Powered by Deep Web Technologies
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

Airborne Measurement of Liquid and Total Water Content  

Science Conference Proceedings (OSTI)

Two identical liquid water content (LWC) King probes—one total water content/liquid water content (TWC/LWC) Nevzorov probe and two constant-temperature T probes that are different in size to distinguish particles of different densities and ...

German Vidaurre; John Hallett; David C. Rogers

2011-09-01T23:59:59.000Z

2

Determination of Supercooled Liquid Water Content by Measuring Rime Rate  

Science Conference Proceedings (OSTI)

A ground-based technique is described for determining the liquid water content of supercooled clouds orfog by measuring the mass rate of rime accumulation on a small rotating wire. Development of the techniqueis described, examples of the data ...

David C. Rogers; Darrel Baumgardner; Gabor Vali

1983-01-01T23:59:59.000Z

3

Spectral Density of Cloud Liquid Water Content at High Frequencies  

Science Conference Proceedings (OSTI)

Aircraft measurements of liquid water content (LWC) made at sampling frequencies of 1 and 2 kHz with a particle volume monitor (PVM) probe from horizontal traverses in stratocumulus clouds during the Southern Ocean Cloud Experiment and cumulus ...

H. Gerber; J. B. Jensen; A. B. Davis; A. Marshak; W. J. Wiscombe

2001-03-01T23:59:59.000Z

4

Cloud Liquid Water and Ice Content Retrieval by Multiwavelength Radar  

Science Conference Proceedings (OSTI)

Cloud liquid water and ice content retrieval in precipitating clouds by the differential attenuation method using a dual-wavelength radar, as a function of the wavelength pair, is first discussed. In the presence of non-Rayleigh scatterers, ...

Nicolas Gaussiat; Henri Sauvageot; Anthony J. Illingworth

2003-09-01T23:59:59.000Z

5

Stratocumulus Liquid Water Content from Dual-Wavelength Radar  

Science Conference Proceedings (OSTI)

A technique is described to retrieve stratocumulus liquid water content (LWC) using the differential attenuation measured by vertically pointing radars at 35 and 94 GHz. Millimeter-wave attenuation is proportional to LWC and increases with ...

Robin J. Hogan; Nicolas Gaussiat; Anthony J. Illingworth

2005-08-01T23:59:59.000Z

6

Assessment of Vertically Integrated Liquid (VIL) Water Content Radar Measurement  

Science Conference Proceedings (OSTI)

Vertically integrated liquid (VIL) water content is a parameter obtained from a radar performing voluminal scanning. This parameter has proven useful in the detection of severe storms and may be a worthwhile indicator for very short-term rainfall ...

Brice Boudevillain; Hervé Andrieu

2003-06-01T23:59:59.000Z

7

Experimental Verification of the Linear Relationship between IR Extinction and Liquid Water Content of Clouds  

Science Conference Proceedings (OSTI)

The IR extinction of clouds has been measured with a CO2 laster transmissometer (? = 10.6 ?m). Using an established linear relationship (based on the Chýlek approximation to the Mie theory) between extinction and liquid water content, the liquid ...

Alan W. Gertler; Roger L. Steele

1980-11-01T23:59:59.000Z

8

Analysis of Rotating Multicylinder Data in Measuring Cloud-Droplet Size and Liquid Water Content  

Science Conference Proceedings (OSTI)

An objective method is presented for the analysis of rotating multicylinder data in measuring the liquid water content and median volume droplet diameter of icing clouds. The method is based on time-dependent numerical modeling of cylinder icing ...

Lasse Makkonen

1992-06-01T23:59:59.000Z

9

Sources of Error in Dual-Wavelength Radar Remote Sensing of Cloud Liquid Water Content  

Science Conference Proceedings (OSTI)

Dual-wavelength ratio (DWR) techniques offer the prospect of producing high-resolution mapping of cloud microphysical properties, including retrievals of cloud liquid water content (LWC) from reflectivity measured by millimeter-wavelength radars. ...

John K. Williams; J. Vivekanandan

2007-08-01T23:59:59.000Z

10

Comparison of Nimbus-7 SMMR and GOES-1 VISSR Atmospheric Liquid Water Content  

Science Conference Proceedings (OSTI)

Vertically integrated atmospheric liquid water content derived from Nimbus-7 Scanning Multichannel Microwave Radiometer (SMMR) brightness temperatures and from GOES-1 Visible and Infrared Spin-Scan Radiometer (VISSR) radiances in the visible are ...

Jean-Yves Lojou; Robert Frouin; René Bernard

1991-02-01T23:59:59.000Z

11

Calibrations of Johnson-Williams Liquid Water Content Meters in a High-Speed Icing Tunnel  

Science Conference Proceedings (OSTI)

Wind tunnel tests have provided calibrations and intercomparisons of 14 Johnson-Williams (J–W) cloud liquid water content (LWC) measuring devices with 23 sensor heads from 10 research organizations. The absolute tunnel LWC was deduced using a ...

J. Walter Strapp; Robert S. Schemenauer

1982-01-01T23:59:59.000Z

12

Ground-Based FSSP and PVM Measurements of Liquid Water Content  

Science Conference Proceedings (OSTI)

Recently published ground-based measurements of liquid water content (LWC) measured in fogs by two microphysical instruments, the FSSP-100 and PVM-100, are evaluated. These publications had suggested that the PVM-100 underestimated LWC ...

H. Gerber; Glendon Frick; Alfred R. Rodi

1999-08-01T23:59:59.000Z

13

Probability Density Functions of Liquid Water Path and Total Water Content of Marine Boundary Layer Clouds: Implications for Cloud Parameterization  

Science Conference Proceedings (OSTI)

Mathematical forms of probability density functions (PDFs) of liquid water path (LWP) and total water content for marine boundary layer clouds are investigated using the homogeneity, skewness, and kurtosis of PDFs of LWP obtained from observations ...

Hideaki Kawai; Joăo Teixeira

2012-03-01T23:59:59.000Z

14

Liquid Water Content of Fogs and Hazes from Visible Light Scattering  

Science Conference Proceedings (OSTI)

A new method is proposed for measuring the liquid water content of fogs and hazes. It consists of a planar circular light sensor placed perpendicular to and coaxial with a narrow collimated light beam of a visible wavelength. The direct light ...

H. Gerber

1984-08-01T23:59:59.000Z

15

Extinction and Liquid Water Content Measurements at CO2 Laser wavelengths  

Science Conference Proceedings (OSTI)

Measurements have been made of both extinction coefficients in an evaporating laboratory cloud at wavelength ? = 10.591 ?m using a CO2 laser, and of liquid water content (LWC) at the center of the cloud using a continuous filtration LWC device. ...

P. F. Nolan; S. G. Jennings

1987-09-01T23:59:59.000Z

16

In Situ Aircraft Measurements of the Vertical Distribution of Liquid and Ice Water Content in Midlatitude Mixed-Phase Clouds  

Science Conference Proceedings (OSTI)

The vertical distribution of liquid and ice water content and their partitioning is studied using 34 cases of in situ measured microphysical properties in midlatitude mixed-phase clouds, with liquid water path ranging from near zero to ~248 g m?2, ...

Yoo-Jeong Noh; Curtis J. Seaman; Thomas H. Vonder Haar; Guosheng Liu

2013-01-01T23:59:59.000Z

17

The Use of Routine Weather Observations to Calculate Liquid Water Content in Summertime High-Elevation Fog  

Science Conference Proceedings (OSTI)

This paper represents a stage within a larger project to estimate acid ion deposition from cloud impacting on high-elevation forests. Acid ion deposition depends principally on three factors: the liquid water content (LWC), the ion concentration(...

John L. Walmsley; William R. Burrows; Robert S. Schemenauer

1999-04-01T23:59:59.000Z

18

Retrieval of Vertical Profiles of Liquid Water and Ice Content in Mixed Clouds from Doppler Radar and Microwave Radiometer Measurements  

Science Conference Proceedings (OSTI)

A new method to retrieve vertical profiles of liquid water content Mw(z), ice water content Mi(z), and ice particle size distribution Ni(D, z), (where D is the ice particle size and z the vertical coordinate) in mixed nonprecipitating clouds ...

Henri Sauvageot

1996-01-01T23:59:59.000Z

19

Wind Tunnel Measurements of the Response of Hot-Wire Liquid Water Content Instruments to Large Droplets  

Science Conference Proceedings (OSTI)

Wet wind tunnel tests were performed on more than 23 cloud liquid water content (LWC) probes and drop spectrometers at the NASA Icing Research Tunnel, with a main objective to characterize their response to large-droplet conditions. As a part of ...

J. W. Strapp; J. Oldenburg; R. Ide; L. Lilie; S. Bacic; Z. Vukovic; M. Oleskiw; D. Miller; E. Emery; G. Leone

2003-06-01T23:59:59.000Z

20

Measurement of Condensed Water Content in Liquid and Ice Clouds Using an Airborne Counterflow Virtual Impactor  

Science Conference Proceedings (OSTI)

Condensed water content (CWC) measured using a counterflow virtual impactor (CVI) with a Lyman-? hygrometer downstream is compared with that measured by other airborne instruments (a hot-wire probe, a PMS FSSP, and a PMS 2D-C). Results indicate ...

Cynthia H. Twohy; Allen J. Schanot; William A. Cooper

1997-02-01T23:59:59.000Z

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.


21

Sensitivity of Cloud Liquid Water Content Estimates to the Temperature-Dependent Thermodynamic Phase: A Global Study Using CloudSat Data  

Science Conference Proceedings (OSTI)

The main purpose of this study is to underline the sensitivity of cloud liquid water content (LWC) estimates purely to 1) the shape of computationally simplified temperature-dependent thermodynamic phase and 2) the range of subzero temperatures ...

Abhay Devasthale; Manu Anna Thomas

2012-10-01T23:59:59.000Z

22

Thermodynamics of Icing Cylinder for Measurements of Liquid Water Content in Supercooled Clouds  

Science Conference Proceedings (OSTI)

The Rosemount Icing Detector (RICE) has been used extensively over the last three decades for aircraft measurements of the rate of ice riming in supercooled liquid and mixed clouds. Because of difficulties related to calibration and ...

I. P. Mazin; A. V. Korolev; A. Heymsfield; G. A. Isaac; S. G. Cober

2001-04-01T23:59:59.000Z

23

Active probing of cloud multiple scattering, optical depth, vertical thickness, and liquid water content using wide-angle imaging LIDAR.  

SciTech Connect

At most optical wavelengths, laser light in a cloud lidar experiment is not absorbed but merely scattered out of the beam, eventually escaping the cloud via multiple scattering. There is much information available in this light scattered far from the input beam, information ignored by traditional 'on-beam' lidar. Monitoring these off-beam returns in a fully space- and time-resolved manner is the essence of our unique instrument, Wide Angle Imaging Lidar (WAIL). In effect, WAIL produces wide-field (60-degree full-angle) 'movies' of the scattering process and records the cloud's radiative Green functions. A direct data product of WAIL is the distribution of photon path lengths resulting from multiple scattering in the cloud. Following insights from diffusion theory, we can use the measured Green functions to infer the physical thickness and optical depth of the cloud layer, and, from there, estimate the volume-averaged liquid water content. WAIL is notable in that it is applicable to optically thick clouds, a regime in which traditional lidar is reduced to ceilometry. Here we present recent WAIL data oti various clouds and discuss the extension of WAIL to full diurnal monitoring by means of an ultra-narrow magneto-optic atomic line filter for daytime measurements.

Love, Steven P.; Davis, A. B. (Anthony B.); Rohde, C. A. (Charles A.); Tellier, L. L. (Larry L.); Ho, Cheng,

2002-01-01T23:59:59.000Z

24

ARM - Measurement - Ice water content  

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

to hear from you Send us a note below or call us at 1-888-ARM-DATA. Send Measurement : Ice water content The concentration (massvol) of ice water particles in a cloud....

25

ARM - Measurement - Liquid water content  

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

Instruments ETA : Eta Model Runs ECMWFDIAG : European Centre for Medium Range Weather Forecasts Diagnostic Analyses ECMWF : European Centre for Medium Range Weather Forecasts Model...

26

Icing Wind Tunnel Tests on the CSIRO Liquid Water Probe  

Science Conference Proceedings (OSTI)

Wet wind tunnel tests have been Performed on several versions of the CSIRO probe designed for the airborne measurement of liquid water content. Four different controller units and 17 different Probe sensors (including half-size and shielded ...

W. D. King; J. E. Dye; D. Baumgardner; J. W. Strapp; D. Huffman

1985-09-01T23:59:59.000Z

27

ARM: Microwave Radiometer data (MWR Profiles - QME), water vapor, temp, cloud liquid water, precip water retrievals  

DOE Data Explorer (OSTI)

Microwave Radiometer data (MWR Profiles - QME), water vapor, temp, cloud liquid water, precip water retrievals

Maria Cadeddu

28

Electrokinetic Power Generation from Liquid Water Microjets  

E-Print Network (OSTI)

Electrokinetic power generation using liquid water microjetscalculations of power generation and conversion efficiency.for electrokinetic power generation. By creating a jet of

Duffin, Andrew M.

2008-01-01T23:59:59.000Z

29

Further Performance Tests on the CSIRO Liquid Water Probe  

Science Conference Proceedings (OSTI)

A further 400 h of flying experience with the CSIRO hot-wire probe has shown that it can accurately measure liquid water content in clouds. Computations and experiments suggest that when an epoxy coating is used for protection, it should be less ...

W. D. King; C. T. Maher; G. A. Hepburn

1981-02-01T23:59:59.000Z

30

Rain Rate and Water Content in Hurricanes Compared with Summer Rain in Miami, Florida  

Science Conference Proceedings (OSTI)

Liquid water content (g m?3), precipitation rate (mm h?1), and radar reflectivity (dBZ) are inferred from cross sections of particle images obtained by aircraft. Each dataset is presented in a probability format to display changing functional ...

Robert A. Black; John Hallett

2012-12-01T23:59:59.000Z

31

Electrokinetic Power Generation from Liquid Water Microjets  

DOE Green Energy (OSTI)

Although electrokinetic effects are not new, only recently have they been investigated for possible use in energy conversion devices. We have recently reported the electrokinetic generation of molecular hydrogen from rapidly flowing liquid water microjets [Duffin et al. JPCC 2007, 111, 12031]. Here, we describe the use of liquid water microjets for direct conversion of electrokinetic energy to electrical power. Previous studies of electrokinetic power production have reported low efficiencies ({approx}3%), limited by back conduction of ions at the surface and in the bulk liquid. Liquid microjets eliminate energy dissipation due to back conduction and, measuring only at the jet target, yield conversion efficiencies exceeding 10%.

Duffin, Andrew M.; Saykally, Richard J.

