fractional crystallization trends have been used in order to assess the conditions under which magmas are likely to undergo SLI. Predicted liquid lines of descent indicate that it is the late-stage residual liquids of lunar basalts with relatively low-Mg# (e.g., ?50) may not intersect the two-liquid field depending upon the fractionation trends in the late-stage mesostasis pockets. For samples that undergo SLI, the apatite/melt-partition coefficients required for back-calculating water abundances of the parental melts are compromised by the generation of two populations of apatites-merrillites from conjugate immiscible liquids. This process highlights an important complexity inherent to all water back-calculations that use apatite, as this requires an additional set of partition coefficients. We emphasize that the complex petrologic nature and common development of SLI of apatite-bearing, late-stage mesostasis pockets have not been considered in published apatite-volatile data. These factors, in additional to other considerations, illustrate why water back-calculations to model the primary melts from such data must be viewed with caution.

J.F. Pernet-Fisher; G.H. Howarth; Y. Liu; Y. Chen; L.A. Taylor

2014-01-01T23:59:59.000Z

24

ARM - PI Product - Large Scale Ice Water Path and 3-D Ice Water Content  

NLE Websites -- All DOE Office Websites (Extended Search)

ProductsLarge Scale Ice Water Path and 3-D Ice Water ProductsLarge Scale Ice Water Path and 3-D Ice Water Content Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send PI Product : Large Scale Ice Water Path and 3-D Ice Water Content Site(s) SGP TWP General Description Cloud ice water concentration is one of the most important, yet poorly observed, cloud properties. Developing physical parameterizations used in general circulation models through single-column modeling is one of the key foci of the ARM program. In addition to the vertical profiles of temperature, water vapor and condensed water at the model grids, large-scale horizontal advective tendencies of these variables are also required as forcing terms in the single-column models. Observed horizontal advection of condensed water has not been available because the

25

Structure and Depletion at Fluorocarbon and Hydrocarbon/Water Liquid/Liquid Interfaces  

Science Journals Connector (OSTI)

The results of x-ray reflectivity studies of two oil/water (liquid/liquid) interfaces are inconsistent with recent predictions of the presence of a vaporlike depletion region at hydrophobic/aqueous interfaces. One of the oils, perfluorohexane, is a fluorocarbon whose superhydrophobic interface with water provides a stringent test for the presence of a depletion layer. The other oil, heptane, is a hydrocarbon and, therefore, is more relevant to the study of biomolecular hydrophobicity. These results are consistent with the subangstrom proximity of water to soft hydrophobic materials.

Kaoru Kashimoto; Jaesung Yoon; Binyang Hou; Chiu-hao Chen; Binhua Lin; Makoto Aratono; Takanori Takiue; Mark L. Schlossman

2008-08-14T23:59:59.000Z

26

The Thermal Insulation Properties for Wall Material with Various Water Contents  

Science Journals Connector (OSTI)

The thermal conductivities of wall material were measured under various water contents to investigate the effect of water content on the thermal insulation properties. The results show that water contents have adverse impact to heat insulation of wall ... Keywords: the thermal conductivity, water contents, the thermal insulation properties

Zhang Chuancheng; Lu Haijun

2010-05-01T23:59:59.000Z

27

Near Surface Water Content Estimation using GPR Data  

E-Print Network (OSTI)

waves can be used to estimate soil water content � Short pulses of High frequency EM energy � Variations) Improved irrigation management; 3) Improved understanding of ecosystem responses and terroir; 4) May assist, evapotranspiration, and groundwater storage From Or and Rubin, 1990 ** Accurate Spatial and Temporal Variations

Rubin, Yoram

28

The use of a permanent magnet for water content measurements of wood chips  

E-Print Network (OSTI)

Diagram of a Wood Chip Moisture Content Measurement DeviceMeasurement of Moisture Content in Wood Chips Using NMR andWood chip water-content tests were done over a broad range of moisture contents

2001-01-01T23:59:59.000Z

29

Air-Assisted Liquid Liquid–Microextraction for the Analysis of Fungicides from Environmental Water and Juice Samples  

Science Journals Connector (OSTI)

......2014 research-article Article Air-Assisted Liquid Liquid-Microextraction...work, a rapid method based on air-assisted liquid liquid microextraction...the continuous injection of air by a 20-mL glass syringe...resulting in the possible pollution of water, fruits and vegetables......

Shiju Wu; Tingting Jin; Jing Cheng; Hongbin Zhou; Min Cheng

2014-10-01T23:59:59.000Z

30

Equation of State for Supercooled Water Near the Liquid-Liquid Critical Point  

E-Print Network (OSTI)

We have developed a scaled parametric equation of state to describe and predict thermodynamic properties of supercooled water. The equation of state, built on the growing evidence that the critical point of supercooled liquid-liquid water separation exists, is universal in terms of theoretical scaling fields and is shown to belong to the Ising-model class of universality. The theoretical scaling fields are postulated to be analytical combinations of the physical fields, pressure and temperature. The equation of state enables us to accurately locate the "Widom line" (the locus of stability minima) and determine that the critical pressure is considerably lower than predicted by computer simulations.

M. A. Anisimov; D. A. Fuentevilla

2006-09-19T23:59:59.000Z

31

An Evaluation of MWR Retrievals of Liquid Water Path  

NLE Websites -- All DOE Office Websites (Extended Search)

Evaluation of MWR Retrievals Evaluation of MWR Retrievals of Liquid Water Path and Precipitable Water Vapor R. T. Marchand and T. P. Ackerman Pacific Northwest National Laboratory Richland, Washington Introduction This paper offers some observations on the quality of Microwave Radiometer (MWR) retrievals of precipitable water vapor (PWV) and liquid water path (LWP). The paper shows case study comparisons between the standard "statistical" approach and those obtained using an iterative solution of the microwave radiative transfer equations. These examples show how improvements in the retrieval of LWP can be obtained by using an iterative approach, but that possible improvements are limited by the accuracy of the forward model absorption coefficients and errors in the brightness temperature measurements. Each of these effects limits the

32

Evaluating the phase equilibria of liquid water + natural gas mixtures using cubic equations of state with asymmetric mixing rules  

Science Journals Connector (OSTI)

Based on a previously developed liquid–liquid mixing rule we present a modified and robust mixing rule for accurate prediction of water content of natural gas mixtures and the natural gas solubility in liquid water phase. The non-density dependent mixing rule (NDD) and the new mixing rule are incorporated into the Peng–Robinson (PR), Soave–Redlich–Kwong (SRK), and Nasrifar–Bolland (NB) equations of state to investigate their accuracies in estimating the water content of the gas phase as well as the gas solubility in the aqueous phase. For each binary system water + hydrocarbon, water + carbon dioxide, water + hydrogen sulfide, and water + nitrogen, three binary interaction parameters are required to describe the gas–liquid water equilibria. In this work, experimental data from literature were used to tune the parameters. The results are in good agreement with experimental data, demonstrating the reliability of the new mixing rule and the thermodynamic approach used in this work.

P. Reshadi; Kh. Nasrifar; M. Moshfeghian

2011-01-01T23:59:59.000Z

33

Water content test for EOR crude simulates desalter  

SciTech Connect

Crude oil produced from enhanced oil recovery (EOR) projects employing micellar/polymer flooding can require an alternative test method for water content to the ASTM centrifuge test, or grindout procedure. The reason is that centrifuging cannot break the surfactant-stabilized emulsion. As an alternative, Marathon Oil Co. has developed a simulated desalter test (SDT) and necessary apparatus for the accurate evaluation of the quality of crude oil from such projects. Oil quality parameters such as basic sediment and water values are used almost universally for determining the acceptability of crude oil into pipeline or refinery systems.

Duke, R.B. (Marathon Oil Co., Littleton, CO (US))

1991-02-25T23:59:59.000Z

34

Empirical Relationships for Estimating Liquid Water Fraction of Melting Snowflakes  

Science Journals Connector (OSTI)

The liquid water fraction of individual snowflakes f is an important parameter when calculating the radar reflectivity of a melting layer. A ground-based observation of f at Nagaoka, Japan, was conducted by using dye-treated filter papers that ...

Ryohei Misumi; Hiroki Motoyoshi; Satoru Yamaguchi; Sento Nakai; Masaaki Ishizaka; Yasushi Fujiyoshi

2014-10-01T23:59:59.000Z

35

Water Calibration Measurements for Neutron Radiography: Application to Water Content Quantification in Porous Media  

SciTech Connect

Using neutron radiography, the measurement of water thickness was performed using aluminum (Al) water calibration cells at the High Flux Isotope Reactor (HFIR) Cold-Guide (CG) 1D neutron imaging facility at Oak Ridge National Laboratory, Oak Ridge, TN, USA. Calibration of water thickness is an important step to accurately measure water contents in samples of interest. Neutron attenuation by water does not vary linearly with thickness mainly due to beam hardening and scattering effects. Transmission measurements for known water thicknesses in water calibration cells allow proper correction of the underestimation of water content due to these effects. As anticipated, strong scattering effects were observed for water thicknesses greater than 2 mm when the water calibration cells were positioned close to the face of the detector / scintillator (0 and 2.4 cm away, respectively). The water calibration cells were also positioned 24 cm away from the detector face. These measurements resulted in less scattering and this position (designated as the sample position) was used for the subsequent experimental determination of the neutron attenuation coefficient for water. Neutron radiographic images of moist Flint sand in rectangular and cylindrical containers acquired at the sample position were used to demonstrate the applicability of the water calibration. Cumulative changes in the water volumes within the sand columns during monotonic drainage determined by neutron radiography were compared with those recorded by direct reading from a burette connected to a hanging water column. In general, the neutron radiography data showed very good agreement with those obtained volumetrically using the hanging water-column method. These results allow extension of the calibration equation to the quantification of unknown water contents within other samples of porous media.

Kang, Misun [ORNL; Bilheux, Hassina Z [ORNL; Voisin, Sophie [ORNL; Cheng, Chu-lin [University of Tennessee, Knoxville (UTK); Perfect, Edmund [University of Tennessee, Knoxville (UTK); Horita, Juske [Texas Tech University (TTU); Warren, Jeffrey [ORNL

2013-01-01T23:59:59.000Z

36

Elastic parameters of a water-based magnetic liquid  

SciTech Connect

The authors repeat studies on the acoustic parameters of water-based magnetic liquids to find a better method of measuring the speed and to cover a wider concentration range. The pulse method is used, as it works well in measuring the speed of sound in ordinary liquids. A figure shows the block diagram. Figures show the dependence of magnetization on field strength and temperature dependence of ultrasound. The speeds measured for the specimens show that the parameter obtained remains constant within the errors of measurement in longitudinal and transverse fields.

Berkovskii, B.M.

1986-07-01T23:59:59.000Z

37

Pore-scale simulation of liquid CO2 displacement of water using...  

NLE Websites -- All DOE Office Websites (Extended Search)

Pore-scale simulation of liquid CO2 displacement of water using a two-phase lattice Boltzmann model. Pore-scale simulation of liquid CO2 displacement of water using a two-phase...

38

ARM - PI Product - MWR Retrievals of Cloud Liquid Water and Water Vapor  

NLE Websites -- All DOE Office Websites (Extended Search)

govDataPI Data ProductsMWR Retrievals of Cloud Liquid Water and Water govDataPI Data ProductsMWR Retrievals of Cloud Liquid Water and Water Vapor Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send PI Product : MWR Retrievals of Cloud Liquid Water and Water Vapor 2005.02.01 - 2011.04.25 Site(s) FKB GRW HFE NIM PYE SBS General Description A new algorithm is being developed for the ARM Program to derive liquid water path (LWP) and precipitable water vapor (PWV) from the 2-channel (23.8 and 31.4 GHz) microwave radiometers (MWRs) deployed at ARM climate research facilities. This algorithm utilizes the "monoRTM" radiative transfer model (http://rtweb.aer.com), a combination of both an advanced statistical and physical-iterative retrieval, and brightness temperature offsets applied before the retrieval is performed. This allows perhaps the

39

Changes in Free Water Content and Energy Metabolism of the Brain in Experimental Hydrocephalus  

Science Journals Connector (OSTI)

In acute and subacute hydrocephalus periventricular oedema is most prominent. At these stages of hydrocephalus, the free water content is increased and the bound water content, to the contrary, significantly d...

N. Tamaki M.D.; T. Nagashima; K. Ehara; M. Kimura; S. Matsumoto…

1990-01-01T23:59:59.000Z

40

Liquid-Water Uptake and Removal in PEM Fuel-Cell Components  

SciTech Connect

Management of liquid water is critical for optimal fuel-cell operation, especially at low temperatures. It is therefore important to understand the wetting properties and water holdup of the various fuel-cell layers. While the gas-diffusion layer is relatively hydrophobic and exhibits a strong intermediate wettability, the catalyst layer is predominantly hydrophilic. In addition, the water content of the ionomer in the catalyst layer is lower than that of the bulk membrane, and is affected by platinum surfaces. Liquid-water removal occurs through droplets on the surface of the gas-diffusion layer. In order to predict droplet instability and detachment, a force balance is used. While the pressure or drag force on the droplet can be derived, the adhesion or surface-tension force requires measurement using a sliding-angle approach. It is shown that droplets produced by forcing water through the gas-diffusion layer rather than placing them on top of it show much stronger adhesion forces owing to the contact to the subsurface water.

Das, Prodip K.; Gunterman, Haluna P.; Kwong, Anthony; Weber, Adam Z.

2011-09-23T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


41

Effects of liquid pore water on acoustic wave propagation in snow as a Biot-type porous material  

E-Print Network (OSTI)

A method to estimate phase velocity and attenuation of acoustic waves in the presence of liquid water in a snowpack is presented. The method is based on Biot's theory of wave propagation in porous materials. Empirical relations and a priori information is used to characterize snow as a porous material as a function of porosity. Plane wave theory and an equivalent pore fluid are used to solve Biot's differential equations and to asses the impact of the air and water in the pore space. The liquid water in the pore space of a snow pack reduces the velocity of the first compressional wave by roughly 300 m/s for every 0.1 increase in liquid water saturation. Also the attenuation of the compressional waves is increased with increasing liquid water content. Two end member models for compaction are evaluated to asses the importance of an independent density measurement for an estimate of liquid pore water saturation in snow with acoustic waves. The two end members correspond to no compaction at all and to a melting s...

Sidler, Rolf

2015-01-01T23:59:59.000Z

42

Gas-Liquid Coexistence in the Primitive Model for Water  

E-Print Network (OSTI)

We evaluate the location of the gas-liquid coexistence line and of the associated critical point for the primitive model for water (PMW), introduced by Kolafa and Nezbeda [J. Kolafa and I. Nezbeda, Mol. Phys. 61, 161 (1987)]. Besides being a simple model for a molecular network forming liquid, the PMW is representative of patchy proteins and novel colloidal particles interacting with localized directional short-range attractions. We show that the gas-liquid phase separation is metastable, i.e. it takes place in the region of the phase diagram where the crystal phase is thermodynamically favored, as in the case of articles interacting via short-range attractive spherical potentials. Differently from spherical potentials, we do not observe crystallization close to the critical point. The region of gas-liquid instability of this patchy model is significantly reduced as compared to equivalent models of spherically interacting particles, confirming the possibility of observing kinetic arrest in an homogeneous sample driven by bonding as opposed to packing.

F. Romano; P. Tartaglia; F. Sciortino

2007-05-08T23:59:59.000Z

43

Spin states of para-water and ortho-water molecule in gas and liquid phases  

E-Print Network (OSTI)

Spin degrees of freedom of water molecule in gas and liquid state were investigated in order to provide a reasonable answer about the unsolved problem of a long-term behavior of water spin isomers. The approach used involves an assumption that molecules change their spin state from a pure state to a mixed one when they interact with some sorts of adsorbent surface. Some models and conceptions of the quantum information processing were used.

V. K. Konyukhov

2009-09-23T23:59:59.000Z

44

Treatment of Liquid Radioactive Waste with High Salt Content by Colloidal Adsorbents - 13274  

SciTech Connect

Treatment processes have been fully developed for most of the liquid radioactive wastes generated during the operation of nuclear power plants. However, a process for radioactive liquid waste with high salt content, such as waste seawater generated from the unexpected accident at nuclear power station, has not been studied extensively. In this study, the adsorption efficiencies of cesium (Cs) and strontium (Sr) in radioactive liquid waste with high salt content were investigated using several types of zeolite with different particle sizes. Synthesized and commercial zeolites were used for the treatment of simulated seawater containing Cs and Sr, and the reaction kinetics and adsorption capacities of colloidal zeolites were compared with those of bulk zeolites. The experimental results demonstrated that the colloidal adsorbents showed fast adsorption kinetic and high binding capacity for Cs and Sr. Also, the colloidal zeolites could be successfully applied to the static adsorption condition, therefore, an economical benefit might be expected in an actual processes where stirring is not achievable. (authors)

Lee, Keun-Young; Chung, Dong-Yong; Kim, Kwang-Wook; Lee, Eil-Hee; Moon, Jei-Kwon [Korea Atomic Energy Research Institute - KAERI, 989-111 Daedeok-daero, Yuseong-gu, Daejeon, 305-353 (Korea, Republic of)] [Korea Atomic Energy Research Institute - KAERI, 989-111 Daedeok-daero, Yuseong-gu, Daejeon, 305-353 (Korea, Republic of)

2013-07-01T23:59:59.000Z

45

Distribution of binding energies of a water molecule in the water liquid-vapor interface  

SciTech Connect

Distributions of binding energies of a water molecule in the water liquid-vapor interface are obtained on the basis of molecular simulation with the SPC/E model of water. These binding energies together with the observed interfacial density profile are used to test a minimally conditioned Gaussian quasi-chemical statistical thermodynamic theory. Binding energy distributions for water molecules in that interfacial region clearly exhibit a composite structure. A minimally conditioned Gaussian quasi-chemical model that is accurate for the free energy of bulk liquid water breaks down for water molecules in the liquid-vapor interfacial region. This breakdown is associated with the fact that this minimally conditioned Gaussian model would be inaccurate for the statistical thermodynamics of a dilute gas. Aggressive conditioning greatly improves the performance of that Gaussian quasi-chemical model. The analogy between the Gaussian quasi-chemical model and dielectric models of hydration free energies suggests that naive dielectric models without the conditioning features of quasi-chemical theory will be unreliable for these interfacial problems. Multi-Gaussian models that address the composite nature of the binding energy distributions observed in the interfacial region might provide a mechanism for correcting dielectric models for practical applications.

Chempath, Shaji [Los Alamos National Laboratory; Pratt, Lawrence R [TULANE UNIV

2008-01-01T23:59:59.000Z

46

Does Water Content or Flow Rate Control Colloid Transport in Unsaturated Porous Media?  

SciTech Connect

Mobile colloids can play an important role in contaminant transport in soils: many contaminants exist in colloidal form, and colloids can facilitate transport of otherwise immobile contaminants. In unsaturated soils, colloid transport is, among other factors, affected by water content and flow rate. Our objective was to determine whether water content or flow rate is more important for colloid transport. We passed negatively charged polystyrene colloids (220 nm diameter) through unsaturated sand-filled columns under steady-state flow at different water contents (effective water saturations Se ranging from 0.1 to 1.0, with Se = (? – ?r)/(?s – ?r)) and flow rates (pore water velocities v of 5 and 10 cm/min). Water content was the dominant factor in our experiments. Colloid transport decreased with decreasing water content, and below a critical water content (Se < 0.1), colloid transport was inhibited, and colloids were strained in water films. Pendular ring and water film thickness calculations indicated that colloids can move only when pendular rings are interconnected. The flow rate affected retention of colloids in the secondary energy minimum, with less colloids being trapped when the flow rate increased. These results confirm the importance of both water content and flow rate for colloid transport in unsaturated porous media and highlight the dominant role of water content.

Thorsten Knappenberger; Markus Flury; Earl D. Mattson; James B. Harsh

2014-03-01T23:59:59.000Z

47

Combustion of Nano-Aluminum and Liquid Water G.A. Risha, S.F. Son  

E-Print Network (OSTI)

1 Combustion of Nano-Aluminum and Liquid Water G.A. Risha, S.F. Son , R.A. Yetter, V. Yang, and B: Supplemental materials submitted #12;2 Combustion of Nano-Aluminum and Liquid Water G.A. Risha, S.F. Son, R of nano-aluminum (nAl) and liquid water has been conducted. In particular, linear and mass-burning rates

Yang, Vigor

48

Field-scale estimation of volumetric water content using ground-penetrating radar ground wave techniques  

E-Print Network (OSTI)

sampling, time domain reflectometry (TDR), neutron probe logging, and tensiometers [Prichard, 1999 were compared to gravimetric water content, time domain reflectometry, and soil texture measurements

Hubbard, Susan

49

STABILIZATION OF THE NITRITE CONTENT OF SEA WATER BY ...  

Science Journals Connector (OSTI)

Figure 2 shows the ZG5 content of 11 samples of ... However, the ZnC” content of both salps. ( collected before ... Uses of Atomic Energy, 18: 434-438. MURTHY ...

1999-12-23T23:59:59.000Z

50

Detachment of Liquid-Water Droplets from Gas-Diffusion Layers  

E-Print Network (OSTI)

PEMFC cathode where liquid-water is produced in the catalystcathode side of the PEMFC, causing less oxygen to reach the active catalyst

Das, Prodip K.

2013-01-01T23:59:59.000Z

51

Detachment of Liquid-Water Droplets from Gas-Diffusion Layers  

SciTech Connect

A critical issue for optimal water management in proton-exchange-membrane fuel cells at lower temperatures is the removal of liquid water from the cell. This pathway is intimately linked with the phenomena of liquid-water droplet removal from surface of the gas-diffusion layer and into the flow channel. Thus, a good understanding of liquid-water transport and droplet growth and detachment from the gas-diffusion layer is critical. In this study, liquid-water droplet growth and detachment on the gas-diffusion layer surfaces are investigated experimentally to improve the understating of water transport through and removal from gas-diffusion layers. An experiment using a sliding-angle measurement is designed and used to quantify and directly measure the adhesion force for liquid-water droplets, and to understand the droplets? growth and detachment from the gas-diffusion layers.

Das, Prodip K.; Grippin, Adam; Weber, Adam Z.

2011-07-01T23:59:59.000Z

52

A Content Validity Study of the Water Training Institute Curriculum.  

E-Print Network (OSTI)

??Content validity methods, such as matching matrices, have been used to assist in the design and evaluation of training programs. In the present study, the… (more)

Turner, Alicia

2010-01-01T23:59:59.000Z

53

The influence of changes in water content on the electrical resistivity of a natural unsaturated loess  

E-Print Network (OSTI)

1 The influence of changes in water content on the electrical resistivity of a natural unsaturated these methods, the measurements based on the electrical resistivity are simple and reliable thanks to the clear relationship between the water content and the electrical resistivity of soils. In this work, a new electrical

Paris-Sud XI, Université de

54

Characterization of Soil Water Content Variability and Soil Texture using GPR Groundwave Techniques  

E-Print Network (OSTI)

measurements. Precipitation and irrigation were both shown to increase the spatial variability of water content the soil water content is well character- ized across a field. In addition to crop yield, the quality JEEG, September 2010, Volume 15, Issue 3, pp. 93­110 #12;of some crops, such as wine grapes, partially

Hubbard, Susan

55

Drop Simulation of 6M Drum with Locking-Ring Closure and Liquid Contents  

SciTech Connect

This paper presents the dynamic simulation of the 6M drum with a locking-ring type closure subjected to a 4.9-foot drop. The drum is filled with water to 98 percent of overflow capacity. A three dimensional finite-element model consisting of metallic, liquid and rubber gasket components is used in the simulation. The water is represented by a hydrodynamic material model in which the material's volume strength is determined by an equation of state. The explicit numerical method based on the theory of wave propagation is used to determine the combined structural response to the torque load for tightening the locking-ring closure and to the impact load due to the drop.

Wu, T

2006-04-17T23:59:59.000Z

56

Probing Liquid Water Saturation in Diffusion Media of Polymer Electrolyte Fuel Cells  

E-Print Network (OSTI)

of information strongly needed to characterize the level of cathode DM flooding or anode dry-out. In this paper liquid water in the anode DM for the thin membrane case. In addition, the two-phase simulation results be realized. One of these is related to flooding phenomena. Due to the presence of liquid water inside a PEFC

57

Estimating the Atmospheric Water Vapor Content from Sun Photometer Measurements  

Science Journals Connector (OSTI)

The differential absorption technique for estimating columnar water vapor values from the analysis of sunphotometric measurements with wide- and narrowband interferential filters centered near 0.94 ?m is discussed and adapted. Water vapor line ...

Artemio Plana-Fattori; Michel Legrand; Didier Tanré; Claude Devaux; Anne Vermeulen; Philippe Dubuisson

1998-08-01T23:59:59.000Z

58

Water content of 1997 vulcanian pumices at Soufriere Hills Volcano (Montserrat) and implications on pre-eruptive conduit conditions  

E-Print Network (OSTI)

Water content of 1997 vulcanian pumices at Soufriere Hills Volcano (Montserrat) and implications of the eruptive products. We used quantitative analysis of water content in residual glasses (matrix glass. To better link water content to structural level, we performed new water solubility experiments at low

Paris-Sud XI, Université de

59

Liquid-liquid phase transition model incorporating evidence for ferroelectric state near the lambda-point anomaly in supercooled water  

E-Print Network (OSTI)

We propose a unified model combining the first-order liquid-liquid and the second-order ferroelectric phase transitions models and explaining various features of the $\\lambda$-point of liquid water within a single theoretical framework. It becomes clear within the proposed model that not only does the long-range dipole-dipole interaction of water molecules yield a large value of dielectric constant $\\epsilon$ at room temperatures, our analysis shows that the large dipole moment of the water molecules also leads to a ferroelectric phase transition at a temperature close to the lambda-point. Our more refined model suggests that the phase transition occurs only in the low density component of the liquid and is the origin of the singularity of the dielectric constant recently observed in experiments with supercooled liquid water at temperature T~233K. This combined model agrees well with nearly every available set of experiments and explains most of the well-known and even recently obtained results of MD simulations.

Peter O. Fedichev; Leonid I. Menshikov

2012-01-30T23:59:59.000Z

60

Water-saving liquid-gas conditioning system  

DOE Patents (OSTI)

A method for treating a process gas with a liquid comprises contacting a process gas with a hygroscopic working fluid in order to remove a constituent from the process gas. A system for treating a process gas with a liquid comprises a hygroscopic working fluid comprising a component adapted to absorb or react with a constituent of a process gas, and a liquid-gas contactor for contacting the working fluid and the process gas, wherein the constituent is removed from the process gas within the liquid-gas contactor.

Martin, Christopher; Zhuang, Ye

2014-01-14T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


61

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays  

NLE Websites -- All DOE Office Websites (Extended Search)

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print The geometric structure of liquid water has been investigated in detail by many techniques, but many details are still under debate, such as the actual number of hydrogen bonds (at a given time) between the various water molecules. Even less is known about the electronic structure. Since it is the intermittent bonding between water molecules that gives liquid water its peculiar characteristics, the electronic structure plays a crucial role in understanding the properties of the liquid state. Consequently, information essential for insight into chemical and biological processes in aqueous environments is lacking. To address this need, researchers from Germany and the U.S. have used soft x-ray spectroscopy at the ALS to gain detailed insight into the electronic structure of liquid water. Their spectra show a strong isotope and a weak temperature effect, and, for the first time, a splitting of the primary emission line in x-ray emission spectra. By making use of the internal "femtosecond clock" of the core-hole lifetime, a detailed picture of the electronic structure can be painted that involves fast dissociation processes of the probed water molecules.

62

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays  

NLE Websites -- All DOE Office Websites (Extended Search)

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print The geometric structure of liquid water has been investigated in detail by many techniques, but many details are still under debate, such as the actual number of hydrogen bonds (at a given time) between the various water molecules. Even less is known about the electronic structure. Since it is the intermittent bonding between water molecules that gives liquid water its peculiar characteristics, the electronic structure plays a crucial role in understanding the properties of the liquid state. Consequently, information essential for insight into chemical and biological processes in aqueous environments is lacking. To address this need, researchers from Germany and the U.S. have used soft x-ray spectroscopy at the ALS to gain detailed insight into the electronic structure of liquid water. Their spectra show a strong isotope and a weak temperature effect, and, for the first time, a splitting of the primary emission line in x-ray emission spectra. By making use of the internal "femtosecond clock" of the core-hole lifetime, a detailed picture of the electronic structure can be painted that involves fast dissociation processes of the probed water molecules.

63

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays  

NLE Websites -- All DOE Office Websites (Extended Search)

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print The geometric structure of liquid water has been investigated in detail by many techniques, but many details are still under debate, such as the actual number of hydrogen bonds (at a given time) between the various water molecules. Even less is known about the electronic structure. Since it is the intermittent bonding between water molecules that gives liquid water its peculiar characteristics, the electronic structure plays a crucial role in understanding the properties of the liquid state. Consequently, information essential for insight into chemical and biological processes in aqueous environments is lacking. To address this need, researchers from Germany and the U.S. have used soft x-ray spectroscopy at the ALS to gain detailed insight into the electronic structure of liquid water. Their spectra show a strong isotope and a weak temperature effect, and, for the first time, a splitting of the primary emission line in x-ray emission spectra. By making use of the internal "femtosecond clock" of the core-hole lifetime, a detailed picture of the electronic structure can be painted that involves fast dissociation processes of the probed water molecules.

64

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays  

NLE Websites -- All DOE Office Websites (Extended Search)

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print The geometric structure of liquid water has been investigated in detail by many techniques, but many details are still under debate, such as the actual number of hydrogen bonds (at a given time) between the various water molecules. Even less is known about the electronic structure. Since it is the intermittent bonding between water molecules that gives liquid water its peculiar characteristics, the electronic structure plays a crucial role in understanding the properties of the liquid state. Consequently, information essential for insight into chemical and biological processes in aqueous environments is lacking. To address this need, researchers from Germany and the U.S. have used soft x-ray spectroscopy at the ALS to gain detailed insight into the electronic structure of liquid water. Their spectra show a strong isotope and a weak temperature effect, and, for the first time, a splitting of the primary emission line in x-ray emission spectra. By making use of the internal "femtosecond clock" of the core-hole lifetime, a detailed picture of the electronic structure can be painted that involves fast dissociation processes of the probed water molecules.