2008-02-15T23:59:59.000Z

32

Liquid Water Oceans in Ice Giants  

E-Print Network (OSTI)

Aptly named, ice giants such as Uranus and Neptune contain significant amounts of water. While this water cannot be present near the cloud tops, it must be abundant in the deep interior. We investigate the likelihood of a liquid water ocean existing in the hydrogen-rich region between the cloud tops and deep interior. Starting from an assumed temperature at a given upper tropospheric pressure (the photosphere), we follow a moist adiabat downward. The mixing ratio of water to hydrogen in the gas phase is small in the photosphere and increases with depth. The mixing ratio in the condensed phase is near unity in the photosphere and decreases with depth; this gives two possible outcomes. If at some pressure level the mixing ratio of water in the gas phase is equal to that in the deep interior, then that level is the cloud base. Alternately, if the mixing ratio of water in the condensed phase reaches that in the deep interior, then the surface of a liquid ocean will occur. We find that Neptune is both too warm (photospheric temperature too high) and too dry (mixing ratio of water in the deep interior too low) for liquid oceans to exist at present. To have a liquid ocean, Neptune's deep interior water to gas ratio would have to be higher than current models allow, and the density at 19 kbar would have to be ~ 0.8 g/cm^3. Such a high density is inconsistent with gravitational data obtained during the Voyager flyby. As Neptune cools, the probability of a liquid ocean increases. Extrasolar "hot Neptunes," which presumably migrate inward toward their parent stars, cannot harbor liquid water oceans unless they have lost almost all of the hydrogen and helium from their deep interiors.

Sloane J. Wiktorowicz; Andrew P. Ingersoll

2006-09-26T23:59:59.000Z

33

Fluid Metrology Calibration Services - Gas, Water, or Liquid ...  

Science Conference Proceedings (OSTI)

Fluid Metrology Calibration Services - Gas, Water, Natural Gas, or Liquid Hydrocarbon Flows Special Tests. Fluid Metrology ...

2013-01-25T23:59:59.000Z

34

Liquid chromatographic determination of water  

DOE Green Energy (OSTI)

A sensitive method for the determination of water in the presence of common interferences is presented. The detection system is based on the effect of water on the equilibrium which results from the reaction aryl aldehydes, such as cinnamaldehyde and methanol in the eluent to form cinnamaldehyde dimethylacetal, plus water. This equilibrium is shifted in a catalytic atmosphere of a hydrogen ion form past column reactor. The extent of the shift and the resulting change in absorbance are proportional to the amount of water present.

Fortier, Nancy E. (Fairfield, OH); Fritz, James S. (Ames, IA)

1990-11-13T23:59:59.000Z

35

An Integrated Approach toward Retrieving Physically Consistent Profiles of Temperature, Humidity, and Cloud Liquid Water  

Science Conference Proceedings (OSTI)

A method is presented for deriving physically consistent profiles of temperature, humidity, and cloud liquid water content. This approach combines a ground-based multichannel microwave radiometer, a cloud radar, a lidar-ceilometer, the nearest ...

Ulrich Löhnert; Susanne Crewell; Clemens Simmer

2004-09-01T23:59:59.000Z

36

Near-Global Survey of Effective Droplet Radii in Liquid Water Clouds Using ISCCP Data  

Science Conference Proceedings (OSTI)

A global survey of cloud particle size variations can provide crucial constraints on how cloud processes determine cloud liquid water contents and their variation with temperature, and further, may indicate the magnitude of aerosol effects on ...

Qingyuan Han; William B. Rossow; Andrew A. Lacis

1994-04-01T23:59:59.000Z

37

The Temperature Dependence of the Liquid Water Path of Low Clouds in the Southern Great Plains  

Science Conference Proceedings (OSTI)

Satellite observations of low-level clouds have challenged the idea that increasing liquid water content with temperature combined with constant physical thickness will lead to a negative cloud optics feedback in a decadal climate change. The ...

Anthony D. Del Genio; Audrey B. Wolf

2000-10-01T23:59:59.000Z

38

USE OF IONIC LIQUIDS IN PRODUCED WATER CLEAN UP J. McFarlane  

E-Print Network (OSTI)

USE OF IONIC LIQUIDS IN PRODUCED WATER CLEAN UP J. McFarlane Oak Ridge National Laboratory P.O. Box amounts of contaminated water along with the hydrocarbon phase, termed "produced water" by the industry 1 Agency (EPA) limit on oil and grease content in produced water discharged in the ocean is a daily maximum

39

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.

40

Molecular mean field theory for liquid water  

E-Print Network (OSTI)

Attractive bonding interactions between molecules typically have inherent conservation laws which influence the statistical properties of such systems in terms of corresponding sum rules. We considered lattice water as an example and enunciated the consequences of the sum rule through a general computational procedure called "Molecular mean field" theory. Fluctuations about mean field are computed and many of the liquid properties have been deduced and compared with Monte Carlo simulation, molecular dynamics and experimental results. Large correlation lengths are seen to be a consequence of the sum rule in liquid phase. Long range Coulomb interactions are shown to have minor effects on our results.

Jampa Maruthi Pradeep Kanth; Ramesh Anishetty

2010-04-09T23:59:59.000Z

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

Thin Liquid Water Clouds: Their Importance and Our Challenge  

Science Conference Proceedings (OSTI)

Many of the clouds important to the Earth's energy balance, from the Tropics to the Arctic, contain small amounts of liquid water. Longwave and shortwave radiative fluxes are very sensitive to small perturbations of the cloud liquid water path (...

D. D. Turner; A. M. Vogelmann; K. Johnson; M. Miller; R. T. Austin; J. C. Barnard; C. Flynn; C. Long; S. A. McFarlane; K. Cady-Pereira; S. A. Clough; J. C. Chiu; M. M. Khaiyer; J. Liljegren; B. Lin; P. Minnis; A. Marshak; S. Y. Matrosov; Q. Min; W. O'Hirok; Z. Wang; W. Wiscombe

2007-02-01T23:59:59.000Z

42

Cold Water Model Simulation of Aluminum Liquid Fluctuations ...  

Science Conference Proceedings (OSTI)

Symposium, Electrode Technology for Aluminium Production ... Cold Water Model Simulation of Aluminum Liquid Fluctuations Induced by Anodic Gas in New ...

43

On the Fluctuations that Order and Frustrate Liquid Water  

E-Print Network (OSTI)

Quantitative water model . . . . . . . . . . . . . . . .5.3 Determining T g for water . . . . . . . . . . . . . . .iv Contents 6 Frustrating water at ordered surfaces 6.1

Limmer, David

2013-01-01T23:59:59.000Z

44

CONTENTS Water Issues Dominate Oil and  

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

Water Issues Dominate Oil and Gas Production ...1 Editor's Letter ...2 Zero Discharge Water Management for Horizontal Shale...

45

A Review Of Water Contents Of Nominally Anhydrous Natural Minerals...  

Open Energy Info (EERE)

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...

46

The Drop-Size Response of the CSIRO Liquid Water Probe  

Science Conference Proceedings (OSTI)

The response of the CSIRO liquid water content (LWC) device to water drops of different sizes has been investigated in a wind tunnel. Two series of experiments were conducted. The first compared the probe-measured LWC of sprays with different ...

C. J. Biter; J. E. Dye; D. Huffman; W. D. King

1987-09-01T23:59:59.000Z

47

Cloud Liquid Water Measurements on the Armored T-28: Intercomparison between Johnson–Williams Cloud Water Meter and CSIRO (King) Liquid Water Probe  

Science Conference Proceedings (OSTI)

Comparisons are made between liquid water concentration (LWC) readings obtained from a Johnson–Williams (J–W) cloud water meter and a King (Commonwealth Scientific and Industrial Research Organisation) liquid water probe, both mounted on the ...

Rand E. Feind; Andrew G. Detwiler; Paul L. Smith

2000-12-01T23:59:59.000Z

48

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

49

A new soil water content sensor with temperature compensation design  

Science Conference Proceedings (OSTI)

The design and construction of a soil water content sensor with temperature compensation using the piecewise linear interpolation method was presented in this paper. The sensor out put often influenced by temperature, so temperature compensation must ... Keywords: circuitry system, geological disaster, interpolation method, piecewise linear, soil water content sensor, temperature compensation

Shi Ge; Li Qing

2009-05-01T23:59:59.000Z

50

Liquid Fuels from CO2, Water, and Solar Energy  

Science Conference Proceedings (OSTI)

Symposium, Energy Technologies and Carbon Dioxide Management. Presentation Title, Liquid Fuels from CO2, Water, and Solar Energy. Author(s), Aldo ...

51

Ab Initio Quantum Liquid Water and Aqueous Ionic Solutions |...  

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

250 Million Year: 2013 Research Domain: Physics A highly accurate and detailed understanding of the microscopic structure of liquid water is of great importance to a number of...

52

Effect of Water Content on SOFC Single Cell Testing: Materials ...  

Science Conference Proceedings (OSTI)

The cell was tested at 800C using pure H2 with different water content (~3% and ~30%). Impedance, IV curve, and power density were recorded. SEM and OM ...

53

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.

54

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.

55

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.

56

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

57

MODELING OF WATER SOLUBLE ORGANIC CONTENT IN PRODUCED WATER J. McFarlane  

E-Print Network (OSTI)

MODELING OF WATER SOLUBLE ORGANIC CONTENT IN PRODUCED WATER J. McFarlane Oak Ridge National Laboratory P.O. Box 2008 Oak Ridge, TN 37830-6181 INTRODUCTION Off-shore discharge of produced water into the North Sea is limited to a monthly average of 40 mg·L-1 3 . Effective remediation of produced water off

58

Improved Measurements of the Ice Water Content in Cirrus Using a Total-Water Probe  

Science Conference Proceedings (OSTI)

This note describes an improved method for the measurement of the ice water content (IWC) of cirrus cloud using a total water content probe. A previous version of this technique assumed that the air in cloud-containing regions was saturated with ...

Philip R. A. Brown; Peter N. Francis

1995-04-01T23:59:59.000Z

59

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

60

Determination of Liquid Water Altitudes Using Combined Remote Sensors  

Science Conference Proceedings (OSTI)

Methods by which attitude ranges of supercooled cloud liquid water in the atmosphere may be estimated are explored using measurements from a combination of ground-based remote sensors. The tests were conducted as part of the Winter Icing and ...

Marcia K. Politovich; B. Boba Stankov; Brooks E. Martner

1995-09-01T23:59:59.000Z

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.


61

Cloud Top Liquid Water from Lidar Observations of Marine Stratocumulus  

Science Conference Proceedings (OSTI)

Maine stratus clouds were simultaneously observed by nadir Nd:YAG lidar measurements and in situ cloud physics measurements. A procedure was applied to derive the two-dimensional vertical cross section of the liquid water from within the cloud ...

J. D. Spinhirne; R. Boers; W. D. Hart

1989-02-01T23:59:59.000Z

62

Microwave measurement of water content in flowing crude oil  

Science Conference Proceedings (OSTI)

A microwave method and a microwave device for measurement of water content in flowing crude oil are proposed. The method is based on measuring power of electromagnetic waves propagated through a transmission line and reflected from the load that is a ...

Yu. V. Makeev; A. P. Lifanov; A. S. Sovlukov

2013-01-01T23:59:59.000Z

63

Process for blending coal with water immiscible liquid  

DOE Patents (OSTI)

A continuous process for blending coal with a water immiscible liquid produces a uniform, pumpable slurry. Pulverized raw feed coal and preferably a coal derived, water immiscible liquid are continuously fed to a blending zone (12 and 18) in which coal particles and liquid are intimately admixed and advanced in substantially plug flow to form a first slurry. The first slurry is withdrawn from the blending zone (12 and 18) and fed to a mixing zone (24) where it is mixed with a hot slurry to form the pumpable slurry. A portion of the pumpable slurry is continuously recycled to the blending zone (12 and 18) for mixing with the feed coal.

Heavin, Leonard J. (Olympia, WA); King, Edward E. (Gig Harbor, WA); Milliron, Dennis L. (Lacey, WA)

1982-10-26T23:59:59.000Z

64

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

65

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

E-Print Network (OSTI)

Water Content Measurements of Wood Chips * P. J. Barale, C.measures the water content of wood chips, pulp and brownwater content measurements in wood chips in a magnetic field

2001-01-01T23:59:59.000Z

66

Comparison of Cloud Liquid Content Measured by Two Independent Ground-Based Systems  

Science Conference Proceedings (OSTI)

We report on observations of liquid water in clouds made by two independent ground-based microwave instruments. One system is a dual-frequency (20.6, 31.65 GHz) microwave radiometer designed to measure emission from the precipitable water vapor ...

J. B. Snider; F. O. Guiraud; D. C. Hogg

1980-05-01T23:59:59.000Z

67

The Putative Liquid-Liquid Transition is a Liquid-Solid Transition in Atomistic Models of Water, Part II  

E-Print Network (OSTI)

This paper extends our earlier studies of free energy functions of density and crystalline order parameters for models of supercooled water, which allows us to examine the possibility of two distinct metastable liquid phases [J. Chem. Phys. 135, 134503 (2011) and arXiv:1107.0337v2]. Low-temperature reversible free energy surfaces of several different atomistic models are computed: mW water, TIP4P/2005 water, SW silicon and ST2 water, the last of these comparing three different treatments of long-ranged forces. In each case, we show that there is one stable or metastable liquid phase, and there is an ice-like crystal phase. The time scales for crystallization in these systems far exceed those of structural relaxation in the supercooled metastable liquid. We show how this wide separation in time scales produces an illusion of a low-temperature liquid-liquid transition. The phenomenon suggesting metastability of two distinct liquid phases is actually coarsening of the ordered ice-like phase, which we elucidate u...

Limmer, David T

2013-01-01T23:59:59.000Z

68

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

69

The Putative Liquid-Liquid Transition is a Liquid-Solid Transition in Atomistic Models of Water, Part II  

E-Print Network (OSTI)

This paper extends our earlier studies of free energy functions of density and crystalline order parameters for models of supercooled water, which allows us to examine the possibility of two distinct metastable liquid phases [J. Chem. Phys. 135, 134503 (2011) and arXiv:1107.0337v2]. Low-temperature reversible free energy surfaces of several different atomistic models are computed: mW water, TIP4P/2005 water, SW silicon and ST2 water, the last of these comparing three different treatments of long-ranged forces. In each case, we show that there is one stable or metastable liquid phase, and there is an ice-like crystal phase. The time scales for crystallization in these systems far exceed those of structural relaxation in the supercooled metastable liquid. We show how this wide separation in time scales produces an illusion of a low-temperature liquid-liquid transition. The phenomenon suggesting metastability of two distinct liquid phases is actually coarsening of the ordered ice-like phase, which we elucidate using both analytical theory and computer simulation. For the latter, we describe robust methods for computing reversible free energy surfaces, and we consider effects of electrostatic boundary conditions. We show that sensible alterations of models and boundary conditions produce no qualitative changes in low-temperature phase behaviors of these systems, only marginal changes in equations of state. On the other hand, we show that altering sampling time scales can produce large and qualitative nonequilibrium effects. Recent reports of evidence of a liquid-liquid critical point in computer simulations of supercooled water are considered in this light.

David T. Limmer; David Chandler

2013-03-13T23:59:59.000Z

70

Bubble statistics and coarsening dynamics for quasi-two dimensional foams with increasing liquid content  

E-Print Network (OSTI)

We report on the statistics of bubble size, topology, and shape and on their role in the coarsening dynamics for foams consisting of bubbles compressed between two parallel plates. The design of the sample cell permits control of the liquid content, through a constant pressure condition set by the height of the foam above a liquid reservoir. We find that in the scaling state, all bubble distributions are independent not only of time but also of liquid content. For coarsening, the average rate decreases with liquid content due to the blocking of gas diffusion by Plateau borders inflated with liquid. By observing the growth rate of individual bubbles, we find that von Neumann's law becomes progressively violated with increasing wetness and with decreasing bubble size. We successfully model this behavior by explicitly incorporating the border blocking effect into the von Neumann argument. Two dimensionless bubble shape parameters naturally arise, one of which is primarily responsible for the violation of von Neumann's law for foams that are not perfectly dry.

A. E. Roth; C. D. Jones; D. J. Durian

2012-06-30T23:59:59.000Z

71

Structure and Depletion at Fluoro- and Hydro-carbon/Water Liquid/Liquid Interfaces  

E-Print Network (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 vapor-like depletion region at hydrophobic/aqueous interfaces. One of the oils, perfluorohexane, is a fluorocarbon whose super-hydrophobic 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 sub-angstrom 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

2008-07-18T23:59:59.000Z

72

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

73

Effect of higher water vapor content on TBC performance  

Science Conference Proceedings (OSTI)

Coal gasification, or IGCC (integrated gasification combined cycle), is one pathway toward cleaner use of coal for power generation with lower emissions. However, when coal-derived synthesis gas (i.e., syngas) is burned in turbines designed for natural gas, turbine manufacturers recommend 'derating,' or lowering the maximum temperature, which lowers the efficiency of the turbine, making electricity from IGCC more expensive. One possible reason for the derating is the higher water vapor contents in the exhaust gas. Water vapor has a detrimental effect on many oxidation-resistant high-temperature materials. In a turbine hot section, Ni-base superalloys are coated with a thermal barrier coating (TBC) allowing the gas temperature to be higher than the superalloy solidus temperature. TBCs have a low thermal conductivity ceramic top coating (typically Y{sub 2}O{sub 3}-stabilized ZrO{sub 2}, or YSZ) and an oxidation-resistant metallic bond coating. For land-based gas turbines, the industry standard is air plasma sprayed (APS) YSZ and high velocity oxygen fuel (HVOF) sprayed NiCoCrAlY bond coatings. To investigate the role of higher water vapor content on TBC performance and possible mitigation strategies, furnace cycling experiments were conducted in dry O{sub 2} and air with 10% (typical with natural gas or jet fuel) or 50 vol% water vapor. Cycle frequency and temperature were accelerated to one hour at 1100 C (with 10 minute cooling to {approx}30 C between each thermal cycle) to induce early failures in coatings that are expected to operate for several years with a metal temperature of {approx}900 C. Coupons (16 mm diameter x 2 mm thick) of commercial second-generation single crystal superalloy CMSX4 were HVOF coated on both sides with {approx}125 {micro}m of Ni-22wt%Co-17Cr-12Al either with 0.7Y or 0.7Y-0.3Hf-0.4Si. One side was then coated with 190-240 {micro}m of APS YSZ. Coatings were cycled until the YSZ top coating spalled. Figure 2 shows the results of the initial phase of experiments. Compared to dry O{sub 2}, the addition of 10% water vapor decreased the lifetime of MCrAlY by {approx}30% for the conventional CMSX4 substrates. Higher average lifetimes were observed with Hf in the bond coating, but a similar decrease in lifetime was observed when water vapor was added. The addition of Y and La to the superalloy substrate did not change the YSZ lifetime with 10% water vapor. However, increasing water vapor content from 10 to 50% did not further decrease the lifetime of either bond coating with the doped superalloy substrate. Thus, these results suggest that higher water vapor contents cannot explain the derating of syngas-fired turbines, and other factors such as sulfur and ash from imperfect syngas cleanup (or upset conditions) need to be explored. Researchers continue to study effects of water vapor on thermally grown alumina scale adhesion and growth rate, and are looking for bond coating compositions more resistant to oxidation in the presence of water vapor.

Pint, Bruce A [ORNL; Haynes, James A [ORNL

2012-01-01T23:59:59.000Z

74

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

75

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

E-Print Network (OSTI)

Molecular dynamics simulations are used to examine the relationship between water-like anomalies and the liquid-liquid critical point in a family of model fluids with multi-Gaussian, core-softened pair interactions. The core-softened pair interactions have two length scales, such that the longer length scale associated with a shallow, attractive well is kept constant while the shorter length scale associated with the repulsive shoulder is varied from an inflexion point to a minimum of progressively increasing depth. As the shoulder well depth increases, the pressure required to form the high density liquid decreases and the temperature up to which the high-density liquid is stable increases, resulting in the shift of the liquid-liquid critical point to much lower pressures and higher temperatures. The pair correlation entropy is computed to show that the excess entropy anomaly diminishes when the shoulder well depth increases. Excess entropy scaling of diffusivity in this class of fluids is demonstrated, showing that decreasing strength of the excess entropy anomaly with increasing shoulder depth results in the progressive loss of water-like thermodynamic, structural and transport anomalies. Instantaneous normal mode analysis was used to index the overall curvature distribution of the fluid and the fraction of imaginary frequency modes was shown to correlate well with the anomalous behaviour of the diffusivity and the pair correlation entropy. The results suggest in the case of core-softened potentials, in addition to the presence of two length scales, energetic and entropic effects associated with local minima and curvatures of the pair interaction play an important role in determining the presence of water-like anomalies and the liquid-liquid phase transition.

Evy Salcedo; Alan B. de Oliveira; Ney M. Barraz Jr; Charusita Chakravarty; Marcia C. Barbosa

2011-03-21T23:59:59.000Z

76

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

77

Liquid-liquid interfaces of semifluorinated alkane diblock copolymers with water, alkanes, and perfluorinated alkanes.  

DOE Green Energy (OSTI)

The liquid-liquid interface between semifluorinated alkane diblock copolymers of the form F3C(CF2)n-1-(CH2)m-1CH3 and water, protonated alkanes, and perfluorinated alkanes are studied by fully atomistic molecular dynamics simulations. A modified version of the OPLS-AA (Optimized Parameter for Liquid Simulation All-Atom) force field of Jorgensen et al. has been used to study the interfacial behavior of semifluorinated diblocks. Aqueous interfaces are found to be sharp, with correspondingly large values of the interfacial tension. Due to the reduced hydrophobicity of the protonated block compared to the fluorinated block, hydrogen enhancement is observed at the interface. Water dipoles in the interfacial region are found to be oriented nearly parallel to the liquid-liquid interface. A number of protonated alkanes and perfluorinated alkanes are found to be mutually miscible with the semifluorinated diblocks. For these liquids, interdiffusion follows the expected Fickian behavior, and concentration-dependent diffusivities are determined.

Perahia, Dvora, Dr. (Clemson University, Clemson, SC); Pierce, Flint (Clemson University, Clemson, SC); Tsige, Mesfin (Southern Illinois University, Carbondale, IL); Grest, Gary Stephen, Dr.

2008-08-01T23:59:59.000Z

78

Performance Evaluation of Advanced LLW Liquid Processing Technology: Boiling Water Reactor Liquid Processing  

Science Conference Proceedings (OSTI)

This report provides condensed information on boiling water reactor (BWR) membrane based liquid radwaste processing systems. The report presents specific details of the technology, including design, configuration, and performance. This information provides nuclear plant personnel with data useful in evaluating the merits of applying advanced processes at their plant.

2001-11-26T23:59:59.000Z

79

In situ separation of root hydraulic redistribution of soil water from liquid and vapor transport  

SciTech Connect

Nocturnal increases in water potential ( ) and water content (WC) in the upper soil profile are often attributed to root water efflux into the soil, a process termed hydraulic lift or hydraulic redistribution (HR). We have previously reported HR values up to ~0.29 mm day-1 in the upper soil for a seasonally dry old-growth ponderosa pine site. However, unsaturated liquid or vapor flux of water between soil layers independent of roots also contributes to the diurnal patterns in WC, confounding efforts to determine the actual magnitude of HR. In this study, we estimated liquid (Jl) and vapor (Jv) soil water fluxes and their impacts on quantifying HR in situ by applying existing data sets of , WC, temperature (T) and soil physical properties to soil water transport equations. Under moist conditions, Jl between layers was estimated to be larger than necessary to account for measured nocturnal increases in WC of upper soil layers. However, as soil drying progressed unsaturated hydraulic conductivity declined rapidly such that Jl was irrelevant (< 2E-06 cm hr-1 at 0-60 cm depths) to total water flux by early August. In surface soil at depths above 15 cm, large T fluctuations can impact Jv leading to uncertainty concerning the role, if any, of HR in nocturnal WC dynamics. Vapor flux was estimated to be the highest at the shallowest depths measured (20 - 30 cm) where it could contribute up to 40% of hourly increases in nocturnal soil moisture depending on thermal conditions. While both HR and net soil water flux between adjacent layers contribute to WC in the 15-65 cm soil layer, HR was the dominant process and accounted for at least 80% of the diurnal increases in WC. While the absolute magnitude of HR is not easily quantified, total diurnal fluctuations in upper soil water content can be quantified and modeled, and remain highly applicable for establishing the magnitude and temporal dynamics of total ecosystem water flux.

Warren, Jeffrey [ORNL; Brooks, J Renee [U.S. Environmental Protection Agency, Corvallis, OR; Dragila, Maria [Oregon State University, Corvallis; Meinzer, Rick [USDA Forest Service

2011-01-01T23:59:59.000Z

80

Comparisons of SSM/I Liquid Water Paths with Aircraft Measurements  

Science Conference Proceedings (OSTI)

Comparisons have been made between in situ aircraft measurements of integrated liquid water and retrievals of integrated liquid water path (LWP) from algorithms using SSM/I brightness temperatures. The aircraft measurements were made over the ...

Stewart G. Cober; Andre Tremblay; George A. Isaac

1996-03-01T23:59:59.000Z

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

Characteristics of Supercooled Liquid Water in Clouds at Mountaintop Sites in the Colorado Rockies  

Science Conference Proceedings (OSTI)

Observations and measurements were made of supercooled liquid water in clouds which enveloped high elevation sites in the Colorado Rocky Mountains for the winters of 1980/81 through 1983/84. The observations showed that liquid water was more ...

Edward E. Hindman

1986-09-01T23:59:59.000Z

82

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

83

Liquid-Water-Droplet Adhesion-Force Measurements on Fresh and...  

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

tilted plate, wettability Abstract Optimal water management in proton-exchange-membrane fuel cells at lower temperatures requires the efficient removal of liquid water from the...

84

Liquid water transport in fuel cell gas diffusion layers Aimy Ming Jii Bazylak  

E-Print Network (OSTI)

Liquid water transport in fuel cell gas diffusion layers by Aimy Ming Jii Bazylak Bachelor means, without the permission of the author. #12;ii Liquid water transport in fuel cell gas diffusion State University) Abstract Liquid water management has a major impact on the performance and durability

Victoria, University of

85

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

Science Conference Proceedings (OSTI)

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

86

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

2007-03-14T23:59:59.000Z

87

Atmospheric Water Content over the Tropical Pacific Derived from the Nimbus-6 Scanning Microwave Spectrometer  

Science Conference Proceedings (OSTI)

The scanning microwave spectrometer (SCAMS) aboard Nimbus-6 contains a 22.23 GHz water vapor channel and 31.65 GHz window channel for deriving integrated water vapor (precipitable water) and cloud liquid water through a column over the oceans. ...

N. C. Grody; A. Gruber; W. C. Shen

1980-08-01T23:59:59.000Z

88

Retrieval of Cloud Water and Water Vapor Contents from Doppler Radar Data in a Tropical Squall Line  

Science Conference Proceedings (OSTI)

This paper describes the retrieval of cloud water and water vapor contents from Doppler radar data. The convective part of a tropical squall line (22 June 1981) observed during the COPT 81 (Convection Profonde Tropicale 1981) West African ...

Daničle Hauser; Paul Amayenc

1986-04-01T23:59:59.000Z

89

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

90

Determination of 3-D Cloud Ice Water Contents by Combining Multiple...  

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

Determination of 3-D Cloud Ice Water Contents by Combining Multiple Data Sources from Satellite, Ground Radar, and a Numerical Model Liu, Guosheng Florida State University Seo,...

91

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

E-Print Network (OSTI)

in comparison with gas-phase water, ice close to the meltingcrystalline ice at two different temperatures, and gas-phaseof gas-phase water, liquid water and crystalline ice using

Nordlund, Dennis

2008-01-01T23:59:59.000Z

92

Contents  

Science Conference Proceedings (OSTI)

... gen; radiation correction; thermal con- with measurements on liquid toluene as ductivity; thermal diffusivity; toluene; well as argon and nitrogen gas. ...

2003-10-07T23:59:59.000Z

93

Bond orientational ordering in liquids: Towards a unified description of water-like anomalies, liquid-liquid transition, glass transition, and crystallization  

E-Print Network (OSTI)

There are at least three fundamental states of matter, depending upon temperature and pressure: gas, liquid, and solid (crystal). These states are separated by first-order phase transitions between them. In both gas and liquid phases the complete translational and rotational symmetry exist, whereas in a solid phase both symmetries are broken. In intermediate phases between liquid and solid, which include liquid crystal and plastic crystal phases, only one of the two symmetries is preserved. Among the fundamental states of matter, the liquid state is most poorly understood. We argue that it is crucial for a better understanding of liquid to recognize that a liquid generally has a tendency to have local structural order and its presence is intrinsic and universal to any liquid. Such structural ordering is a consequence of many body correlations, more specifically, bond angle correlations, which we believe are crucial for the description of the liquid state. We show that this physical picture may naturally explain difficult unsolved problems associated with the liquid state, such as anomalies of water-type liquids (water, Si, Ge, ...), liquid-liquid transition, liquid-glass transition, crystallization and quasicrystal formation, in a unified manner. In other words, we need a new order parameter representing low local free-energy configuration, which is bond orientational order parameter in many cases, in addition to density order parameter for the physical description of these phenomena. Here we review our two-order-parameter model of liquid and consider how transient local structural ordering is linked to all of the above-mentioned phenomena. The relationship between these phenomena are also discussed.

Hajime Tanaka

2013-07-02T23:59:59.000Z

94

Simulations of the Effects of Water Vapor, Cloud Liquid Water, and Ice on AMSU Moisture Channel Brightness Temperatures  

Science Conference Proceedings (OSTI)

Radiative transfer simulations are performed to determine how water vapor and nonprecipitating cloud liquid water and ice particles within typical midlatitude atmospheres affect brightness temperatures TB's of moisture sounding channels used in ...

Bradley M. Muller; Henry E. Fuelberg; Xuwu Xiang

1994-10-01T23:59:59.000Z

95

Estimating the Atmospheric Water Vapor Content from Sun Photometer Measurements  

Science Conference Proceedings (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

96

Measurements of the Ice Water Content in Cirrus Using an Evaporative Technique  

Science Conference Proceedings (OSTI)

A technique for the measurement of the ice water content (IWC) of cirrus clouds is described. The IWC is obtained by the measurement of the total water content (TWC) and the subtraction of the saturation specific humidity with respect to ice at ...

Philip R. A. Brown

1993-08-01T23:59:59.000Z

97

Contents  

Science Conference Proceedings (OSTI)

Page 1. Volume 97, Number 5, September-October 1992 Journal of Research of the National Institute of Standards and Technology Contents ...

2003-10-15T23:59:59.000Z

98

Contents  

Science Conference Proceedings (OSTI)

Page 1. Volume 96, Number 2, March-April 1991 Journal of Research of the National Institute of Standards and Technology Contents Articles ...

2003-10-06T23:59:59.000Z

99

Contents  

Science Conference Proceedings (OSTI)

Page 1. Volume 96, Number 6, November-December 1991 Journal of Research of the National Institute of Standards and Technology Contents ...