65

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays  

NLE Websites -- All DOE Office Websites (Extended Search)

Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print Isotope and Temperature Effects in Liquid Water Probed by Soft X Rays Print The geometric structure of liquid water has been investigated in detail by many techniques, but many details are still under debate, such as the actual number of hydrogen bonds (at a given time) between the various water molecules. Even less is known about the electronic structure. Since it is the intermittent bonding between water molecules that gives liquid water its peculiar characteristics, the electronic structure plays a crucial role in understanding the properties of the liquid state. Consequently, information essential for insight into chemical and biological processes in aqueous environments is lacking. To address this need, researchers from Germany and the U.S. have used soft x-ray spectroscopy at the ALS to gain detailed insight into the electronic structure of liquid water. Their spectra show a strong isotope and a weak temperature effect, and, for the first time, a splitting of the primary emission line in x-ray emission spectra. By making use of the internal "femtosecond clock" of the core-hole lifetime, a detailed picture of the electronic structure can be painted that involves fast dissociation processes of the probed water molecules.

66

High-Resolution Estimation of Near-Subsurface Water Content using Surface GPR Ground Wave Information  

E-Print Network (OSTI)

-scarce agricultural areas. Conventional measurements of water content (such as from time domain reflectometry [TDR], neutron probe or gravimetric techniques) are intrusive and provide information at a 'point' scale, which

Rubin, Yoram

67

The use of a permanent magnet for water content measurements ofwood chips  

SciTech Connect

The Lawrence Berkeley National Laboratory has developed a device that measures the water content of wood chips, pulp and brown stock for the paper industry. This device employs a permanent magnet as the central part of a NMR measurement system. This report describes the magnet and the NMR measurement system. The results of water content measurements in wood chips in a magnetic field of 0.47 T are presented.

Barale, P.J.; Fong, C.G.; Green, M.A.; Luft, P.A.; McInturff,A.D.; Reimer, J.A.; Yahnke, M.

2001-09-20T23:59:59.000Z

68

Effect of Upgraded Lignite Product Water Content on the Propensity for Spontaneous Ignition  

Science Journals Connector (OSTI)

At the end of 2005, worldwide lignite reserves were 207.4 billion tons and accounted for 17.7% of total coal. ... Therefore, there is still considerable interest in the propensity for spontaneous ignition of upgraded lignites products with different moisture contents and also the recommended water content for upgraded lignite products. ...

Kai Zhang; Changfu You

2012-12-11T23:59:59.000Z

69

CONTENTS  

NLE Websites -- All DOE Office Websites (Extended Search)

Operations Office RPD relative percent difference RSD relative standard deviation TIC tentatively identified compound DOERL-96-68, HASQARD Table of Contents, Rev. 3 Volume...

70

CONTENTS  

NLE Websites -- All DOE Office Websites (Extended Search)

3.0 - CRITICAL, SPECIAL, & ENGINEERED LIFTS March 21, 2013 Rev 1 Page 1 CHAPTER 3.0 TABLE OF CONTENTS 3.0 CRITICAL LIFTS ......

71

CONTENTS  

NLE Websites -- All DOE Office Websites (Extended Search)

assurancecontrol) 3. Responsible operations manager 4. Equipment custodian 5. Cognizant engineer. *Reviewapproval is mandatory. 18.3.3 Hostile Environment Plan Contents The plan...

72

A Review Of Water Contents Of Nominally Anhydrous Natural Minerals In The  

Open Energy Info (EERE)

A Review Of Water Contents Of Nominally Anhydrous Natural Minerals In The A Review Of Water Contents Of Nominally Anhydrous Natural Minerals In The Mantles Of Earth, Mars And The Moon Jump to: navigation, search GEOTHERMAL ENERGYGeothermal Home Journal Article: A Review Of Water Contents Of Nominally Anhydrous Natural Minerals In The Mantles Of Earth, Mars And The Moon Details Activities (0) Areas (0) Regions (0) Abstract: Olivine, pyroxene and garnet are nominally anhydrous but can accommodate tens to hundreds of parts per million (ppm) H2O or "water" in the form of protons incorporated in defects in their mineral structure. This review concerns the amount of water in nominally anhydrous minerals from mantle and mantle-derived rocks: peridotites, eclogites, megacrysts, basalts and kimberlites. Trends between internal and external parameters

73

Ultrafast, Unimpeded Liquid Water Transport Through Graphene-Based Nanochannels Measured by Isotope Labelling  

E-Print Network (OSTI)

Graphene-based laminates, with ultralong and tortuous nanocapillaries formed by simply stacking graphene flakes together, have great promises in filtration and separation. However, the information on liquid water trans-membrane permeation is lacking, which is the most fundamental problem and of crucial importance in solution-based mass transport. Here, based on isotope labelling, we investigate the liquid water transportation through graphene-based nanocapillaries under no external hydrostatic pressures. Liquid water can afford an unimpeded permeation through graphene-based nanochannels with a diffusion coefficient 4~5 orders of magnitude larger than through sub-micrometer-sized polymeric channels. When dissolving ions in sources, the diffusion coefficient of ions through graphene channels lies in the same order of magnitude as water, while the ion diffusion is faster than water, indicating that the ions are mainly transported by fast water flows and the delicate interactions between ions and nanocapillary wa...

Sun, Pengzhan; Wang, Kunlin; Zhong, Minlin; Wu, Dehai; Zhu, Hongwei

2014-01-01T23:59:59.000Z

74

Volatile liquid hydrocarbon characterization of underwater hydrocarbon vents and formation waters from offshore production operations  

Science Journals Connector (OSTI)

Volatile liquid hydrocarbon characterization of underwater hydrocarbon vents and formation waters from offshore production operations ... The environmental implications of offshore oil and gas activities ... The environmental implications of offshore oil and gas activities ...

Theodor C. Sauer

1981-08-01T23:59:59.000Z

75

The Near Infrared Absorption Band of Liquid Water at 1.79?  

Science Journals Connector (OSTI)

The near infrared absorption band of liquid water at 1.79? has been studied at various temperatures. No apparent changes in the band were detected in the temperature range from 4°C to 137°C.

J. R. Collins

1937-07-15T23:59:59.000Z

76

Ab initio calculation of the electronic absorption spectrum of liquid water  

SciTech Connect

The electronic absorption spectrum of liquid water was investigated by coupling a one-body energy decomposition scheme to configurations generated by classical and Born-Oppenheimer Molecular Dynamics (BOMD). A Frenkel exciton Hamiltonian formalism was adopted and the excitation energies in the liquid phase were calculated with the equation of motion coupled cluster with single and double excitations method. Molecular dynamics configurations were generated by different approaches. Classical MD were carried out with the TIP4P-Ew and AMOEBA force fields. The BLYP and BLYP-D3 exchange-correlation functionals were used in BOMD. Theoretical and experimental results for the electronic absorption spectrum of liquid water are in good agreement. Emphasis is placed on the relationship between the structure of liquid water predicted by the different models and the electronic absorption spectrum. The theoretical gas to liquid phase blue-shift of the peak positions of the electronic absorption spectrum is in good agreement with experiment. The overall shift is determined by a competition between the O–H stretching of the water monomer in liquid water that leads to a red-shift and polarization effects that induce a blue-shift. The results illustrate the importance of coupling many-body energy decomposition schemes to molecular dynamics configurations to carry out ab initio calculations of the electronic properties in liquid phase.

Martiniano, Hugo F. M. C.; Galamba, Nuno [Grupo de Física Matemática da Universidade de Lisboa, Av. Professor Gama Pinto 2, 1649-003 Lisboa (Portugal)] [Grupo de Física Matemática da Universidade de Lisboa, Av. Professor Gama Pinto 2, 1649-003 Lisboa (Portugal); Cabral, Benedito J. Costa, E-mail: ben@cii.fc.ul.pt [Grupo de Física Matemática da Universidade de Lisboa, Av. Professor Gama Pinto 2, 1649-003 Lisboa (Portugal) [Grupo de Física Matemática da Universidade de Lisboa, Av. Professor Gama Pinto 2, 1649-003 Lisboa (Portugal); Departamento de Química e Bioquímica, Faculdade de Ciências, Universidade de Lisboa, 1749-016 Lisboa (Portugal); Instituto de Física da Universidade de São Paulo, CP 66318, 05314-970 São Paulo, SP (Brazil)

2014-04-28T23:59:59.000Z

77

Nuclear tanker producing liquid fuels from air and water  

E-Print Network (OSTI)

Emerging technologies in CO? air capture, high temperature electrolysis, microchannel catalytic conversion, and Generation IV reactor plant systems have the potential to create a shipboard liquid fuel production system ...

Galle-Bishop, John Michael

2011-01-01T23:59:59.000Z

78

Analysing chromatographic data using data mining to monitor petroleum content in water  

E-Print Network (OSTI)

Analysing chromatographic data using data mining to monitor petroleum content in water Geoffrey the concentrations of petroleum compounds in water samples. Experiments demonstrate that the framework can be used, New Zealand. Abstract Chromatography is an important analytical technique that has wide- spread use

Frank, Eibe

79

Non-invasive field measurements of soil water content using a pulsed 14 MeV neutron generator  

E-Print Network (OSTI)

Non-invasive field measurements of soil water content using a pulsed 14 MeV neutron generator S to the atmosphere. Soil water sensors routinely are used in applications such as research on crop production, water-3120, United States 1. Introduction Knowledge of soil water content is critical to agricultural, hydrological

Johnson, Peter D.

80

Nuclear quantum effects in liquid water from an ab initio force matching approach  

E-Print Network (OSTI)

We have applied path integral simulations, in combination with new ab initio based water potentials, to investigate nuclear quantum effects in liquid water. Because direct ab initio path integral simulations are computationally expensive, a flexible water model is parameterized by force-matching to density functional theory-based molecular dynamics simulations. The resulting effective potentials provide an inexpensive replacement for direct \\textit{ab inito} molecular dynamics simulations and furthermore allow an efficient simulation of nuclear quantum effects. Static and dynamic properties of liquid water at ambient conditions are presented and the role of nuclear quantum effects, exchange-correlation functionals and dispersion corrections are discussed in regards to reproducing the experimental properties of liquid water.

Spura, Thomas; Habershon, Scott; Kühne, Thomas D

2014-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


81

Drought stress influences leaf water content, photosynthesis, and water-use efficiency of Hibiscus rosa-sinensis at three potassium concentrations  

Science Journals Connector (OSTI)

The influence of drought stress (DS) upon whole-plant water content, water relations, photosynthesis, and water-use efficiency of Hibiscus rosa-sinensis cv. Leprechaun (Hibiscus...) plants at three levels of pota...

J. N. Egilla; F. T. Davies Jr.; T. W. Boutton

82

Simultaneous liquid–liquid and vapour–liquid equilibria predictions of selected oxygenated aromatic molecules in mixtures with alkanes, alcohols, water, using the polar GC-PC-SAFT  

Science Journals Connector (OSTI)

Abstract Phase equilibria of oxygen-bearing aromatic compounds, hydrocarbons and water mixtures are of essential interest in many processes using feeds originating from biomass. The strong non-ideal thermodynamic behavior of these systems sometimes results in immiscibility with both water and alkanes. To address this problem, the GC-PPC-SAFT equation of state [Tamouza et al., 2004; Nguyen-Huynh et al., 2008a] is extended to some selected components: phenol, alkyl-phenols, alkyl-benzoates, benzaldehyde and anisole. However, as in these multifunctional compounds, the proximity of polar functional groups may result in a lack of transferability of the parameters from the monofunctional homologous species, some parameters have been adapted in view of physical arguments. Next, liquid–vapour and liquid–liquid equilibria of mixtures with n-alkanes were evaluated, using a predictive method for the binary interaction parameters (kij) [Nguyen-Huynh et al., 2008b]. Finally, mixtures with other associating compounds, as alcohols and water have also been considered. In all cases, both correlations and predictions are qualitatively and quantitatively satisfactory. The relative deviations obtained on bubble pressure of vapor–liquid equilibria are 4–8%, that is comparable to those obtained on previously investigated systems.

Nguyen-Huynh Dong; de Hemptinne Jean-Charles; Lugo Rafael; Passarello Jean-Philippe; Tobaly Pascal

2014-01-01T23:59:59.000Z

83

A liquid water management strategy for PEM fuel cell stacks  

E-Print Network (OSTI)

Gas and water management are key to achieving good performance from a PEM fuel cell stack. Previous experimentation had found, and this experimentation confirms, that one very effective method of achieving proper gas and water management is the use...

Van Nguyen, Trung; Knobbe, M. W.

2003-02-25T23:59:59.000Z

84

Determination of triclosan and triclocarban in environmental water samples with ionic liquid/ionic liquid dispersive liquid-liquid microextraction prior to HPLC-ESI-MS/MS  

Science Journals Connector (OSTI)

A hydrophobic ionic liquid was finely dispersed in aqueous solution along with a hydrophilic ionic liquid. Following centrifugation, the two phases aggregate to form relatively large droplets. Based on this pheno...

Ru-Song Zhao; Xia Wang; Jing Sun; Cong Hu; Xi-Kui Wang

2011-07-01T23:59:59.000Z

85

Liquid Water Dynamics in a Model Polymer Electrolyte Fuel Cell Flow Channel  

E-Print Network (OSTI)

Liquid Water Dynamics in a Model Polymer Electrolyte Fuel Cell Flow Channel by Chris Miller in a Model Polymer Electrolyte Fuel Cell Flow Channel by Chris Miller Bachelors of Engineering, University in a polymer electrolyte fuel cell is a critical issue in ensuring high cell performance. The water production

Victoria, University of

86

Mesoscopic modeling of liquid water transport in polymer electrolyte fuel cells  

SciTech Connect

A key performance limitation in polymer electrolyte fuel cells (PEFC), manifested in terms of mass transport loss, originates from liquid water transport and resulting flooding phenomena in the constituent components. Liquid water leads to the coverage of the electrochemically active sites in the catalyst layer (CL) rendering reduced catalytic activity and blockage of the available pore space in the porous CL and fibrous gas diffusion layer (GDL) resulting in hindered oxygen transport to the active reaction sites. The cathode CL and the GDL therefore playa major role in the mass transport loss and hence in the water management of a PEFC. In this article, we present the development of a mesoscopic modeling formalism coupled with realistic microstructural delineation to study the profound influence of the pore structure and surface wettability on liquid water transport and interfacial dynamics in the PEFC catalyst layer and gas diffusion layer.

Mukherjee, Partha P [Los Alamos National Laboratory; Wang, Chao Yang [PENNSTATE UNIV.

2008-01-01T23:59:59.000Z

87

Short-range precipitation forecasts using assimilation of simulated satellite water vapor profiles and column cloud liquid water amounts  

SciTech Connect

These observing system simulation experiments investigate the assimilation of satellite-observed water vapor and cloud liquid water data in the initialization of a limited-area primitive equations model with the goal of improving short-range precipitation forecasts. The assimilation procedure presented includes two aspects: specification of an initial cloud liquid water vertical distribution and diabatic initialization. The satellite data is simulated for the next generation of polar-orbiting satellite instruments, the Advanced Microwave Sounding Unit (AMSU) and the High-Resolution Infrared Sounder (HIRS), which are scheduled to be launched on the NOAA-K satellite in the mid-1990s. Based on cloud-top height and total column cloud liquid water amounts simulated for satellite data a diagnostic method is used to specify an initial cloud water vertical distribution and to modify the initial moisture distribution in cloudy areas. Using a diabatic initialization procedure, the associated latent heating profiles are directly assimilated into the numerical model. The initial heating is estimated by time averaging the latent heat release from convective and large-scale condensation during the early forecast stage after insertion of satellite-observed temperature, water vapor, and cloud water formation.

Wu, X.; Diak, G.R.; Hayden, C.M.; Young, J.A. [Univ. of Wisconsin, Madison, WI (United States)] [Univ. of Wisconsin, Madison, WI (United States)

1995-02-01T23:59:59.000Z

88

Integration of Global Positioning System and Scanning Water Vapor Radiometers for Precipitable Water Vapor and Cloud Liquid Path Estimates  

NLE Websites -- All DOE Office Websites (Extended Search)

Integration of Global Positioning System and Scanning Integration of Global Positioning System and Scanning Water Vapor Radiometers for Precipitable Water Vapor and Cloud Liquid Path Estimates V. Mattioli and P. Basili Department of Electronic and Information Engineering University of Perugia Perugia, Italy E. R. Westwater Cooperative Institute for Research in Environmental Sciences University of Colorado National Oceanic and Atmospheric Administration Environmental Technology Laboratory Boulder, Colorado Introduction In recent years the Global Positioning System (GPS) has proved to be a reliable instrument for measuring precipitable water vapor (PWV) (Bevis et al. 1992), offering an independent source of information on water vapor when compared with microwave radiometers (MWRs), and/or radiosonde

89

TECHNICAL NOTES Long-Term Behavior of Water Content and Density  

E-Print Network (OSTI)

in Champaign, Ill. in 1987. A pond of water 0.31 m deep was maintained on top of the 7.3 m X 14.6 m X 0.9 mTECHNICAL NOTES Long-Term Behavior of Water Content and Density in an Earthen Liner Timothy E thick liner for 14 years. One of the goals of the project was to evaluate the long-term performance

90

Equations Governing Space-Time Variability of Liquid Water Path in Stratus Clouds  

NLE Websites -- All DOE Office Websites (Extended Search)

Equations Governing Space-Time Variability of Equations Governing Space-Time Variability of Liquid Water Path in Stratus Clouds K. Ivanova Pennsylvania State University University Park, Pennsylvania T. P. Ackerman Pacific Northwest National Laboratory Richland, Washington M. Ausloos University of Liège B-4000 Liège, Belgium Abstract We present a method on how to derive an underlying mathematical (statistical or model free) equation for a liquid water path (LWP) signal directly from empirical data. The evolution of the probability density functions (PDFs) from small to large time scales is explicitly derived in the framework of Fokker-Planck equation. A drift and a diffusion term describing the deterministic and stochastic influences on the non-Gaussian fat tails of the liquid water probability distributions are obtained from

91

The existence of supercooled liquid water at 150?K  

Science Journals Connector (OSTI)

... previously. The growth conditions used here produce optically flat non-porous water films,. A roughened interface between the isotopic layers, which in the worst case would result in intermixing ...

R. Scott Smith; Bruce D. Kay

1999-04-29T23:59:59.000Z

92

Gas-liquid-liquid equilibria in mixtures of water, light gases, and hydrocarbons  

SciTech Connect

Phase equilibrium in mixtures of water + light gases and water + heavy hydrocarbons has been investigated with the development of new local composition theory, new equations of state, and new experimental data. The preferential segregation and orientation of molecules due to different energies of molecular interaction has been simulated with square well molecules. Extensive simulation has been made for pure square well fluids and mixtures to find the local composition at wide ranges of states. A theory of local composition has been developed and an equation of state has been obtained for square well fluids. The new local composition theory has been embedded in several equations of state. The pressure of water is decoupled into a polar pressure and non-polar pressure according to the molecular model of water of Jorgensen et al. The polar pressure of water is combined with the BACK equation for the general description of polar fluids and their mixtures. Being derived from the steam table, the Augmented BACK equation is particularly suited for mixtures of water + non-polar substances such as the hydrocarbons. The hydrophobic character of the hydrocarbons had made their mixtures with water a special challenge. A new group contribution equation of state is developed to describe phase equilibrium and volumetric behavior of fluids while requiring only to know the molecular structure of the components. 15 refs., 1 fig.

Chao, K.C.

1990-01-01T23:59:59.000Z

93

Heating-induced glass-glass and glass-liquid transformations in computer simulations of water  

SciTech Connect

Water exists in at least two families of glassy states, broadly categorized as the low-density (LDA) and high-density amorphous ice (HDA). Remarkably, LDA and HDA can be reversibly interconverted via appropriate thermodynamic paths, such as isothermal compression and isobaric heating, exhibiting first-order-like phase transitions. We perform out-of-equilibrium molecular dynamics simulations of glassy water using the ST2 model to study the evolution of LDA and HDA upon isobaric heating. Depending on pressure, glass-to-glass, glass-to-crystal, glass-to-vapor, as well as glass-to-liquid transformations are found. Specifically, heating LDA results in the following transformations, with increasing heating pressures: (i) LDA-to-vapor (sublimation), (ii) LDA-to-liquid (glass transition), (iii) LDA-to-HDA-to-liquid, (iv) LDA-to-HDA-to-liquid-to-crystal, and (v) LDA-to-HDA-to-crystal. Similarly, heating HDA results in the following transformations, with decreasing heating pressures: (a) HDA-to-crystal, (b) HDA-to-liquid-to-crystal, (c) HDA-to-liquid (glass transition), (d) HDA-to-LDA-to-liquid, and (e) HDA-to-LDA-to-vapor. A more complex sequence may be possible using lower heating rates. For each of these transformations, we determine the corresponding transformation temperature as function of pressure, and provide a P-T “phase diagram” for glassy water based on isobaric heating. Our results for isobaric heating dovetail with the LDA-HDA transformations reported for ST2 glassy water based on isothermal compression/decompression processes [Chiu et al., J. Chem. Phys. 139, 184504 (2013)]. The resulting phase diagram is consistent with the liquid-liquid phase transition hypothesis. At the same time, the glass phase diagram is sensitive to sample preparation, such as heating or compression rates. Interestingly, at least for the rates explored, our results suggest that the LDA-to-liquid (HDA-to-liquid) and LDA-to-HDA (HDA-to-LDA) transformation lines on heating are related, both being associated with the limit of kinetic stability of LDA (HDA)

Chiu, Janet; Giovambattista, Nicolas [Department of Physics, Brooklyn College of the City University of New York, Brooklyn, New York 11210 (United States)] [Department of Physics, Brooklyn College of the City University of New York, Brooklyn, New York 11210 (United States); Starr, Francis W. [Department of Physics, Wesleyan University, Middletown, Connecticut 06459 (United States)] [Department of Physics, Wesleyan University, Middletown, Connecticut 06459 (United States)

2014-03-21T23:59:59.000Z

94

Remote sensing of total integrated water vapor, wind speed, and cloud liquid water over the ocean using the Special Sensor Microwave/Imager (SSM/I)  

E-Print Network (OSTI)

A modified D-matrix retrieval method is the basis of the refined total integrated water vapor (TIWV), total integrated cloud liquid water (CLW), and surface wind speed (WS) retrieval methods that are developed. The 85 GHZ polarization difference...

Manning, Norman Willis William

2012-06-07T23:59:59.000Z

95

Large Scale Ice Water Path and 3-D Ice Water Content  

DOE Data Explorer (OSTI)

Cloud ice water concentration is one of the most important, yet poorly observed, cloud properties. Developing physical parameterizations used in general circulation models through single-column modeling is one of the key foci of the ARM program. In addition to the vertical profiles of temperature, water vapor and condensed water at the model grids, large-scale horizontal advective tendencies of these variables are also required as forcing terms in the single-column models. Observed horizontal advection of condensed water has not been available because the radar/lidar/radiometer observations at the ARM site are single-point measurement, therefore, do not provide horizontal distribution of condensed water. The intention of this product is to provide large-scale distribution of cloud ice water by merging available surface and satellite measurements. The satellite cloud ice water algorithm uses ARM ground-based measurements as baseline, produces datasets for 3-D cloud ice water distributions in a 10 deg x 10 deg area near ARM site. The approach of the study is to expand a (surface) point measurement to an (satellite) areal measurement. That is, this study takes the advantage of the high quality cloud measurements at the point of ARM site. We use the cloud characteristics derived from the point measurement to guide/constrain satellite retrieval, then use the satellite algorithm to derive the cloud ice water distributions within an area, i.e., 10 deg x 10 deg centered at ARM site.

Liu, Guosheng

96

Comment on "Structure and dynamics of liquid water on rutile TiO2(110)  

SciTech Connect

Liu and co-workers [Phys. Rev. B 82, 161415 (2010)] discussed the long-standing debate regarding whether H2O molecules on the defect-free (110) surface of rutile ( -TiO2) sorb associatively, or there is dissociation of some or all first-layer water to produce hydroxyl surface sites. They conducted static density functional theory (DFT) and DFT molecular dynamics (DFT-MD) investigations using a range of cell configurations and functionals. We have reproduced their static DFT calculations of the influence of crystal slab thickness on water sorption energies. However, we disagree with several assertions made by these authors: (a) that second-layer water structuring and hydrogen bonding to surface oxygens and adsorbed water molecules are weak ; (b) that translational diffusion of water molecules in direct contact with the surface approaches that of bulk liquid water; and (c) that there is no dissociation of adsorbed water at this surface in contact with liquid water. These assertions directly contradict our publishedwork, which compared synchrotron x-ray crystal truncation rod, second harmonic generation, quasielastic neutron scattering, surface charge titration, and classical MD simulations of rutile (110) single-crystal surfaces and (110)-dominated powders in contact with bulk water, and (110)-dominated rutile nanoparticles with several monolayers of adsorbed water.

Wesolowski, David J [ORNL; Sofo, Jorge O. [Pennsylvania State University; Bandura, Andrei V. [St. Petersburg State University, St. Petersburg, Russia; Zhang, Zhan [Argonne National Laboratory (ANL); Mamontov, Eugene [ORNL; Predota, M. [University of South Bohemia, Czech Republic; Kumar, Nitin [ORNL; Kubicki, James D. [Pennsylvania State University; Kent, Paul R [ORNL; Vlcek, Lukas [ORNL; Machesky, Michael L. [Illinois State Water Survey, Champaign, IL; Fenter, Paul [Argonne National Laboratory (ANL); Cummings, Peter T [ORNL; Anovitz, Lawrence {Larry} M [ORNL; Skelton, A A [Vanderbilt University; Rosenqvist, Jorgen K [ORNL

2012-01-01T23:59:59.000Z

97

Time-Dependent Properties of Liquid Water:? A Comparison of Car?Parrinello and Born?Oppenheimer Molecular Dynamics Simulations  

Science Journals Connector (OSTI)

Time-Dependent Properties of Liquid Water:? A Comparison of Car?Parrinello and Born?Oppenheimer Molecular Dynamics Simulations ... Dynamical information of water interacting with its local environment can be gleaned from the vibrational power spectrum. ...

I-Feng W. Kuo; Christopher J. Mundy; Matthew J. McGrath; J. Ilja Siepmann

2006-07-27T23:59:59.000Z

98

Nuclear quantum effects in liquid water from path-integral simulations using an ab initio force matching approach  

E-Print Network (OSTI)

We have applied path integral simulations, in combination with new ab initio based water potentials, to investigate nuclear quantum effects in liquid water. Because direct ab initio path integral simulations are computationally expensive, a flexible water model is parameterized by force-matching to density functional theory-based molecular dynamics simulations. The resulting effective potentials provide an inexpensive replacement for direct ab inito molecular dynamics simulations and allow efficient simulation of nuclear quantum effects. Static and dynamic properties of liquid water at ambient conditions are presented and the role of nuclear quantum effects, exchange-correlation functionals and dispersion corrections are discussed in regards to reproducing the experimental properties of liquid water.

Thomas Spura; Christopher John; Scott Habershon; Thomas D. Kühne

2014-02-06T23:59:59.000Z

99

Distributed Reforming of Renewable Liquids via Water Splitting using Oxygen Transport Membrane (OTM) (Presentation)  

NLE Websites -- All DOE Office Websites (Extended Search)

Reforming of Renewable Reforming of Renewable Liquids via Water Splitting using Oxygen Transport Membrane (OTM) * U. (Balu) Balachandran, T. H. Lee, C. Y. Park, and S. E. Dorris Energy Systems Division E-mail: balu@anl.gov * Work supported by the Hydrogen, Fuel Cells, and Infrastructure Technologies Program of DOE's Office of Energy Efficiency and Renewable Energy Presented at the Bio-derived Liquids Working Group (BILIWG) Meeting, Nov. 6, 2007. BILIWG Meeting, Nov. 6, 2007 2 Objective & Rationale Objective: Develop compact dense ceramic membrane reactors that enable the efficient and cost-effective production of hydrogen by reforming renewable liquid fuels using pure oxygen produced by water splitting and transported by an OTM. Rationale: Membrane technology provides the means to attack barriers to the

100

Methane Consumption in Temperate and Subarctic Forest Soils: Rates, Vertical Zonation, and Responses to Water and Nitrogen  

Science Journals Connector (OSTI)

...diffusive gas transport...sphere and the water content of...29). Soil nitrogen content and...Influence of nitrogen fertilization...in mineral waters with resorcinol...Low-pressure solubility of gases in liquid water. Chem. Rev...

A. P. S. Adamsen; G. M. King

1993-02-01T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


101

Optical Kerr effect of liquid and supercooled water: the experimental and data analysis perspective  

E-Print Network (OSTI)

The time-resolved optical Kerr effect spectroscopy (OKE) is a powerful experimental tool enabling accurate investigations of the dynamic phenomena in molecular liquids. We introduced innovative experimental and fitting procedures, that permit a safe deconvolution of sample response function from the instrumental function. This is a critical issue in order to measure the dynamics of sample presenting weak signal, e.g. liquid water. We report OKE data on water measuring intermolecular vibrations and the structural relaxation processes in an extended temperature range, inclusive of the supercooled states. The unpreceded data quality makes possible a solid comparison with few theoretical models; the multi-mode Brownian oscillator model, the Kubo's discrete random jump model and the schematic mode-coupling model. All these models produce reasonable good fits of the OKE data of stable liquid water, i.e. over the freezing point. The features of water dynamics in the OKE data becomes unambiguous only at lower temperatures, i.e. for water in the metastable supercooled phase. Hence this data enable a valid comparison between the model fits. We found that the schematic mode-coupling model provides the more rigorous and complete model for water dynamics, even if is intrinsic hydrodynamic approach hide the molecular information.