2003-10-10T23:59:59.000Z

100

Contents  

Science Conference Proceedings (OSTI)

Page 1. Volume 98, Number 6, November-December 1993 Journal of Research of the National Institute of Standards and Technology Contents ...

2003-10-21T23:59:59.000Z

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

Contents  

Science Conference Proceedings (OSTI)

Page 1. Volume 96, Number 4, July-August 1991 Journal of Research of the National Institute of Standards and Technology Contents Articles ...

2003-10-08T23:59:59.000Z

102

CONTENTS  

Science Conference Proceedings (OSTI)

Page 1. JOURNAL OF RESEARCH of the National Bureau of Standards Vol. 88, No. 6, November-December 1983 CONTENTS Page ...

2003-07-03T23:59:59.000Z

103

Contents  

Science Conference Proceedings (OSTI)

Page 1. Volume 97, Number 6, November-December 1992 Journal of Research of the National Institute of Standards and Technology Contents ...

2003-10-15T23:59:59.000Z

104

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

105

Electrokinetic Hydrogen Generation from Liquid WaterMicrojets  

SciTech Connect

We describe a method for generating molecular hydrogen directly from the charge separation effected via rapid flow of liquid water through a metal orifice, wherein the input energy is the hydrostatic pressure times the volume flow rate. Both electrokinetic currents and hydrogen production rates are shown to follow simple equations derived from the overlap of the fluid velocity gradient and the anisotropic charge distribution resulting from selective adsorption of hydroxide ions to the nozzle surface. Pressure-driven fluid flow shears away the charge balancing hydronium ions from the diffuse double layer and carries them out of the aperture. Downstream neutralization of the excess protons at a grounded target electrode produces gaseous hydrogen molecules. The hydrogen production efficiency is currently very low (ca. 10-6) for a single cylindrical jet, but can be improved with design changes.

Duffin, Andrew M.; Saykally, Richard J.

2007-05-31T23:59:59.000Z

106

Influence of gravity on the collective molecular dynamics of liquid water: the case of the floating water bridge  

E-Print Network (OSTI)

Quantum electrodynamics (QED) produces a picture of liquid water as a mixture of a low density coherent phase and an high density non-coherent phase. Consequently, the Archimedes principle prescribes that, within a gravitational field, liquid water should be made up, at surface, mainly of the coherent fraction, which becomes a cage where the gas-like non-coherent fraction is trapped, acquiring a non-vanishing pressure (vapor tension). Therefore, it is possible to probe the QED picture by observing the behavior of liquid water under reduced gravity conditions. The floating water bridge could be a useful test model.

Emilio Del Giudice; Giuseppe Vitiello

2010-09-29T23:59:59.000Z

107

Thermal signature reduction through liquid nitrogen and water injection  

E-Print Network (OSTI)

The protection of aircraft against shoulder fired heat seeking missiles is of growing concern in the aviation community. This thesis presents a simple method for shielding the infrared signature of a jet engine from heat seeking missiles. The research efforts investigated two approaches to shield the thermal signature of the Noel Penny Type 401 turbojet at the Texas A&M University Propulsion Lab Test Cell. First, liquid nitrogen was injected through a manifold at a flow rate equivalent to the flow rate of exhaust gases, producing a small temperature reduction in the exhaust but no infrared shielding. Second, water was injected at a flow rate of 13% of the flow of exhaust gases, producing a greater temperature reduction and some shielding. Water was then injected through a manifold at a ?ow rate of 118% of the flow rate of exhaust gases, producing a substantial reduction in temperature and complete shielding of the infrared signature. Additionally, numerical simulations were performed using FLUENT to support these experiments. Results are presented in the form of thermocouple data and thermal images from the experiments, and in the form of temperature contours and streamtraces from the simulations.

Guarnieri, Jason Antonio

2004-12-01T23:59:59.000Z

108

Column Water Vapor Content in Clear and Cloudy Skies  

Science Conference Proceedings (OSTI)

With radiosonde data from 15 Northern Hemisphere stations, surface-to-400-mb column water vapor is computed from daytime soundings for 1988–1990. On the basis of simultaneous surface visual cloud observations, the data are categorized according ...

Dian J. Gaffen; William P. Elliott

1993-12-01T23:59:59.000Z

109

Measurements of the Total Water Content of Cirrus Clouds. Part I: Instrument Details and Calibration  

Science Conference Proceedings (OSTI)

This paper describes an instrument designed to measure the sum of gas phase and solid phase water, or total water, in cirrus clouds, and to be mounted in a pallet in the underbelly of the NASA WB-57 research aircraft. The ice water content of ...

E. M. Weinstock; J. B. Smith; D. Sayres; J. R. Spackman; J. V. Pittman; N. Allen; J. Demusz; M. Greenberg; M. Rivero; L. Solomon; J. G. Anderson

2006-11-01T23:59:59.000Z

110

A New Fast Response Instrument for Measuring Total Water Content from Aircraft  

Science Conference Proceedings (OSTI)

A device for measuring the total water content of a parcel of air from an aircraft has been developed. The total water of a parcel of air is a conserved quantity, independent of phase changes, provided there is no transport of water through the ...

S. Nicholls; J. Leighton; R. Barker

1990-10-01T23:59:59.000Z

111

Contents  

Science Conference Proceedings (OSTI)

... initially to meet the O&M needs of wastewater and water treatment systems designed ... OMI has a unique, high-energy team culture, developed ...

2001-05-01T23:59:59.000Z

112

Alpha and gamma radiation effects on air-water systems at high gas/liquid ratios  

SciTech Connect

Radiolysis tests were conducted on air-water systems to examine the effects of radiation on liquid phase chemistry under high gas/liquid volume (G/L) ratios that are characteristic of an unsaturated nuclear waste repository setting. Test parameters included temperatures of 25, 90, and 200{degrees}C; gamma vs. alpha radiation; dose rates of {approximately}3500 and 50,000 rad/h; and G/L ratios of 10 and 100. Formate, oxalate, and total organic carbon contents increased during irradiation of the air-water systems in gamma and alpha tests at low-dose rate ({approximately}3500 rad/h). Increases in organic components were not observed for tests run at 200{degrees}C or high-dose rates (50,000 rad/h). In the tests where increases in organics occurred, the formate and oxalate were preferentially enriched in solutions that were rinsed from the test vessel walls. Nitrate (NO{sub 3}{sup {minus}}) is the dominant anion produced during the radiolysis reactions. Significant nitrite (NO{sub 2}{sup {minus}}) also occurs in some high-dose rate tests, with the reduced form of nitrogen possibly resulting from reactions with the test vessels. These results indicate that nitrogen acids are being produced and concentrated in the limited quantities of solution present in the tests. Nitrate + nitrite production varied inversely with temperature, with the lowest quantities being detected for the higher temperature tests. The G(NO{sub 3}{sup {minus}} + NO{sub 2}{sup {minus}}) values for the 25, 90, and 200{degrees}C experiments with gamma radiation are 3.2 {+-} 0.7, 1.3 {+-} 1.0, and 0.4 {+-} 0.3, respectively. Thus, the elevated temperatures expected early in the life of a repository may counteract pH decreases resulting from nitrogen acid production. Little variation was observed in G values as a function of dose rate or gas/liquid ratio.

Wronkiewicz, D.J.; Bates, J.K.

1993-08-01T23:59:59.000Z

113

Elucidating through-plane liquid water profile in a polymer electrolyte membrane fuel cell.  

DOE Green Energy (OSTI)

In this paper, a numerical model incorporating micro-porous layers (MPLs) is presented for simulating water transport within the gas diffusion layers (GDLs) and MPLs as well as across their interfaces in a polymer electrolyte membrane (PEM) fuel cell. One-dimensional analysis is conducted to investigate the impacts of MPL and GDL properties on the liquid-water profile across the anode GDL-MPL and cathode MPL-GDL regions. Furthermore, two-dimensional numerical simulations that take MPLs into account are also carried out to elucidate liquid water transport, particularly through-plane liquid-water profile in a PEM fuel cell. Results from case studies are presented.

Wang, Yun (University of California, Irvine, CA); Chen, Ken Shuang

2010-10-01T23:59:59.000Z

114

Estimating Soil Water Contents from Soil Temperature Measurements by Using an Adaptive Kalman Filter  

Science Conference Proceedings (OSTI)

A simple soil heat transfer model is used together with an adaptive Kalman filter to estimate the daily averaged soil volumetric water contents from diurnal variations of the soil temperatures measured at different depths. In this method, the ...

Shu-Wen Zhang; Chong-Jian Qiu; Qin Xu

2004-02-01T23:59:59.000Z

115

Radar Reflectivity-Ice Water Content Relationships for Use above the Melting Level in Hurricanes  

Science Conference Proceedings (OSTI)

Regression equations linking radar reflectivity (Ze) and ice water content (IWC) were calculated from airborne radar and particle image data that were collected above the melting level in two hurricanes. The Ze ? IWC equation from the stratiform ...

Robert A. Black

1990-09-01T23:59:59.000Z

116

A Scheme for Parameterizing Ice-Cloud Water Content in General Circulation Models  

Science Conference Proceedings (OSTI)

The optical properties of ice clouds are a primary issue for climate and climate change. Evaluating these optical properties in three-dimensional models for studying climate will require a method to calculate the ice water content of such clouds. ...

Andrew J. Heymsfield; Leo J. Donner

1990-08-01T23:59:59.000Z

117

Diurnal Water Content Changes in the Bare Soil of a Coastal Desert  

Science Conference Proceedings (OSTI)

The deposition of dew is a common meteorological phenomenon that has been recognized as an important ecosystem element, especially in arid areas. There is some evidence that indicates that there is an increase in the water content of the topsoil ...

Nurit Agam (Ninari)P. R. Berliner

2004-10-01T23:59:59.000Z

118

A Technique for Deriving Column-integrated Water Content Using VAS Split-Window Data  

Science Conference Proceedings (OSTI)

An algorithm is examined that uses Visible?Infrared Spin Scan Radiometer (VISSR) Atmospheric Sounder (VAS) 11- and 12-µm (split-window) data to derive column-integrated water content (IWC) at mesoscale resolution. The algorithm is physically ...

Anthony R. Guillory; Gary J. Jedlovec; Henry E. Fuelberg

1993-07-01T23:59:59.000Z

119

Initialization of Soil-Water Content in Regional-Scale Atmospheric Prediction Models  

Science Conference Proceedings (OSTI)

The purpose of this study is to demonstrate the feasibility of determining the soil-water content fields required as initial conditions for land surface components within atmospheric prediction models. This is done using a model of the hydrologic ...

Christopher B. Smith; Mercedes N. Lakhtakia; William J. Capehart; Toby N. Carlson

1994-04-01T23:59:59.000Z

120

Cirrus Cloud Ice Water Content Radar Algorithm Evaluation Using an Explicit Cloud Microphysical Model  

Science Conference Proceedings (OSTI)

A series of cirrus cloud simulations performed using a model with explicit cloud microphysics is applied to testing ice water content retrieval algorithms based on millimeter-wave radar reflectivity measurements. The simulated ice particle size ...

Kenneth Sassen; Zhien Wang; Vitaly I. Khvorostyanov; Graeme L. Stephens; Angela Bennedetti

2002-06-01T23:59:59.000Z

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

Comments on “Estimating Soil Water Contents from Soil Temperature Measurements by Using an Adaptive Kalman Filter”  

Science Conference Proceedings (OSTI)

A scheme was proposed by Zhang et al. to estimate soil water content from soil temperature measurements by using an adaptive Kalman filter. Their scheme is based on the fact that soil heat capacity and thermal conductivity are a monotonic ...

Kun Yang; Toshio Koike

2005-04-01T23:59:59.000Z

122

Gas processing/The boiling behavior of LPG and liquid ethane, ethylene, propane, and n-butane spilled on water  

SciTech Connect

Boiling-rate calorimeter studies showed that unlike liquid nitrogen, methane, and LNG, LPG (84.7% propane, 6.0% ethane, and 9.3% n-butane; 442/sup 0/C bp), or pure propane, when rapidly spilled on water, reacted violently, ejecting water and ice into the vapor space; but in 1-2 sec, a coherent ice layer was formed and further boiloff was quiet and well predicted by a simple one-dimensional, moving-boundary-value, heat transfer model with a growing ice shield. Increasing the content of ethane and butane in LPG to 20% and 10%, respectively, had almost no effect on the LPG boiling, indicating that boiling may be modeled by using pure propane. Ethane, ethylene, and n-butane behaved quite differently from LPG. In spills of pure liquid propane on solid ice, the boiloff rate was almost identical to that predicted by the moving-boundary model.

Reid, R.C.; Smith, K.A.

1978-04-01T23:59:59.000Z

123

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

Science Conference Proceedings (OSTI)

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

124

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

125

The Use of lce-Liquid Water Potential Temperature as a Thermodynamic Variable In Deep Atmospheric Models  

Science Conference Proceedings (OSTI)

Previous studies have shown liquid water potential temperature to be an inappropriate choice for a thermodynamic variable in a deep cumulus convection model. In this study, an alternate form of this variable called ice-liquid water potential ...

Gregory J. Tripoli; William R. Cotton

1981-05-01T23:59:59.000Z

126

CONTENTS  

E-Print Network (OSTI)

February 2010This document is in the public domain and may be freely copied or reprinted. Disclaimer Mention of any company or product does not constitute endorsement by the National Institute for Occupational Safety and Health (NIOSH). In addition, citations to Web sites external to NIOSH do not constitute NIOSH endorsement of the sponsoring organizations or their programs or products. Furthermore, NIOSH is not responsible for the content of these Web sites. Ordering Information To receive documents or other information about occupational safety and health topics, contact NIOSH at

A. Breslin, Ph.D.

2010-01-01T23:59:59.000Z

127

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 of liquid water using electron pulses produced by a table-top terawatt laser system (T3 ). The results

Umstadter, Donald

128

Sound speed in liquid–gas mixtures: Water–air and water  

E-Print Network (OSTI)

The sound speed of a two-phase fluid, such as a magma-gas, water-air, or water-steam mixture, is dramatically different from the sound speed of either pure component. In numerous geologic situations the sound speed of such two-phase systems may be of interest: in the search for magma reservoirs, in seismic exploration of geothermal areas, in prediction of P wave velocity decreases prior to earthquakes, and in inversion of crustal and upper mantle seismic records. Probably most dramatically, fluid flow characteristics during eruptions of volcanoes and geysers are strongly dependent on the sound speed of erupting two-phase (or multiphase) fluids. In this paper the sound speeds of water, air, steam, water-air mixtures, and water-steam mixtures are calculated. It is demonstrated that sound speeds calculated from classical acoustic and fluid dynamics analyses agree with results obtained from finite amplitude 'vaporization wave ' theory. To the extent that air and steam are represented as perfect gases with an adiabatic exponent •, independent of temperature, their sound speeds vary in a simple manner directly with the square root of the absolute temperature. The sound speed of pure liquid water is a complex function of pressure and temperature and is given here to 8 kbar, 900řC. In pure water at all pressures the sound speed attains a maximum value near 100řC and decreases at higher temperatures; at high pressures the decrease is continuous, but at pressures below 1 kbar the sound speed reaches a minimum value in the

Susan Werner Kieffer

1977-01-01T23:59:59.000Z

129

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.

130

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.

131

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.

132

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.

133

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.

134

Relating x-ray attenuation measurements to water content and distribution in SB-15D core  

DOE Green Energy (OSTI)

Making improved estimates of the water content of The Geysers reservoir is fundamental to efficient and economic long term production of steam power from the resource. A series of coordinated physical properties measurements form core recovered from the SB-15D, reported in this volume in a series of papers, have been made to better understand water storage and to relate water content and distribution to observable geophysical properties such as electrical conductivity and seismic velocities. A principal objective here is to report new interpretations of x-ray scans made within 72 hours of core recovery from SB-15D, which suggest, taking advantage of preliminary measurements of capillary suction for metagraywacke, that water content was low in much of the preserved core.

Bonner, B.P.; Roberts, J.J.; Schneberk, D.J

1996-09-30T23:59:59.000Z

135

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

E-Print Network (OSTI)

Non-destructive methods of measuring water content in soils have been extensively developed in the last decades, especially in soil science. Among 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 resistivity probe was developed to monitor the change in local water content in the triaxial apparatus. The probe is composed of two-pair of electrodes, and an electrical current is induced through the soil at the vicinity of the contact between the probe and the specimen. Some experimental data on the changes in resistivity with the degree of saturation were obtained in specimens of a natural unsaturated loess from Northern France. Two theoretical models of resistivity were also used to analyze the obtained data. Results are finally discussed with respect to the loess's water retention properties.

Munoz-Castelblanco, José; Delage, Pierre; Cui, Yu Jun

2013-01-01T23:59:59.000Z

136

CONTENTS  

E-Print Network (OSTI)

This report was prepared by Sargent & Lundy, L.L.C., hereinafter referred to as S&L, expressly for Perrin Quarles Associates, Inc., hereinafter referred to as PQA, under EPA Contract No. EP-W-07-064. Neither S&L nor any person acting on its behalf (a) makes any warranty, express or implied, with respect to the use of any information or methods disclosed in this report or (b) assumes any liability with respect to the use of any information or methods disclosed in this report. Although prepared with EPA funding and reviewed by the EPA, this report has not been approved by the EPA for publication as an EPA report. The contents do not necessarily reflect the views or policies of the EPA, nor does mention of trade names or commercial products constitute endorsement or recommendation for use. COAL-FIRED POWER PLANT HEAT RATE REDUCTIONS i

unknown authors

2009-01-01T23:59:59.000Z

137

Molecular mode-coupling theory for supercooled liquids: Application to water L. Fabbian,1  

E-Print Network (OSTI)

Molecular mode-coupling theory for supercooled liquids: Application to water L. Fabbian,1 A. Latz,2 observed in supercooled molecular liquids close to the glass transition. The mode-coupling theory MCT, rigid molecules. We compare the predictions of the theory for the q-vector dependence of the molecular

Sciortino, Francesco

138

The Role of Eddy Diffusivity Profiles on Stratocumulus Liquid Water Path Biases  

Science Conference Proceedings (OSTI)

Results from simulations of the stratocumulus-topped boundary layer with one-dimensional versions of general simulation models typically exhibit a wide range of spread in the modeled liquid water path (LWP). These discrepancies are often ...

Stephan R. de Roode

2007-07-01T23:59:59.000Z

139

Multiple Remote Sensor Observations of Supercooled Liquid Water in a Winter Storm at Beaver, Utah  

Science Conference Proceedings (OSTI)

The temporal and spatial distribution of cloud liquid water in a winter storm from the 1983 Utah/NOAA Cooperative Weather Modification Program is characterized using remote sensing observations. The remote sensors, located at a mountain-base site ...

Kenneth Sassen; Robert M. Rauber; J. B. Snider

1986-06-01T23:59:59.000Z

140

Radiometric Observations of Supercooled Liquid Water within a Split Front over the Sierra Nevada  

Science Conference Proceedings (OSTI)

A storm bearing close structural resemblance to a katafront was observed from the ground with microwave radiometry and a vertically pointing Ka-band radar over the Sierra Nevada of California. The onset and duration of supercooled liquid water ...

Mark F. Heggli; David W. Reynolds

1985-11-01T23:59:59.000Z

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

A Comparison of Several Radiometric Methods of Deducing Path-Integrated Cloud Liquid Water  

Science Conference Proceedings (OSTI)

Using radiometer data collected during the Canadian Atlantic Storms Program, we have investigated five different methods of estimating the path-integrated, or columnar, cloud liquid water. The methods consist of one- and two-channel physical ...

Chong Wei; H. G. Leighton; R. R. Rogers

1989-12-01T23:59:59.000Z

142

Doppler Cloud Radar Derived Drop Size Distributions in Liquid Water Stratus Clouds  

Science Conference Proceedings (OSTI)

A cloud particle size retrieval algorithm that uses radar reflectivity factor and Doppler velocity obtained by a 35-GHz Doppler radar and liquid water path estimated from microwave radiometer radiance measurements is developed to infer the size ...

Seiji Kato; Gerald G. Mace; Eugene E. Clothiaux; James C. Liljegren; Richard T. Austin

2001-10-01T23:59:59.000Z

143

Turbulence, Condensation, and Liquid Water Transport in Numerically Simulated Nonprecipitating Stratocumulus Clouds  

Science Conference Proceedings (OSTI)

Condensation and turbulent liquid water transport in stratocumulus clouds involve complicated interactions between turbulence dynamics and cloud microphysical processes, and play essential roles in defining the cloud structure. This work aims at ...

Shouping Wang; Qing Wang; Graham Feingold

2003-01-01T23:59:59.000Z

144

Comparison of Simultaneous Airborne and Radiometric Measurements of Supercooled Liquid Water  

Science Conference Proceedings (OSTI)

Simultaneous measurements of supercooled liquid water by an instrumented aircraft and a dual-frequency microwave radiometer were made at Lake Ontario, New York, during wintertime. The geographic location and typical meteorological conditions for ...

Geoffrey E. Hill

1991-07-01T23:59:59.000Z

145

Further Comparisons of Simultaneous Airborne and Radiometric Measurements of Supercooled Liquid Water  

Science Conference Proceedings (OSTI)

Simultaneous measurements of supercooled liquid water were made by an instrumented aircraft and a microwave radiometer at Muskegon, Michigan during wintertime. The purpose was to confirm recent findings that there is good agreement between the ...

Geoffrey E. Hill

1992-04-01T23:59:59.000Z

146

Analysis of Supercooled Liquid Water Measurements Using Microwave Radiometer and Vibrating Wire Devices  

Science Conference Proceedings (OSTI)

A review is made of the theoretical basis for using a vibrating wire to measure supercooled liquid water in clouds. The device consists of a vibrating wire and associated electronics added to radiosondes. The sensing wire that collects ...

Geoffrey E. Hill

1994-10-01T23:59:59.000Z

147

Spatial Variability of Liquid Water Path in Marine Low Cloud: The Importance of Mesoscale Cellular Convection  

Science Conference Proceedings (OSTI)

Liquid water path (LWP) mesoscale spatial variability in marine low cloud over the eastern subtropical oceans is examined using two months of daytime retrievals from the Moderate Resolution Imaging Spectroradiometer (MODIS) on the NASA Terra ...

Robert Wood; Dennis L. Hartmann

2006-05-01T23:59:59.000Z

148

Evaluation of Liquid Water Measuring Instruments in Cold Clouds Sampled during FIRE  

Science Conference Proceedings (OSTI)

Liquid water measurements from the Rosemount icing detector (RICE), Particle Measuring Systems (PMS) forward scattering spectrometer probe (FSSP), and Johnson–williams and King hot-wire probes used on the NCAR King Air aircraft are evaluated for ...

Andrew J. Heymsfield; Larry M. Miloshevich

1989-06-01T23:59:59.000Z

149

Entrainment Rate, Cloud Fraction, and Liquid Water Path of PBL Stratocumulus Clouds  

Science Conference Proceedings (OSTI)

The large eddy simulation technique is used to search for key factors in determining the entrainment rate, cloud fraction, and liquid water path in the stratocumulus-topped boundary layer (STBL), with the goal of developing simple schemes of ...

Chin-Hoh Moeng

2000-11-01T23:59:59.000Z

150

Process for hydrogen isotope concentration between liquid water and hydrogen gas  

DOE Patents (OSTI)

A process for hydrogen isotope exchange and concentration between liquid water and hydrogen gas, wherein liquid water and hydrogen gas are contacted, in an exchange section, with one another and with at least one catalyst body comprising at least one metal selected from Group VIII of the Periodic Table and preferably a support therefor, the catalyst body has a liquid-water-repellent, gas permeable polymer or organic resin coating, preferably a fluorinated olefin polymer or silicone coating, so that the isotope concentration takes place by two simultaneously occurring steps, namely, ##EQU1## WHILE THE HYDROGEN GAS FED TO THE EXCHANGE SECTION IS DERIVED IN A REACTOR VESSEL FROM LIQUID WATER THAT HAS PASSED THROUGH THE EXCHANGE SECTION.

Stevens, William H. (Deep River, CA)

1976-09-21T23:59:59.000Z

151

Liquid Water Cloud Measurements Using the Raman Lidar Technique: Current Understanding and Future Research Needs  

Science Conference Proceedings (OSTI)

This paper describes recent work in the Raman lidar liquid water cloud measurement technique. The range-resolved spectral measurements at the National Aeronautics and Space Administration Goddard Space Flight Center indicate that the Raman ...

Tetsu Sakai; David N. Whiteman; Felicita Russo; David D. Turner; Igor Veselovskii; S. Harvey Melfi; Tomohiro Nagai; Yuzo Mano

2013-07-01T23:59:59.000Z

152

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

153

Polymer formulation for removing hydrogen and liquid water from an enclosed space  

DOE Patents (OSTI)

This invention describes a solution to the particular problem of liquid water formation in hydrogen getters exposed to quantities of oxygen. Water formation is usually desired because the recombination reaction removes hydrogen without affecting gettering capacity and the oxygen removal reduces the chances for a hydrogen explosion once free oxygen is essentially removed. The present invention describes a getter incorporating a polyacrylate compound that can absorb up to 500% of its own weight in liquid water without significantly affecting its hydrogen gettering/recombination properties, but that also is insensitive to water vapor.

Shepodd, Timothy J. (Livermore, CA)

2006-02-21T23:59:59.000Z

154

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

E-Print Network (OSTI)

and solid phases of water, including an accurate universal force field. The quest to achieve an accurate of the surfaces of either ice or liquid water (3), nor do we understand the origin of the intriguing anomalies difficult to accurately parameterize these interactions from ab initio calcu- lations. Moreover, the ab

Cohen, Ronald C.

155

Evaluating Soil Water Content in a WRF-NOAH Downscaling Experiment  

Science Conference Proceedings (OSTI)

Soil water content (SWC) depends on and impacts the energy flux partitioning at the land atmosphere interface. Above all, the latent heat flux is limited by SWC of the root zone on the one hand side and radiation on the other hand side. Therefore ...

Peter Greve; Kirsten Warrach-Sagi; Volker Wulfmeyer

156

Improved Airborne Hot-Wire Measurements of Ice Water Content in Clouds  

Science Conference Proceedings (OSTI)

Airborne measurements of ice water content (IWC) in both ice and mixed phase clouds remain one of the long standing problems in experimental cloud physics. For nearly three decades, IWC has been measured with the help of the Nevzorov hot-wire ...

A. Korolev; J. W. Strapp; G. A. Isaac; E. Emery

157

A Thermal Device for Aircraft Measurement of the Solid Water Content of Clouds  

Science Conference Proceedings (OSTI)

A constant temperature probe for the measurement of solid water content of clouds is described. The probe is operated at a temperature of approximately 25°C, and is designed to collect and melt ice particles that impact in an open half-cylinder, ...

W. D. King; D. E. Turvey

1986-09-01T23:59:59.000Z

158

Results of Sun Photometer–Derived Precipitable Water Content over a Tropical Indian Station  

Science Conference Proceedings (OSTI)

A compact, hand-held multiband sun photometer (ozone monitor) has been used to measure total precipitable water content (PWC) at the low-latitude tropical station in Pune, India (18°32?N, 73°51?E). Data collected in the daytime (0730–1800 LT) ...

P. Ernest Raj; P. C. S. Devara; R. S. Maheskumar; G. Pandithurai; K. K. Dani; S. K. Saha; S. M. Sonbawne; Y. K. Tiwari

2004-10-01T23:59:59.000Z

159

A Steerable Dual-Channel Microwave Radiometer for Measurement of Water Vapor and Liquid in the Troposphere  

Science Conference Proceedings (OSTI)

An instrument that remotely senses the integrated amounts of water vapor and liquid on a path through the atmosphere is discussed. The vapor and liquid are measured simultaneously but independently by microwave radiometers. Comparison of the ...

D. C. Hogg; F. O. Guiraud; J. B. Snider; M. T. Decker; E. R. Westwater

1983-05-01T23:59:59.000Z

160

On-sample water content measurement for a complete local monitoring in triaxial testing of unsaturated soils  

E-Print Network (OSTI)

To provide a complete local monitoring of the state of an unsaturated soil sample during triaxial testing, a local water content measurement device was adapted to a triaxial device comprising the measurement of local displacements (Hall effect transducers) and suction (High capacity transducer). Water content was locally monitored by means of a resistivity probe. The water content/resistivity calibration curves of an intact natural unsaturated loess from Northern France extracted by block sampling at two depths (1 and 3.3 m) were carefully determined, showing good accuracy and repeatability. The validity of two models giving the resistivity of unsaturated soils with respect to their water content was examined.

Munoz-Castelblanco, José; Pereira, Jean-Michel; Cui, Yu-Jun

2013-01-01T23:59:59.000Z

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.


161

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

162

Prepulse effect on laser-induced water-window radiation from a liquid nitrogen jet  

E-Print Network (OSTI)

is schematically shown in Fig. 1. A high-purity nitrogen gas was cooled and liquefied through the cooling stagesPrepulse effect on laser-induced water-window radiation from a liquid nitrogen jet J. Son,a M. Cho.3­4.4 nm x ray from a liquid nitrogen jet. It is observed that a prepulse of only 2 mJ enhances

Kim, Jae-Hoon

163

Coupling atomistic and continuum hydrodynamics through a mesoscopic model: application to liquid water  

E-Print Network (OSTI)

We have conducted a triple-scale simulation of liquid water by concurrently coupling atomistic, mesoscopic, and continuum models of the liquid. The presented triple-scale hydrodynamic solver for molecular liquids enables the insertion of large molecules into the atomistic domain through a mesoscopic region. We show that the triple-scale scheme is robust against the details of the mesoscopic model owing to the conservation of linear momentum by the adaptive resolution forces. Our multiscale approach is designed for molecular simulations of open domains with relatively large molecules, either in the grand canonical ensemble or under non-equilibrium conditions.

Rafael Delgado-Buscalioni; Kurt Kremer; Matej Praprotnik

2009-08-04T23:59:59.000Z

164

Revisiting the total ion yield x-ray absorption spectra of liquid water microjets  

SciTech Connect

Measurements of the total ion yield (TIY) x-ray absorption spectrum (XAS) of liquid water by Wilson et al. (2002 J. Phys.: Condens. Matter 14 L221 and 2001 J. Phys. Chem. B 105 3346) have been revisited in light of new experimental and theoretical efforts by our group. Previously, the TIY spectrum was interpreted as a distinct measure of the electronic structure of the liquid water surface. However, our new results indicate that the previously obtained spectrum may have suffered from as yet unidentified experimental artifacts. Although computational results indicate that the liquid water surface should exhibit a TIY-XAS that is fundamentally distinguishable from the bulk liquid XAS, the new experimental results suggest that the observable TIY-XAS is actually nearly identical in appearance to the total electron yield (TEY-)XAS, which is a bulk probe. This surprising similarity between the observed TIY-XAS and TEY-XAS likely results from large contributions from x-ray induced electron stimulated desorption of ions, and does not necessarily indicate that the electronic structure of the bulk liquid and liquid surface are identical.