A. Taschin; P. Bartolini; R. Eramo; R. Righini; R. Torre

2014-06-20T23:59:59.000Z

102

Measurement of Liquid Water Accumulation in a PEMFC with Dead-Ended Anode  

E-Print Network (OSTI)

Measurement of Liquid Water Accumulation in a PEMFC with Dead-Ended Anode Jason B. Siegel,a, *,z electrolyte membrane fuel cell PEMFC with a dead-ended anode is observed using neutron imaging gas diffusion layer. Even though dry hydrogen is supplied to the anode via pressure regulation

Stefanopoulou, Anna

103

Monte Carlo Simulation of Electromagnetic Interactions of Radiation with Liquid Water in  

E-Print Network (OSTI)

; nevertheless the concept of dose is not adequate to estimate the radiation effects when microscopic entitiesMonte Carlo Simulation of Electromagnetic Interactions of Radiation with Liquid Water. They address a physics domain relevant to the simulation of radiation effects in biological systems, where

Paris-Sud XI, Université de

104

Pulse radiolysis of liquid water using picosecond electron pulses produced by a table-top terawatt laser system  

E-Print Network (OSTI)

Pulse radiolysis of liquid water using picosecond electron pulses produced by a table-top terawatt into a supersonic helium gas jet are used to ionize liquid water. The decay of the hydrated electrons produced electron generator is shown, for the first time, to produce sufficient charge to conduct time resolved

Umstadter, Donald

105

Ultrafast conversions between hydrogen bonded structures in liquid water observed by femtosecond x-ray spectroscopy  

SciTech Connect

We present the first femtosecond soft x-ray spectroscopy in liquids, enabling the observation of changes in hydrogen bond structures in water via core-hole excitation. The oxygen K-edge of vibrationally excited water is probed with femtosecond soft x-ray pulses, exploiting the relation between different water structures and distinct x-ray spectral features. After excitation of the intramolecular OH stretching vibration, characteristic x-ray absorption changes monitor the conversion of strongly hydrogen-bonded water structures to more disordered structures with weaker hydrogen-bonding described by a single subpicosecond time constant. The latter describes the thermalization time of vibrational excitations and defines the characteristic maximum rate with which nonequilibrium populations of more strongly hydrogen-bonded water structures convert to less-bonded ones. On short time scales, the relaxation of vibrational excitations leads to a transient high-pressure state and a transient absorption spectrum different from that of statically heated water.

Wen, Haidan; Huse, Nils; Schoenlein, Robert W.; Lindenberg, Aaron M.

2010-05-01T23:59:59.000Z

106

Radiative Importance of ThinŽ Liquid Water Clouds  

NLE Websites -- All DOE Office Websites (Extended Search)

Program Program Accomplishments of the Instantaneous Radiative Flux (IRF) Working Group August 2006 AERI Observations at Southern Great Plains Improve Infrared Radiative Transfer Models Turner et al., JAS, 2004 * AERI observations used to evaluate clear sky IR radiative transfer models * Long-term comparisons have improved - Spectral line database parameters - Water vapor continuum absorption models * Reduced errors in computation of downwelling radiative IR flux by approx 4; current uncertainty is on the order of 1.5 W/m 2 AERI - (Pre-ARM Model) AERI - (Model in 2003) 1 RU = 1 mW / (m 2 sr cm -1 ) Excellent Agreement in Clear Sky Shortwave Radiative Transfer Between Obs and Calcs Shortwave Flux Bias (Solid) Shortwave Flux RMS (Hatched) W m -2 * Comparison of shortwave radiative flux at the surface

107

The effect of soil water content on the phytotoxicity of diuron, fluridone, metribuzin and trifluralin  

E-Print Network (OSTI)

of Soil Water Content on the Phytotoxicity of Diuron, Fluridone, Netribuzin and Trifluralin (August 1979) Paul Alan Baumann, B. S. Southwest Missouri State (kuversity, Springfield Chairman of Advisory Ccnrnittee: Qr. Norris G. Nerkle 'The effect... that simazine hect less effective in reducing top growth of oats (Avena sativa L. var. "Rodney") as the moisture level of the soil decreased. Almost three times as much simazine was required to give 50% reduction in growth when the xoisture level of the soil...

Baumann, Paul A

2012-06-07T23:59:59.000Z

108

Capillary filling with giant liquid/solid slip: dynamics of water uptake by carbon nanotubes  

E-Print Network (OSTI)

This article discusses the way the standard description of capillary filling dynamics has to be modified to account for liquid/solid slip in nanometric pores. It focuses in particular on the case of a large slip length compared to the pore size. It is shown that the liquid viscosity does not play a role, and that the flow is only controlled by the friction coefficient of the liquid at the wall. Moreover in the Washburn regime, the filling velocity does not depend on the tube radius. Finally, molecular dynamics simulations suggest that this standard description fails to describe the early stage of capillary filling of carbon nanotubes by water, since viscous dissipation at the tube entrance must be taken into account.

Laurent Joly

2011-12-06T23:59:59.000Z

109

Low-Dimensional Water on Ru(0001)Model System for X-ray Absorption Spectroscopy Studies of Liquid Water  

SciTech Connect

We present an x-ray absorption spectroscopy results for fully broken to a complete H-bond network of water molecules on Ru(0001) by varying the morphology from isolated water molecules via two-dimensional clusters to a fully covered monolayer as probed by scanning tunneling microscopy. The sensitivity of x-ray absorption to the symmetry of H-bonding is further elucidated for the amino (-NH{sub 2}) group in glycine adsorbed on Cu(110) where the E-vector is parallel either to the NH donating an H-bond or to the non-H-bonded NH. The results give further evidence for the interpretation of the various spectral features of liquid water and for the general applicability of x-ray absorption spectroscopy to analyze H-bonded systems.

Nordlund, D

2012-02-14T23:59:59.000Z

110

Low-Dimensional Water on Ru(0001); Model System for X-ray Absorption Spectroscopy Studies of Liquid Water  

SciTech Connect

We present an x-ray absorption spectroscopy results for fully broken to a complete H-bond network of water molecules on Ru(0001) by varying the morphology from isolated water molecules via two-dimensional clusters to a fully covered monolayer as probed by scanning tunneling microscopy. The sensitivity of x-ray absorption to the symmetry of H-bonding is further elucidated for the amino (-NH{sub 2}) group in glycine adsorbed on Cu(110) where the E-vector is parallel either to the NH donating an H-bond or to the non-H-bonded NH. The results give further evidence for the interpretation of the various spectral features of liquid water and for the general applicability of x-ray absorption spectroscopy to analyze H-bonded systems.

Nordlund, D.; Ogasawara, H.; Andersson, K.J.; Tatarkhanov, M.; Salmeron, M.; Pettersson, L. G. M.; Nilsson, A.

2009-05-11T23:59:59.000Z

111

Validation of Satellite-Derived Liquid Water Paths Using ARM SGP Microwave Radiometers  

NLE Websites -- All DOE Office Websites (Extended Search)

Satellite-Derived Liquid Water Paths Using Satellite-Derived Liquid Water Paths Using ARM SGP Microwave Radiometers M. M. Khaiyer and J. Huang Analytical Services & Materials, Inc. Hampton, Virginia P. Minnis, B. Lin, and W. L. Smith, Jr. National Aeronautics and Space Administration Langley Research Center Hampton, Virginia A. Fan Science Applications International Corporation Hampton, Virginia A. Rapp Colorado State University Fort Collins, Colorado Introduction Satellites are useful for monitoring climatological parameters over large domains. They are especially useful for measuring various cloud microphysical and radiative parameters where ground-based instruments are not available. The geostationary operational environmental satellite (GOES) has been used to retrieve cloud and radiative properties over an extended domain centered on the Atmospheric

112

Ab-initio molecular dynamics simulation of liquid water by Quantum Monte Carlo  

E-Print Network (OSTI)

Despite liquid water is ubiquitous in chemical reactions at roots of life and climate on earth, the prediction of its properties by high-level ab initio molecular dynamics simulations still represents a formidable task for quantum chemistry. In this article we present a room temperature simulation of liquid water based on the potential energy surface obtained by a many-body wave function through quantum Monte Carlo (QMC) methods. The simulated properties are in excellent agreement with recent neutron scattering and X-ray experiments, particularly concerning the position of the oxygen-oxygen peak in the radial distribution function, at variance of previous Density Functional Theory attempts. Given the excellent performances of QMC on large scale supercomputers, this work opens new perspectives for predictive and reliable ab-initio simulations of complex chemical systems.

Zen, Andrea; Mazzola, Guglielmo; Guidoni, Leonardo; Sorella, Sandro

2014-01-01T23:59:59.000Z

113

Ab-initio molecular dynamics simulation of liquid water by Quantum Monte Carlo  

E-Print Network (OSTI)

Despite liquid water is ubiquitous in chemical reactions at roots of life and climate on earth, the prediction of its properties by high-level ab initio molecular dynamics simulations still represents a formidable task for quantum chemistry. In this article we present a room temperature simulation of liquid water based on the potential energy surface obtained by a many-body wave function through quantum Monte Carlo (QMC) methods. The simulated properties are in excellent agreement with recent neutron scattering and X-ray experiments, particularly concerning the position of the oxygen-oxygen peak in the radial distribution function, at variance of previous Density Functional Theory attempts. Given the excellent performances of QMC on large scale supercomputers, this work opens new perspectives for predictive and reliable ab-initio simulations of complex chemical systems.

Andrea Zen; Ye Luo; Guglielmo Mazzola; Leonardo Guidoni; Sandro Sorella

2014-12-09T23:59:59.000Z

114

Ionic Liquid?Water Mixtures: Enhanced Kw for Efficient Cellulosic Biomass Conversion  

Science Journals Connector (OSTI)

† Departments of Chemistry and ... Under relatively mild conditions (?140 °C, 1 atm) and in the absence of added acid catalysts typically employed in biomass conversion, cellulose dissolved in certain ionic liquids (ILs) has been converted into water-soluble reducing sugars in high total reducing sugar yield (up to 97%), or directly into the biomass platform chemical 5-hydroxymethyl furfural (HMF) in high conversion (up to 89%) when CrCl2 is added. ...

Yuetao Zhang; Hongbo Du; Xianghong Qian; Eugene Y.-X. Chen

2010-03-10T23:59:59.000Z

115

Ice-water and liquid-vapor phase transitions by a Ginzburg–Landau model  

Science Journals Connector (OSTI)

A model for the first order phase transitions as ice-water and liquid-vapor is proposed using the Ginzburg–Landau equation for the order parameter ? . In this model the density ? is composed of two quantities ? 0 and ? 1 such that 1 / ? = 1 / ? 0 + 1 / ? 1 where ? 1 is strictly connected to the order parameter ? . By means of this decomposition we are able to represent the Andrew diagram without the use of the heuristic van der Waals equation.

Mauro Fabrizio

2008-01-01T23:59:59.000Z

116

Three-dimensional effects of liquid water flooding in the cathode of a PEM fuel cell  

E-Print Network (OSTI)

. Researchers all over the world are focusing on optimizing this system to be cost competitive with energy conversion devices currently available. It is a well known fact that the cathode of the PEM fuel cell is the performance limiting component due...THREE DIMENSIONAL EFFECTS OF LIQUID WATER FLOODING IN THE CATHODE OF A PEM FUEL CELL by Dilip Natarajan and Trung Van Nguyen* Department of Chemical and Petroleum Engineering University of Kansas Lawrence, KS 66045, USA Submitted...

Natarajan, Dilip; Van Nguyen, Trung

2003-03-27T23:59:59.000Z

117

Neutron scattering from polycrystalline ice (Ih): Some keys to understanding the collective behavior of liquid water  

Science Journals Connector (OSTI)

The phonon dispersion in the second Brillouin zone of polycrystalline ice (Ih) has been measured. The results confirm the predictions of a previous lattice-dynamics calculation [A. Criado, F.J. Bermejo, M. García-Hernández, and J.L. Martínez, Phys. Rev. E 47, 3516 (1993)] where anomalously steep dispersion curves of an apparent acoustic origin were found. The relevance of the present findings for explaining some apparently anomalous features concerning the collective dynamics of liquid water is finally discussed.

F. J. Bermejo; E. Frikkee; M. García-Hernández; J. L. Martínez; A. Criado

1993-09-01T23:59:59.000Z

118

Electronic structure effects in liquid water studied by photoelectron spectroscopy and density functional theory  

SciTech Connect

We present valence photoelectron emission spectra of liquid water in comparison with gas-phase water, ice close to the melting point, low temperature amorphous and crystalline ice. All aggregation states have major electronic structure changes relative to the free molecule, with rehybridization and development of bonding and anti-bonding states accompanying the hydrogen bond formation. Sensitivity to the local structural order, most prominent in the shape and splitting of the occupied 3a{sub 1} orbital, is understood from the electronic structure averaging over various geometrical structures, and reflects the local nature of the orbital interaction.

Nordlund, Dennis; Odelius, Michael; Bluhm, Hendrik; Ogasawara, Hirohito; Pettersson, Lars G.M.; Nilsson, Anders

2008-04-29T23:59:59.000Z

119

Zero Liquid Discharge (ZLD) System for Flue-Gas Derived Water From Oxy-Combustion Process  

SciTech Connect

Researchers at the National Energy Technology Laboratory (NETL) located in Albany, Oregon, have patented a process - Integrated Pollutant Removal (IPR) that uses off-the-shelf technology to produce a sequestration ready CO{sub 2} stream from an oxy-combustion power plant. Capturing CO{sub 2} from fossil-fuel combustion generates a significant water product which can be tapped for use in the power plant and its peripherals. Water condensed in the IPR{reg_sign} process may contain fly ash particles, sodium (from pH control), and sulfur species, as well as heavy metals, cations and anions. NETL is developing a treatment approach for zero liquid discharge while maximizing available heat from IPR. Current treatment-process steps being studied are flocculation/coagulation, for removal of cations and fine particles, and reverse osmosis, for anion removal as well as for scavenging the remaining cations. After reverse osmosis process steps, thermal evaporation and crystallization steps will be carried out in order to build the whole zero liquid discharge (ZLD) system for flue-gas condensed wastewater. Gypsum is the major product from crystallization process. Fast, in-line treatment of water for re-use in IPR seems to be one practical step for minimizing water treatment requirements for CO{sub 2} capture. The results obtained from above experiments are being used to build water treatment models.

Sivaram Harendra; Danylo Oryshchyn; Thomas Ochs; Stephen J. Gerdemann; John Clark

2011-10-16T23:59:59.000Z

120

Uranium content variations in thermal waters from the West Rhodope cristalline massif during earthquakes in the Chepino Valley (South Bulgaria)  

Science Journals Connector (OSTI)

The uranium content of the thermal waters in the Chepino valley was determined in a period of increased seismic activity. Significant changes in the uranium concentration, much above the normal background valu...

I. Kuleff; P. Petrov; K. Kostadinov

1980-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


121

Water Content Determination of Rubber Stoppers Utilized for Sealing Lyophilized Pharmaceutical Products: Assessment of Two Karl Fischer Titration Methods  

E-Print Network (OSTI)

to factors such as the storage environment and the drug's container/closure system, typically a vial, stopper, and cap. The water present in the rubber stopper may interact with the vial contents, potentially influencing the drug product's stability...

Voth, Laura Marie

2013-08-31T23:59:59.000Z

122

Rapid analysis of cyanuric acid in swimming pool waters by high performance liquid chromatography using porous graphitic carbon  

Science Journals Connector (OSTI)

An approach is presented for reducing analysis times of cyanuric acid in swimming pool waters by high performance liquid chromatography (HPLC ... ) to fully resolve cyanuric acid from other pool interferences wit...

R. Cantú; O. Evans; M. L. Magnuson

2001-04-01T23:59:59.000Z

123

Chemical Characterization and Water Content Determination of Bio-Oils Obtained from Various Biomass Species using 31P NMR Spectroscopy  

SciTech Connect

Pyrolysis is a promising approach to utilize biomass for biofuels. One of the key challenges for this conversion is how to analyze complicated components in the pyrolysis oils. Water contents of pyrolysis oils are normally analyzed by Karl Fischer titration. The use of 2-chloro-4,4,5,5,-tetramethyl-1,3,2-dioxaphospholane followed by {sup 31}P NMR analysis has been used to quantitatively analyze the structure of hydroxyl groups in lignin and whole biomass. Results: {sup 31}P NMR analysis of pyrolysis oils is a novel technique to simultaneously characterize components and analyze water contents in pyrolysis oils produced from various biomasses. The water contents of various pyrolysis oils range from 16 to 40 wt%. The pyrolysis oils obtained from Loblolly pine had higher guaiacyl content, while that from oak had a higher syringyl content. Conclusion: The comparison with Karl Fischer titration shows that {sup 31}P NMR could also reliably be used to measure the water content of pyrolysis oils. Simultaneously with analysis of water content, quantitative characterization of hydroxyl groups, including aliphatic, C-5 substituted/syringyl, guaiacyl, p-hydroxyl phenyl and carboxylic hydroxyl groups, could also be provided by {sup 31}P NMR analysis.

David, K.; Ben, H.; Muzzy, J.; Feik, C.; Iisa, K.; Ragauskas, A.

2012-03-01T23:59:59.000Z

124

A ‘first principles’ potential energy surface for liquid water from VRT spectroscopy of water clusters  

Science Journals Connector (OSTI)

...the many-body induction energy (Leforestier et al. 2005). This new potential was named VRT...ordinary water: substance. New York: Hafner. Dyke, T. R...mechanics and path integrals New York: McGraw- Hill. Frenkel...

2005-01-01T23:59:59.000Z

125

Effect of direct liquid water injection and interdigitated flow field on the performance of proton exchange membrane fuel cells  

E-Print Network (OSTI)

70-108B One Cyclotron Road Berkeley, California 94720 December 2, 1997 Key Words: Proton Exchange Membrane fuel cells, humidification, gas distribution, direct liquid water injection, interdigitated flow fields. * Corresponding... of the catalyst layers were made of waterproof, carbon fiber cloths. Liquid water was injected by two metering pumps into two heated stainless steel coils, where it was preheated to the cell operating temperatures, and then directly into the gas streams...

Wood, D. L.; Yi, Y. S.; Nguyen, Trung Van

1998-01-01T23:59:59.000Z

126

Ionic liquid effects on mass transfer efficiency in extractive distillation of water–ethanol mixtures  

Science Journals Connector (OSTI)

Abstract The relatively high viscosities of ionic liquids could reduce the mass transfer efficiency of the extractive distillation process. The rate-based model was adopted to analyze this phenomenon since it predicted the performance of an extractive distillation pilot plant using ionic liquids as solvent. For the water–ethanol separation, three ionic liquids: 1-ethyl-3-methylimidazolium chloride, 1-ethyl-3-methylimidazolium acetate and 1-ethyl-3-methylimidazolium dicyanamide and the organic solvent ethylene glycol were used for the analysis. Simulations were conducted for sieve trays and Mellapak® 250Y. The results indicate that relatively high viscosities affect the mass transfer efficiency. However, the improvements in relative volatilities obtained from the ionic liquids help to overcome this effect. However, with high solvent viscosities (>65 mPa s at T = 353.15 K) it was not possible to overcome the reductions. Additionally, at higher distillate rates high relative volatilities yielded negative effects on mass transfer efficiency because of a decrease in vapor velocity.

E. Quijada-Maldonado; G. Wytze Meindersma; André B. de Haan

2014-01-01T23:59:59.000Z

127

Effect of potassium halide salts on mutual solubility of water + aromatic hydrocarbons liquid–liquid interface studied with surface and interfacial tensions  

Science Journals Connector (OSTI)

Abstract Surface tension (?, mN/m) of benzene, toluene and ethylbenzene (EB) aromatic hydrocarbons (AHCs, low density liquids, LDL) and interfacial tension (IFT, mN/m) both with water and aqueous 0.1, 0.5, 1.0 mol kg? 1 KF, KCl, KBr, KI (high density liquids, HDL) separately at 303.15 K are reported. Contributions of –CH3 and –CH2CH3 of toluene and EB to hydrophobic interactions are calculated from ?toluene–?benzene and ?EB–?benzene, respectively. \\{IFTs\\} of water + AHCs liquid–liquid interfaces (LLI) are as toluene (34.71) > EB (32.35) > benzene (32.32 mN m? 1), with a ~ 32.32 mN m? 1 decrease from 71.40 mN m? 1 of water. \\{AHCs\\} with hyperconjugation (HC) and positive inductive effects (+ ve IE) with toluene and EB LLI have reduced IFT by 39.08, 2.39, ? 1.56 mN m? 1, respectively. The effects of ?-conjugation, –H, –CH3 and –CH2CH3 on surface tension are calculated as ?-conjugation = ?(IFTair–liquid ? IFTAPHS–benzene), –CH3 = ?(IFTAPHS–toluene ? IFTAPHS–benzene). The effects of halide salts on hypercongugation –H(–CH3)/3, –CH2CH3 are obtained from ?(IFTAPHS–EB ? IFTAPHS–benzene).

Man Singh

2014-01-01T23:59:59.000Z

128

Nanoparticle enhanced evaporation of liquids: A case study of silicone oil and water  

E-Print Network (OSTI)

Evaporation is a fundamental physical phenomenon, of which many challenging questions remain unanswered. Enhanced evaporation of liquids in some occasions is of enormous practical significance. Here we report the enhanced evaporation of the nearly permanently stable silicone oil by dispersing with nanopariticles including CaTiO3, anatase and rutile TiO2. The results can inspire the research of atomistic mechanism for nanoparticle enhanced evaporation and exploration of evaporation control techniques for treatment of oil pollution and restoration of dirty water.

Wenbin Zhang; Rong Shen; Kunquan Lu; Ailing Ji; Zexian Cao

2012-10-23T23:59:59.000Z

129

Kinematical relations among radar-observed water concentrations, vertical motions, and liquid-water drop-size spectra in convective clouds  

E-Print Network (OSTI)

and liquid- water concentration, a one-dimensional (vertical) continuity equation for water substance is considered. Atmospheric values of parameters which appear in the continuity equation are determined from radar reflectivity measurements. Empirical... viii I INTRODUCTION Cloud Motions in General Equations Governing Cloud Parameters A Kinematical Equation Based on the Continuity of Water Substance Determinati. on of the Values of the Atmospheric Variables Appearing in the Kinematical Equation...

Runnels, Robert Clayton

2012-06-07T23:59:59.000Z

130

Probing Properties of Glassy Water and Other Liquids with Site Selective Spectroscopies  

SciTech Connect

The standard non-photochemical hole burning (NPHB) mechanism, which involves phonon-assisted tunneling in the electronically excited state, was originally proposed to explain the light-induced frequency change of chemically stable molecules in glassy solids at liquid helium temperatures by this research group more than two decades ago. The NPHB mechanism was then further elucidated and the concept of intrinsic to glass configurational relaxation processes as pre-mediating step to the hole burning process was introduced. The latter provided the theoretical basis for NPHB to evolve into a powerful tool probing the dynamics and nature of amorphous media, which aside from ''simple'' inorganic glasses may include also ''complex'' biological systems such as living cells and cancerous/normal tissues. Presented in this dissertation are the experimental and theoretical results of hole burning properties of aluminum phthalocyanine tetrasulphonate (APT) in several different matrices: (1) hyperquenched glassy water (HGW); (2) cubic ice (I{sub c}); and (3) water confined into poly(2-hydroxyethylmethacrylate) (poly-HEMA). In addition, results of photochemical hole burning (PHB) studies obtained for phthalocyanine tetrasulphonate (PcT) in HGW and free base phthalocyanine (Pc) in ortho-dichlorobenzene (DCB) glass are reported. The goal of this dissertation was to provide further evidence supporting the NPHB mechanism and to provide more insight that leads to a better understanding of the kinetic events (dynamics) in glasses, and various dynamical processes of different fluorescent chromorphores in various amorphous solids and the liquid that exist above the glass transition temperature (T{sub g}). The following issues are addressed in detail: (1) time evolution of hole being burned under different conditions and in different hole burning systems; (2) temperature dependent hole profile; and (3) the structure/dynamics of water in confined space, which has been studied, in part because of the importance of non-freezable water in biological systems.

Nhan Chuong Dang

2005-08-12T23:59:59.000Z

131

Isotopic mass-dependence of metal cation diffusion coefficients in liquid water  

SciTech Connect

Isotope distributions in natural systems can be highly sensitive to the mass (m) dependence of solute diffusion coefficients (D) in liquid water. Isotope geochemistry studies routinely have assumed that this mass dependence either is negligible (as predicted by hydrodynamic theories) or follows a kinetic-theory-like inverse square root relationship (D {proportional_to} m{sup -0.5}). However, our recent experimental results and molecular dynamics (MD) simulations showed that the mass dependence of D is intermediate between hydrodynamic and kinetic theory predictions (D {proportional_to} m{sup -{beta}} with 0 {<=} {beta} < 0.2 for Li{sup +}, Cl{sup -}, Mg{sup 2+}, and the noble gases). In this paper, we present new MD simulations and experimental results for Na{sup +}, K{sup +}, Cs{sup +}, and Ca{sup 2+} that confirm the generality of the inverse power-law relation D {proportional_to} m{sup -{beta}}. Our new findings allow us to develop a general description of the influence of solute valence and radius on the mass dependence of D for monatomic solutes in liquid water. This mass dependence decreases with solute radius and with the magnitude of solute valence. Molecular-scale analysis of our MD simulation results reveals that these trends derive from the exponent {beta} being smallest for those solutes whose motions are most strongly coupled to solvent hydrodynamic modes.

Bourg, I.C.; Richter, F.M.; Christensen, J.N.; Sposito, G.

2009-01-11T23:59:59.000Z

132

Local Depolarization in Hydrophobic and Hydrophilic Ionic Liquids/Water Mixtures: Car–Parrinello and Classical Molecular Dynamics Simulation  

Science Journals Connector (OSTI)

Local Depolarization in Hydrophobic and Hydrophilic Ionic Liquids/Water Mixtures: Car–Parrinello and Classical Molecular Dynamics Simulation ... Their analysis of the molecular electrostatic properties compared with the previous work on smaller number of ion pairs per unit cell shows that the immediate liquid environment predominantly affects the molecular electric dipole moments, whereas the bulk contributions appear to be minor. ... The ion-pair/water interaction energy (Einter), which is defined as the difference between the energy of the ion pair and water system (EIL-W) and the sum of the energies of the single ion pair (EIL) and water (EW), can be calculated by:(1)Each complex and corresponding water and anion were optimized for structure and energy at the B3LYP/6-311++G(d,p) level of theory by the above computational procedure. ...

Mohammad Hadi Ghatee; Amin Reza Zolghadr

2013-01-08T23:59:59.000Z

133

Utilizing the heat content of gas-to-liquids by-product streams for commercial power generation  

E-Print Network (OSTI)

and sulphur. They have no aromatics due to the isomerisation of the highly paraffinic Fischer-Tropsch liquids into GTL fuels and are practically100%iso-paraffinic,thustheyhaveveryhighcetaneratings. The... and sulphur. They have no aromatics due to the isomerisation of the highly paraffinic Fischer-Tropsch liquids into GTL fuels and are practically100%iso-paraffinic,thustheyhaveveryhighcetaneratings. The...

Adegoke, Adesola Ayodeji

2006-10-30T23:59:59.000Z

134

16/05/12 3:57 PMWATER: Floating robots use GPS-enabled smartphones to track water flow, help water management Page 1 of 4http://www.lakeconews.com/index.php?option=com_content&view=article...o-track-water-flow-help-water-management&catid=1:latest&Itemid=1  

E-Print Network (OSTI)

management Page 1 of 4http://www.lakeconews.com/index.php?option=com_content&view=article...o-track-water-flow-help-water-management management WATER:'Floating'robots'use'GPS8 enabled'smartphones'to'track'water flow,'help'water'management-enabled smartphones to track water flow, help water management Page 2 of 4http://www.lakeconews.com/index.php?option

135

An Assessment of Microwave Absorption Models and Retrievals of Cloud Liquid Water Using Clear-Sky Data  

SciTech Connect

Passive microwave radiometers have a long history in the remote sensing of atmospheric liquid and water vapor. Retrievals of these quantities are sensitive to variations in pressure and temperature of the liquid and water vapor. Rather than use a statistical or climatological approach to account for the natural variability in atmospheric pressure and temperature, additional information on the atmospheric profile at the time of the radiometer measurements can be directly incorporated into the retrieval process. Such an approach has been referred to in the literature as a “physical-iterative” solution. This paper presents an assessment of the accuracy of the column liquid water path that can be expected using such an iterative technique as a result of uncertainties in the microwave emissions from oxygen and water vapor. It is shown that the retrieval accuracy is influenced by the accuracy of the instrument measurements and the quality of the atmospheric profiles of temperature and pressure, as one would expect. But also critical is the uncertainty in the absorption coefficients used in the underlying microwave radiative transfer model. The uncertainty in the absorption coefficients is particularly problematic in that it may well bias the liquid water retrieval. The differences between 3 absorption models examined in this paper are equivalent to a bias of 15 to 30 g/m2, depending on the total column water vapor. An examination of typical liquid water paths from the Southern Great Plains region of the United States shows that errors of this magnitude have significant implications for shortwave radiation and retrievals of cloud effective particle size.

Marchand, Roger T.; Ackerman, Thomas P.; Westwater, Ed R.; Clough, Shepard A.; Cady-Pereira, Karen; Liljegren, James C.

2003-12-19T23:59:59.000Z

136

Sensitivity of the simulated climate to a diagnostic formulation for cloud liquid water  

SciTech Connect

The accurate treatment of clouds and their radiative properties is widely regarded to be among the most important problems facing global climate modeling. A number of the more serious systematic simulation biases in the NCAR Community Climate Model (CCM2) appear to be related to deficiencies in the treatment of cloud optical properties. In this paper, a simple diagnostic parameterization for cloud liquid water is presented. The sensitivity of the simulated climate to this alternative formulation, both in terms of mean climate metrics and measures of the climate system response, is illustrated. Resulting simulations show significant reductions in CCM2 systematic biases, particularly with respect to surface temperature, precipitation, and extratropical geopotential height-field anomalies. Many aspects of the simulated response to ENSO forcing are also substantially improved.

Hack, J.J. [National Center for Atmospheric Research, Boulder, CO (United States)] [National Center for Atmospheric Research, Boulder, CO (United States)

1998-07-01T23:59:59.000Z

137

The Influence of Chain Dynamics on the Far Infrared Spectrum of Liquid Methanol-Water Mixtures  

SciTech Connect

Far-infrared absorption spectroscopy has been used to study the low frequency ({center_dot} 100 cm{sup -1}) intermolecular modes of methanol in mixtures with water. With the aid of a first principles molecular dynamics simulation on an equivalent system, a detailed understanding about the origin of the low frequency IR modes has been established. The total dipole spectrum from the simulation suggests that the bands appearing in the experimental spectra at approximately 55 cm{sup -1} and 70 cm{sup -1} in methanol and methanol-rich mixtures arise from both fluctuations and torsional motions occurring within the methanol hydrogen-bonded chains. The influence of these modes on both the solvation dynamics and the relaxation mechanisms in the liquid are discussed within the context of recent experimental and theoretical results that have emerged from studies focusing on the short time dynamics in the methanol hydrogen bond network.

Woods, K.N.; /Stanford U., Phys. Dept.; Wiedemann, H.; /SLAC, SSRL; ,

2005-07-12T23:59:59.000Z

138

Don't water down: Enhance content learning through the unit organizer routine  

E-Print Network (OSTI)

The writer considers a content enhancement routine called the unit organizer routine. This routine focuses on how a teacher introduces, builds, and gains closure on a content area unit's critical ideas and information. In ...