Saykally, Richard J; Cappa, Chris D.; Smith, Jared D.; Wilson, Kevin R.; Saykally, Richard J.

2008-02-16T23:59:59.000Z

165

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

166

Modeling and High-Resolution-Imaging Studies of Water-Content Profiles in a Polymer-Electrolyte-Fuel-Cell Membrane-Electrode Assembly  

E-Print Network (OSTI)

is much lower and water is produced at the cathode. However,transport. Liquid water is produced at the catalyst layer

Weber, A.Z.

2008-01-01T23:59:59.000Z

167

Information Content and Uncertainties in Thermodynamic Profiles and Liquid Cloud Properties Retrieved from the Ground-Based Atmospheric Emitted Radiance Interferometer (AERI)  

Science Conference Proceedings (OSTI)

The Atmospheric Emitted Radiance Interferometer (AERI) observes spectrally resolved downwelling radiance emitted by the atmosphere in the infrared portion of the electromagnetic spectrum. Profiles of temperature and water vapor, and cloud liquid ...

D.D. Turner; U. Löhnert

168

Non-invasive Field Measurements of Soil Water Content Using a Pulsed 14 MeV Neutron Generator  

DOE Green Energy (OSTI)

Current techniques of soil water content measurement are invasive and labor-intensive. Here, we demonstrate that an in situ soil carbon (C) analyzer with a multi-elemental analysis capability, developed for studies of terrestrial C sequestration, can be used concurrently to non-invasively measure the water content of large-volume ({approx}0.3 m{sup 3}) soil samples. Our objectives were to investigate the correlations of the hydrogen (H) and oxygen (O) signals with water to the changes in the soil water content in laboratory experiments, and in an agricultural field. Implementing prompt gamma neutron activation analyses we showed that in the field, the signal from the H nucleus better indicates the soil water content than does that from the O nucleus. Using a field calibration, we were able to use the H signal to estimate a minimum detectable change of {approx}2% volumetric water in a 0-30 cm depth of soil.

Mitra S.; Wielopolski L.; Omonode, R.; Novak, J.; Frederick, J.; Chan, A.

2012-01-26T23:59:59.000Z

169

Impact of the Vertical Variation of Cloud Droplet Size on the Estimation of Cloud Liquid Water Path and Rain Detection  

Science Conference Proceedings (OSTI)

Cloud droplet effective radius (DER) and liquid water path (LWP) are two key parameters for the quantitative assessment of cloud effects on the exchange of energy and water. Chang and Li presented an algorithm using multichannel measurements made ...

Ruiyue Chen; Fu-Lung Chang; Zhanqing Li; Ralph Ferraro; Fuzhong Weng

2007-11-01T23:59:59.000Z

170

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

171

A Balloonborne Instrument for the Measurement of Vertical Profiles of Supercooled Liquid Water Concentration  

Science Conference Proceedings (OSTI)

A vibrating wire placed in the humidity duct of a standard U.S. rawinsonde is used to measure vertical profiles of the concentration of supercooled liquid water in clouds. The natural frequency of vibration varies according to the mass of ice ...

Geoffrey E. Hill; Duard S. Woffinden

1980-11-01T23:59:59.000Z

172

Summary of Zero Liquid Discharge (ZLD) Water Management Installations at U.S. Power Plants  

Science Conference Proceedings (OSTI)

This report presents an inventory of zero liquid discharge (ZLD) water management systems currently operating at U.S. power generating stations. A total of 146 ZLD operations were identified and described. The report discusses the numerous treatment methods used at these ZLD facilities along with their merits and detractions of each method.

2008-12-12T23:59:59.000Z

173

Determination of Cloud Liquid Water Distribution by Inversion of Radiometric Data  

Science Conference Proceedings (OSTI)

A method is described whereby the distribution of liquid water through a cross section of a cloud may be determined from radiometric data. It involves the scanning of the cloud by a pair of ground-based centimeter wave radiometers and measuring ...

J. Warner; J. F. Drake; P. R. Krehbiel

1985-09-01T23:59:59.000Z

174

Laboratory Calibration of a Vibrating Wire Device for Measuring Concentrations of Supercooled Liquid Water  

Science Conference Proceedings (OSTI)

Laboratory measurements of supercooled liquid water are made by a vibrating-wire sensor whose frequency of vibration varies according to the mass of ice collected on it. The vibrating-wire system is designed to be placed in the humidity duct of ...

Geoffrey E. Hill

1989-12-01T23:59:59.000Z

175

Influence of Water on Diffusion in Imidazolium-Based Ionic Liquids by NMR  

E-Print Network (OSTI)

Influence of Water on Diffusion in Imidazolium-Based Ionic Liquids by NMR Sergey Vasenkov AMRIS - Chemical Engineering, University of Florida In this work we applied a novel pulsed field gradient (PFG) NMR) NMR and high magnetic field gradients (up to 30 T/m). Application of high field allows for an easy

Weston, Ken

176

Quantifying the Water Content in the Cathode of Enzyme Fuel Cells via Neutron Imaging  

SciTech Connect

Neutron imaging was used to study cathode water content over time in a three-dimensional-cathode enzyme fuel cell (EFC). A porous carbon felt cathode allowed air to flow through the electrode. A solution with laccase and a mediator formed an aqueous layer on the electrode surface. Water loss was observed in situ via neutron imaging for varying experimental conditions, including flow rates of hydrogen and air, cathode inlet humidity, volume of enzyme solution, and its composition. Cathode water loss occurred for all experimental conditions, but the loss rate was noticeably reduced when a high-salt-concentration enzyme solution was used in the cathode in conjunction with increased humidity in the air feed stream. Results from neutron imaging and power density analysis were used in analyzing the causes that could contribute to EFC water loss. An increase in temperature due to the exothermic cathode reaction is considered a plausible cause of cathode water loss via evaporation. This is the first reported application of neutron imaging as a technique to study EFC water management. The results suggest that neutron imaging can be employed to provide a better understanding of EFC phenomena and thereby contribute to design and operational improvements of EFCs.

Aaron, D [Georgia Institute of Technology; Borole, Abhijeet P [ORNL; Hussey (NIST), Daniel [National Institute of Standards and Technology (NIST); Jacobson, David [National Institute of Standards and Technology (NIST); Yiacoumi, Sotira [Georgia Institute of Technology; Tsouris, Costas [ORNL

2011-01-01T23:59:59.000Z

177

Radiative Importance of ÂŤThinÂŽ 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

178

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

DOE Green Energy (OSTI)

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

179

Radiometric Determination of Uranium in Natural Waters after Enrichment and Separation by Cation-Exchange and Liquid-Liquid Extraction  

E-Print Network (OSTI)

The alpha-radiometric determination of uranium after its pre-concentration from natural water samples using the cation-exchange resin Chelex-100, its selective extraction by tributylphosphate and electrodeposition on stainless steel discs is reported. The validity of the separation procedure and the chemical recoveries were checked by addition of uranium standard solution as well as by tracing with U-232. The average uranium yield was determined to be (97 +- 2) % for the cation-exchange, (95 +- 2) % for the liquid-liquid extraction, and more than 99% for the electrodeposition. Employing high-resolution alpha-spectroscopy, the measured activity of the U-238 and U-234 radioisotopes was found to be of similar magnitude; i.e. ~7 mBq/L and ~35 mBq/L for ground- and seawater samples, respectively. The energy resolution (FWHM) of the alpha-peaks was 22 keV, while the Minimum Detectable Activity (MDA) was estimated to be 1 mBq/L (at the 95% confidence limit).

I. Pashalidis; H. Tsertos

2003-04-28T23:59:59.000Z

180

Retrieval of Soil Moisture and Vegetation Water Content Using SSM/I Data over a Corn and Soybean Region  

Science Conference Proceedings (OSTI)

The potential for soil moisture and vegetation water content retrieval using Special Sensor Microwave Imager (SSM/I) brightness temperature over a corn and soybean field region was analyzed and assessed using datasets from the Soil Moisture ...

Jun Wen; Thomas J. Jackson; Rajat Bindlish; Ann Y. Hsu; Z. Bob Su

2005-12-01T23:59:59.000Z

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.


181

A Parameterization of the Visible Extinction Coefficient of Ice Clouds in Terms of the Ice/Water Content  

Science Conference Proceedings (OSTI)

This article describes a parameterization of the visible extinction coefficient of cirrus and frontal ice cloud in terms of the ice/water content. The parameterization is based on the discovery that the ice cloud particle size spectra from a ...

C. Martin R. Platt

1997-08-01T23:59:59.000Z

182

Mass-transport considerations pertinent to aqueous-phase reactions of gases in liquid-water clouds  

SciTech Connect

Reactions of gases in liquid-water clouds are potentially important in the transformation of atmospheric pollutants affecting their transport in the atmosphere and subsequent removal and deposition to the surface. Such processes consist of the following sequence of steps. Mass-transport of the reagent gas or gases to the air-water interface; transfer across the interface and establishment of solubility equilibria locally at the interface; mass-transport of the dissolved gas or gases within the aqeuous phase; aqueous-phase chemical reactions(s); mass-transport of reaction product(s) and possible subsequent evolution into the gas-phase. Description of the rate of the overall process requires identification of the rate-limiting step (or steps) and evaluation of the rate of such step(s). Identification of the rate-limiting step may be achieved by evaluation and comparison of the characteristic times pertinent to the several processes and may be readily carried out by methods outlined herein, for known or assumed reagent concentrations, drop size, and fundamental constants as follows: gas- and aqueous-phase diffusion coefficients; Henry's law coefficient and other pertinent equilibrium constants; interfacial mass-transfer accommodation coefficient; aqueous-phase reaction rate constant(s). A graphical method is described whereby it may be ascertained whether a given reaction is controlled solely by reagent solubility and intrinsic chemical kinetics or is mass-transport limited by one or another of the above processes. In the absence of mass-transport limitation, reaction rates may be evaluated uniformly for the entire liquid-water content of the cloud using equilibrium reagent concentrations. In contrast, where appreciable mass-transport limitation is indicated, evaluation of the overall rate requires knowledge of and integration over the drop-size distribution characterizing the cloud. 68 references, 16 figures.

Schwartz, S.E.

1983-01-01T23:59:59.000Z

183

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

DOE Green Energy (OSTI)

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

184

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

185

Ultrafast dynamics of liquid water: Frequency fluctuations of the OH stretch and the HOH bend  

SciTech Connect

Frequency fluctuations of the OH stretch and the HOH bend in liquid water are reported from the third-order response function evaluated using the TTM3-F potential for water. The simulated two-dimensional infrared (IR) spectra of the OH stretch are similar to previously reported theoretical results. The present study suggests that the frequency fluctuation of the HOH bend is faster than that of the OH stretch. The ultrafast loss of the frequency correlation of the HOH bend is due to the strong couplings with the OH stretch as well as the intermolecular hydrogen bond bend.

Imoto, Sho; Xantheas, Sotiris S.; Saito, Shinji

2013-07-28T23:59:59.000Z

186

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

DOE Green Energy (OSTI)

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

187

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

Science Conference Proceedings (OSTI)

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

188

Crystalline, liquid crystalline, and isotropic phases of sodium deoxycholate in water  

SciTech Connect

Sodium deoxycholate (NaDC) is an important example of bile salts, representing systems with complex phase behavior involving both crystalline and mesophase structures. In this study, properties of NaDC-water mixtures were evaluated as a function of composition and temperature via X-ray diffraction with synchrotron (sXRD) and laboratory radiation sources, water sorption, polarized light, hot-stage microscopy, and freezing-point osmometry. Several phases were detected depending on the composition and temperature, including isotropic solution phase, liquid crystalline (LC) phase, crystalline hydrate, and ice. The LC phase was identified as hexagonal structure by sXRD, with up to 14 high-order reflections detected. The crystalline phase was found to be nonstoichiometric hydrate, based on XRD and water sorption data. The phase diagram of NaDC-water system has been refined based on both results of this study and other reports in literature.

Su, Ziyang; Luthra, Suman; Krzyzaniak, Joseph F.; Agra-Kooijman, Dena M.; Kumar, Satyendra; Byrn, Stephen R.; Shalaev, Evgenyi Y. (Pfizer); (Purdue); (Kent)

2012-09-06T23:59:59.000Z

189

The Vertical Profile of Liquid and Ice Water Content in Midlatitude Mixed-Phase Altocumulus Clouds  

Science Conference Proceedings (OSTI)

The microphysical properties of mixed-phase altocumulus clouds are investigated using in situ airborne measurements acquired during the ninth Cloud Layer Experiment (CLEX-9) over a midlatitude location. Approximately ? of the sampled profiles are ...

Lawrence D. Carey; Jianguo Niu; Ping Yang; J. Adam Kankiewicz; Vincent E. Larson; Thomas H. Vonder Haar

2008-09-01T23:59:59.000Z

190

Toward a Standard Procedure for Validation of Satellite-Derived Cloud Liquid Water Path: A Study with SEVIRI Data  

Science Conference Proceedings (OSTI)

Differences between satellite-derived and ground-based values of cloud liquid water path (LWPsat and LWPgr, respectively) in validation studies are partly associated with the validation itself, in particular with scale differences and parallax. ...

W. Greuell; R. A. Roebeling

2009-08-01T23:59:59.000Z

191

Nationwide Comparisons of Hail Size with WSR-88D Vertically Integrated Liquid Water and Derived Thermodynamic Sounding Data  

Science Conference Proceedings (OSTI)

This study tests hypothetical correspondences between size of severe hail, WSR-88D derived vertically integrated liquid water (VIL), and an array of thermodynamic variables derived from computationally modified sounding analyses. In addition, ...

Roger Edwards; Richard L. Thompson

1998-06-01T23:59:59.000Z

192

Importance of Accurate Liquid Water Path for Estimation of Solar Radiation in Warm Boundary Layer Clouds: An Observational Study  

Science Conference Proceedings (OSTI)

A 1-yr observational study of overcast boundary layer stratus at the U.S. Department of Energy Atmospheric Radiation Measurement Program Southern Great Plains site illustrates that surface radiation has a higher sensitivity to cloud liquid water ...

Manajit Sengupta; Eugene E. Clothiaux; Thomas P. Ackerman; Seiji Kato; Qilong Min

2003-09-01T23:59:59.000Z

193

Potential Applications of the SSM/I Cloud Liquid Water Parameter to the Estimation of Marine Aircraft Icing  

Science Conference Proceedings (OSTI)

Images of integrated cloud liquid water derived from the Special Sensor Microwave Imager (SSM/I) aboard the Defense Meteorological Satellite Program polar-orbiting satellite are presented. Examples with infrared and visible images and synoptic ...

Thomas F. Lee; James R. Clark; Steven D. Swadley

1994-06-01T23:59:59.000Z

194

Cloud Liquid Water Path from Satellite-Based Passive Microwave Observations: A New Climatology over the Global Oceans  

Science Conference Proceedings (OSTI)

This work describes a new climatology of cloud liquid water path (LWP), termed the University of Wisconsin (UWisc) climatology, derived from 18 yr of satellite-based passive microwave observations over the global oceans. The climatology is based ...