Bouda, Daniel J.; Lenz, B. Keith; Bulgren, Janis A.; Schumaker, Jean B.; Deshler, Donald D.

2000-01-01T23:59:59.000Z

139

System and method for monitoring water content or other dielectric influences in a medium  

DOE Patents (OSTI)

A sensor system is provided that measures water content or other detectable properties in a medium along the entire length of the sensor at any point in time. The sensor system includes an electromagnetic signal generator and a transmission line disposed in a medium to be monitored. Alternatively, the transmission line can be configured for movement across a medium to be monitored, or the transmission line can be fixed relative to a moving medium being monitored. A signal is transmitted along the transmission line at predetermined frequencies, and the signal is returned back along the transmission line and/or into an optional receive line in proximity to the transmission line. The returned signal is processed to generate a one-dimensional data output profile that is a function of a detectable property of the medium. The data output profile can be mapped onto a physical system to generate a two-dimensional or three-dimensional profile if desired. The sensor system is useful in a variety of different applications such as agriculture, horticulture, biofiltration systems for industrial offgases, leak detection in landfills or drum storage facilities at buried waste sites, and in many other applications.

Cherry, Robert S. (Idaho Falls, ID); Anderson, Allen A. (Firth, ID)

2001-01-01T23:59:59.000Z

140

In situ diagnostic of liquid water distribution in cathode catalyst layer in an operating PEMFC by high-resolution soft X-ray radiography  

Science Journals Connector (OSTI)

To investigate the water transport behavior in the cathode catalyst layer (CCL) of an operating proton exchange membrane fuel cell (PEMFC), we examined transversal liquid water distributions in the CCL by using high-resolution soft X-ray radiography. The liquid water concentration gradient across the CCL was observed at a spatial resolution of 1.5 ?m. More liquid water accumulated in the CCL at the gas diffusion layer side than at the polymer electrolyte membrane side. The effect of accumulated liquid water in the CCL on the charge-transfer resistance was confirmed by electrochemical impedance spectroscopy. Liquid water accumulation in the CCL corresponds to deterioration of charge-transfer in the electrode.

Phengxay Deevanhxay; Takashi Sasabe; Shohji Tsushima; Shuichiro Hirai

2012-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


141

Analysis of two independent methods for retrieving liquid water profiles in spring and summer Arctic boundary clouds  

E-Print Network (OSTI)

-based remote sensing, optimal estimation, LES model with explicit microphysics, cloud liquid water algorithms Heat Budget of the Arctic Ocean (SHEBA) project. An algorithm developed by Frisch et al. [1995, 1998 matrix of the LWC profile is calculated, an optimal estimation method is applied to the SHEBA data

Shupe, Matthew

142

Charge transfer effects of ions at the liquid water/vapor interface  

SciTech Connect

Charge transfer (CT), the movement of small amounts of electron density between non-bonded pairs, has been suggested as a driving force for a variety of physical processes. Herein, we examine the effect of CT on ion adsorption to the water liquid-vapor interface. Using a CT force field for molecular dynamics, we construct a potential of mean force (PMF) for Na{sup +}, K{sup +}, Cl{sup ?}, and I{sup ?}. The PMFs were produced with respect to an average interface and an instantaneous interface. An analysis of the PMF relative to the instantaneous surface reveals that the area in which the anions experience a free energy minimum is quite narrow, and the cations feel a steeply repulsive free energy near the interface. CT is seen to have only minor effects on the overall free energy profiles. However, the long-ranged effects of ions are highlighted by the CT model. Due to CT, the water molecules at the surface become charged, even when the ion is over 15 Å away from the surface.

Soniat, Marielle; Rick, Steven W., E-mail: srick@uno.edu [Department of Chemistry, University of New Orleans, New Orleans, Louisiana 70148 (United States)

2014-05-14T23:59:59.000Z

143

Absorption spectra of liquid water and aqueous buffers between 0.3 and Department of Physics, University of California, Santa Barbara, California 93106  

E-Print Network (OSTI)

Absorption spectra of liquid water and aqueous buffers between 0.3 and 3.72 THz Jing Xua Department-dependent terahertz absorption with attenuation lengths on the order of tens of micrometers. To access this spectral.5 THz, these studies provide a well- documented absorption spectrum for liquid water, at approxi- mately

Xu, Jing

144

Measurement of Total Water with a Tunable Diode Laser Hygrometer: Inlet Analysis, Calibration Procedure, and Ice Water Content Determination  

Science Journals Connector (OSTI)

The University of Colorado closed-path tunable diode laser hygrometer (CLH), a new instrument for the in situ measurement of enhanced total water (eTW, the sum of water vapor and condensed water enhanced by a subisokinetic inlet), has recently ...

Sean M. Davis; A. Gannet Hallar; Linnea M. Avallone; William Engblom

2007-03-01T23:59:59.000Z

145

Sewage sludge dewatering using flowing liquid metals  

DOE Patents (OSTI)

A method and apparatus for reducing the moisture content of a moist sewage sludge having a moisture content of about 50% to 80% and formed of small cellular micro-organism bodies having internally confined water is provided. A hot liquid metal is circulated in a circulation loop and the moist sewage sludge is injected in the circulation loop under conditions of temperature and pressure such that the confined water vaporizes and ruptures the cellular bodies. The vapor produced, the dried sludge, and the liquid metal are then separated. Preferably, the moist sewage sludge is injected into the hot liquid metal adjacent the upstream side of a venturi which serves to thoroughly mix the hot liquid metal and the moist sewage sludge. The venturi and the drying zone after the venturi are preferably vertically oriented. The dried sewage sludge recovered is available as a fuel and is preferably used for heating the hot liquid metal.

Carlson, Larry W. (Oswego, IL)

1986-01-01T23:59:59.000Z

146

The Individual and Collective Effects of Exact Exchange and Dispersion Interactions on the Ab Initio Structure of Liquid Water  

E-Print Network (OSTI)

In this work, we report the results of a series of density functional theory (DFT) based ab initio molecular dynamics (AIMD) simulations of ambient liquid water using a hierarchy of exchange-correlation (XC) functionals to investigate the individual and collective effects of exact exchange (Exx), via the PBE0 hybrid functional, non-local vdW/dispersion interactions, via a fully self-consistent density-dependent dispersion correction, and approximate nuclear quantum effects (aNQE), via a 30 K increase in the simulation temperature, on the microscopic structure of liquid water. Based on these AIMD simulations, we found that the collective inclusion of Exx, vdW, and aNQE as resulting from a large-scale AIMD simulation of (H$_2$O)$_{128}$ at the PBE0+vdW level of theory, significantly softens the structure of ambient liquid water and yields an oxygen-oxygen structure factor, $S_{\\rm OO}(Q)$, and corresponding oxygen-oxygen radial distribution function, $g_{\\rm OO}(r)$, that are now in quantitative agreement with the best available experimental data. This level of agreement between simulation and experiment as demonstrated herein originates from an increase in the relative population of water molecules in the interstitial region between the first and second coordination shells, a collective reorganization in the liquid phase which is facilitated by a weakening of the hydrogen bond strength by the use of the PBE0 hybrid XC functional, coupled with a relative stabilization of the resultant disordered liquid water configurations by the inclusion of non-local vdW/dispersion interactions.

Robert A. DiStasio Jr.; Biswajit Santra; Zhaofeng Li; Xifan Wu; Roberto Car

2014-05-20T23:59:59.000Z

147

An evaluation of hydrologic, geotechnical, and chemical behavior of processed oil shale solid waste 2; The use of time domain reflectometry (TDR) for monitoring in-situ volumetric water content in processed oil shale  

SciTech Connect

This paper describes the use of time domain reflectometry (TDR) for monitoring volumetric water contents in processed oil shale solid waste. TDR measures soil water content via a correlation between the dielectric constant (K) of the 3 phase (soil-water-air) system and the volumetric water content ({theta}{sub v}). An extensive bench top research program has been conducted to evaluate and verify the use of this technique in processed oil shale solid waste. This study utilizes columns of processed oil shale packed to known densities and varying water contents and compares the columetric water content measured via TDR and the volumetric water content measured through gravimetric determination.

Reeves, T.L.; Elgezawi, S.M. (Wyoming Univ., Laramie, WY (USA). Dept. of Civil Engineering); Kaser, T.G. (GIGO Computer and Electronic, Laramie, WY (US))

1989-01-01T23:59:59.000Z

148

The effect of water content, cooling rate, and growth temperature on the freezing temperature of 4 Tillandsia species  

E-Print Network (OSTI)

the exotherm initiation temperatures (EIT) of leaf sections. The effect of 2 growth temperatures (5 and 25oC) on the absolute water content and EIT of T. recurvata and T. usneoides was also determined. All p * * pt T. mb'1 ', f o t ld temperatures at 80... used to detect ice formation in plant tissues by exotherm detection. An electronic device is used to measure the heat released (exotherm) when water freezes. From this information, the freezing and supercooling temperatures of plant tissues can...

Hagar, Christopher Flint

1990-01-01T23:59:59.000Z

149

The mineral content of water as a variable in the quality control of reconstituted non-fat dry milk products  

E-Print Network (OSTI)

LibK?ARr '< A 4 M CuLLEftE ?F TEXAf. THE MINERAL CONTENT OF WATER AS A VARIABLE IN THE QUALITY CONTROL OF RECONSTITUTED NONFAT DRY MILK PRODUCTS By JOHN 0. KAPSAUS A Dissertation Submitted to the Graduate School of the Agricultural...). This is the CO2 evolved in the milk, which has been reconstituted with the respective level of bicarbonate water, in the uninoculated tube. (E) CO2 produced from the action of the apparent milk acidity on the bicarbonate. This is the CO2 calculated from...

Kapsalis, John G.

2013-10-04T23:59:59.000Z

150

Distributed Reforming of Renewable Liquids via Water Splitting using Oxygen Transport Membrane (OTM) (Presentation)  

Energy.gov (U.S. Department of Energy (DOE))

Presented at the 2007 Bio-Derived Liquids to Hydrogen Distributed Reforming Working Group held November 6, 2007 in Laurel, Maryland.

151

E-Print Network 3.0 - additional water content Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

supports more than half the world... specified. In addition to water footprinting and LCA, this analysis examines in lesser detail the WBCSD... of production. Understanding...

152

The use of a permanent magnet for water content measurements of wood chips  

E-Print Network (OSTI)

the FID Cellulose and Water,” TAPPI Journal, June 1996, Vol.were compared with the TAPPI standard method of measuringmade using the standard TAPPI test employing oven drying.

2001-01-01T23:59:59.000Z

153

Removal of a liquid paraffin film from a water surface by short pulses from a CO{sub 2} laser  

SciTech Connect

The process of removal of a liquid paraffin film from a water surface irradiated by 40 - 270-{mu}s pulses from a CO{sub 2} laser is studied experimentally and theoretically. It is found for the first time that the mass of removed paraffin can exceed that of paraffin located in the region irradiated by the laser pulse. A theoretical model is proposed which explains the results obtained. (laser applications and other topics in quantum electronics)

Antonova, L I; Drobyazko, S V; Evdokimov, I A; Krasyukov, A G; Likhanskii, V V; Loboiko, A I; Senatorov, Yu M [State Research Center of Russian Federation 'Troitsk Institute for Innovation and Fusion Research', Troitsk, Moscow Region (Russian Federation)

2002-02-28T23:59:59.000Z

154

TIME-DEPENDENT PROPERTIES OF LIQUID WATER: A COMPARISON OF CAR-PARRINELLO AND BORN-OPPENHIEMER MOLECULAR DYNAMICS SIMULATIONS  

SciTech Connect

A series of 30 ps first principles molecular dynamics simulations in the microcanonical ensemble were carried out to investigate transport and vibrational properties of liquid water. To allow for sufficient sampling, the thermodynamic constraints were set to an elevated temperature of around 423 K and a density of 0.71 g/cm{sup 3} corresponding to the saturated liquid density for the Becke-Lee-Yang-Parr (BLYP) representation of water. Four simulations using the Car-Parrinello molecular dynamics (CPMD) technique with varying values of the fictitious electronic mass ({mu}) and two simulations using the Born-Oppenheimer molecular dynamics (BOMD) technique are analyzed to yield structural and dynamical information. At the selected state point, the simulations are found to exhibit non-glassy dynamics and yield consistent results for the liquid structure and the self-diffusion coefficient, although the statistical uncertainties in the latter quantity are quite large. Consequently, it can be said that the CPMD and BOMD methods produce equivalent results for these properties on the time scales reported here. However, it was found that the choice of {mu} affects the frequency spectrum of the intramolecular modes, shifting them slightly to regions of lower frequency. Using a value of {mu} = 400 a.u. results in a significant drift in the electronic kinetic energy of the system over the course of 30 ps and a downward drift in the ionic temperature. Therefore, for long trajectories at elevated temperatures, lower values of this parameter are recommended for CPMD simulations of water.

Kuo, I W; Mundy, C; McGrath, M; Siepmann, J I

2005-12-29T23:59:59.000Z

155

The Individual and Collective Effects of Exact Exchange and Dispersion Interactions on the Ab Initio Structure of Liquid Water  

E-Print Network (OSTI)

In this work, we report the results of a series of density functional theory (DFT) based ab initio molecular dynamics (AIMD) simulations of ambient liquid water using a hierarchy of exchange-correlation (XC) functionals to investigate the individual and collective effects of exact exchange (Exx), via the PBE0 hybrid functional, non-local vdW/dispersion interactions, via a fully self-consistent density-dependent dispersion correction, and approximate nuclear quantum effects (aNQE), via a 30 K increase in the simulation temperature, on the microscopic structure of liquid water. Based on these AIMD simulations, we found that the collective inclusion of Exx, vdW, and aNQE as resulting from a large-scale AIMD simulation of (H$_2$O)$_{128}$ at the PBE0+vdW level of theory, significantly softens the structure of ambient liquid water and yields an oxygen-oxygen structure factor, $S_{\\rm OO}(Q)$, and corresponding oxygen-oxygen radial distribution function, $g_{\\rm OO}(r)$, that are now in quantitative agreement with ...

DiStasio, Robert A; Li, Zhaofeng; Wu, Xifan; Car, Roberto

2014-01-01T23:59:59.000Z

156

Determination of Selected Herbicides and Phenols in Water and Soils by Solid-Phase Extraction and High-Performance Liquid Chromatography  

Science Journals Connector (OSTI)

......1987). 6. G.E. Batley. Applications of liquid chromatography with electro- chemical detection to the analysis of oil shale process waters. J. Chromatogr. 382: 409416 (1987). 7. H. Farber, K. Nick, and H.F. Scoeler. Determination......

Irena Baranowska; Celina Pieszko

2000-05-01T23:59:59.000Z

157

A liquid film motor  

Science Journals Connector (OSTI)

It is well known that electro-hydrodynamical effects in freely suspended liquid films can force liquids to flow. Here, we report a purely electrically driven rotation in water and some other liquid suspended film...

A. Amjadi; R. Shirsavar; N. Hamedani Radja…

2009-05-01T23:59:59.000Z

158

The Behaviour of Electrolytes in Mixed Solvents. Part I. The Free Energies and Heat Contents of Hydrogen Chloride in Water-Ethyl Alcohol Solutions  

Science Journals Connector (OSTI)

1 November 1929 research-article The Behaviour of Electrolytes in Mixed Solvents. Part I. The Free Energies and Heat Contents of Hydrogen Chloride in Water-Ethyl Alcohol Solutions J. A. V. Butler C. M. Robertson The Royal Society...

1929-01-01T23:59:59.000Z

159

Optimizing the Probability of Flying in High Ice Water Content Conditions in the Tropics Using a Regional-Scale Climatology of Convective Cell Properties  

Science Journals Connector (OSTI)

In this paper, statistical properties of rainfall are derived from 14 years of Tropical Rainfall Measuring Mission data to optimize the use of flight hours for the upcoming High Altitude Ice Crystals (HAIC)/High Ice Water Content (HIWC) program. ...

A. Protat; S. Rauniyar; V. V. Kumar; J. W. Strapp

2014-11-01T23:59:59.000Z

160

TRMM observations of the global relationship between ice water content and lightning  

E-Print Network (OSTI)

to study the fundamental relationship between precipitation ice mass and lightning flash density water path and lightning flash density is relatively invariant between land, ocean and coastal regimes proportionality between charge generation rates on ice and lightning flash rates, predict a linear to slightly non

Rutledge, Steven

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


161

Vadose Zone Transport Field Study: Soil Water Content Distributions by Neutron Moderation  

SciTech Connect

Contaminant transport through the vadose zone is a complex process controlled largely by interactions between subsurface lithologic features, water flow, and fluid properties. Understanding the processes controlling transport is an important prerequisite to the development and implementation of effective soil and ground water remediation programs. However, difficulties in directly observing and sampling the subsurface can complicate attempts to better describe subsurface transport processes and is mostly responsible for the large amount of uncertainty associated with vadose zone processes. The reduction of the uncertainty has been identified as a site need at Hanford by the STCG and the National Research Council (2000a) and is a key aspect of the site?s science and technology effort.

Ward, Anderson L.; Caldwell, Todd G.; Gee, Glendon W.

2000-10-01T23:59:59.000Z

162

Life in the Solar System Assume we need energy, liquid water, and organic materials.  

E-Print Network (OSTI)

would land on the ice pack, use heat from a nuclear reactor to melt through it, and release a hydrobot;Comets ­ Reservoirs of Icy Water #12;Comets ­ Reservoirs of Icy Water #12;Herschel Space Observatory #12

Shirley, Yancy

163

Concentration and High Pressure Liquid Chromatographic Determination of Pyrazon in Water  

Science Journals Connector (OSTI)

......dissolved In the water. A 500 ml sample of lake water with 25% dissolved...evaporated under nitrogen and the residue...been determined in water (1-3), soils...1,4,7), gas chromatography...due to decreased solubility of the herbi......

Gathu Nyagah

1981-10-01T23:59:59.000Z

164

1-Methyl Naphthalene Reorientation at the Air-Liquid Interface upon Water Saturation Studied by Vibrational Broad Bandwidth Sum Frequency Generation Spectroscopy  

E-Print Network (OSTI)

will encounter gas-phase water molecules or may react with atmospheric oxidants. The uptake and reaction1-Methyl Naphthalene Reorientation at the Air-Liquid Interface upon Water Saturation Studied by Vibrational Broad Bandwidth Sum Frequency Generation Spectroscopy Elizabeth L. Hommel and Heather C. Allen

165

Trace determination of triclosan and triclocarban in environmental water samples with ionic liquid dispersive liquid-phase microextraction prior to HPLC–ESI-MS–MS  

Science Journals Connector (OSTI)

A novel and environmentally friendly microextraction method, termed ionic liquid dispersive liquid-phase microextraction (IL-DLPME), has been developed for rapid enrichment of triclosan and triclocarban before an...

Ru-Song Zhao; Xia Wang; Jing Sun; Shan-Shan Wang…

2010-06-01T23:59:59.000Z

166

Pore-Level Liquid Water Transport Through Composite Diffusion Media of PEMFC  

E-Print Network (OSTI)

, and Chao-Yang Wang*,z Electrochemical Engine Center and Department of Mechanical and Nuclear Engineering of liquid injection sites into the GDL. © 2010 The Electrochemical Society. DOI: 10.1149/1.3491359 All, low operation temperature, and low noise. The low operation tempera- ture allows for fast startup

167

Monitoring of Precipitable Water Vapor and Cloud Liquid Path from Scanning Microwave Radiometers During the 2003 Cloudiness Inter-Comparison Experiment  

NLE Websites -- All DOE Office Websites (Extended Search)

Monitoring of Precipitable Water Vapor and Cloud Liquid Monitoring of Precipitable Water Vapor and Cloud Liquid Path from Scanning Microwave Radiometers During the 2003 Cloudiness Inter-Comparison Experiment V. Mattioli Department of Electronic and Information Engineering University of Perugia Perugia, Italy E. R. Westwater Cooperative Institute for Research in Environmental Sciences University of Colorado National Oceanic and Atmospheric Administration Environmental Technology Laboratory Boulder, Colorado V. Morris Pacific Northwest National Laboratory Richland, Washington Introduction Ground-based microwave radiometers (MWR) are widely used to measure atmospheric precipitable water vapor (PWV) and cloud liquid path (CLP). Comparisons of PWV derived from MWRs with water vapor retrievals from instruments like radiosondes, Global Positioning System (GPS) and Raman

168

Decontamination of Nuclear Liquid Wastes Status of CEA and AREVA R and D: Application to Fukushima Waste Waters - 12312  

SciTech Connect

Liquid wastes decontamination processes are mainly based on two techniques: Bulk processes and the so called Cartridges processes. The first technique has been developed for the French nuclear fuel reprocessing industry since the 60's in Marcoule and La Hague. It is a proven and mature technology which has been successfully and quickly implemented by AREVA at Fukushima site for the processing of contaminated waters. The second technique, involving cartridges processes, offers new opportunities for the use of innovative adsorbents. The AREVA process developed for Fukushima and some results obtained on site will be presented as well as laboratory scale results obtained in CEA laboratories. Examples of new adsorbents development for liquid wastes decontamination are also given. A chemical process unit based on co-precipitation technique has been successfully and quickly implemented by AREVA at Fukushima site for the processing of contaminated waters. The asset of this technique is its ability to process large volumes in a continuous mode. Several chemical products can be used to address specific radioelements such as: Cs, Sr, Ru. Its drawback is the production of sludge (about 1% in volume of initial liquid volume). CEA developed strategies to model the co-precipitation phenomena in order to firstly minimize the quantity of added chemical reactants and secondly, minimize the size of co-precipitation units. We are on the way to design compact units that could be mobilized very quickly and efficiently in case of an accidental situation. Addressing the problem of sludge conditioning, cementation appears to be a very attractive solution. Fukushima accident has focused attention on optimizations that should be taken into account in future studies: - To better take account for non-typical aqueous matrixes like seawater; - To enlarge the spectrum of radioelements that can be efficiently processed and especially short lives radioelements that are usually less present in standard effluents resulting from nuclear activities; - To develop reversible solid adsorbents for cartridge-type applications in order to minimize wastes. (authors)

Fournel, B.; Barre, Y.; Lepeytre, C.; Peycelon, H. [CEA Marcoule, DTCD, BP17171, 30207 Bagnols sur Ceze (France); Grandjean, A. [Institut de Chimie Separative de Marcoule, UMR5257 CEA-CNRS-UM2-ENSCM, BP17171, 30207 Bagnols sur Ceze (France); Prevost, T.; Valery, J.F. [AREVA NC, Paris La Defense (France); Shilova, E.; Viel, P. [CEA Saclay, DSM/IRAMIS/SPCSI, 91191 Gif sur Yvette (France)

2012-07-01T23:59:59.000Z

169

7-88 A geothermal power plant uses geothermal liquid water at 160C at a specified rate as the heat source. The actual and maximum possible thermal efficiencies and the rate of heat rejected from this power plant  

E-Print Network (OSTI)

and potential energy changes are zero. 3 Steam properties are used for geothermal water. Properties Using7-31 7-88 A geothermal power plant uses geothermal liquid water at 160ºC at a specified rate saturated liquid properties, the source and the sink state enthalpies of geothermal water are (Table A-4) k

Bahrami, Majid

170

Lithium vanadyl oxalatophosphite: Influence of the water content on the crystal structures and the dehydration scheme  

SciTech Connect

Two new lithium vanadyl oxalatophosphites have been synthesized by hydrothermal treatment. The respective formula are Li{sub 2}(VOHPO{sub 3}){sub 2}C{sub 2}O{sub 4} 6H{sub 2}O (1) and Li{sub 2}(VOHPO{sub 3}){sub 2}C{sub 2}O{sub 4} 4H{sub 2}O (2). The structures of the compounds have been determined by single crystal X-ray diffraction. Compound 1 crystallizes in triclinic symmetry in space group P-1, a=6.3592(2) Å, b=8.0789(3) Å, c=9.1692(3) Å, ?=64.390(2), ?=87.277(2)°, ?=67.624(2) and, compound 2 in monoclinic symmetry, space group P2{sub 1}/a, a=6.3555(2) Å b=12.6368(7) Å c=9.0242(4) Å ?=105.167(3)°. The vanadium phosphite framework consists of infinite chains of corner-sharing vanadium octahedra and hydrogenophosphite tetrahedra. The oxalate groups ensure the connection between the chains. The lithium ions and the water molecules are located between the anionic [(VO){sub 2}(HPO{sub 3}){sub 2}C{sub 2}O{sub 4}]{sup 2?} layers. Thermal behavior of both compounds was carefully studied by combining thermogravimetric analyses and thermal dependant X-ray diffraction in order to study the thermal stability of the layered oxalatophosphites and to see the influence of the decomposition of the carbon-based anions into the final lithium vanadyl phosphate. Various intermediate phases were evidenced and for both compounds the final product was LiVOPO{sub 4}. -- Graphical abstract: Two new lithium vanadyl oxalatophosphites layered compounds, Li{sub 2} (VOHPO{sub 3}){sub 2}C{sub 2}O{sub 4} 6H{sub 2}O (1) and Li{sub 2} (VOHPO{sub 3}){sub 2}C{sub 2}O{sub 4} 4H{sub 2}O (2) have been hydrothermally synthesized. Lithium ions and water molecules are located between the anionic [(VO){sub 2}(HPO{sub 3}){sub 2}C{sub 2}O{sub 4}]{sup 2?} layers. Thermal behaviors were carefully studied by thermogravimetric and thermal dependant X-ray diffraction. Various intermediate phases were evidenced and for both compounds the final product was LiVOPO{sub 4}. Highlights: • The first lithium vanadium oxalatophosphite have been synthesized hydrothermally. • The structure of these compounds is related to vanadium oxalato-phosphates. • Hydrogen bonding in starting material influences the intermediate phase structures. • Thermal decomposition evidences two Li{sub 2}[(VO){sub 2}(HPO{sub 3}){sub 2}C{sub 2}O{sub 4}] anhydrous polymorphs.

Auguste, S.; Alonzo, V. [Sciences Chimiques de Rennes, UMR 6226, Ecole Nationale Supérieure de Chimie de Rennes, CNRS, 11 Allée de Beaulieu, CS 50837, 35708 Rennes Cedex 7 (France); Université Européenne de Bretagne, 12 avenue Janvier, 35000 Rennes (France); Bataille, T. [Sciences Chimiques de Rennes, UMR 6226, Université de Rennes 1, CNRS, Campus de Beaulieu, 35042 Rennes Cedex (France); Université Européenne de Bretagne, 12 avenue Janvier, 35000 Rennes (France); Le Pollès, L. [Sciences Chimiques de Rennes, UMR 6226, Ecole Nationale Supérieure de Chimie de Rennes, CNRS, 11 Allée de Beaulieu, CS 50837, 35708 Rennes Cedex 7 (France); Université Européenne de Bretagne, 12 avenue Janvier, 35000 Rennes (France); Cañón-Mancisidor, W.; Venegas-Yazigi, D. [Facultad de Quimia y Biologia, Universitad de Santiago de Chile, USACH, Casilla, 40 Correo 33, Santiago (Chile); Centro para el Desarrollo de Nanociencias y Nanotecnología, CEDENNA (Chile); Le Fur, E., E-mail: eric.le-fur@ensc-rennes.fr [Sciences Chimiques de Rennes, UMR 6226, Ecole Nationale Supérieure de Chimie de Rennes, CNRS, 11 Allée de Beaulieu, CS 50837, 35708 Rennes Cedex 7 (France); Université Européenne de Bretagne, 12 avenue Janvier, 35000 Rennes (France)

2014-03-15T23:59:59.000Z

171

Evaluation of plasma melter technology for verification of high-sodium content low-level radioactive liquid wastes: Demonstration test No. 4 preliminary test report  

SciTech Connect

This document provides a preliminary report of plasma arc vitrification testing by a vendor in support of the Hanford Tank Waste Remediation System Low-Level Waste (LLW) Vitrification Program. Phase I test conduct included 26 hours (24 hours steady state) of melting of simulated high-sodium low-level radioactive liquid waste. Average processing rate was 4.9 kg/min (peak rate 6.2 kg/min), producing 7330 kg glass product. Free-flowing glass pour point was 1250 C, and power input averaged 1530 kW(e), for a total energy consumption of 19,800 kJ/kg glass. Restart capability was demonstrated following a 40-min outage involving the scrubber liquor heat exchanger, and glass production was continued for another 2 hours. Some volatility losses were apparent, probably in the form of sodium borates. Roughly 275 samples were collected and forwarded for analysis. Sufficient process data were collected for heat/material balances. Recommendations for future work include lower boron contents and improved tuyere design/operation.

McLaughlin, D.F.; Gass, W.R.; Dighe, S.V.; D`Amico, N.; Swensrud, R.L.; Darr, M.F.

1995-01-10T23:59:59.000Z

172

Liquid-Water Uptake and Removal in PEM Fuel-Cell Components  

E-Print Network (OSTI)

Uptake and Removal in PEM Fuel-Cell Components Prodip K. DasWater management in PEM fuel cells is critical for optimumof droplet dynamics in PEM fuel-cell gas flow channels has

Das, Prodip K.

2013-01-01T23:59:59.000Z

173

Advanced Scintillator Detector Concept (ASDC): A Concept Paper on the Physics Potential of Water-Based Liquid Scintillator  

E-Print Network (OSTI)

The recent development of Water-based Liquid Scintillator (WbLS), and the concurrent development of high-efficiency and high-precision-timing light sensors, has opened up the possibility for a new kind of large-scale detector capable of a very broad program of physics. The program would include determination of the neutrino mass hierarchy and observation of CP violation with long-baseline neutrinos, searches for proton decay, ultra-precise solar neutrino measurements, geo- and supernova neutrinos including diff?use supernova antineutrinos, and neutrinoless double beta decay. We outline here the basic requirements of the Advanced Scintillation Detector Concept (ASDC), which combines the use of WbLS, doping with a number of potential isotopes for a range of physics goals, high efficiency and ultra-fast timing photosensors, and a deep underground location. We are considering such a detector at the Long Baseline Neutrino Facility (LBNF) far site, where the ASDC could operate in conjunction with the liquid argon t...

Alonso, J R; Bergevin, M; Bernstein, A; Bignell, L; Blucher, E; Calaprice, F; Conrad, J M; Descamps, F B; Diwan, M V; Dwyer, D A; Dye, S T; Elagin, A; Feng, P; Grant, C; Grullon, S; Hans, S; Jaffe, D E; Kettell, S H; Klein, J R; Lande, K; Learned, J G; Luk, K B; Maricic, J; Marleau, P; Mastbaum, A; McDonough, W F; Oberauer, L; Gann, G D Orebi; Rosero, R; Rountree, S D; Sanchez, M C; Shaevitz, M H; Shokair, T M; Smy, M B; Strait, M; Svoboda, R; Tolich, N; Vagins, M R; van Bibber, K A; Viren, B; Vogelaar, R B; Wetstein, M J; Winslow, L; Wonsak, B; Worcester, E T; Wurm, M; Yeh, M; Zhang, C

2014-01-01T23:59:59.000Z

174

Advanced Scintillator Detector Concept (ASDC): A Concept Paper on the Physics Potential of Water-Based Liquid Scintillator  

E-Print Network (OSTI)

The recent development of Water-based Liquid Scintillator (WbLS), and the concurrent development of high-efficiency and high-precision-timing light sensors, has opened up the possibility for a new kind of large-scale detector capable of a very broad program of physics. The program would include determination of the neutrino mass hierarchy and observation of CP violation with long-baseline neutrinos, searches for proton decay, ultra-precise solar neutrino measurements, geo- and supernova neutrinos including diffuse supernova antineutrinos, and neutrinoless double beta decay. We outline here the basic requirements of the Advanced Scintillation Detector Concept (ASDC), which combines the use of WbLS, doping with a number of potential isotopes for a range of physics goals, high efficiency and ultra-fast timing photosensors, and a deep underground location. We are considering such a detector at the Long Baseline Neutrino Facility (LBNF) far site, where the ASDC could operate in conjunction with the liquid argon tracking detector proposed by the LBNE collaboration. The goal is the deployment of a 30-100 kiloton-scale detector, the basic elements of which are being developed now in experiments such as WATCHMAN, ANNIE, SNO+, and EGADS.

J. R. Alonso; N. Barros; M. Bergevin; A. Bernstein; L. Bignell; E. Blucher; F. Calaprice; J. M. Conrad; F. B. Descamps; M. V. Diwan; D. A. Dwyer; S. T. Dye; A. Elagin; P. Feng; C. Grant; S. Grullon; S. Hans; D. E. Jaffe; S. H. Kettell; J. R. Klein; K. Lande; J. G. Learned; K. B. Luk; J. Maricic; P. Marleau; A. Mastbaum; W. F. McDonough; L. Oberauer; G. D. Orebi Gann; R. Rosero; S. D. Rountree; M. C. Sanchez; M. H. Shaevitz; T. M. Shokair; M. B. Smy; A. Stahl; M. Strait; R. Svoboda; N. Tolich; M. R. Vagins; K. A. van Bibber; B. Viren; R. B. Vogelaar; M. J. Wetstein; L. Winslow; B. Wonsak; E. T. Worcester; M. Wurm; M. Yeh; C. Zhang

2014-10-24T23:59:59.000Z

175

The influence of irrigation water salinity on optimal nitrogen, phosphorus, and potassium liquid fertilizer rates  

E-Print Network (OSTI)

of nitrogen fertilizer to compensate for leaching losses (Miyamoto, 1984). The effect of salt stress on mineral status of plants has been studied extensively for many agronomic and horticultural crops (Al-Saidi and Alawi, 1984; Al-Saidi et al. , 1985... cultivars (Al-Saidi and Alawi, 1984; Al- Saidi et al. , 1985). Ten flowering annuals were grown in saline water with electrical conductivities of 0. 8, 1. 5, 3. 0, or 4. 5 dS m from a 2:1 equivalent weight basis of CaCI2 and NaCI in tap water (Devitt...

Campos Nu?n?ez, Ricardo

2012-06-07T23:59:59.000Z

176

Organic Tank Safety Project: development of a method to measure the equilibrium water content of Hanford organic tank wastes and demonstration of method on actual waste  

SciTech Connect

Some of Hanford`s underground waste storage tanks contain Organic- bearing high level wastes that are high priority safety issues because of potentially hazardous chemical reactions of organics with inorganic oxidants in these wastes such as nitrates and nitrites. To ensure continued safe storage of these wastes, Westinghouse Hanford Company has placed affected tanks on the Organic Watch List and manages them under special rules. Because water content has been identified as the most efficient agent for preventing a propagating reaction and is an integral part of the criteria developed to ensure continued safe storage of Hanford`s organic-bearing radioactive tank wastes, as part of the Organic Tank Safety Program the Pacific Northwest National Laboratory developed and demonstrated a simple and easily implemented procedure to determine the equilibrium water content of these potentially reactive wastes exposed to the range of water vapor pressures that might be experienced during the wastes` future storage. This work focused on the equilibrium water content and did not investigate the various factors such as @ ventilation, tank surface area, and waste porosity that control the rate that the waste would come into equilibrium, with either the average Hanford water partial pressure 5.5 torr or other possible water partial pressures.

Scheele, R.D.; Bredt, P.R.; Sell, R.L.

1996-09-01T23:59:59.000Z

177

Liquid Water Transport in Gas Diffusion Layer of Polymer Electrolyte Fuel Cells  

E-Print Network (OSTI)

. In addition, at high current densities, excessive amount of water is generated and condenses, filling as a promising candidate for high-efficiency, low-emission power sources. High-current-density operation of PEFCs, The Pennsylvania State University, University Park, Pennsylvania 16802, USA High-current-density performance

178

Water clusters: Untangling the mysteries of the liquid, one molecule at a time  

Science Journals Connector (OSTI)

...the structures of clathrate hydrates (95). The hexamer represents...water hexamer determined in the gas phase resembles the basic unit...100 Feynman R P Leighton R B Sands M ( 1964 ) in The Feynman Lectures...eds Feynman R P Leighton R B Sands M ( Addison–Wesley , Reading...

Frank N. Keutsch; Richard J. Saykally

2001-01-01T23:59:59.000Z

179

Limestone-Particle-Stabilized Macroemulsion of Liquid and Supercritical Carbon Dioxide in Water for Ocean Sequestration  

Science Journals Connector (OSTI)

In relation to ocean disposal of CO2 from power plants, a comprehensive plume model was developed to simulate the dynamic, near-field behavior of CO2 released in the water column as either a buoyant liq. ... from flue gases and injected into the oceans. ...

D. Golomb; E. Barry; D. Ryan; C. Lawton; P. Swett

2004-07-20T23:59:59.000Z

180

Task 15 -- Remediation of organically contaminated soil using hot/liquid (subcritical) water. Semi-annual report, April 1--September 30, 1997  

SciTech Connect

This activity involves a pilot-scale demonstration of the use of hot/liquid water for the removal of organic contaminants from soil at the pilot (20 to 40 kg) scale. Lab-scale studies are being performed to determine the optimum temperature, contact time, and flow rates for removal of the organic contaminants. Initial investigations into using carbon sorbents to clean the extractant water for recycle use and to concentrate the extracted contaminants in a small volume for disposal are also being performed. Liquid water is normally considered to be too polar a solvent to be effective for removal of organic contaminants from contaminated soils and sludges. However, the Energy and Environmental Research Center (EERC) has demonstrated that the polarity of liquid water can be changed from that of a very polar solvent at ambient conditions to that of an organic solvent (e.g., ethanol or acetonitrile) by simply raising the temperature. The EERC has exploited this unique property of liquid water to obtain highly selective extractions of polar (at lower temperatures) to nonpolar (at 200 to 250 C) organics from contaminated soils and sludges. Only moderate pressures (a maximum of about 45 atm at 250 C and lower pressures at lower temperatures) are required. With this procedure, all detectable hazardous organics were removed from the sludge, thus making the remaining material (about 99% of the original mass) a nonhazardous material. The present understanding of hot/liquid water extraction for the removal of hazardous organics from contaminated soils and sludges is being used to develop the engineering parameters needed to perform a pilot-scale demonstration of the remediation technology. Progress during the report period is summarized.

Hawthorne, S.B.

1997-12-31T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


181

Generating Singlet Oxygen Bubbles: A New Mechanism for Gas–Liquid Oxidations in Water  

Science Journals Connector (OSTI)

Our interest in developing a singlet oxygen [1O2 (1?g)]-sparging reactor came from small-scale devices for disinfection of, for example, municipal and well water, but which used filtration, ozone, and/or UV light. ... In front of the A10449 mechanical shutter of the detector was placed either a 25-mm-diameter, 1150 nm long pass filter (FEL1150, Thorlabs Inc.) or one of three 25-mm-diameter NIR bandpass filters centered at 1220, 1270, and 1315 nm (OD4 blocking, fwhm = 15 nm, Omega, Brattleboro, VT). ... (19) Drying of the composite was done at 50 °C for 10 h to avoid destruction of the confined phthalocyanine molecules, producing an aerogel that shrunk ?10% where some, but not all adsorbed water was removed. ...

Dorota Bartusik; David Aebisher; BiBi Ghafari; Alan M. Lyons; Alexander Greer

2012-01-20T23:59:59.000Z

182

Viscosity, specific (for liquids)  

Science Journals Connector (OSTI)

n. The ratio between the viscosity of a liquid and the viscosity of water at the same temperature. Specific viscosity is sometimes used interchangeably with relative viscosity for liquids.

2007-01-01T23:59:59.000Z

183

Pore-scale simulation of liquid CO2 displacement of water using a two-phase lattice Boltzmann model  

SciTech Connect

A lattice Boltzmann color-fluid model, which was recently proposed by Liu et al. [H. Liu, A.J. Valocchi, and Q. Kang. Three-dimensional lattice Boltzmann model for immiscible two-phase flow simulations. Phys. Rev. E, 85:046309, 2012.] based on a concept of continuum surface force, is improved to simulate immiscible two-phase flows in porous media. The new improvements allow the model to account for different kinematic viscosities of both fluids and to model fluid-solid interactions. The capability and accuracy of this model is first validated by two benchmark tests: a layered two-phase flow with a viscosity ratio, and a dynamic capillary intrusion. This model is then used to simulate liquid CO2 (LCO2) displacing water in a dual-permeability pore network. The extent and behavior of LCO2 preferential flow (i.e., fingering) is found to depend on the capillary number (Ca), and three different displacement patterns observed in previous micromodel experiments are reproduced. The predicted variation of LCO2 saturation with Ca, as well as variation of specific interfacial length with LCO2 saturation, are both in good agreement with the experimental observations. To understand the effect of heterogeneity on pore-scale displacement, we also simulate LCO2 displacing water in a randomly heterogeneous pore network, which has the same size and porosity as the dual-permeability pore network. In comparison to the dual-permeability case, the transition from capillary fingering to viscous fingering occurs at a higher Ca, and LCO2 saturation is higher at low Ca but lower at high Ca. In either pore network, the LCO2-water specific interfacial length is found to obey a power-law dependence on LCO2 saturation.

Liu, Haihu; Valocchi, Albert J.; Werth, Charles J.; Kang, Oinjun; Oostrom, Martinus

2014-11-01T23:59:59.000Z

184

A system to test the effects of materials on the electron drift lifetime in liquid argon and observations on the effect of water  

SciTech Connect

A materials test system (MTS) has been developed at FNAL to assess the suitability of materials for use in a large liquid argon time projection chamber. During development of the MTS, it was noted that controlling the cryostat pressure with a 'raining' condenser reduced the electron drift lifetime in the liquid argon. The effect of condensing has been investigated using a series of passive materials to filter the condensate. We report the results of these studies and of tests on different candidate materials for detector construction. The inferred reduction of electron drift lifetime by water concentrations in the parts per trillion is of particular interest.

Andrews, R.; Jaskierny, W.; Jostlein, H.; Kendziora, C.; Pordes, S.; Tope, T.; /Fermilab; ,

2009-07-01T23:59:59.000Z

185

Ceramicrete stabilization of radioactive-salt-containing liquid waste and sludge water. Final CRADA report.  

SciTech Connect

It was found that the Ceramicrete Specimens incorporated the Streams 1 and 2 sludges with the adjusted loading about 41.6 and 31.6%, respectively, have a high solidity. The visible cracks in the matrix materials and around the anionite AV-17 granules included could not obtain. The granules mentioned above fixed by Ceramicrete matrix very strongly. Consequently, we can conclude that irradiation of Ceramecrete matrix, goes from the high radioactive elements, not result the structural degradation. Based on the chemical analysis of specimens No.462 and No.461 used it was shown that these matrix included the formation elements (P, K, Mg, O), but in the different samples their correlations are different. These ratios of the content of elements included are about {+-} 10%. This information shows a great homogeneity of matrix prepared. In the list of the elements founded, expect the matrix formation elements, we detected also Ca and Si (from the wollastonite - the necessary for Ceramicrete compound); Na, Al, S, O, Cl, Fe, Ni also have been detected in the Specimen No.642 from the waste forms: NaCl, Al(OH){sub 3}, Na{sub 2}SO{sub 4}. Fe(OH){sub 3}, nickel ferrocyanide and Ni(NO{sub 3})2. The unintelligible results also were found from analysis of an AV-17 granules, in which we obtain the great amount of K. The X-ray radiographs of the Ceramicrete specimens with loading 41.4 % of Stream 1 and 31.6% of Stream 2, respectively showed that the realization of the advance technology, created at GEOHKI, leads to formation of excellent ceramic matrix with high amount of radioactive streams up to 40% and more. Really, during the interaction with start compounds MgO and KH{sub 2}PO{sub 4} with the present of H{sub 3}BO{sub 3} and Wollastonite this process run with high speed under the controlled regimes. That fact that the Ceramicrete matrix with 30-40% of Streams 1 and 2 have a crystalline form, not amorphous matter, allows to permit that these matrix should be very stable, reliable for incorporation of a radionuclides.

Ehst, D.; Nuclear Engineering Division

2010-08-04T23:59:59.000Z

186

CEDR Content  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

CEDR Content" CEDR Content" "The Consolidated Energy Data Report (CEDR) consists of 27 worksheets that should be completed by each site, as applicable, and included as part each site's SSP in a MS Excel electronic format. The CEDR is due to the SPO no later than December 9th." "Worksheet",,"Overview","Action" 1.1,"Content","Stand-alone overview of the CEDR tabs.","None" 2.1,"Funds, Meters, Training","Collects information on energy and water spending, and metering status.","If applicable, complete cells highlighted in orange. Edited and new data cells should be highlighted in light blue." 3.1,"BTU & Gal Key","Reference tab containing all factors and dropdown menu information for all tabs starting with ""3"". If you need to divide up the CEDR, please keep all tabs starting with ""3"" together to ensure calculation links are not broken. ","None"

187

Using radiative transfer models to study the atmospheric water vapor content and to eliminate telluric lines from high-resolution optical spectra  

E-Print Network (OSTI)

The Radiative Transfer Model (RTM) and the retrieval algorithm, incorporated in the SCIATRAN 2.2 software package developed at the Institute of Remote Sensing/Institute of Enviromental Physics of Bremen University (Germany), allows to simulate, among other things, radiance/irradiance spectra in the 2400-24 000 {\\AA} range. In this work we present applications of RTM to two case studies. In the first case the RTM was used to simulate direct solar irradiance spectra, with different water vapor amounts, for the study of the water vapor content in the atmosphere above Sierra Nevada Observatory. Simulated spectra were compared with those measured with a spectrometer operating in the 8000-10 000 {\\AA} range. In the second case the RTM was used to generate telluric model spectra to subtract the atmospheric contribution and correct high-resolution stellar spectra from atmospheric water vapor and oxygen lines. The results of both studies are discussed.

Gardini, A; Pérez, E; Quesada, J A; Funke, B

2012-01-01T23:59:59.000Z

188

Cloud Liquid Water Measurements  

E-Print Network (OSTI)

Pdry ­ Dry Power Term Pwet ­ Wet Power Term P=PdryPwet #12;Dry Power Term Energy is transferred, and temperature PdryC Ts-Ta pv x King et. al, 1981 · C ­ Calibration Constant · x - Calibration Constant · Ts the fact that this model does not pass through (0,0). va=kvx a #12;Calibration Equation Dry Term is: Pdry

Delene, David J.

189

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1997" Annual",2012,"6/30/1997" ,"Data 2","Futures Prices",4,"Annual",2012,"6/30/1993" ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","ng_pri_fut_s1_a.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/ng/ng_pri_fut_s1_a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:13 PM" "Back to Contents","Data 1: Spot Price" "Sourcekey","RNGWHHD","NGM_EPG0_PLC_NUS_DMMBTU" "Date","Henry Hub Natural Gas Spot Price (Dollars per Million Btu)","U.S. Natural Gas Liquid Composite Price (Dollars per Million Btu)"

190

Efficient production of 5-hydroxymethylfurfural through the dehydration of sugars with caprolactam hydrogen sulfate ([CPL]HSO4) ionic liquid catalyst in a water/proprylene glycol monomethyl ether mixed solvent  

Science Journals Connector (OSTI)

Efficient production of 5-hydroxymethylfurfural (HMF) through the dehydration of sugars...4) ionic liquid or using metal halide as the co-catalyst in a new water/proprylene glycol monomethyl ether solvent system....

Pingzhen Huang; Aijuan Gu; Jinxing Wang

2014-04-01T23:59:59.000Z

191

FDR for non destructive evaluation: inspection of external post-tensioned ducts and measurement of water content in concrete  

E-Print Network (OSTI)

are involved in research programs dedicated to concrete Thermo-Hydro- Mechanical (THM) modeling and to in situ content in concrete (nuclear structures and nuclear waste repositories) is a major topic to understand to Structure Safety for Nuclear and Pressurized Components, France (2013)" #12;The height of each material hn

Boyer, Edmond

192

Energetics of Hydrogen Bond Network Rearrangements in Liquid...  

NLE Websites -- All DOE Office Websites (Extended Search)

Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Energetics of Hydrogen Bond Network Rearrangements in Liquid Water Print Wednesday, 25 May 2005 00:00 The unique...

193

Formation of Liquid Methane-Water Mixture during Combustion of a Laminar Methane Jet at Supercritical Pressures  

E-Print Network (OSTI)

and sometimes exceeding 10 MPa. For example, current aviation gas turbines operate at conditions approaching 4 MPa, and the pressures in the liquid propellant rocket engine combustion chambers may reach up to 20

Gülder, �mer L.

194

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Gas Plant Liquids Production, Gaseous Equivalent (Million Cubic Feet)","Alaska--State Offshore Natural Gas Plant Liquids Production, Gaseous Equivalent (Million Cubic...

195

Frostbite Theater - Liquid Nitrogen Experiments - Dry Ice vs. Liquid  

NLE Websites -- All DOE Office Websites (Extended Search)

Egg + Liquid Nitrogen + Time-lapse! Egg + Liquid Nitrogen + Time-lapse! Previous Video (Egg + Liquid Nitrogen + Time-lapse!) Frostbite Theater Main Index Next Video (Liquid Nitrogen Cooled Dry Ice in Water!) Liquid Nitrogen Cooled Dry Ice in Water! Dry Ice vs. Liquid Nitrogen! Dry ice is cold. Liquid nitrogen is cold, too. What happens when the two are mixed together? [ Show Transcript ] Announcer: Frostbite Theater presents... Cold Cuts! No baloney! Joanna and Steve: Just science! Joanna: Hi! I'm Joanna! Steve: And I'm Steve! Joanna: Have you ever wondered what happens when you mix dry ice and liquid nitrogen? Steve: Well, we just happen to have a chunk of dry ice left over from when we filmed 'How to Make a Cloud Chamber,' and here at Jefferson Lab, liquid nitrogen flows like water, so we're going to find out!

196

Effect of Water Content on Conversion of d-Cellobiose into 5-Hydroxymethyl-2-furaldehyde in a Dimethyl Sulfoxide–Water Mixture  

Science Journals Connector (OSTI)

Noncatalytic conversion of d-cellobiose (at 0.5 M) into 5-hydroxymethyl-2-furaldehyde (5-HMF), a platform chemical for fuels and synthetic materials, was analyzed at 120–200 °C over a wide range of water mole fraction, xw = 0.007–1 in a binary dimethyl sulfoxide (DMSO)–water mixture by means of the in situ 13C NMR spectroscopy. ... Biomass has attracted attention as a promising source of sustainable fuels and valuable platform chemicals. ... For developing the conversion of cellulosic biomass into 5-HMF, we should move forward to examine model oligosaccharides closer to cellulosic biomass from the viewpoint of green chemistry. ...

Hiroshi Kimura; Ken Yoshida; Yasuhiro Uosaki; Masaru Nakahara

2013-10-23T23:59:59.000Z

197

Methodology for Predicting Water Content in Supercritical Gas Vapor and Gas Solubility in Aqueous Phase for Natural Gas Process  

Science Journals Connector (OSTI)

The streams in the natural gas process contain light hydrocarbons, mainly methane and ethane, associated with non-hydrocarbon supercritical gases (nitrogen, hydrogen, argon, etc.). ... For system that contains supercritical gases, the gas solubility in water can be related to the Henry's law constant. ...

Chorng H. Twu; Suphat Watanasiri; Vince Tassone

2007-09-22T23:59:59.000Z

198

Design of a Shadowband Spectral Radiometer for the Retrieval of Thin Cloud Optical Depth, Liquid Water Path, and the Effective Radius  

SciTech Connect

The design and operation of a Thin-Cloud Rotating Shadowband Radiometer (TCRSR) described here was used to measure the radiative intensity of the solar aureole and enable the simultaneous retrieval of cloud optical depth, drop effective radius, and liquid water path. The instrument consists of photodiode sensors positioned beneath two narrow metal bands that occult the sun by moving alternately from horizon to horizon. Measurements from the narrowband 415-nm channel were used to demonstrate a retrieval of the cloud properties of interest. With the proven operation of the relatively inexpensive TCRSR instrument, its usefulness for retrieving aerosol properties under cloud-free skies and for ship-based observations is discussed.

Bartholomew M. J.; Reynolds, R. M.; Vogelmann, A. M.; Min, Q.; Edwards, R.; Smith, S.

2011-11-01T23:59:59.000Z

199

Physiological changes in cultured Sorghum bicolor (L.) Moench cells in response to induced water stress: osmotic potential, relative water content, carbohydrates, organic acids, potassium, and amino acids  

E-Print Network (OSTI)

, Table 1). At week 2 the weight of absorbed PEG in DT-s was 50% of its DW and 1. 8 times more than that of DS-s. It is obvious then that calculations could be misleading if the added weight of PEG is not subtracted 28 v 9 / III 9 S00 450 400 2S0... differences, and Duncan's test of pEG content of DT and DS calli in control and stressed conditions. (a). Cultivar-treatment WEEK 0 1 2 4 7 DT-c DT-s S S S S DT-c DS-c DT-s DS-s S S DS-c DS-s S S S S 29 TABLE 1. Continued. (h) WEEK 0...

Diquez, Ricardo

2012-06-07T23:59:59.000Z

200

Surfactant-assisted spreading of an oil-in-water emulsion on the surface of a liquid bath  

E-Print Network (OSTI)

This fluid dynamics video shows how an oil-in-water emulsion stabilized by an ionic surfactant spreads on the free surface of a layer of pure water. The spreading shows two intriguing features: a transparent area surrounding the source of oil droplets, and a fast retraction of the layer of oil droplets on itself once the source has emptied. We show that the dynamics of spreading are strongly connected to the interfacial/bulk properties of the surfactant.

Roche, Matthieu; Griffiths, Ian; Saint-Jalmes, Arnaud; Stone, Howard A

2010-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


201

Comparison of Cloud Fraction and Liquid Water Path between ECMWF simulations and ARM long-term Observations at the NSA Site  

NLE Websites -- All DOE Office Websites (Extended Search)

this poster, seasonal and annual variations of this poster, seasonal and annual variations of cloudiness and liquid water path (LWP) from European Center for Medium-Range Weather Forecasts (ECMWF) model were compared with surface measurement from the ARM Climate Research Facility (ARCF) North Slope of Alaska ( N S A ) s i t e b e t we e n J a n u a r y 1 9 9 9 and December 2004. ● Model simulated large scale features match well with observations. ● There are significant differences in cloud vertical and temporal distributions and in the magnitude. FIG. 1: Time-height display of cloud fraction from model simulations and observations in September 1999. ● Model overestimates high clouds, especially in warm seasons. ● Model makes close estimation for middle clouds. ● Model underestimates low clouds in warm seasons, especially in

202

Water and Energy Issues in Gas-to-Liquid Processes: Assessment and Integration of Different Gas-Reforming Alternatives  

Science Journals Connector (OSTI)

Energy and water management effects are analyzed for the development of syngas processes under the integration of three gas reforming alternatives ... Gandrick et al.(9) considered the recycling of the light gas from FT synthesis and refining areas to fire gas turbines to produce electricity and the reuse of the gas turbines to produce superheated steam. ... We address in this paper several aspects related to such issues: (a) A comparative analysis is developed for assesing the impact of the use of different reforming technologies on energy and water usage. ...

Diana Yered Martínez; Arturo Jiménez-Gutiérrez; Patrick Linke; Kerron J. Gabriel; Mohamed M. B. Noureldin; Mahmoud M. El-Halwagi

2013-10-24T23:59:59.000Z

203

Solid-Phase Extraction Combined with High-Performance Liquid Chromatography?Atmospheric Pressure Chemical Ionization?Mass Spectrometry Analysis of Pesticides in Water:? Method Performance and Application in a Reconnaissance Survey of Residues in Drinking Water in Greater Cairo, Egypt  

Science Journals Connector (OSTI)

Solid-Phase Extraction Combined with High-Performance Liquid Chromatography?Atmospheric Pressure Chemical Ionization?Mass Spectrometry Analysis of Pesticides in Water:? Method Performance and Application in a Reconnaissance Survey of Residues in Drinking Water in Greater Cairo, Egypt ... Each shipment, which included 24 cartridges, weighed <454 g and cost approximately 200 Egyptian pounds ($40 U.S.). ...

Thomas L. Potter; Mahmoud A. Mohamed; Hannah Ali

2006-12-22T23:59:59.000Z

204

Parameterization of GDL Liquid Water Front Propagation and Channel Accumulation for Anode Purge Scheduling in Fuel Cells  

E-Print Network (OSTI)

. I. INTRODUCTION Water produced at the cathode catalyst layer can diffuse back to the anode side due of the catalyst support in the cathode [4]. Therefore, scheduling an occasional purge of the anode volume that was observed via neutron imaging of an operational 53 cm2 PEMFC. Simulation results for the GDL and Membrane

Stefanopoulou, Anna

205

ESTABLISHMENT OF A METHOD FOR 222RN DETERMINATION IN WATER BY LOW-LEVEL LIQUID SCINTILLATION COUNTER  

Science Journals Connector (OSTI)

......region, northern part of Serbia: it includes Novi Sad-the capital city of Vojvodina with 400 000 inhabitants, and Fruska Gora...because of numerous underground hot springs and sources of natural gas, as well as some crude oil reservoirs(6). The water samples......

Nataša Todorovi?; Ivana Jakoni?; Jovana Nikolov; Jan Hansman; Miroslav Veskovi?

2014-07-01T23:59:59.000Z

206

1.2 What pressure difference must be generated across the length of a 15 cm vertical drinking straw in order to drink a water-like liquid of density 1.0 g cm-3  

E-Print Network (OSTI)

in order to drink a water-like liquid of density 1.0 g cm-3 ? 1.6 Charles' law is sometimes expressed1.2 What pressure difference must be generated across the length of a 15 cm vertical drinking straw

Findley, Gary L.

207

ARM - Measurement - Total cloud water  

NLE Websites -- All DOE Office Websites (Extended Search)

cloud water cloud water ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Measurement : Total cloud water The total concentration (mass/vol) of ice and liquid water particles in a cloud; this includes condensed water content (CWC). Categories Cloud Properties Instruments The above measurement is considered scientifically relevant for the following instruments. Refer to the datastream (netcdf) file headers of each instrument for a list of all available measurements, including those recorded for diagnostic or quality assurance purposes. External Instruments NCEPGFS : National Centers for Environment Prediction Global Forecast System Field Campaign Instruments CSI : Cloud Spectrometer and Impactor PDI : Phase Doppler Interferometer

208

Indirect thermal liquefaction process for producing liquid fuels from biomass  

SciTech Connect

A progress report on an indirect liquefaction process to convert biomass type materials to quality liquid hydrocarbon fuels by gasification followed by catalytic liquid fuels synthesis has been presented. A wide variety of feedstocks can be processed through the gasification system to a gas with a heating value of 500 + Btu/SCF. Some feedstocks are more attractive than others with regard to producing a high olefin content. This appears to be related to hydrocarbon content of the material. The H/sub 2//CO ratio can be manipulated over a wide range in the gasification system with steam addition. Some feedstocks require the aid of a water-gas shift catalyst while others appear to exhibit an auto-catalytic effect to achieve the conversion. H/sub 2/S content (beyond the gasification system wet scrubber) is negligible for the feedstocks surveyed. The water gas shift reaction appears to be enhanced with an increase in pyrolysis reactor temperature over the range of 1300 to 1700/sup 0/F. Reactor temperature in the Fischer-Tropsch step is a significant factor with regard to manipulating product composition analysis. The optimum temperature however will probably correspond to maximum conversion to liquid hydrocarbons in the C/sub 5/ - C/sub 17/ range. Continuing research includes integrated system performance assessment, alternative feedstock characterization (through gasification) and factor studies for gasification (e.g., catalyst usage, alternate heat transfer media, steam usage, recycle effects, residence time study) and liquefaction (e.g., improved catalysts, catalyst activity characterization).

Kuester, J.L.

1980-01-01T23:59:59.000Z

209

Sub-second Morphological Changes in Nafion during Water Uptake Detected by Small-Angle X-Ray Scattering  

SciTech Connect

The ability of Nafion® membrane to absorb water rapidly and create a network of hydrated interconnected water domains provides this material with an unmatched ability to conduct ions through a chemically and mechanically robust membrane. The morphology and composition of these hydrated membranes significantly affects their transport properties and performance. This work demonstrates that differences in interfacial interactions between the membranes exposed to vapor or liquid water can cause significant changes in kinetics of water uptake. In-situ small-angle X-ray scattering (SAXS) experiments captured the rapid swelling of the membrane in liquid water with nanostructure rearrangement on the order of seconds. For membranes in contact with water vapor, morphological changes are four-orders-of-magnitude slower than in liquid water, suggesting that interfacial resistance limits the penetration of water into the membrane. Also, upon water absorption from liquid water, a structural rearrangement from a distribution of spherical and cylindrical domains to exclusively cylindrical-like domains is suggested. These differences in water-uptake kinetics and morphology provide a new perspective into Schroeder’s Paradox, which dictates different water contents for vaporand liquid-equilibrated ionomers at unit activity. The findings of this work provide critical insights into the fast kinetics of water absorption of Nafion membrane, which can aid in the design of energy conversion devices that operate under frequent changes in environmental conditions.