Christopher W. O’Dell; Frank J. Wentz; Ralf Bennartz

2008-04-01T23:59:59.000Z

195

Validation of Cloud Liquid Water Path Retrievals from SEVIRI Using One Year of CloudNET Observations  

Science Conference Proceedings (OSTI)

The accuracy and precision are determined of cloud liquid water path (LWP) retrievals from the Spinning Enhanced Visible and Infrared Imager (SEVIRI) on board Meteosat-8 using 1 yr of LWP retrievals from microwave radiometer (MWR) measurements of ...

R. A. Roebeling; H. M. Deneke; A. J. Feijt

2008-01-01T23:59:59.000Z

196

Polymer Electrolyte Fuel Cells Membrane Hydration by Direct Liquid Water Contact  

DOE Green Energy (OSTI)

An effective means of providing direct liquid hydration of the membrane tends to improve performance particularly of cells with thicker membranes or at elevated temperatures. Supplying the water to the membrane from the anode flow-field through the anode backing via wicks would appear to have advantages over delivering the water through the thickness of the membrane with regards to the uniformity and stability of the supply and the use of off-the-shelf membranes or MEAs. In addition to improving cell performance, an important contribution of direct liquid hydration approaches may be that the overall fuel cell system becomes simpler and more effective. The next steps in the evolution of this approach are a demonstration of the effectiveness of this technique with larger active area cells as well as the implementation of an internal flow-field water reservoir (to eliminate the injection method). Scale-up to larger cell sizes and the use of separate water channels within the anode flow-field is described.

Wilson, M.S.; Zawodzinski, C.; Gottesfeld, S.

1998-11-01T23:59:59.000Z

197

Molecular origin of the difference in the HOH bend of the IR spectra between liquid water and ice  

SciTech Connect

The intensity of the HOH bend in the IR spectrum of ice is significantly smaller than the corresponding one in liquid water. This difference in the IR intensities of the HOH bend in the two systems is investigated using MD simulations with the flexible, polarizable, ab-initio based TTM3-F model for water, a potential that correctly reproduces the experimentally observed increase of the HOH bend in liquid water and ice from the water monomer value. We have identified two factors that are responsible for the difference in the intensity of the HOH bend in liquid water and ice: (i) the decrease of the intensity of the HOH bend in ice caused by the strong anti-correlation between the permanent dipole moment of a molecule and the induced dipole moment of a neighboring hydrogen bond acceptor molecule and (ii) the weakening of this anti-correlation by the disordered hydrogen bond network in liquid water. The presence of the anti-correlation in ice is further confirmed by ab initio electronic structure calculations of water pentamer clusters extracted from the trajectories of the MD simulations for ice and liquid water.

Imoto, Sho; Xantheas, Sotiris S.; Saito, Shinji

2013-02-07T23:59:59.000Z

198

Method and apparatus for electrokinetic co-generation of hydrogen and electric power from liquid water microjets  

SciTech Connect

A method and apparatus for producing both a gas and electrical power from a flowing liquid, the method comprising: a) providing a source liquid containing ions that when neutralized form a gas; b) providing a velocity to the source liquid relative to a solid material to form a charged liquid microjet, which subsequently breaks up into a droplet spay, the solid material forming a liquid-solid interface; and c) supplying electrons to the charged liquid by contacting a spray stream of the charged liquid with an electron source. In one embodiment, where the liquid is water, hydrogen gas is formed and a streaming current is generated. The apparatus comprises a source of pressurized liquid, a microjet nozzle, a conduit for delivering said liquid to said microjet nozzle, and a conductive metal target sufficiently spaced from said nozzle such that the jet stream produced by said microjet is discontinuous at said target. In one arrangement, with the metal nozzle and target electrically connected to ground, both hydrogen gas and a streaming current are generated at the target as it is impinged by the streaming, liquid spray microjet.

Saykally, Richard J; Duffin, Andrew M; Wilson, Kevin R; Rude, Bruce S

2013-02-12T23:59:59.000Z

199

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

200

Errors in determination of soil water content using time-domain reflectometry caused by soil compaction around wave guides  

Science Conference Proceedings (OSTI)

Application of time domain reflectometry (TDR) in soil hydrology often involves the conversion of TDR-measured dielectric permittivity to water content using universal calibration equations (empirical or physically based). Deviations of soil-specific calibrations from the universal calibrations have been noted and are usually attributed to peculiar composition of soil constituents, such as high content of clay and/or organic matter. Although it is recognized that soil disturbance by TDR waveguides may have impact on measurement errors, to our knowledge, there has not been any quantification of this effect. In this paper, we introduce a method that estimates this error by combining two models: one that describes soil compaction around cylindrical objects and another that translates change in bulk density to evolution of soil water retention characteristics. Our analysis indicates that the compaction pattern depends on the mechanical properties of the soil at the time of installation. The relative error in water content measurement depends on the compaction pattern as well as the water content and water retention properties of the soil. Illustrative calculations based on measured soil mechanical and hydrologic properties from the literature indicate that the measurement errors of using a standard three-prong TDR waveguide could be up to 10%. We also show that the error scales linearly with the ratio of rod radius to the interradius spacing.

Ghezzehei, T.A.

2008-05-29T23:59:59.000Z

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

Nondestructive Evaluation of Low-Level Radioactive Waste Canisters for Free-Water Content  

Science Conference Proceedings (OSTI)

Federal regulations set limits on free-standing liquid in radioactive waste containers. This report identifies four nondestructive evaluation methods that may provide nuclear power plant operators with reliable and accurate determinations of the existence and amount of free-standing liquids in low-level radioactive waste (LLW) containers.

1991-06-17T23:59:59.000Z

202

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

203

Structure and Dynamics of Forsterite-scCO2/H2O Interfaces as a Function of Water Content  

Science Conference Proceedings (OSTI)

Molecular dynamics (MD) simulations of forsterite surfaces in contact with supercritical carbon dioxide (scCO2) fluids of varying water content were performed to determine the partition of water between the scCO2 fluid and the mineral surface, the nature of CO2 and H2O bonding at the interface, and the regions of the interface that may be conducive to HxCO3(2-x)- formation. Calculations of the free energy of the associative adsorption of water onto the (010) forsterite surface from the scCO2 phase indicated that the formation of a water film up to three-monolayer thick can be exothermic even for water contents below the water saturation concentration of the scCO2 fluid. In MD simulations of scCO2/H2O mixtures in contact with the (010) forsterite surface, H2O was found to readily displace CO2 at the surface and, therefore, CO2 directly contacted the surface only for water coverages below two monolayers. For thicker water films, a two-monolayer hydration layer formed that CO2 could not penetrate. Simulations of the hydroxylated (010) surface and of the (011) surface suggested that this conclusion can be extended to forsterite surfaces with different surface structures and/or compositions. The density, diffusion, and degree of hydration of CO2 as well as the extent of CO2/H2O mixing at the interface were all predicted to depend strongly on the thickness of the water-rich film, i.e., on the water content of the scCO2 fluid.

Kerisit, Sebastien N.; Weare, John H.; Felmy, Andrew R.

2012-05-01T23:59:59.000Z

204

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

Science Conference Proceedings (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

205

Resonant x-ray emission spectroscopy of liquid water: novel instrumentation, high resolution, and the"map" approach  

DOE Green Energy (OSTI)

Techniques to study the electronic structure of liquids are rare. Most recently, resonant x-ray emission spectroscopy (XES) has been shown to be an extremely versatile spectroscopy to study both occupied and unoccupied electronic states for liquids in thermodynamic equilibrium. However, XES requires high-brilliance soft x-ray synchrotron radiation and poses significant technical challenges to maintain a liquid sample in an ultra-high vacuum environment. Our group has therefore developed and constructed a novel experimental setup for the study of liquids, with the long-term goal of investigating the electronic structure of biological systems in aqueous environments. We have developed a flow-through liquid cell in which the liquid is separated from vacuum by a thin Si3N4 or SiC window and which allows a precise control of temperature. This approach has significant advantages compared to static liquids cells used in the past. Furthermore, we have designed a dedicated high-transmission, high-resolution soft x-ray spectrometer. The high transmission makes it possible to measure complete resonant XES"maps" in less than an hour, giving unprecedented detailed insight into the electronic structure of the investigated sample. Using this new equipment we have investigated the electronic structure of liquid water. Furthermore, our XES spectra and maps give information about ultra-fast dissociation on the timescale of the O 1s core hole lifetime, which is strongly affected by the initial state hydrogen bonding configuration.

Weinhardt, L.; Fuchs, O.; Blum, M.; Bär, M.; Weigand, M.; Denlinger, J.D.; Zubavichus, Y.; Zharnikov, M.; Grunze, M.; Heske, C.; Umbach, E.

2008-06-17T23:59:59.000Z

206

Water Detritiation: Better SCK-CEN Catalysts for Liquid Phase Catalytic Exchange  

SciTech Connect

A technically and economically sound technology for water detritiation is mandatory for the future of fusion. This technology is expected to be based on water electrolysis and Liquid Phase Catalytic Exchange (LPCE). LPCE requires an efficient hydrophobic catalyst. SCK-CEN invented and developed such a catalyst in the past, which is prepared by depositing platinum on an activated charcoal carrier and mixing it with polytetrafluorethylene as a hydrophobic material. In combination with an appropriate wettable packing, different batches of this catalyst performed very well during years of extensive testing, allowing us to develop the ELEX process for water detritiation at inland reprocessing plants. Recently we succeeded in reproducing this catalyst and preparing a slightly different but clearly ameliorated type. By extrapolation these new results would allow us to obtain, at 40 deg. C and under typical but conservative operating conditions, a decontamination factor of 10000 with a column of less than 3 meters long. Such performances would make this catalyst an excellent candidate for application at JET or ITER. To confirm the performances of our improved catalyst for a longer period of time and in a longer column, we are now starting experiments in a newly built installation and we are collaborating with ICSI, Romania.

Bruggeman, Aime; Braet, Johan; Vanderbiesen, Sven [SCK-CEN (Belgium)

2005-07-15T23:59:59.000Z

207

Liquid CO2 Displacement of Water in a Dual-Permeability Pore Network Micromodel  

Science Conference Proceedings (OSTI)

Permeability contrasts exist in multilayer geological formations under consideration for carbon sequestration. To improve our understanding of heterogeneous pore-scale displacements, liquid CO2 (LCO2) - water displacement was evaluated in a pore network micromodel with two distinct permeability zones. Due to the low viscosity ratio (logM = -1.1), unstable displacement occurred at all injection rates over two orders of magnitude. LCO2 displaced water only in the high permeability zone at low injection rates with the mechanism shifting from capillary fingering to viscous fingering with increasing flow rate. At high injection rates, LCO2 displaced water in the low permeability zone with capillary fingering as the dominant mechanism. LCO2 saturation (SLCO2) as a function of injection rate was quantified using fluorescent microscopy. In all experiments, more than 50% of LCO2 resided in the active flowpaths, and this fraction increased as displacement transitioned from capillary to viscous fingering. A continuum-scale two-phase flow model with independently determined fluid and hydraulic parameters was used to predict SLCO2 in the dual-permeability field. Agreement with the micromodel experiments was obtained for low injection rates. However, the numerical model does not account for the unstable viscous fingering processes observed experimentally at higher rates and hence overestimated SLCO2.

Zhang, Changyong; Oostrom, Martinus; Grate, Jay W.; Wietsma, Thomas W.; Warner, Marvin G.

2011-09-01T23:59:59.000Z

208

Method of extracting iodine from liquid mixtures of iodine, water and hydrogen iodide  

DOE Green Energy (OSTI)

The components of a liquid mixture consisting essentially of HI, water and at least about 50 w/o iodine are separated in a countercurrent extraction zone by treating with phosphoric acid containing at least about 90 w/o H.sub.3 PO.sub.4. The bottom stream from the extraction zone is substantially completely molten iodine, and the overhead stream contains water, HI, H.sub.3 PO.sub.4 and a small fraction of the amount of original iodine. When the water and HI are present in near-azeotropic proportions, there is particular advantage in feeding the overhead stream to an extractive distillation zone wherein it is treated with additional concentrated phosphoric acid to create an anhydrous HI vapor stream and bottoms which contain at least about 85 w/o H.sub.3 PO.sub.4. Concentration of these bottoms provides phosphoric acid infeed for both the countercurrent extraction zone and for the extractive distillation zone.

Mysels, Karol J. (La Jolla, CA)

1979-01-01T23:59:59.000Z

209

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

DOE Green Energy (OSTI)

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

210

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  

Science Conference Proceedings (OSTI)

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

211

Measurements of the Total Water Content of Cirrus Clouds. Part II: Instrument Performance and Validation  

Science Conference Proceedings (OSTI)

This paper describes the performance and in-flight validation of an instrument mounted in a pallet on the NASA WB-57 research aircraft that measures the sum of gas phase and solid phase water, or total water, in cirrus clouds. Using a heated ...

E. M. Weinstock; J. B. Smith; D. Sayres; J. V. Pittman; N. Allen; J. G. Anderson

2006-11-01T23:59:59.000Z

212

Search for the First-Order Liquid-to-Liquid Phase Transition in Low-Temperature Confined Water by Neutron Scattering  

SciTech Connect

It has been conjectured that a 1st order liquid-to-liquid (L-L) phase transition (LLPT) between high density liquid (HDL) and low density liquid (LDL) in supercooled water may exist, as a thermodynamic extension to the liquid phase of the 1st order transition established between the two bulk solid phases of amorphous ice, the high density amorphous ice (HDA) and the low density amorphous ice (LDA). In this paper, we first recall our previous attempts to establish the existence of the 1st order L-L phase transition through the use of two neutron scattering techniques: a constant Q elastic diffraction study of isobaric temperature scan of the D2O density, namely, the equation of state (EOS) measurements. A pronounced density hysteresis phenomenon in the temperature scan of the density above P = 1500 bar is observed which gives a plausible evidence of crossing the 1st order L-L phase transition line above this pressure; an incoherent quasi-elastic scattering measurements of temperature-dependence of the alpha-relaxation time of H2O at a series of pressures, namely, the study of the Fragile-to-Strong dynamic crossover (FSC) phenomenon as a function of pressure which we interpreted as the results of crossing the Widom line in the one-phase region. In this new experiment, we used incoherent inelastic neutron scattering (INS) to measure the density of states (DOS) of H atoms in H2O molecules in confined water as function of temperature and pressure, through which we may be able to follow the emergence of the LDL and HDL phases at supercooled temperature and high pressures. We here report for the first time the differences of librational and translational DOSs between the hypothetical HDL and LDL phases, which are similar to the corresponding differences between the well-established HDA and LDA ices. This is plausible evidence that the HDL and LDL phases are the thermodynamic extensions of the corresponding amorphous solid water HDA and LDA ices.