Kusoglu, Ahmet; Modestino, Miguel A.; Hexemer, Alexander; Segalman, Rachel A.; Weber, Adam Z.

2011-09-30T23:59:59.000Z

210

Constrained water cloud generator  

Science Journals Connector (OSTI)

The fast generation of large cloudy volumes with imposed cloud cover fractions and ambient vertical profiles is very important for the realistic simulation of atmospheric scenes. The model proposed here is the second step of a two-step model composed on the one hand of a volume generator based on a Fourier filtering method and on the other hand of a physical generator filling the volume with physical parameters. After a description of the general generation scheme, this paper focuses on the simulation of vertical profiles of water content (liquid, vapour) coupled with other state parameters (temperature, pressure, vertical velocity) via thermodynamic and hydrodynamic equations by local forcing of ambient conditions. The method for solving these equations is explained and applied to practical cases. First, by assuming that the actual temperature at the cloud base is equal to the dew temperature and by imposing a moist pseudo-adiabatic temperature gradient between the cloud top and bottom, the temperature profile in the cloud is found. When conditional instability occurs, the initial temperature profile between the ground and the cloud base is iteratively shifted to lower values until absolute stability is reached. Then the liquid water content is calculated by integrating the equation of water conservation, and the water vapour content by assuming that the cloud is everywhere saturated. Eventually, the vertical velocity is estimated by integration of the momentum equation. This method gives results in good agreement with published measurements, analytical and numerical models. Eventually, further developments of the column model, including the effects of phase transitions, turbulence, horizontal motions and mixing with the surrounding medium, are proposed in the concluding section.

Roland P.H. Berton

2008-01-01T23:59:59.000Z

211

Numerical Simulation of Hydrodynamics of a Heavy Liquid Drop Covered by Vapor Film in a Water Pool  

SciTech Connect

A numerical study on the hydrodynamics of a droplet covered by vapor film in water pool is carried out. Two level set functions are used as to implicitly capture the interfaces among three immiscible fluids (melt-drop, vapor and coolant). This approach leaves only one set of conservation equations for the three phases. A high-order Navier-Stokes solver, called Cubic-Interpolated Pseudo-Particle (CIP) algorithm, is employed in combination with level set approach, which allows large density ratios (up to 1000), surface tension and jump in viscosity. By this calculation, the hydrodynamic behavior of a melt droplet falling into a volatile coolant is simulated, which is of great significance to reveal the mechanism of steam explosion during a hypothetical severe reactor accident. (authors)

Ma, W.M.; Yang, Z.L.; Giri, A.; Sehgal, B.R. [Royal Institute of Technology (KTH), Drottning Kristinas vaeg 33 A, 100 44, Stockholm (Sweden)

2002-07-01T23:59:59.000Z

212

Reading Comprehension - Liquid Nitrogen  

NLE Websites -- All DOE Office Websites (Extended Search)

Liquid Nitrogen Liquid Nitrogen Nitrogen is the most common substance in Earth's _________ crust oceans atmosphere trees . In the Earth's atmosphere, nitrogen is a gas. The particles of a gas move very quickly. They run around and bounce into everyone and everything. The hotter a gas is, the _________ slower faster hotter colder the particles move. When a gas is _________ cooled warmed heated compressed , its particles slow down. If a gas is cooled enough, it can change from a gas to a liquid. For nitrogen, this happens at a very _________ strange warm low high temperature. If you want to change nitrogen from a gas to a liquid, you have to bring its temperature down to 77 Kelvin. That's 321 degrees below zero _________ Kelvin Celsius Centigrade Fahrenheit ! Liquid nitrogen looks like water, but it acts very differently. It

213

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Name","Description"," Of Series","Frequency","Latest Data for" ,"Data 1","New York Heat Content of Natural Gas Deliveries to Consumers (BTU per Cubic...

214

energy content  

Science Journals Connector (OSTI)

energy content, (weight) strength ? Arbeitsvermögen n (im ballistischen Mörser gemessen), Sprengenergie f (im ballistischen Mörser gemessen) [Mit 10 g Sprengstoff ermittelt

2014-08-01T23:59:59.000Z

215

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Heat Content of Natural Gas Deliveries to Consumers (BTU per Cubic Foot)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

216

Effect of differing mineral contents in process water on the quantity and nitrogen concentration of protein isolates from defatted soy and cottonseed flours  

E-Print Network (OSTI)

solids and nitrogen in the whey fractions. Positive effects of using deionized process waters in the cotton- seed protein isolation process were shown only with non-storage protein (NSP) curds, the minor isolates. Deionized process waters increased... of deionization of process water on curd 25 28 Effect of deionization of process water on whey . . . . . 35 Results from cottonseed protein isolation process . . . . . . . 36 Effect of deionization of process water on residue . 42 Effect of deionization...

Kim, Heikyung

2012-06-07T23:59:59.000Z

217

Energy content: 43 to 47 KJ/gram not much different from candlewax or candybars (physical density of gasoline is about .73 times that of water (.73 g/cc...it floats!).  

E-Print Network (OSTI)

GASOLINE: Energy content: 43 to 47 KJ/gram not much different from candlewax or candybars (physical density of gasoline is about .73 times that of water (.73 g/cc...it floats!). Coal...15 to 19 KJ/gram H H-C-C-C-C-C-C-C-C-H Decane | | | | | | | | | | H H H H H H H H H H Typical molecules found in gasoline Rough Values of Power

218

Frostbite Theater - Liquid Nitrogen Experiments - Liquid Nitrogen and  

NLE Websites -- All DOE Office Websites (Extended Search)

Freeze the Rainbow! Freeze the Rainbow! Previous Video (Freeze the Rainbow!) Frostbite Theater Main Index Next Video (Liquid Nitrogen and Fire!) Liquid Nitrogen and Fire! Liquid Nitrogen and Antifreeze! What happens when the freezing power of liquid nitrogen meets the antifreezing power of ethylene glycol? [ Show Transcript ] Announcer: Frostbite Theater presents... Cold Cuts! No baloney! Joanna and Steve: Just science! Joanna: Hi! I'm Joanna! Steve: And I'm Steve! Joanna: What happens when the freezing power of liquid nitrogen... Steve: ...meets the antifreezing power of ethylene glycol! Joanna: While a mix of 70 percent ethylene glycol and 30 percent water doesn't freeze until 60 degrees below zero, it's still no match for liquid nitrogen. At 321 degrees below zero, liquid nitrogen easily freezes

219

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

222014 5:11:47 PM" "Back to Contents","Data 1: U.S. Gasoline and Diesel Retail Prices" "Sourcekey","EMMEPM0PTENUSDPG","EMMEPM0UPTENUSDPG","EMMEPM0RPTENUS...

220

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,,"(202) 586-8800",,,"1162014 3:08:27 PM" "Back to Contents","Data 1: Missouri Natural Gas Gross Withdrawals from Oil Wells (MMcf)" "Sourcekey","N9012MO2" "Date","Missouri...

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


221

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,,"(202) 586-8800",,,"9262014 3:44:37 PM" "Back to Contents","Data 1: Natural Gas Pipeline & Distribution Use " "Sourcekey","N9170US2","NA1480SAL2","NA1480SAK2","NA1480SAZ...

222

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

PM" "Back to Contents","Data 1: Price of Liquefied U.S. Natural Gas Re-Exports to Russia (Dollars per Thousand Cubic Feet)" "Sourcekey","NGMEPG0ERENUS-NRSDMCF"...

223

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:55 PM" "Back to Contents","Data 1: Natural...

224

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:03 PM" "Back to Contents","Data 1: Texas...

225

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:41 PM" "Back to Contents","Data 1: Natural...

226

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:11:23 PM" "Back to Contents","Data 1:...

227

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:32:23 PM" "Back to Contents","Data 1:...

228

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:04 PM" "Back to Contents","Data 1: Virginia...

229

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:26:30 PM" "Back to Contents","Data 1: Alabama...

230

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:01 PM" "Back to Contents","Data 1: Rhode...

231

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:58 PM" "Back to Contents","Data 1: Natural...

232

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:23 PM" "Back to Contents","Data 1: Vermont...

233

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:10 PM" "Back to Contents","Data 1:...

234

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:00 PM" "Back to Contents","Data 1: Oregon...

235

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:53 PM" "Back to Contents","Data 1: Utah...

236

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:06:23 PM" "Back to Contents","Data 1: Michigan...

237

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:30 PM" "Back to Contents","Data 1: New...

238

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:52 PM" "Back to Contents","Data 1: Natural...

239

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:24:23 PM" "Back to Contents","Data 1: Kansas...

240

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:07 PM" "Back to Contents","Data 1: U.S....

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


241

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:02 PM" "Back to Contents","Data 1: South...

242

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:03 PM" "Back to Contents","Data 1: Tennessee...

243

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:23 PM" "Back to Contents","Data 1: Montana...

244

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:32 PM" "Back to Contents","Data 1: New...

245

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:54 PM" "Back to Contents","Data 1: Natural...

246

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:04 PM" "Back to Contents","Data 1: Utah...

247

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:31 PM" "Back to Contents","Data 1: Natural...

248

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:00 PM" "Back to Contents","Data 1: Oklahoma...

249

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:08:23 PM" "Back to Contents","Data 1: Illinois...

250

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:06:23 PM" "Back to Contents","Data 1: Maryland...

251

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:23 PM" "Back to Contents","Data 1: Percent...

252

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:01 PM" "Back to Contents","Data 1:...

253

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:54 PM" "Back to Contents","Data 1: Virginia...

254

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:08 PM" "Back to Contents","Data 1: U.S....

255

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:04:51 PM" "Back to Contents","Data 1: Natural...

256

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:05:23 PM" "Back to Contents","Data 1: Natural...

257

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:05 PM" "Back to Contents","Data 1:...

258

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:07 PM" "Back to Contents","Data 1: Wyoming...

259

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:05 PM" "Back to Contents","Data 1: Vermont...

260

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U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:57 PM" "Back to Contents","Data 1:...

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


261

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:23:07 PM" "Back to Contents","Data 1: West...

262

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:00:57 PM" "Back to Contents","Data 1: Iowa...

263

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1162014 3:01:45 PM" "Back to Contents","Data 1: South...

264

Orifice mixing of immiscible liquids  

E-Print Network (OSTI)

measured with an Ostwald Viscosimeter relative to tap water also, All of these physical measurements were made at 83c F, the average tempera- ture noted during the runs. The liquid upon which these measurements were made were samples of the liquids...

McDonough, Joseph Aloysius

1960-01-01T23:59:59.000Z

265

ARM - Measurement - Liquid water path  

NLE Websites -- All DOE Office Websites (Extended Search)

Cloud Products Using Visst Algorithm PRECIPRET : Precipitation Retrievals WRF-CHEM : Weather Research and Forecasting (WRF) Model Output Value-Added Products MWRAVG :...

266

Three-Phase Vapor?Liquid?Liquid Equilibria for Methane + n-Octane + Monoethylene Glycol + Water at Pressures from (3.1 to 15.0) MPa and Temperatures from (281 to 363) K  

Science Journals Connector (OSTI)

There are several commercial processes available for the dehydration of gas, such as the use of liquid or solid desiccants and expansion refrigeration. ... The gaseous part of the liquid samples, and the gas phase samples direct from the equilibrium cell, were expanded into a series of evacuated vessels of known volume from which the total amount of substance was determined from the perfect gas equation using the measured low-pressure PVT data. ... To predict the losses of MEG in processes for the dehydration of natural gas, the concentrations of MEG in the vapor phase are of interest to the gas industry. ...

Stanley J. Ashcroft; Gerd Brunner; Hansjörg Vollmer; Christopher W. Sweeney

2009-03-06T23:59:59.000Z

267

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Workbook Contents" Workbook Contents" ,"U.S. State-to-State capacity" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description","Units of Measurement","Frequency","Updated Date" ,"Pipeline State-to-State Capacity","State-to-State capacity","Million cubic feet per day (MMcf/d)","Quarterly","application/vnd.ms-excel" ,"State Inflow Capacity","Inflow capacity from other States","Million cubic feet per day (MMcf/d)","Quarterly","application/vnd.ms-excel" ,"State Outflow Capacity","Outflow capacity to other States","Million cubic feet per day (MMcf/d)","Quarterly","application/vnd.ms-excel"

268

Freezing of a Liquid Marble  

E-Print Network (OSTI)

In this study, we present for the first time the observations of a freezing liquid marble. In the experiment, liquid marbles are gently placed on the cold side of a Thermo-Electric Cooler (TEC) and the morphological changes are recorded and characterized thereafter. These liquid marbles are noticed to undergo a shape transition from a spherical to a flying-saucer shaped morphology. The freezing dynamics of liquid marbles is observed to be very different from that of a freezing water droplet on a superhydrophobic surface. For example, the pointy tip appearing on a frozen water drop could not be observed for a frozen liquid marble. In the end, we highlight a possible explanation for the observed morphology.

Ali Hashmi; Adam Strauss; Jie Xu

2012-07-03T23:59:59.000Z

269

RELATIONS BETWEEN THE DETECTION OF METHYL TERT-BUTYL ETHER (MTBE) IN SURFACE AND GROUND WATER AND ITS CONTENT IN GASOLINE  

E-Print Network (OSTI)

AND ITS CONTENT IN GASOLINE By Michael J. Moran, Mike J. Halde, Rick M. Clawges and John S. Zogorski U in the United States as an octane enhancer and oxygenate in gasoline. Octane enhancement began in the late 1970's with the phase-out of tetraethyl lead from gasoline. The use of oxygenates was expanded

270

IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING, VOL. 39, NO. 1, JANUARY 2001 173 Impact of Variable Atmospheric Water Vapor Content  

E-Print Network (OSTI)

Canada during the 1996 growing season, together with reanalyzed IWV content data, were employed operating in the optical part of the electromagnetic spectrum. The scattering and absorption of solar are with the Canada Centre for Remote Sensing, Ottawa, ON, Canada K1A 0Y7 (e-mail: josef.cihlar@ccrs. nrcan.gc.ca). I

Li, Zhanqing

271

Enrichment and Determination of Trace Estradiol in Environmental Water Samples by Hollow-Fiber Liquid-Phase Microextraction Prior to HPLC  

Science Journals Connector (OSTI)

......samples were sur- face water collected from the...immersed in the aqueous water. The extraction...dryness at 90 C under nitrogen gas for about 20 min...were performed in water at an estradiol concentration...should have a low solubility in water and non-volatile......

Haixia Li; Ye Jiang; Yan Liu

2011-10-01T23:59:59.000Z

272

Water Content and Buildup of Poly(diallyldimethylammonium chloride)/ Poly(sodium 4-styrenesulfonate) and Poly(allylamine hydrochloride)/ Poly(sodium 4-styrenesulfonate) Polyelectrolyte Multilayers Studied by an in Situ Combination of a Quartz Crystal Micr  

E-Print Network (OSTI)

ABSTRACT: The buildup of polyelectrolyte multilayers (PEMs), fabricated by the layer-by-layer (LBL) assembly, was followed in situ by the combination of a quartz crystal microbalance with dissipation monitoring (QCM-D) and spectroscopic ellipsometry in a single device. PEMs composed of poly(allylamine hydrochloride) (PAH) and poly(sodium 4-styrenesulfonate) (PSS) polyelectrolyte pairs and of poly-(diallyldimethyl ammonium chloride) (PDADMAC) and PSS were built up to 17 layers. The combination of ellipsometry andQCM-D allowed simultaneous determination of the acousticmass, which comprises both the mass of the polymer and solvent, and the optical mass which corresponds to the polymer mass alone. From these parameters, the hydration of the PEMwas calculated layer by layer. The linearly growing PAH/ PSS PEMs showed a constant absolute content of water throughout the assembly, while the relative contribution of water to the PEM mass content approached zero, when grown in 0.5 M NaCl. Rinses with water between polyelectrolyte deposition steps resulted in a hydration of approximately 40%. The supralinearly growing PDADMAC/PSS PEMs exhibited a remarkable dependence of the hydration on the polyelectrolyte that was deposited last. Implications for the mechanism of assembly of the PEMs are discussed.

Jagoba J. Iturri Ramos; Stefan Stahl; Ralf P. Richter; Sergio E. Moya

2010-01-01T23:59:59.000Z

273

EMSL - liquids  

NLE Websites -- All DOE Office Websites (Extended Search)

liquids en Iodine Solubility in Low-Activity Waste Borosilicate Glass at 1000 °C. http:www.emsl.pnl.govemslwebpublicationsiodine-solubility-low-activity-waste-borosilicate...

274

Structure and dynamics of liquid water on rutile TiO2(110) Li-Min Liu, Changjun Zhang, Geoff Thornton, and Angelos Michaelides  

E-Print Network (OSTI)

those between water and titanium dioxide TiO2 . Water-TiO2 interfaces are relevant to photocatalysis on which adsorption state the water molecules are in at the interface: dissociated or molecular? Many, density-functional theory DFT studies predict either molecular or dissociative adsorption on the perfect

Alavi, Ali

275

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1981" Annual",2012,"6/30/1981" ,"Data 2","Crude Oil",8,"Annual",2012,"6/30/1981" ,"Data 3","Natural Gas and Petroleum Gases",57,"Annual",2012,"6/30/1986" ,"Data 4","Other Liquids",84,"Annual",2012,"6/30/1981" ,"Data 5","Finished Products",161,"Annual",2012,"6/30/1981" ,"Release Date:","9/27/2013" ,"Next Release Date:","9/26/2014" ,"Excel File Name:","pet_sum_snd_d_r10_mbblpd_a_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r10_mbblpd_a_cur.htm" ,"Source:","Energy Information Administration"

276

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1981" Annual",2012,"6/30/1981" ,"Data 2","Crude Oil",9,"Annual",2012,"6/30/1981" ,"Data 3","Natural Gas and Petroleum Gases",64,"Annual",2012,"6/30/1981" ,"Data 4","Other Liquids",92,"Annual",2012,"6/30/1981" ,"Data 5","Finished Products",184,"Annual",2012,"6/30/1981" ,"Release Date:","9/27/2013" ,"Next Release Date:","9/26/2014" ,"Excel File Name:","pet_sum_snd_d_r50_mbbl_a_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r50_mbbl_a_cur.htm" ,"Source:","Energy Information Administration"

277

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1956" Monthly","9/2013","1/15/1956" ,"Data 2","Crude Oil",8,"Monthly","9/2013","1/15/1920" ,"Data 3","Natural Gas and Petroleum Gases",57,"Monthly","9/2013","1/15/1967" ,"Data 4","Other Liquids",92,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",165,"Monthly","9/2013","1/15/1936" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_nus_mbbl_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_nus_mbbl_m_cur.htm"

278

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1981" Monthly","9/2013","1/15/1981" ,"Data 2","Crude Oil",8,"Monthly","9/2013","1/15/1981" ,"Data 3","Natural Gas and Petroleum Gases",57,"Monthly","9/2013","2/15/1973" ,"Data 4","Other Liquids",82,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",158,"Monthly","9/2013","1/15/1981" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_r50_mbblpd_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r50_mbblpd_m_cur.htm"

279

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1981" Annual",2012,"6/30/1981" ,"Data 2","Crude Oil",9,"Annual",2012,"6/30/1981" ,"Data 3","Natural Gas and Petroleum Gases",64,"Annual",2012,"6/30/1981" ,"Data 4","Other Liquids",81,"Annual",2012,"6/30/1981" ,"Data 5","Finished Products",176,"Annual",2012,"6/30/1981" ,"Release Date:","9/27/2013" ,"Next Release Date:","9/26/2014" ,"Excel File Name:","pet_sum_snd_d_r40_mbbl_a_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r40_mbbl_a_cur.htm" ,"Source:","Energy Information Administration"

280

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1981" Monthly","9/2013","1/15/1981" ,"Data 2","Crude Oil",8,"Monthly","9/2013","1/15/1981" ,"Data 3","Natural Gas and Petroleum Gases",57,"Monthly","9/2013","2/15/1973" ,"Data 4","Other Liquids",71,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",150,"Monthly","9/2013","1/15/1981" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_r40_mbblpd_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r40_mbblpd_m_cur.htm"

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


281

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1981" Monthly","9/2013","1/15/1981" ,"Data 2","Crude Oil",9,"Monthly","9/2013","1/15/1981" ,"Data 3","Natural Gas and Petroleum Gases",64,"Monthly","9/2013","1/15/1973" ,"Data 4","Other Liquids",81,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",176,"Monthly","9/2013","1/15/1981" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_r40_mbbl_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r40_mbbl_m_cur.htm"

282

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1963" Monthly","9/2013","1/15/1963" ,"Data 2","Crude Oil",7,"Monthly","9/2013","1/15/1920" ,"Data 3","Natural Gas and Petroleum Gases",50,"Monthly","9/2013","2/15/1971" ,"Data 4","Other Liquids",80,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",139,"Monthly","9/2013","1/15/1936" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_nus_mbblpd_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_nus_mbblpd_m_cur.htm"

283

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1981" Annual",2012,"6/30/1981" ,"Data 2","Crude Oil",8,"Annual",2012,"6/30/1981" ,"Data 3","Natural Gas and Petroleum Gases",57,"Annual",2012,"6/30/1986" ,"Data 4","Other Liquids",71,"Annual",2012,"6/30/1981" ,"Data 5","Finished Products",150,"Annual",2012,"6/30/1981" ,"Release Date:","9/27/2013" ,"Next Release Date:","9/26/2014" ,"Excel File Name:","pet_sum_snd_d_r40_mbblpd_a_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r40_mbblpd_a_cur.htm" ,"Source:","Energy Information Administration"

284

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1981" Monthly","9/2013","1/15/1981" ,"Data 2","Crude Oil",9,"Monthly","9/2013","1/15/1981" ,"Data 3","Natural Gas and Petroleum Gases",64,"Monthly","9/2013","1/15/1973" ,"Data 4","Other Liquids",94,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",187,"Monthly","9/2013","1/15/1981" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_r10_mbbl_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r10_mbbl_m_cur.htm"

285

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1981" Annual",2012,"6/30/1981" ,"Data 2","Crude Oil",8,"Annual",2012,"6/30/1981" ,"Data 3","Natural Gas and Petroleum Gases",57,"Annual",2012,"6/30/1986" ,"Data 4","Other Liquids",86,"Annual",2012,"6/30/1981" ,"Data 5","Finished Products",162,"Annual",2012,"6/30/1981" ,"Release Date:","9/27/2013" ,"Next Release Date:","9/26/2014" ,"Excel File Name:","pet_sum_snd_d_r20_mbblpd_a_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r20_mbblpd_a_cur.htm" ,"Source:","Energy Information Administration"

286

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1981" Monthly","9/2013","1/15/1981" ,"Data 2","Crude Oil",9,"Monthly","9/2013","1/15/1981" ,"Data 3","Natural Gas and Petroleum Gases",64,"Monthly","9/2013","1/15/1973" ,"Data 4","Other Liquids",96,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",185,"Monthly","9/2013","1/15/1981" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_r30_mbbl_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r30_mbbl_m_cur.htm"

287

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1981" Monthly","9/2013","1/15/1981" ,"Data 2","Crude Oil",9,"Monthly","9/2013","1/15/1981" ,"Data 3","Natural Gas and Petroleum Gases",64,"Monthly","9/2013","1/15/1973" ,"Data 4","Other Liquids",93,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",184,"Monthly","9/2013","1/15/1981" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_r50_mbbl_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r50_mbbl_m_cur.htm"

288

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1981" Monthly","9/2013","1/15/1981" ,"Data 2","Crude Oil",8,"Monthly","9/2013","1/15/1981" ,"Data 3","Natural Gas and Petroleum Gases",57,"Monthly","9/2013","2/15/1973" ,"Data 4","Other Liquids",84,"Monthly","9/2013","1/15/1981" ,"Data 5","Finished Products",161,"Monthly","9/2013","1/15/1981" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_sum_snd_d_r10_mbblpd_m_cur.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_sum_snd_d_r10_mbblpd_m_cur.htm"

289

An ecological study examining the correlation of end-stage renal disease and ground water heavy metal content in Texas counties  

E-Print Network (OSTI)

An ecological study was conducted to examine the correlation of end-stage renal disease (ESRD) and the ground water heavy metal level of lead, arsenic, cadmium, mercury and the cumulative level of all four metals in Texas counties. The heavy meal...

Bishop, Scott Alan

2012-06-07T23:59:59.000Z

290

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","ngm_epg0_fgc_sky_mmcfa.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/ngm_epg0_fgc_sky_mmcfa.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:59:11 AM" "Back to Contents","Data 1: Kentucky Natural Gas Gross Withdrawals from Coalbed Wells (MMcf) " "Sourcekey","NGM_EPG0_FGC_SKY_MMCF" "Date","Kentucky Natural Gas Gross Withdrawals from Coalbed Wells (MMcf) "

291

ccsd00001732, Development behavior of liquid plasma produced by  

E-Print Network (OSTI)

water with a melted NaCl is used as a test liquid. The liquid plasma is produced by the fundamental waveccsd­00001732, version 2 ­ 7 Nov 2004 Development behavior of liquid plasma produced by YAG laser the hazardous material called the environment material. Then, the plasma produced in liquid by the laser light

292

An Unprecedented Constraint on Water Content in the Sunlit Lunar Exosphere Seen by Lunar-Based Ultraviolet Telescope of Chang'e-3 Mission  

E-Print Network (OSTI)

The content of $\\mathrm{OH/H_2O}$ molecules in the tenuous exosphere of the Moon is still an open issue at present. We here report an unprecedented upper limit of the content of the OH radicals, which is obtained from the in-situ measurements carried out \\rm by the Lunar-based Ultraviolet Telescope, a payload of Chinese Chang'e-3 mission. By analyzing the diffuse background in the images taken by the telescope, the column density and surface concentration of the OH radicals are inferred to be $<10^{11}\\ \\mathrm{cm^{-2}}$ and $<10^{4}\\ \\mathrm{cm^{-3}}$ (by assuming a hydrostatic equilibrium with a scale height of 100km), respectively, by assuming that the recorded background is fully contributed by their resonance fluorescence emission. The resulted concentration is lower than the previously reported value by about two orders of magnitude, and is close to the prediction of the sputtering model. In addition, the same measurements and method allow us to derive a surface concentration of $<10^{2}\\ \\math...

Wang, J; Qiu, Y L; Meng, X M; Cai, H B; Cao, L; Deng, J S; Han, X H; Wei, J Y

2015-01-01T23:59:59.000Z

293

Spiers Memorial Lecture Recent experimental advances in studies of liquid/liquid  

E-Print Network (OSTI)

complicated processes such as molecular transport across cell membranes. A variety of techniques have been on the interaction of a hydrophobic surface with water, and ion and solute transport across these and other liquid/hydrophilic properties of liquid/ liquid interfaces. In biological systems, protein folding and membrane formation rely

Richmond, Geraldine L.

294

Influence of surface passivation and water content on mineral reactions in unsaturated porous media: Implications for brucite carbonation and CO2 sequestration  

Science Journals Connector (OSTI)

Abstract The evolution of mineral reactive surface area is an important control on the progress of carbon mineralization reactions that sequester anthropogenic CO2. Dry conditions in unsaturated porous media and the passivation of reactive surface area by secondary phase precipitation complicate predictions of reactive surface during carbon mineralization reactions. Unsaturated brucite [Mg(OH)2] bearing column experiments were used to evaluate the effects of water saturation and hydrous Mg-carbonate precipitation on reaction of brucite with 10% CO2 gas streams at ambient conditions. We demonstrate that a lack of available water severely limits reaction progress largely due to the requirement of water as a reactant to form hydrated Mg-carbonates. The precipitation of a poorly crystalline carbonate phase in the early stages of the reaction does not significantly hinder brucite dissolution, as the carbonate coating remains sufficiently permeable. It is postulated that the conversion of this phase to substantially less porous, crystalline nesquehonite [MgCO3·3H2O] results in passivation of the brucite surface. Although a mechanistic model describing the passivating effect of nesquehonite remains elusive, reactive transport modeling using MIN3P-DUSTY confirms that conventional geometric surface area update models do not adequately reproduce observed reaction progress during brucite carbonation, while an empirically based model accounting for surface passivation is able to capture the transient evolution of CO2 uptake. Both water limits and surface passivation effects may limit the efficiency of CO2 sequestration efforts that rely on the conversion of mafic and ultramafic rock to carbonate minerals.

Anna L. Harrison; Gregory M. Dipple; Ian M. Power; K. Ulrich Mayer

2015-01-01T23:59:59.000Z

295

Radioactive Liquid Waste Treatment Facility Discharges in 2011  

SciTech Connect

This report documents radioactive discharges from the TA50 Radioactive Liquid Waste Treatment Facilities (RLWTF) during calendar 2011. During 2011, three pathways were available for the discharge of treated water to the environment: discharge as water through NPDES Outfall 051 into Mortandad Canyon, evaporation via the TA50 cooling towers, and evaporation using the newly-installed natural-gas effluent evaporator at TA50. Only one of these pathways was used; all treated water (3,352,890 liters) was fed to the effluent evaporator. The quality of treated water was established by collecting a weekly grab sample of water being fed to the effluent evaporator. Forty weekly samples were collected; each was analyzed for gross alpha, gross beta, and tritium. Weekly samples were also composited at the end of each month. These flow-weighted composite samples were then analyzed for 37 radioisotopes: nine alpha-emitting isotopes, 27 beta emitters, and tritium. These monthly analyses were used to estimate the radioactive content of treated water fed to the effluent evaporator. Table 1 summarizes this information. The concentrations and quantities of radioactivity in Table 1 are for treated water fed to the evaporator. Amounts of radioactivity discharged to the environment through the evaporator stack were likely smaller since only entrained materials would exit via the evaporator stack.

Del Signore, John C. [Los Alamos National Laboratory

2012-05-16T23:59:59.000Z

296

Sorptive extraction using polydimethylsiloxane/metal–organic framework coated stir bars coupled with high performance liquid chromatography-fluorescence detection for the determination of polycyclic aromatic hydrocarbons in environmental water samples  

Science Journals Connector (OSTI)

Abstract In this work, metal–organic frameworks (MOFs, Al-MIL-53-NH2) were synthesized via the hydrothermal method, and novel polydimethylsiloxane/metal–organic framework (PDMS/MOFs, PDMS/Al-MIL-53-NH2)-coated stir bars were prepared by the sol–gel technique. The preparation reproducibility of the PDMS/MOFs-coated stir bar was good, with relative standard deviations (RSDs) ranging from 4.8% to 14.9% (n = 7) within one batch and from 6.2% to 16.9% (n = 6) among different batches. Based on this fact, a new method of PDMS/MOFs-coated stir bar sorptive extraction (SBSE) and ultrasonic-assisted liquid desorption (UALD) coupled with high performance liquid chromatography-fluorescence detection (HPLC-FLD) was developed for the determination of polycyclic aromatic hydrocarbons (PAHs) in environmental water samples. To obtain the best extraction performance for PAHs, several parameters affecting SBSE, such as extraction time, stirring rate, and extraction temperature, were investigated. Under optimal experimental conditions, wide linear ranges and good \\{RSDs\\} (n = 7) were obtained. With enrichment factors (EFs) of 16.1- to 88.9-fold (theoretical EF, 142-fold), the limits of detection (LODs, S/N = 3) of the developed method for the target \\{PAHs\\} were found to be in the range of 0.05–2.94 ng/L. The developed method was successfully applied to the analysis of \\{PAHs\\} in Yangtze River and East Lake water samples.

Cong Hu; Man He; Beibei Chen; Cheng Zhong; Bin Hu

2014-01-01T23:59:59.000Z

297

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010pa2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010pa2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:52 PM" "Back to Contents","Data 1: Pennsylvania Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010PA2" "Date","Pennsylvania Natural Gas Residential Consumption (MMcf)" 24653,279817 25019,285978 25384,295027 25749,297022 26114,304327

298

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Bcf)" Bcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description","# Of Series","Frequency","Latest Data for" ,"Data 1","U.S. Dry Natural Gas Production (Bcf)",1,"Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9070us1m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9070us1m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:33:14 PM" "Back to Contents","Data 1: U.S. Dry Natural Gas Production (Bcf)"

299

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","na1504_nus_4m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/na1504_nus_4m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:46:14 PM" "Back to Contents","Data 1: U.S. Natural Gas % of Total Residential - Sales (%)" "Sourcekey","NA1504_NUS_4" "Date","U.S. Natural Gas % of Total Residential - Sales (%)" 37271,98.3 37302,98.5 37330,98.4 37361,98.1

300

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n5050us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n5050us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:29:09 PM" "Back to Contents","Data 1: U.S. Total Natural Gas Injections into Underground Storage (MMcf)" "Sourcekey","N5050US2" "Date","U.S. Total Natural Gas Injections into Underground Storage (MMcf)" 26679 26710 26738 26769 26799

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


301

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010hi2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010hi2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:19 PM" "Back to Contents","Data 1: Hawaii Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010HI2" "Date","Hawaii Natural Gas Residential Consumption (MMcf)" 29402,1416 29767,1289 30132,1197 30497,1121 30863,1048 31228,625 31593,579 31958,591

302

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010tx2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010tx2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:59 PM" "Back to Contents","Data 1: Texas Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010TX2" "Date","Texas Natural Gas Residential Consumption (MMcf)" 24653,201407 25019,211763 25384,220728 25749,232189 26114,237387 26480,240662

303

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040nd2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040nd2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:40 AM" "Back to Contents","Data 1: North Dakota Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040ND2" "Date","North Dakota Natural Gas Vented and Flared (MMcf)" 35079,232 35110,193 35139,232 35170,176 35200,230 35231,258 35261,269

304

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010de3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010de3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:15 PM" "Back to Contents","Data 1: Delaware Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010DE3" "Date","Delaware Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

305

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020fl2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020fl2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:29 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Florida (MMcf)" "Sourcekey","N3020FL2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Florida (MMcf)"

306

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ct2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ct2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:23 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Connecticut (MMcf)" "Sourcekey","N3020CT2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Connecticut (MMcf)"

307

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020az2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020az2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:17 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Arizona (MMcf)" "Sourcekey","N3020AZ2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Arizona (MMcf)"

308

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ca2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ca2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:19 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in California (MMcf)" "Sourcekey","N3020CA2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in California (MMcf)"

309

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020dc2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020dc2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:24 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in the District of Columbia (MMcf)" "Sourcekey","N3020DC2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in the District of Columbia (MMcf)"

310

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020co2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020co2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:21 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Colorado (MMcf)" "Sourcekey","N3020CO2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Colorado (MMcf)"

311

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010md2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010md2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:30 PM" "Back to Contents","Data 1: Maryland Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010MD2" "Date","Maryland Natural Gas Residential Consumption (MMcf)" 24653,77130 25019,79015 25384,84406 25749,86811 26114,87617 26480,89042

312

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040or2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040or2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:43 AM" "Back to Contents","Data 1: Oregon Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040OR2" "Date","Oregon Natural Gas Vented and Flared (MMcf)" 35079 35110 35139 35170 35200 35231 35261 35292 35323 35353 35384 35414 35445,0

313

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010wv3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010wv3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:07 PM" "Back to Contents","Data 1: West Virginia Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010WV3" "Date","West Virginia Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

314

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010la2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010la2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:28 PM" "Back to Contents","Data 1: Louisiana Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010LA2" "Date","Louisiana Natural Gas Residential Consumption (MMcf)" 24653,74386 25019,77762 25384,82965 25749,86148 26114,79893 26480,82847

315

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010al3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010al3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:07 PM" "Back to Contents","Data 1: Alabama Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010AL3" "Date","Alabama Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

316

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010nm3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010nm3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:45 PM" "Back to Contents","Data 1: New Mexico Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010NM3" "Date","New Mexico Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

317

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010id2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010id2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:22 PM" "Back to Contents","Data 1: Idaho Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010ID2" "Date","Idaho Natural Gas Residential Consumption (MMcf)" 24653,6179 25019,6545 25384,6980 25749,7711 26114,8455 26480,10887 26845,9947 27210,9652

318

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010wa2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010wa2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:05 PM" "Back to Contents","Data 1: Washington Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010WA2" "Date","Washington Natural Gas Residential Consumption (MMcf)" 24653,23160 25019,26342 25384,30479 25749,31929 26114,33934 26480,38631

319

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ok2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ok2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:42 AM" "Back to Contents","Data 1: Oklahoma Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040OK2" "Date","Oklahoma Natural Gas Vented and Flared (MMcf)" 35079 35110 35139 35170 35200 35231 35261 35292 35323 35353 35384 35414 35445,0

320

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9132us3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9132us3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:27 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas Pipeline Exports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9132US3" "Date","Price of U.S. Natural Gas Pipeline Exports (Dollars per Thousand Cubic Feet)" 35445,4.08

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


321

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040nm2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040nm2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:40 AM" "Back to Contents","Data 1: New Mexico Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040NM2" "Date","New Mexico Natural Gas Vented and Flared (MMcf)" 24653,5992 25019,5987 25384,4058 25749,2909 26114,2823 26480,5696 26845,3791 27210,1227

322

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040sd2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040sd2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:43 AM" "Back to Contents","Data 1: South Dakota Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040SD2" "Date","South Dakota Natural Gas Vented and Flared (MMcf)" 24653,0 25019,0 25384,0 25749,0 26114,0 26480,0 26845,0 27210,0 27575,4 27941,5

323

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040co2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040co2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:33 AM" "Back to Contents","Data 1: Colorado Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040CO2" "Date","Colorado Natural Gas Vented and Flared (MMcf)" 24653,2656 25019,1514 25384,1326 25749,7126 26114,2843 26480,4758 26845,3008 27210,2957

324

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3035us4a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3035us4a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:25:09 PM" "Back to Contents","Data 1: Percent of Industrial Natural Gas Deliveries in U.S. Total Represented by the Price (%)" "Sourcekey","N3035US4" "Date","Percent of Industrial Natural Gas Deliveries in U.S. Total Represented by the Price (%)"

325

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U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ny2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ny2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:41 AM" "Back to Contents","Data 1: New York Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040NY2" "Date","New York Natural Gas Vented and Flared (MMcf)" 33253,0 33284,0 33312,1 33343,0 33373,0 33404,0 33434,0 33465,0 33496,0

326

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ma2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ma2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:29 PM" "Back to Contents","Data 1: Massachusetts Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010MA2" "Date","Massachusetts Natural Gas Residential Consumption (MMcf)" 24653,73471 25019,74919 25384,78451 25749,82646 26114,83434 26480,86171

327

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040mt2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040mt2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:39 AM" "Back to Contents","Data 1: Montana Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040MT2" "Date","Montana Natural Gas Vented and Flared (MMcf)" 35079,32 35110,38 35139,34 35170,40 35200,43 35231,27 35261,63 35292,59 35323,60

328

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040us2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040us2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:45 AM" "Back to Contents","Data 1: U.S. Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040US2" "Date","U.S. Natural Gas Vented and Flared (MMcf)" 13331,392528 13696,526159 14061,649106 14426,677311 14792,655967 15157,630212 15522,626782 15887,684115

329

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040mi2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040mi2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:38 AM" "Back to Contents","Data 1: Michigan Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040MI2" "Date","Michigan Natural Gas Vented and Flared (MMcf)" 35079,277 35110,277 35139,277 35170,277 35200,277 35231,277 35261,277

330

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9012us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9012us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:55:55 AM" "Back to Contents","Data 1: U.S. Natural Gas Gross Withdrawals from Oil Wells (MMcf)" "Sourcekey","N9012US2" "Date","U.S. Natural Gas Gross Withdrawals from Oil Wells (MMcf)" 33253,475614 33526,500196 33984,513068 34015,462218

331

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ne2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ne2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:40 AM" "Back to Contents","Data 1: Nebraska Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040NE2" "Date","Nebraska Natural Gas Vented and Flared (MMcf)" 33253,0 33284,0 33312,0 33343,0 33373,0 33404,0 33434,0 33465,0 33496,0

332

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040pa2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040pa2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:43 AM" "Back to Contents","Data 1: Pennsylvania Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040PA2" "Date","Pennsylvania Natural Gas Vented and Flared (MMcf)" 33253,0 33284,0 33312,0 33343,0 33373,0 33404,0 33434,0 33465,0

333

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9050us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9050us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:57:04 AM" "Back to Contents","Data 1: U.S. Natural Gas Marketed Production (MMcf)" "Sourcekey","N9050US2" "Date","U.S. Natural Gas Marketed Production (MMcf)" 26679,1948000 26710,1962000 26738,1907000 26769,1814000 26799,1898000 26830,1839000

334

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

mbbl_a.xls" mbbl_a.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_crd_crpdn_adc_mbbl_a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"11/27/2013 9:07:23 AM" "Back to Contents","Data 1: Crude Oil Production" "Sourcekey","MCRFPUS1","MCRFPP11","MCRFPFL1","MCRFPNY1","MCRFPPA1","MCRFPVA1","MCRFPWV1","MCRFPP21","MCRFPIL1","MCRFPIN1","MCRFPKS1","MCRFPKY1","MCRFP_SMI_1","MCRFPMO1","MCRFPNE1","MCRFPND1","MCRFPOH1","MCRFPOK1","MCRFPSD1","MCRFPTN1","MCRFPP31","MCRFPAL1","MCRFPAR1","MCRFPLA1","MCRFPMS1","MCRFPNM1","MCRFPTX1","MCRFP3FM1","MCRFPP41","MCRFPCO1","MCRFPMT1","MCRFPUT1","MCRFPWY1","MCRFPP51","MCRFPAK1","MCRFPAKS1","MANFPAK1","MCRFPAZ1","MCRFPCA1","MCRFPNV1","MCRFP5F1"

335

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020al2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020al2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:11 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Alabama (MMcf)" "Sourcekey","N3020AL2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Alabama (MMcf)"

336

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9100us3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9100us3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 3:53:51 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas Imports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9100US3" "Date","Price of U.S. Natural Gas Imports (Dollars per Thousand Cubic Feet)" 31228,3.21 31593,2.43 31958,1.95 32324,1.84

337

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","rngc1a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/rngc1a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:41 PM" "Back to Contents","Data 1: Natural Gas Futures Contract 1 (Dollars per Million Btu)" "Sourcekey","RNGC1" "Date","Natural Gas Futures Contract 1 (Dollars per Million Btu)" 34515,1.934 34880,1.692 35246,2.502 35611,2.475 35976,2.156 36341,2.319

338

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9130us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9130us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:23 PM" "Back to Contents","Data 1: U.S. Natural Gas Exports (MMcf)" "Sourcekey","N9130US2" "Date","U.S. Natural Gas Exports (MMcf)" 26679,5808 26710,6079 26738,4021 26769,8017 26799,8741 26830,4131 26860,5744 26891,8726 26922,6403 26952,5473

339

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ks3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ks3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:26 PM" "Back to Contents","Data 1: Kansas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010KS3" "Date","Kansas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

340

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ca2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ca2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:33 AM" "Back to Contents","Data 1: California Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040CA2" "Date","California Natural Gas Vented and Flared (MMcf)" 35079,97 35110,103 35139,109 35170,107 35200,107 35231,104 35261,108

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


341

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9103us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9103us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 3:54:17 PM" "Back to Contents","Data 1: U.S. Liquefied Natural Gas Imports (MMcf)" "Sourcekey","N9103US2" "Date","U.S. Liquefied Natural Gas Imports (MMcf)" 35445,9977 35476,7667 35504,2530 35535,2557 35565,5007 35596,5059 35626,5026 35657,7535

342

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040mt2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040mt2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:39 AM" "Back to Contents","Data 1: Montana Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040MT2" "Date","Montana Natural Gas Vented and Flared (MMcf)" 24653,5022 25019,12551 25384,26458 25749,5203 26114,4917 26480,4222 26845,3691 27210,3901

343

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040tx2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040tx2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:44 AM" "Back to Contents","Data 1: Texas Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040TX2" "Date","Texas Natural Gas Vented and Flared (MMcf)" 33253,2478 33284,2147 33312,2113 33343,2353 33373,3203 33404,2833 33434,3175

344

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9130us3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9130us3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:24 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas Exports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9130US3" "Date","Price of U.S. Natural Gas Exports (Dollars per Thousand Cubic Feet)" 31228,4.77 31593,2.81 31958,3.07 32324,2.74

345

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ny2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ny2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:41 AM" "Back to Contents","Data 1: New York Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040NY2" "Date","New York Natural Gas Vented and Flared (MMcf)" 24653,0 25019,0 25384,0 25749,0 26114,0 26480,0 26845,0 27210,0 27575,0 27941,0 28306,0 28671,0

346

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ks2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ks2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:35 AM" "Back to Contents","Data 1: Kansas Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040KS2" "Date","Kansas Natural Gas Vented and Flared (MMcf)" 24653,2630 25019,2529 25384,2666 25749,2713 26114,2669 26480,2681 26845,2377 27210,889 27575,846

347

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ar2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ar2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:32 AM" "Back to Contents","Data 1: Arkansas Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040AR2" "Date","Arkansas Natural Gas Vented and Flared (MMcf)" 33253,23 33284,13 33312,12 33343,7 33373,13 33404,28 33434,28 33465,30

348

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010de2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010de2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:15 PM" "Back to Contents","Data 1: Delaware Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010DE2" "Date","Delaware Natural Gas Residential Consumption (MMcf)" 24653,6844 25019,7068 25384,7475 25749,7843 26114,8172 26480,8358 26845,7514

349

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

mbblpd_a.xls" mbblpd_a.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_crd_crpdn_adc_mbblpd_a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"11/27/2013 9:07:25 AM" "Back to Contents","Data 1: Crude Oil Production" "Sourcekey","MCRFPUS2","MCRFPP12","MCRFPFL2","MCRFPNY2","MCRFPPA2","MCRFPVA2","MCRFPWV2","MCRFPP22","MCRFPIL2","MCRFPIN2","MCRFPKS2","MCRFPKY2","MCRFP_SMI_2","MCRFPMO2","MCRFPNE2","MCRFPND2","MCRFPOH2","MCRFPOK2","MCRFPSD2","MCRFPTN2","MCRFPP32","MCRFPAL2","MCRFPAR2","MCRFPLA2","MCRFPMS2","MCRFPNM2","MCRFPTX2","MCRFP3FM2","MCRFPP42","MCRFPCO2","MCRFPMT2","MCRFPUT2","MCRFPWY2","MCRFPP52","MCRFPAK2","MCRFPAKS2","MANFPAK2","MCRFPAZ2","MCRFPCA2","MCRFPNV2","MCRFP5F2"

350

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","ngm_epg0_fgc_sky_mmcfm.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/ngm_epg0_fgc_sky_mmcfm.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:59:11 AM" "Back to Contents","Data 1: Kentucky Natural Gas Gross Withdrawals from Coalbed Wells (MMcf) " "Sourcekey","NGM_EPG0_FGC_SKY_MMCF" "Date","Kentucky Natural Gas Gross Withdrawals from Coalbed Wells (MMcf) "

351

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020hi3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020hi3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:34 PM" "Back to Contents","Data 1: Hawaii Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3020HI3" "Date","Hawaii Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"

352

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

poe2_dcu_nus-z00_a.xls" poe2_dcu_nus-z00_a.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/ng/ng_move_poe2_dcu_nus-z00_a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"12/12/2013 6:58:44 PM" "Back to Contents","Data 1: U.S. Total Exports " "Sourcekey","N9132US2","N9132US3","N9133US2","N9133US3" "Date","U.S. Natural Gas Pipeline Exports (MMcf)","Price of U.S. Natural Gas Pipeline Exports (Dollars per Thousand Cubic Feet)","Liquefied U.S. Natural Gas Exports (MMcf)","Price of Liquefied U.S. Natural Gas Exports (Dollars per Thousand Cubic Feet)"

353

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ms2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ms2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:38 AM" "Back to Contents","Data 1: Mississippi Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040MS2" "Date","Mississippi Natural Gas Vented and Flared (MMcf)" 24653,7098 25019,5910 25384,8097 25749,7233 26114,5090 26480,3672 26845,10767 27210,10787

354

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ok3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ok3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:50 PM" "Back to Contents","Data 1: Oklahoma Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010OK3" "Date","Oklahoma Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

355

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010nd3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010nd3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:40 PM" "Back to Contents","Data 1: North Dakota Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010ND3" "Date","North Dakota Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

356

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040or2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040or2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:42 AM" "Back to Contents","Data 1: Oregon Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040OR2" "Date","Oregon Natural Gas Vented and Flared (MMcf)" 35246 35611,0 35976,0 36341,0 36707,0 37072,0 37437,0 37802,0 38168,0 38533,0 38898,0 39263,0

357

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ky2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ky2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:27 PM" "Back to Contents","Data 1: Kentucky Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010KY2" "Date","Kentucky Natural Gas Residential Consumption (MMcf)" 24653,69542 25019,75824 25384,83815 25749,86473 26114,84197 26480,85881

358

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9160us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9160us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:33:48 PM" "Back to Contents","Data 1: U.S. Natural Gas Lease and Plant Fuel Consumption (MMcf)" "Sourcekey","N9160US2" "Date","U.S. Natural Gas Lease and Plant Fuel Consumption (MMcf)" 29235,93000 29266,87000 29295,93000 29326,85000

359

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9030us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9030us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:28 AM" "Back to Contents","Data 1: U.S. Nonhydrocarbon Gases Removed from Natural Gas (MMcf)" "Sourcekey","N9030US2" "Date","U.S. Nonhydrocarbon Gases Removed from Natural Gas (MMcf)" 26679 26710 26738 26769 26799 26830 26860 26891

360

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010mi3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010mi3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:33 PM" "Back to Contents","Data 1: Michigan Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010MI3" "Date","Michigan Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


361

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9070us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9070us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:57:08 AM" "Back to Contents","Data 1: U.S. Dry Natural Gas Production (MMcf)" "Sourcekey","N9070US2" "Date","U.S. Dry Natural Gas Production (MMcf)" 35445,1617923 35476,1465907 35504,1627602 35535,1551268 35565,1610527 35596,1525325

362

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9102us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9102us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 3:53:55 PM" "Back to Contents","Data 1: U.S. Natural Gas Pipeline Imports (MMcf)" "Sourcekey","N9102US2" "Date","U.S. Natural Gas Pipeline Imports (MMcf)" 35445,268310 35476,232878 35504,254455 35535,235621 35565,236725 35596,227059 35626,230567

363

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010wy2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010wy2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:08 PM" "Back to Contents","Data 1: Wyoming Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010WY2" "Date","Wyoming Natural Gas Residential Consumption (MMcf)" 24653,11939 25019,12592 25384,16592 25749,17984 26114,19463 26480,22242 26845,13868

364

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ak2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ak2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:09 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Alaska (MMcf)" "Sourcekey","N3020AK2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Alaska (MMcf)"

365

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:00 PM" "Back to Contents","Data 1: U.S. Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010US2" "Date","U.S. Natural Gas Residential Consumption (MMcf)" 26679,843900 26710,747331 26738,648504 26769,465867 26799,326313

366

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010mt2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010mt2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:38 PM" "Back to Contents","Data 1: Montana Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010MT2" "Date","Montana Natural Gas Residential Consumption (MMcf)" 24653,19756 25019,19711 25384,21463 25749,24794 26114,25379 26480,23787 26845,24923

367

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9103us3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9103us3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 3:54:18 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas LNG Imports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9103US3" "Date","Price of U.S. Natural Gas LNG Imports (Dollars per Thousand Cubic Feet)" 35445,3 35476,3

368

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9132us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9132us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:27 PM" "Back to Contents","Data 1: U.S. Natural Gas Pipeline Exports (MMcf)" "Sourcekey","N9132US2" "Date","U.S. Natural Gas Pipeline Exports (MMcf)" 35445,6424 35476,6846 35504,10601 35535,8211 35565,6284 35596,5741 35626,6380 35657,10101

369

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3035us4m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3035us4m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:25:10 PM" "Back to Contents","Data 1: Percent of Industrial Natural Gas Deliveries in U.S. Total Represented by the Price (%)" "Sourcekey","N3035US4" "Date","Percent of Industrial Natural Gas Deliveries in U.S. Total Represented by the Price (%)"

370

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010wi3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010wi3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:06 PM" "Back to Contents","Data 1: Wisconsin Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010WI3" "Date","Wisconsin Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

371

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040al2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040al2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:31 AM" "Back to Contents","Data 1: Alabama Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040AL2" "Date","Alabama Natural Gas Vented and Flared (MMcf)" 35079,194 35110,200 35139,140 35170,132 35200,106 35231,82 35261,205 35292,152

372

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040wv2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040wv2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:46 AM" "Back to Contents","Data 1: West Virginia Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040WV2" "Date","West Virginia Natural Gas Vented and Flared (MMcf)" 33253,0 33284,0 33312,0 33343,0 33373,0 33404,0 33434,0 33465,0

373

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1993" Monthly","9/2013","1/15/1993" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_pnp_pct_dc_nus_pct_m.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_pnp_pct_dc_nus_pct_m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"11/25/2013 11:23:48 AM" "Back to Contents","Data 1: U.S. Refinery Yield" "Sourcekey","MLRRYUS3","MGFRYUS3","MGARYUS3","MKJRYUS3","MKERYUS3","MDIRYUS3","MRERYUS3","MNFRYUS3","MOTRYUS3","MNSRYUS3","MLURYUS3","MWXRYUS3","MCKRYUS3","MAPRYUS3","MSGRYUS3","MMSRYUS3","MPGRYUS3"

374

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:23:36 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in the U.S. (MMcf)" "Sourcekey","N3020US2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in the U.S. (MMcf)"

375

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:45 AM" "Back to Contents","Data 1: U.S. Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040US2" "Date","U.S. Natural Gas Vented and Flared (MMcf)" 26679 26710 26738 26769 26799 26830 26860 26891 26922 26952 26983 27013 27044 27075 27103

376

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","11/2013","1/15/1997" Monthly","11/2013","1/15/1997" ,"Data 2","Futures Prices",4,"Monthly","11/2013","12/15/1993" ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","ng_pri_fut_s1_m.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/ng/ng_pri_fut_s1_m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:17 PM" "Back to Contents","Data 1: Spot Price" "Sourcekey","RNGWHHD","NGM_EPG0_PLC_NUS_DMMBTU"

377

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010pa3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010pa3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:52 PM" "Back to Contents","Data 1: Pennsylvania Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010PA3" "Date","Pennsylvania Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

378

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ut3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ut3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:02 PM" "Back to Contents","Data 1: Utah Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010UT3" "Date","Utah Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

379

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010dc2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010dc2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:13 PM" "Back to Contents","Data 1: District of Columbia Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010DC2" "Date","District of Columbia Natural Gas Residential Consumption (MMcf)" 29402,13730 29767,13686 30132,13041 30497,13007

380

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010tx3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010tx3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:00 PM" "Back to Contents","Data 1: Texas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010TX3" "Date","Texas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


381

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1993" Annual",2012,"6/30/1993" ,"Release Date:","9/27/2013" ,"Next Release Date:","9/26/2014" ,"Excel File Name:","pet_stoc_typ_d_nus_skn_mbbl_a.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_stoc_typ_d_nus_skn_mbbl_a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"11/25/2013 11:41:29 AM" "Back to Contents","Data 1: U.S. Natural Gas Processing Plant " "Sourcekey","MAOSNUS1","MPPSNUS1","MLPSNUS1","METSNUS1","MPRSNUS1","MBNSNUS1","MBISNUS1"

382

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040az2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040az2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:32 AM" "Back to Contents","Data 1: Arizona Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040AZ2" "Date","Arizona Natural Gas Vented and Flared (MMcf)" 26114,347 26480,367 26845,277 27210,26 27575,47 27941,32 29036,101 29402,143 29767,106 30132,162

383

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ca3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ca3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:20 PM" "Back to Contents","Data 1: California Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3020CA3" "Date","California Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"

384

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010oh3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010oh3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:49 PM" "Back to Contents","Data 1: Ohio Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010OH3" "Date","Ohio Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

385

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020fl3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020fl3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:30 PM" "Back to Contents","Data 1: Florida Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3020FL3" "Date","Florida Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"

386

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ks2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ks2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:36 AM" "Back to Contents","Data 1: Kansas Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040KS2" "Date","Kansas Natural Gas Vented and Flared (MMcf)" 35079,63 35110,63 35139,63 35170,61 35200,62 35231,57 35261,57 35292,55 35323,56

387

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040nv2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040nv2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:41 AM" "Back to Contents","Data 1: Nevada Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040NV2" "Date","Nevada Natural Gas Vented and Flared (MMcf)" 33253,0 33284,0 33312,0 33343,0 33373,0 33404,0 33434,0 33465,0 33496,0 33526,0

388

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ms2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ms2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:38 AM" "Back to Contents","Data 1: Mississippi Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040MS2" "Date","Mississippi Natural Gas Vented and Flared (MMcf)" 35079,217 35110,199 35139,223 35170,219 35200,237 35231,234 35261,239

389

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9103us3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9103us3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 3:54:18 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas LNG Imports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9103US3" "Date","Price of U.S. Natural Gas LNG Imports (Dollars per Thousand Cubic Feet)" 31228,4.6 31593,4.62 32324,2.71

390

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9130us3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9130us3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:24 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas Exports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9130US3" "Date","Price of U.S. Natural Gas Exports (Dollars per Thousand Cubic Feet)" 32523,2.69 32554,2.4

391

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040tx2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040tx2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:44 AM" "Back to Contents","Data 1: Texas Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040TX2" "Date","Texas Natural Gas Vented and Flared (MMcf)" 24653,129403 25019,124584 25384,111499 25749,100305 26114,70222 26480,59821 26845,36133 27210,34431

392

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010al2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010al2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:07 PM" "Back to Contents","Data 1: Alabama Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010AL2" "Date","Alabama Natural Gas Residential Consumption (MMcf)" 24653,45543 25019,51708 25384,54804 25749,55779 26114,54867 26480,53397 26845,55685

393

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010mi2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010mi2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:33 PM" "Back to Contents","Data 1: Michigan Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010MI2" "Date","Michigan Natural Gas Residential Consumption (MMcf)" 24653,302472 25019,315694 25384,333264 25749,340033 26114,343773 26480,355266

394

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010co3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010co3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:12 PM" "Back to Contents","Data 1: Colorado Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010CO3" "Date","Colorado Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

395

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010wa3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010wa3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:05 PM" "Back to Contents","Data 1: Washington Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010WA3" "Date","Washington Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

396

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ak2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ak2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:05 PM" "Back to Contents","Data 1: Alaska Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010AK2" "Date","Alaska Natural Gas Residential Consumption (MMcf)" 24653,1958 25019,2293 25384,4573 25749,6211 26114,6893 26480,8394 26845,5024

397

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ar2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ar2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:08 PM" "Back to Contents","Data 1: Arkansas Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010AR2" "Date","Arkansas Natural Gas Residential Consumption (MMcf)" 24653,52777 25019,56346 25384,58322 25749,59792 26114,48737 26480,47387

398

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2010 Annual",2010 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ok2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ok2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:42 AM" "Back to Contents","Data 1: Oklahoma Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040OK2" "Date","Oklahoma Natural Gas Vented and Flared (MMcf)" 24653,126629 25019,129408 25384,130766 25749,129629 26114,39799 26480,38797 26845,36411

399

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020us4m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020us4m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:23:38 PM" "Back to Contents","Data 1: Percent of Commercial Natural Gas Deliveries in U.S. Total Represented by the Price (%)" "Sourcekey","N3020US4" "Date","Percent of Commercial Natural Gas Deliveries in U.S. Total Represented by the Price (%)"

400

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ak3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ak3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:06 PM" "Back to Contents","Data 1: Alaska Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010AK3" "Date","Alaska Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

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they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
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401

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ca3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ca3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:11 PM" "Back to Contents","Data 1: California Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010CA3" "Date","California Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

402

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040la2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040la2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:37 AM" "Back to Contents","Data 1: Louisiana Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040LA2" "Date","Louisiana Natural Gas Vented and Flared (MMcf)" 33253,1788 33284,1684 33312,1571 33343,1593 33373,1807 33404,1690 33434,2042

403

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040tn2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040tn2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:44 AM" "Back to Contents","Data 1: Tennessee Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040TN2" "Date","Tennessee Natural Gas Vented and Flared (MMcf)" 33253,0 33284,0 33312,0 33343,0 33373,0 33404,0 33434,0 33465,0 33496,0

404

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010wi2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010wi2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:06 PM" "Back to Contents","Data 1: Wisconsin Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010WI2" "Date","Wisconsin Natural Gas Residential Consumption (MMcf)" 24653,90994 25019,93425 25384,101124 25749,105208 26114,109758 26480,104648

405

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020us4a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020us4a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:23:38 PM" "Back to Contents","Data 1: Percent of Commercial Natural Gas Deliveries in U.S. Total Represented by the Price (%)" "Sourcekey","N3020US4" "Date","Percent of Commercial Natural Gas Deliveries in U.S. Total Represented by the Price (%)"

406

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010nh3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010nh3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:43 PM" "Back to Contents","Data 1: New Hampshire Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010NH3" "Date","New Hampshire Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

407

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010in2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010in2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:24 PM" "Back to Contents","Data 1: Indiana Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010IN2" "Date","Indiana Natural Gas Residential Consumption (MMcf)" 24653,139519 25019,145955 25384,156699 25749,158699 26114,162747 26480,169267

408

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ct3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ct3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:23 PM" "Back to Contents","Data 1: Connecticut Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3020CT3" "Date","Connecticut Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"

409

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010mo3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010mo3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:36 PM" "Back to Contents","Data 1: Missouri Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010MO3" "Date","Missouri Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

410

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040la2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040la2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:36 AM" "Back to Contents","Data 1: Louisiana Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040LA2" "Date","Louisiana Natural Gas Vented and Flared (MMcf)" 24653,161849 25019,166439 25384,158852 25749,154089 26114,103564 26480,63667 26845,102091

411

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ut2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ut2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:46 AM" "Back to Contents","Data 1: Utah Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040UT2" "Date","Utah Natural Gas Vented and Flared (MMcf)" 34592,646 34834,696 34865,4590 34895,4767 34926,4382 34957,4389 34987,4603 35018,4932

412

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010az2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010az2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:09 PM" "Back to Contents","Data 1: Arizona Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010AZ2" "Date","Arizona Natural Gas Residential Consumption (MMcf)" 24653,25376 25019,26681 25384,28426 25749,29679 26114,32619 26480,34259 26845,36280

413

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ak3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ak3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:06 PM" "Back to Contents","Data 1: Alaska Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010AK3" "Date","Alaska Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

414

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9132us3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9132us3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:27 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas Pipeline Exports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9132US3" "Date","Price of U.S. Natural Gas Pipeline Exports (Dollars per Thousand Cubic Feet)" 31228,3.92 31593,2.35

415

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010id3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010id3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:23 PM" "Back to Contents","Data 1: Idaho Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010ID3" "Date","Idaho Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

416

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010me2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010me2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:32 PM" "Back to Contents","Data 1: Maine Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010ME2" "Date","Maine Natural Gas Residential Consumption (MMcf)" 24653,3967 25019,3571 25384,4910 25749,5247 26114,5591 26480,6036 26845,6027 27210,6174

417

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ne3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ne3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:42 PM" "Back to Contents","Data 1: Nebraska Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010NE3" "Date","Nebraska Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

418

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040wy2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040wy2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:47 AM" "Back to Contents","Data 1: Wyoming Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040WY2" "Date","Wyoming Natural Gas Vented and Flared (MMcf)" 24653,1498 25019,13038 25384,17632 25749,18419 26114,3860 26480,8376 26845,6618 27210,6102

419

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010mn3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010mn3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:34 PM" "Back to Contents","Data 1: Minnesota Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010MN3" "Date","Minnesota Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

420

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ca2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ca2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:10 PM" "Back to Contents","Data 1: California Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010CA2" "Date","California Natural Gas Residential Consumption (MMcf)" 24653,522122 25019,517636 25384,562127 25749,552544 26114,630998 26480,637289

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


421

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040sd2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040sd2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:43 AM" "Back to Contents","Data 1: South Dakota Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040SD2" "Date","South Dakota Natural Gas Vented and Flared (MMcf)" 33253,384 33284,350 33312,382 33343,380 33373,382 33404,376 33434,405

422

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040nm2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040nm2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:41 AM" "Back to Contents","Data 1: New Mexico Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040NM2" "Date","New Mexico Natural Gas Vented and Flared (MMcf)" 35079,236 35110,220 35139,240 35170,230 35200,241 35231,229 35261,217

423

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010co2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010co2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:11 PM" "Back to Contents","Data 1: Colorado Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010CO2" "Date","Colorado Natural Gas Residential Consumption (MMcf)" 24653,75351 25019,78371 25384,81068 25749,82595 26114,84864 26480,89187

424

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Daily","12/17/2013" Daily","12/17/2013" ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","rngc2d.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/rngc2d.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:40 PM" "Back to Contents","Data 1: Natural Gas Futures Contract 2 (Dollars per Million Btu)" "Sourcekey","RNGC2" "Date","Natural Gas Futures Contract 2 (Dollars per Million Btu)" 34346,2.13 34347,2.072 34348,2.139 34351,2.196 34352,2.131

425

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ar3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ar3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:08 PM" "Back to Contents","Data 1: Arkansas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010AR3" "Date","Arkansas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

426

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040mo2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040mo2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:38 AM" "Back to Contents","Data 1: Missouri Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040MO2" "Date","Missouri Natural Gas Vented and Flared (MMcf)" 33253,0 33284,0 33312,0 33343,0 33373,0 33404,0 33434,0 33465,0 33496,0

427

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Daily","12/17/2013" Daily","12/17/2013" ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","rngc4d.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/rngc4d.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:29 PM" "Back to Contents","Data 1: Natural Gas Futures Contract 4 (Dollars per Million Btu)" "Sourcekey","RNGC4" "Date","Natural Gas Futures Contract 4 (Dollars per Million Btu)" 34323,1.894 34324,1.83 34325,1.859 34326,1.895 34330,1.965

428

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9010us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9010us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:55:17 AM" "Back to Contents","Data 1: U.S. Natural Gas Gross Withdrawals (MMcf)" "Sourcekey","N9010US2" "Date","U.S. Natural Gas Gross Withdrawals (MMcf)" 26679 26710 26738 26769 26799 26830 26860 26891 26922 26952 26983 27013 27044 27075 27103

429

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ut2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ut2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:45 AM" "Back to Contents","Data 1: Utah Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040UT2" "Date","Utah Natural Gas Vented and Flared (MMcf)" 24653,3000 25019,2906 25384,2802 25749,2852 26114,2926 26480,5506 26845,7664 27210,5259 27575,1806

430

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ak2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ak2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:06 PM" "Back to Contents","Data 1: Alaska Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010AK2" "Date","Alaska Natural Gas Residential Consumption (MMcf)" 32523,1793 32554,2148 32582,1566 32613,1223 32643,858 32674,638

431

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040nd2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040nd2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:39 AM" "Back to Contents","Data 1: North Dakota Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040ND2" "Date","North Dakota Natural Gas Vented and Flared (MMcf)" 24653,25795 25019,22050 25384,22955 25749,19862 26114,2686 26480,20786 26845,22533

432

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010al3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010al3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:07 PM" "Back to Contents","Data 1: Alabama Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010AL3" "Date","Alabama Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

433

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ar3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ar3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:09 PM" "Back to Contents","Data 1: Arkansas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010AR3" "Date","Arkansas Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

434

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010va2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010va2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:02 PM" "Back to Contents","Data 1: Virginia Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010VA2" "Date","Virginia Natural Gas Residential Consumption (MMcf)" 24653,41495 25019,43582 25384,46663 25749,49554 26114,49488 26480,55427

435

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040co2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040co2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:33 AM" "Back to Contents","Data 1: Colorado Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040CO2" "Date","Colorado Natural Gas Vented and Flared (MMcf)" 35079,112 35110,77 35139,78 35170,91 35200,100 35231,89 35261,100 35292,106

436

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ga2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ga2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:17 PM" "Back to Contents","Data 1: Georgia Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010GA2" "Date","Georgia Natural Gas Residential Consumption (MMcf)" 24653,80322 25019,84072 25384,87878 25749,87359 26114,88319 26480,85256 26845,86191

437

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020hi2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020hi2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:33 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Hawaii (MMcf)" "Sourcekey","N3020HI2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Hawaii (MMcf)"

438

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ga2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ga2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:31 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Georgia (MMcf)" "Sourcekey","N3020GA2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Georgia (MMcf)"

439

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ar2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ar2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:14 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Arkansas (MMcf)" "Sourcekey","N3020AR2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Arkansas (MMcf)"

440

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ct2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ct2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:12 PM" "Back to Contents","Data 1: Connecticut Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010CT2" "Date","Connecticut Natural Gas Residential Consumption (MMcf)" 24653,26177 25019,26437 25384,29048 25749,31187 26114,31878 26480,32879

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


441

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010dc3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010dc3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:14 PM" "Back to Contents","Data 1: District of Columbia Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010DC3" "Date","District of Columbia Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

442

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ri3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ri3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:54 PM" "Back to Contents","Data 1: Rhode Island Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010RI3" "Date","Rhode Island Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

443

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010sd3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010sd3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:56 PM" "Back to Contents","Data 1: South Dakota Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010SD3" "Date","South Dakota Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

444

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020de2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020de2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:26 PM" "Back to Contents","Data 1: Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Delaware (MMcf)" "Sourcekey","N3020DE2" "Date","Natural Gas Deliveries to Commercial Consumers (Including Vehicle Fuel through 1996) in Delaware (MMcf)"

445

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010tn3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010tn3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:58 PM" "Back to Contents","Data 1: Tennessee Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010TN3" "Date","Tennessee Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

446

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ny3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ny3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:48 PM" "Back to Contents","Data 1: New York Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010NY3" "Date","New York Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

447

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010or2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010or2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:51 PM" "Back to Contents","Data 1: Oregon Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010OR2" "Date","Oregon Natural Gas Residential Consumption (MMcf)" 24653,13427 25019,15126 25384,20507 25749,19742 26114,21217 26480,23331 26845,22271

448

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9140us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9140us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:33:47 PM" "Back to Contents","Data 1: U.S. Natural Gas Total Consumption (MMcf)" "Sourcekey","N9140US2" "Date","U.S. Natural Gas Total Consumption (MMcf)" 36906,2676998 36937,2309464 36965,2246633 36996,1807170 37026,1522382 37057,1444378

449

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Daily","12/17/2013" Daily","12/17/2013" ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","rngc1d.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/rngc1d.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:45 PM" "Back to Contents","Data 1: Natural Gas Futures Contract 1 (Dollars per Million Btu)" "Sourcekey","RNGC1" "Date","Natural Gas Futures Contract 1 (Dollars per Million Btu)" 34347,2.194 34348,2.268 34351,2.36 34352,2.318 34353,2.252

450

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010fl3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010fl3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:16 PM" "Back to Contents","Data 1: Florida Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010FL3" "Date","Florida Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

451

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3035us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3035us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:25:08 PM" "Back to Contents","Data 1: U.S. Natural Gas Industrial Consumption (MMcf)" "Sourcekey","N3035US2" "Date","U.S. Natural Gas Industrial Consumption (MMcf)" 36906,686540 36937,640026 36965,664918 36996,622054 37026,576532 37057,536820

452

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040fl2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040fl2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:34 AM" "Back to Contents","Data 1: Florida Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040FL2" "Date","Florida Natural Gas Vented and Flared (MMcf)" 26114,355 26480,284 27941,837 28306,607 29402,677 29767,428 30132,435 30497,198 30863,34

453

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ok2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ok2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:50 PM" "Back to Contents","Data 1: Oklahoma Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010OK2" "Date","Oklahoma Natural Gas Residential Consumption (MMcf)" 24653,67395 25019,74782 25384,75310 25749,77460 26114,75238 26480,77608

454

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ar2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ar2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:31 AM" "Back to Contents","Data 1: Arkansas Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040AR2" "Date","Arkansas Natural Gas Vented and Flared (MMcf)" 24653,997 25019,895 25384,1326 25749,226 26114,1734 26480,2649 26845,1947 27210,1716 27575,1318

455

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010me3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010me3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:32 PM" "Back to Contents","Data 1: Maine Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010ME3" "Date","Maine Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

456

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3060us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3060us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:27:25 PM" "Back to Contents","Data 1: Natural Gas Delivered to Consumers in the U.S. (MMcf)" "Sourcekey","N3060US2" "Date","Natural Gas Delivered to Consumers in the U.S. (MMcf)" 36906,2505011 36937,2156873 36965,2086568 36996,1663832

457

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010us2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010us2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:00 PM" "Back to Contents","Data 1: U.S. Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010US2" "Date","U.S. Natural Gas Residential Consumption (MMcf)" 11139,295700 11504,294406 11870,298520 12235,283197 12600,288236 12965,313498 13331,343346

458

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010in3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010in3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:25 PM" "Back to Contents","Data 1: Indiana Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010IN3" "Date","Indiana Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

459

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9011us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9011us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:55:36 AM" "Back to Contents","Data 1: U.S. Natural Gas Gross Withdrawals from Gas Wells (MMcf)" "Sourcekey","N9011US2" "Date","U.S. Natural Gas Gross Withdrawals from Gas Wells (MMcf)" 33253,1482053 33526,1363737 33984,1452098 34015,1305490

460

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020us3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020us3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:23:37 PM" "Back to Contents","Data 1: U.S. Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3020US3" "Date","U.S. Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


461

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010nv3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010nv3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:46 PM" "Back to Contents","Data 1: Nevada Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010NV3" "Date","Nevada Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

462

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9133us3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9133us3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:31 PM" "Back to Contents","Data 1: Price of Liquefied U.S. Natural Gas Exports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9133US3" "Date","Price of Liquefied U.S. Natural Gas Exports (Dollars per Thousand Cubic Feet)"

463

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010sc3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010sc3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:55 PM" "Back to Contents","Data 1: South Carolina Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010SC3" "Date","South Carolina Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

464

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010vt2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010vt2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:03 PM" "Back to Contents","Data 1: Vermont Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010VT2" "Date","Vermont Natural Gas Residential Consumption (MMcf)" 29402,1301 29767,1290 30132,1278 30497,1252 30863,1352 31228,1456 31593,1595

465

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Weekly","12/13/2013","1/10/1997" Weekly","12/13/2013","1/10/1997" ,"Data 2","Futures Prices",4,"Weekly","12/13/2013","12/24/1993" ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","ng_pri_fut_s1_w.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/ng/ng_pri_fut_s1_w.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:18 PM" "Back to Contents","Data 1: Spot Price" "Sourcekey","RNGWHHD" "Date","Weekly Henry Hub Natural Gas Spot Price (Dollars per Million Btu)"

466

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040in2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040in2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:35 AM" "Back to Contents","Data 1: Indiana Natural Gas Vented and Flared (Million Cubic Feet)" "Sourcekey","N9040IN2" "Date","Indiana Natural Gas Vented and Flared (Million Cubic Feet)" 33253,0 33284,0 33312,0 33343,0 33373,0

467

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3020ga3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3020ga3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:32 PM" "Back to Contents","Data 1: Georgia Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3020GA3" "Date","Georgia Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"

468

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010hi3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010hi3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:20 PM" "Back to Contents","Data 1: Hawaii Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010HI3" "Date","Hawaii Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

469

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ks2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ks2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:26 PM" "Back to Contents","Data 1: Kansas Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010KS2" "Date","Kansas Natural Gas Residential Consumption (MMcf)" 24653,84912 25019,89372 25384,94320 25749,97317 26114,98644 26480,100720 26845,96468

470

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9100us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9100us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 3:53:50 PM" "Back to Contents","Data 1: U.S. Natural Gas Imports (MMcf)" "Sourcekey","N9100US2" "Date","U.S. Natural Gas Imports (MMcf)" 26679,92694 26710,83870 26738,91581 26769,88407 26799,85844 26830,79121 26860,79428 26891,84400 26922,81157

471

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ga3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ga3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:18 PM" "Back to Contents","Data 1: Georgia Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010GA3" "Date","Georgia Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

472

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9133us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9133us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 2:23:31 PM" "Back to Contents","Data 1: Liquefied U.S. Natural Gas Exports (MMcf)" "Sourcekey","N9133US2" "Date","Liquefied U.S. Natural Gas Exports (MMcf)" 35445,5604 35476,5596 35504,5675 35535,5660 35565,3812 35596,3786 35626,3756 35657,7532

473

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9170us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9170us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:33:48 PM" "Back to Contents","Data 1: U.S. Natural Gas Pipeline & Distribution Use (MMcf)" "Sourcekey","N9170US2" "Date","U.S. Natural Gas Pipeline & Distribution Use (MMcf)" 36906,76386 36937,65770 36965,63626 36996,50736

474

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","na1504_nus_4a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/na1504_nus_4a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:46:13 PM" "Back to Contents","Data 1: U.S. Natural Gas % of Total Residential - Sales (%)" "Sourcekey","NA1504_NUS_4" "Date","U.S. Natural Gas % of Total Residential - Sales (%)" 32689,99.9 33054,99.2 33419,99.2 33785,99.1 34150,99.1 34515,99.1

475

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ct3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ct3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:13 PM" "Back to Contents","Data 1: Connecticut Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010CT3" "Date","Connecticut Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

476

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010us3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010us3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:01 PM" "Back to Contents","Data 1: U.S. Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010US3" "Date","U.S. Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

477

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040fl2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040fl2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:34 AM" "Back to Contents","Data 1: Florida Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040FL2" "Date","Florida Natural Gas Vented and Flared (MMcf)" 35079 35110 35139 35170 35200 35231 35261 35292 35323 35353 35384 35414 35445,0

478

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040mi2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040mi2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:37 AM" "Back to Contents","Data 1: Michigan Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040MI2" "Date","Michigan Natural Gas Vented and Flared (MMcf)" 24653,1861 25019,1120 25384,808 25749,809 26480,1032 26845,1117 27210,1268 27575,1612

479

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010ar2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010ar2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:08 PM" "Back to Contents","Data 1: Arkansas Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010AR2" "Date","Arkansas Natural Gas Residential Consumption (MMcf)" 32523,6774 32554,7118 32582,6736 32613,3835 32643,1927 32674,1402

480

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010la3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010la3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:29 PM" "Back to Contents","Data 1: Louisiana Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010LA3" "Date","Louisiana Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

Note: This page contains sample records for the topic "liquid water content" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


481

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9100us3m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9100us3m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/13/2013 3:53:51 PM" "Back to Contents","Data 1: Price of U.S. Natural Gas Imports (Dollars per Thousand Cubic Feet)" "Sourcekey","N9100US3" "Date","Price of U.S. Natural Gas Imports (Dollars per Thousand Cubic Feet)" 32523,1.72 32554,1.88

482

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ne2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ne2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:40 AM" "Back to Contents","Data 1: Nebraska Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040NE2" "Date","Nebraska Natural Gas Vented and Flared (MMcf)" 24653,0 25019,0 25384,0 25749,0 26114,1558 26480,1263 26845,834 27210,2137 27575,1398 27941,797

483

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9020us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9020us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:13 AM" "Back to Contents","Data 1: U.S. Natural Gas Repressuring (MMcf)" "Sourcekey","N9020US2" "Date","U.S. Natural Gas Repressuring (MMcf)" 26679 26710 26738 26769 26799 26830 26860 26891 26922 26952 26983 27013 27044 27075 27103 27134 27164

484

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2010 Annual",2010 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040pa2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040pa2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:43 AM" "Back to Contents","Data 1: Pennsylvania Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040PA2" "Date","Pennsylvania Natural Gas Vented and Flared (MMcf)" 24653,0 25019,0 25384,0 25749,0 26114,0 26480,0 26845,0 27210,98 27575,96 27941,99

485

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010oh2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010oh2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:48 PM" "Back to Contents","Data 1: Ohio Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010OH2" "Date","Ohio Natural Gas Residential Consumption (MMcf)" 24653,442360 25019,444964 25384,456414 25749,459972 26114,460820 26480,478331 26845,439212

486

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n9040ca2a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n9040ca2a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/19/2013 6:56:32 AM" "Back to Contents","Data 1: California Natural Gas Vented and Flared (MMcf)" "Sourcekey","N9040CA2" "Date","California Natural Gas Vented and Flared (MMcf)" 24653,3565 25019,2780 25384,3074 25749,2499 26114,575 26845,1999 27210,1560 27575,1537

487

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010us3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010us3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:22:01 PM" "Back to Contents","Data 1: U.S. Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010US3" "Date","U.S. Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

488

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","11/2013" Monthly","11/2013" ,"Release Date:","12/18/2013" ,"Next Release Date:","12/27/2013" ,"Excel File Name:","rngc1m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/rngc1m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/18/2013 12:22:41 PM" "Back to Contents","Data 1: Natural Gas Futures Contract 1 (Dollars per Million Btu)" "Sourcekey","RNGC1" "Date","Natural Gas Futures Contract 1 (Dollars per Million Btu)" 34349,2.347 34380,2.355 34408,2.109 34439,2.111 34469,1.941

489

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012 Annual",2012 ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3010az3a.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3010az3a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:21:09 PM" "Back to Contents","Data 1: Arizona Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" "Sourcekey","N3010AZ3" "Date","Arizona Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"

490

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013" Monthly","9/2013" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","n3045us2m.xls" ,"Available from Web Page:","http://tonto.eia.gov/dnav/ng/hist/n3045us2m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"12/12/2013 5:26:13 PM" "Back to Contents","Data 1: U.S. Natural Gas Deliveries to Electric Power Consumers (MMcf)" "Sourcekey","N3045US2" "Date","U.S. Natural Gas Deliveries to Electric Power Consumers (MMcf)" 36906,340292 36937,312843 36965,362843

491

Microsoft Word - contents  

Office of Legacy Management (LM)

GJO-2001-272-TAR GJO-2001-272-TAR MAC-GWDUR 1.1 UMTRA Ground Water Project Site Observational Work Plan for the Durango, Colorado, UMTRA Project Site January 2002 Prepared by U.S. Department of Energy Grand Junction Office Grand Junction, Colorado Project Number UGW 511-0006-10-000 Document Number U0143200 Work Performed Under DOE Contract Number DE-AC13-96GJ87335 This page intentionally left blank Document Number U0143200 Contents DOE/Grand Junction Office Site Observational Work Plan -Durango, Colorado January 2002 Page iii Contents 1.0 Introduction ......................................................................................................................1-1 1.1 Purpose and Scope .................................................................................................1-1

492

LNG liquid-liquid immiscibility  

SciTech Connect

Although natural gas species rarely exhibit liquid-liquid immiscibility in binary systems, the presence of additional components can extend the domain of immiscibility in those few binary systems where it already exists or produce immiscibility in binary systems where it had not existed. If the solute has the proper molecular relation to the solvent mixture background, liquid-liquid-vapor (LLV) behavior will occur; such phenomena greatly complicate the design of LNG processing equipment. To aid LNG engineers, researchers mapped the thermodynamic behavior of four ternary LLV systems and examined the effects of the second solvents - ethane, propane, n-butane, and CO/sub 2/ - on the binary methane + n-octane system.

Luks, K.D.; Kohn, J.P.

1981-09-01T23:59:59.000Z

493

Ionic Liquids as Green Solvents for Alkylation and Acylation  

Science Journals Connector (OSTI)

Many clean solvents like water, ionic liquids, supercritical fluid, polyglycol, fluorine-containing solvents, and so on are employed to replace the conventional organic solvents. Among these, ionic liquids have a...

Zhongkui Zhao; Yitao Dai

2012-01-01T23:59:59.000Z

494

TABLE OF CONTENTS TABLE OF CONTENTS ...........................................................................................................................................II  

NLE Websites -- All DOE Office Websites (Extended Search)

i i ii TABLE OF CONTENTS TABLE OF CONTENTS ...........................................................................................................................................II EXECUTIVE SUMMARY ........................................................................................................................................... 3 INTRODUCTION......................................................................................................................................................... 4 COMPLIANCE SUMMARY ....................................................................................................................................... 6 COMPREHENSIVE ENVIRONMENTAL RESPONSE, COMPENSATION, AND LIABILITY ACT (CERCLA) .................... 6

495

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1997" Monthly","9/2013","1/15/1997" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","ng_sum_lsum_a_epg0_fpd_mmcf_m.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/ng/ng_sum_lsum_a_epg0_fpd_mmcf_m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"12/19/2013 6:41:46 AM" "Back to Contents","Data 1: Natural Gas Dry Production (Annual Supply & Disposition) " "Sourcekey","N9070US2","NA1160_R3FM_2","NA1160_SAL_2","NA1160_SAK_2","NA1160_SAZ_2","NA1160_SAR_2","NA1160_SCA_2","NA1160_SCO_2","NA1160_SFL_2","NA1160_SIL_2","NA1160_SIN_2","NA1160_SKS_2","NA1160_SKY_2","NA1160_SLA_2","NA1160_SMD_2","NA1160_SMI_2","NA1160_SMS_2","NA1160_SMO_2","NA1160_SMT_2","NA1160_SNE_2","NA1160_SNV_2","NA1160_SNM_2","NA1160_SNY_2","NA1160_SND_2","NA1160_SOH_2","NA1160_SOK_2","NA1160_SOR_2","NA1160_SPA_2","NA1160_SSD_2","NA1160_STN_2","NA1160_STX_2","NA1160_SUT_2","NA1160_SVA_2","NA1160_SWV_2","NA1160_SWY_2"

496

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Annual",2012,"6/30/1930" Annual",2012,"6/30/1930" ,"Release Date:","12/12/2013" ,"Next Release Date:","1/7/2014" ,"Excel File Name:","ng_sum_snd_a_epg0_fpd_mmcf_a.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/ng/ng_sum_snd_a_epg0_fpd_mmcf_a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"12/12/2013 7:08:03 PM" "Back to Contents","Data 1: Natural Gas Dry Production (Annual Supply & Disposition) " "Sourcekey","N9070US2","NA1160_SAL_2","NA1160_SAK_2","NA1160_SAZ_2","NA1160_SAR_2","NA1160_SCA_2","NA1160_SCO_2","NA1160_SFL_2","NA1160_R3FM_2","NA1160_SIL_2","NA1160_SIN_2","NA1160_SKS_2","NA1160_SKY_2","NA1160_SLA_2","NA1160_SMD_2","NA1160_SMI_2","NA1160_SMS_2","NA1160_SMO_2","NA1160_SMT_2","NA1160_SNE_2","NA1160_SNV_2","NA1160_SNM_2","NA1160_SNY_2","NA1160_SND_2","NA1160_SOH_2","NA1160_SOK_2","NA1160_SOR_2","NA1160_SPA_2","NA1160_SSD_2","NA1160_STN_2","NA1160_STX_2","NA1160_SUT_2","NA1160_SVA_2","NA1160_SWV_2","NA1160_SWY_2"

497

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

mbblpd_m.xls" mbblpd_m.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_move_exp_dc_nus-z00_mbblpd_m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"11/25/2013 7:27:48 AM" "Back to Contents","Data 1: U.S. Exports of Crude Oil and Petroleum Products" "Sourcekey","MTTEXUS2","MCREXUS2","MNGEXUS2","MPPEXUS2","MLPEXUS2","METEXUS2","MPREXUS2","MBNEXUS2","MBIEXUS2","MOLEXUS2","MOHEXUS2","M_EPOOXXFE_EEX_NUS-Z00_MBBLD","MMTEX_NUS-Z00_2","MOOEX_NUS-Z00_2","M_EPOOR_EEX_NUS-Z00_MBBLD","M_EPOOXE_EEX_NUS-Z00_MBBLD","M_EPOORDB_EEX_NUS-Z00_MBBLD","MBCEXUS2","MO1EX_NUS-Z00_2","MO5EX_NUS-Z00_2","MBAEXUS2","MTPEXUS2","MGFEXUS2","MGREXUS2","MG4EX_NUS-Z00_2","MGAEXUS2","MKJEXUS2","MKEEXUS2","MDIEXUS2","M_EPDXL0_EEX_NUS-Z00_MBBLD","MD1EX_NUS-Z00_2","MDGEXUS2","MREEXUS2","MNFEXUS2","MOTEXUS2","MNSEXUS2","MLUEXUS2","MWXEXUS2","MCKEXUS2","MAPEXUS2","MMSEXUS2"

498

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

mbbl_m.xls" mbbl_m.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_cons_psup_dc_nus_mbbl_m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"11/25/2013 7:26:09 AM" "Back to Contents","Data 1: U.S. Product Supplied for Crude Oil and Petroleum Products" "Sourcekey","MTTUPUS1","MCRUPUS1","MNGUPUS1","MPPUPUS1","MLPUPUS1","METUPUS1","MPRUPUS1","MBNUPUS1","MBIUPUS1","MOLUPUS1","MOHUPUS1","MUOUPUS1","MBCUPUS1","MO1UP_NUS_1","MO5UP_NUS_1","MBAUPUS1","MTPUPUS1","MGFUPUS1","MGRUPUS1","MG4UP_NUS_1","MGAUPUS1","MKJUPUS1","MKEUPUS1","MDIUPUS1","MD0UP_NUS_1","MD1UP_NUS_1","MDGUPUS1","MREUPUS1","MPCUP_NUS_1","MNFUPUS1","MOTUPUS1","MNSUPUS1","MLUUPUS1","MWXUPUS1","MCKUPUS1","MCMUP_NUS_1","MCOUP_NUS_1","MAPUPUS1","MSGUPUS1","MMSUPUS1"

499

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

Monthly","9/2013","1/15/1985" Monthly","9/2013","1/15/1985" ,"Release Date:","11/27/2013" ,"Next Release Date:","Last Week of December 2013" ,"Excel File Name:","pet_pnp_unc_dcu_nus_m.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_pnp_unc_dcu_nus_m.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"11/25/2013 11:30:03 AM" "Back to Contents","Data 1: U.S. Refinery Utilization and Capacity" "Sourcekey","MGIRIUS2","MOCLEUS2","MOCGGUS2","MOCIDUS2","MOPUEUS2" "Date","U.S. Gross Inputs to Refineries (Thousand Barrels Per Day)","U. S. Operable Crude Oil Distillation Capacity (Thousand Barrels per Calendar Day)","U. S. Operating Crude Oil Distillation Capacity (Thousand Barrels per Day)","U. S. Idle Crude Oil Distillation Capacity (Thousand Barrels per Day)","U.S. Percent Utilization of Refinery Operable Capacity"

500

Workbook Contents  

U.S. Energy Information Administration (EIA) Indexed Site

capwork_a_(na)_8sw0_mbbl_a.xls" capwork_a_(na)_8sw0_mbbl_a.xls" ,"Available from Web Page:","http://www.eia.gov/dnav/pet/pet_pnp_capwork_a_(na)_8sw0_mbbl_a.htm" ,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.gov" ,,"(202) 586-8800",,,"6/20/2013 4:20:16 PM" "Back to Contents","Data 1: Total " "Sourcekey","8_NA_8SW0_NUS_MBBL","8_NA_8SW0_R10_MBBL","8_NA_8SW0_R20_MBBL","8_NA_8SW0_R30_MBBL","8_NA_8SW0_R40_MBBL","8_NA_8SW0_R50_MBBL" "Date","U.S. Refinery Working Storage Capacity as of January 1 (Thousand Barrels)","East Coast (PADD 1) Refinery Working Storage Capacity as of January 1 (Thousand Barrels)","Midwest (PADD 2) Refinery Working Storage Capacity as of January 1 (Thousand Barrels)","Gulf Coast (PADD 3) Refinery Working Storage Capacity as of January 1 (Thousand Barrels)","Rocky Mountain (PADD 4) Refinery Working Storage Capacity as of January 1 (Thousand Barrels)","West Coast (PADD 5) Refinery Working Storage Capacity as of January 1 (Thousand Barrels)"