Chen, Sow-Hsin [Massachusetts Institute of Technology (MIT); Wang, Zhe [Massachusetts Institute of Technology (MIT); Kolesnikov, Alexander I [ORNL; Zhang, Yang [ORNL; Liu, Kao-Hsiang [National Taiwan University

2013-01-01T23:59:59.000Z

213

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

E-Print Network (OSTI)

The Gas-to-liquids (GTL) processes produce a large fraction of by-products whose disposal or handling ordinarily becomes a cost rather than benefit. As an alternative strategy to market stranded gas reserves, GTL provides middle distillates to an unsaturated global market and offers opportunities to generate power for commercial purposes from waste by-product streams, which normally are associated with increased expenses incurred from additional handling cost. The key concept investigated in this work is the possibility of integrating the GTL process with power generation using conventional waste by-product steam streams. Simulation of the integrated process was conducted with the aim of identifying the critical operating conditions for successful integration of the GTL and power generation processes. About 500 MW of electric power can be generated from 70% of the exit steam streams, with around 20 to 25% steam plant thermal efficiency. A detailed economic analysis on the LNG, stand-alone GTL, and Integrated GTL Power-Generation plants indicates that the integrated system is more profitable than the other options considered. Justifying the technology and economics involved in the use of the by-product streams to generate power could increase the net revenue and overall profitability of GTL projects. This technology may be transferable to GTL projects in the world, wherever a market for generated power exists.

Adegoke, Adesola Ayodeji

2006-08-01T23:59:59.000Z

214

MWRRET Value-Added Product: The Retrieval of Liquid Water Path and Precipitable Water Vapor from Microwave Radiometer (MWR) Data Sets (Revision 2)  

SciTech Connect

This report provides a short description of the Atmospheric Radiation Measurement (ARM) Climate Research Facility microwave radiometer (MWR) Retrieval (MWRRET) value-added product (VAP) algorithm. This algorithm utilizes a complementary physical retrieval method and applies brightness temperature offsets to reduce spurious liquid water path (LWP) bias in clear skies resulting in significantly improved precipitable water vapor (PWV) and LWP retrievals. We present a general overview of the technique, input parameters, output products, and describe data quality checks. A more complete discussion of the theory and results is given in Turner et al. (2007b).

Gaustad, KL; Turner, DD; McFarlane, SA

2011-07-25T23:59:59.000Z

215

Accurate Liquid Water Path Retrieval from Low-Cost Microwave Radiometers Using Additional Information from a Lidar Ceilometer and Operational Forecast Models  

Science Conference Proceedings (OSTI)

Water clouds have an important impact on the radiative balance of the earth. The use of ground-based dual-frequency microwave radiometers to derive both liquid water path (LWP) and water vapor path (WVP) is well established, but uncertainties ...

Nicolas Gaussiat; Robin J. Hogan; Anthony J. Illingworth

2007-09-01T23:59:59.000Z

216

Subsurface monitoring of reservoir pressure, temperature, relative humidity, and water content at the CAES Field Experiment, Pittsfield, Illinois: system design  

DOE Green Energy (OSTI)

This subsurface-instrumentation design has been developed for the first Compressed Air Energy Storage (CAES) field experiment to be performed in porous media. Energy storage will be accomplished by alternating the injection and withdrawal of compressed air in a confined sandstone aquifer near Pittsfield, Illinois. The overall experiment objective is to characterize the reservoir's geochemical and thermohydraulic response to imposed CAES conditions. Specific experiment objectives require monitoring: air-bubble development; thermal development; cyclic pressure response; reservoir dehydration; and water coning. Supporting these objectives, four parameters will be continuously monitored at depth in the reservoir. They are: temperature; pressure; pore-air relative humidity; and pore-water content. Reservoir temperatures and pressures will range to maximum values approaching 200/sup 0/C and 300 psi, respectively. Both pore-air relative humidity and pore-water content will range from approx. 0 to 100%. This report discusses: instrumentation design; sensor and sensor system calibration; field installation and testing; and instrument-system operation. No comprehensive off-the-shelf instrument package exists to adequately monitor CAES reservoir parameters at depth. The best available sensors were selected and adapted for use under expected ranges of reservoir conditions. The instrumentation design criteria required: suitable sensor accuracy; continuous monitoring capability; redundancy; maximum sensor integrity; contingency planning; and minimum cost-information ratio. Three wells will be instrumented: the injection/withdrawal (I/W) well and the two instrument wells. Sensors will be deployed by wireline suspension in both open and backfilled (with sand) wellbores. The sensors deployed in the I/W well will be retrievable; the instrument-well sensors will not.

Hostetler, D.D.; Childs, S.W.; Phillips, S.J.

1983-03-01T23:59:59.000Z

217

Lidar-Based Characterization of the Geometry and Structure of Water Clouds  

Science Conference Proceedings (OSTI)

Lidar remote sensing measurements of low-level water clouds in the form of vertical soundings and instantaneous (1 min) azimuth-over-elevation scans are reported. Retrievals are made of the liquid water content and effective droplet diameter at ...

Luc R. Bissonnette; Gilles Roy; Grégoire Tremblay

2007-08-01T23:59:59.000Z

218

Modeling the Interactions between Aerosols and Liquid Water Clouds with a Self-Consistent Cloud Scheme in a General Circulation Model  

Science Conference Proceedings (OSTI)

To model aerosol–cloud interactions in general circulation models (GCMs), a prognostic cloud scheme of cloud liquid water and amount is expanded to include droplet number concentration (Nd) in a way that allows them to be calculated using the ...

Yi Ming; V. Ramaswamy; Leo J. Donner; Vaughan T. J. Phillips; Stephen A. Klein; Paul A. Ginoux; Larry W. Horowitz

2007-04-01T23:59:59.000Z

219

Apparatus and method for pumping hot, erosive slurry of coal solids in coal derived, water immiscible liquid  

SciTech Connect

An apparatus for and method of pumping hot, erosive slurry of coal solids in a coal derived, water immiscible liquid to higher pressure involves the use of a motive fluid which is miscible with the liquid of the slurry. The apparatus includes a pump 12, a remote check valve 14 and a chamber 16 between and in fluid communication with the pump 12 and check valve 14 through conduits 18,20. Pump 12 exerts pressure on the motive fluid and thereby on the slurry through a concentration gradient of coal solids within chamber 16 to alternately discharge slurry under pressure from the outlet port of check valve 14 and draw slurry in through the inlet port of check valve 14.

Ackerman, Carl D. (Olympia, WA)

1983-03-29T23:59:59.000Z

220

Calculation of releases of radioactive materials in gaseous and liquid effluents from pressurized water reactors (PWR-GALE Code). Revision 1  

SciTech Connect

This report revises the original issuance of NUREG-0017, ''Calculation of Releases of Radioactive Materials in Gaseous and Liquid Effluents from Pressurized Water Reactors (PWR-GALE-Code)'' (April 1976), to incorporate more recent operating data now available as well as the results of a number of in-plant measurement programs at operating pressurized water reactors. The PWR-GALE Code is a computerized mathematical model for calculating the releases of radioactive material in gaseous and liquid effluents (i.e., the gaseous and liquid source terms). The US Nuclear Regulatory Commission uses the PWR-GALE Code to determine conformance with the requirements of Appendix I to 10 CFR Part 50.

Chandrasekaran, T.; Lee, J.Y.; Willis, C.A.

1985-04-01T23:59:59.000Z

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.


221

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

E-Print Network (OSTI)

geometries other than ice and gas-phase. This approach has1-4 . In its condensed ice Ih phase each water molecule is150 K. Spectra of gas phase and ice 5, 15, 16 are shown as

Nordlund, D.

2009-01-01T23:59:59.000Z

222

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

223

Recovery of Non-Aqueous Phase Liquids from Contaminated Soil by CO2-Supersaturated Water Injection.  

E-Print Network (OSTI)

??Supersaturated water injection (SWI) is a novel remediation technology which is able to remove entrapped residual NAPLs from saturated porous media by both volatilization (partitioning… (more)

Li, Meichun

2009-01-01T23:59:59.000Z

224

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)

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

Bahrami, Majid

225

High-Resolution Electrospray Ionization Mass Spectrometry Analysis of Water- Soluble Organic Aerosols Collected with a Particle into Liquid Sampler  

DOE Green Energy (OSTI)

This work demonstrates the utility of a particle-into-liquid sampler (PILS) a technique traditionally used for identification of inorganic ions present in ambient or laboratory aerosols for the analysis of water soluble organic aerosol (OA) using high resolution electrospray ionization mass spectrometry (HR ESI-MS). Secondary organic aerosol (SOA) was produced from 0.5 ppm mixing ratios of limonene and ozone in a 5 m3 Teflon chamber. SOA was collected simultaneously using a traditional filter sampler and a PILS. The filter samples were later extracted with either water or acetonitrile, while the aqueous PILS samples were analyzed directly. In terms of peak intensities, types of detectable compounds, average O:C ratios, and organic mass to organic carbon ratios, the resulting high resolution mass spectra were essentially identical for the PILS and filter based samples. SOA compounds extracted from both filter/acetonitrile extraction and PILS/water extraction accounted for >95% of the total ion current in ESI mass spectra. This similarity was attributed to high solubility of limonene SOA in water. In contrast, significant differences in detected ions and peak abundances were observed for pine needle biomass burning organic aerosol (BBOA) collected with PILS and filter sampling. The water soluble fraction of BBOA is considerably smaller than for SOA, and a number of unique peaks were detectable only by the filter/acetonitrile method. The combination of PILS collection with HR-ESI-MS analysis offers a new approach for molecular analysis of the water-soluble organic fraction in biogenic SOA, aged photochemical smog, and BBOA.

Bateman, Adam P.; Nizkorodov, Serguei; Laskin, Julia; Laskin, Alexander

2010-10-01T23:59:59.000Z

226

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  

Science Conference Proceedings (OSTI)

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

227

Liquid-phase and vapor-phase dehydration of organic/water solutions  

DOE Patents (OSTI)

Processes for dehydrating an organic/water solution by pervaporation or vapor separation using fluorinated membranes. The processes are particularly useful for treating mixtures containing light organic components, such as ethanol, isopropanol or acetic acid.

Huang, Yu (Palo Alto, CA); Ly, Jennifer (San Jose, CA); Aldajani, Tiem (San Jose, CA); Baker, Richard W. (Palo Alto, CA)

2011-08-23T23:59:59.000Z

228

On a phase field model for solid-liquid phase transitions  

E-Print Network (OSTI)

distinct phases. This is the case for solid-liquid mix- tures (e.g. ice-water or alloys duringOn a phase field model for solid-liquid phase transitions S. Benzoni-Gavage , L. Chupin , D. Jamet , and J. Vovelle December 3, 2010 Contents 1 Introduction 2 2 Phase field equations 3 2.1 Derivation

229

Structure and Dynamics of N, N-diethyl-N-methylammonium Triflate Ionic Liquid, Neat and with Water, from Molecular Dynamics Simulations  

DOE Green Energy (OSTI)

We investigated by means of molecular dynamics simulations the properties (structure, thermodynamics, ion transport, and dynamics) of the protic ionic liquid N,N-diethyl-N-methyl-ammonium triflate (dema:Tfl) and of selected aqueous mixtures of dema:Tfl. This ionic liquid, a good candidate for a water-free proton exchange membrane, is shown to exhibit high ion mobility and conductivity. For bulk melts in the temperature range of 303-453K, both liquid densities and enthalpies of vaporization are found to decrease roughly linearly with increasing temperature. The radial distribution functions reveal a significant long-range structural correlation. The ammonium cations [dema]+ are found to diffuse slightly faster than the triflate anions [Tfl]-, and both types of ions exhibit enhanced mobility at higher temperatures, leading to higher ionic conductivity of these ionic liquids. Analysis of the dynamics of ion pairing clearly points to the existence of long-lived contact ion pairs in this ionic liquid. We also examined the effects of water on the ionic properties of dema:Tfl-water mixtures. From the structural analysis it was found that water molecules tend to replace counter ions in the coordination shell and hydrogen bond to both ions, thus weakening their mutual association. As water concentration increases, water molecules start to connect with each other and eventually form a large network that percolates through the system. It is also found that water has a strong influence on the ion dynamics in the mixtures. As the concentration of water increases, both translational and rotational motion of [dema]+ and [Tfl]- are significantly enhanced. As a result, higher ionic conductivity is observed with increased hydration level. This work was supported by the US Department of Energy Basic Energy Sciences' Chemical Sciences, Geosciences & Biosciences Division. Pacific Northwest National Laboratory is operated by Battelle for the US Department of Energy.

Chang, Tsun-Mei; Dang, Liem X.; Devanathan, Ramaswami; Dupuis, Michel

2010-12-09T23:59:59.000Z

230

Engineering Model of Liquid Storage Utility Tank for Heat Transfer Analysis  

SciTech Connect

The utility or chemical storage tank requires special engineering attention and heat transfer analysis because the tank content is very sensitive to temperature and surrounding environment such as atmospheric or outside air, humidity, and solar radiation heat. A simplified heat transfer model was developed to calculate the liquid content temperature of utility storage tank. The content of the utility storage tanks can be water or any other chemical liquid. An engineering model of liquid storage tank for heat transfer analysis and temperature calculations are presented and discussed in the examples of Tanks No. 1 containing oxalic acid and No. 2 containing sodium tetraphenylborate solution.

Kwon, K.C.

1995-09-27T23:59:59.000Z

231

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"

232

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 is used to restrict the application of the geophysical retrieval algorithms which are developed to handle specific atmospheric absorptive situations. An improved semi-empirical sea surface emissivity model is integrated into this refined D-matrix procedure that is being developed for the Advanced Microwave Sounding Radiometer (AMSR). The purpose of this work is to test the refined geophysical parameter retrieval methods using data from the Special Sensor Microwave / Imager (SSM/I). When comparing the statistical performance of the TIWV, WS, and CLW retrieval methods presented to the statistical performance of published retrieval methods for each geophysical parameter, the retrieval methods developed for this study perform only slightly better. However, it is demonstrated that the new retrieval methods are more physically valid than the comparison retrieval methods. The utilization of the polarization difference of the 85 GHZ channels to restrict the application of specifically-derived retrieval algorithms proves to be a valuable and reliable geophysical parameter retrieval tool.

Manning, Norman Willis William

1997-01-01T23:59:59.000Z

233

Infrared Spectroscopy and Hydrogen-Bond Dynamics of Liquid Water from Centroid Molecular Dynamics with an Ab Initio-Based Force Field  

DOE Green Energy (OSTI)

A molecular-level description of the unique properties of hydrogen-bond networks is critical for understanding many fundamental physico-chemical processes in aqueous environments. In this article a novel simulation approach, combining an ab-initio based force field for water with a quantum treatment of the nuclear motion, is applied to investigate hydrogen-bond dynamics in liquid water with a specific focus on the relationship of these dynamics to vibrational spectroscopy. Linear and nonlinear infrared (IR) spectra are calculated for liquid water, HOD in D2O and HOD in H2O and discussed in the context of the results obtained using other approaches that have been employed in studies of water dynamics. A comparison between the calculated spectra and the available experimental data yields an overall good agreement, indicating the accuracy of the present simulation approach in describing the properties of liquid water at ambient conditions. Possible improvements on the representation of the underlying water interactions as well as the treatment of the molecular motion at the quantum-mechanical level are also discussed. This research was supported by the Division of Chemical Sciences, Biosciences and Geosciences, US Department of Energy. Battelle operates the Pacific Northwest National Laboratory for the US Department of Energy.

Paesani, Francesco; Xantheas, Sotiris S.; Voth, Gregory A.

2009-10-01T23:59:59.000Z

234

Probability Density Functions of Liquid Water Path and Cloud Amount of Marine Boundary Layer Clouds: Geographical and Seasonal Variations and Controlling Meteorological Factors  

Science Conference Proceedings (OSTI)

The subgrid-scale variability of the liquid water path (LWP) of marine boundary layer clouds in areas that correspond to the typical grid size of large-scale (global climate and weather prediction) atmospheric models (200 km × 200 km) is ...

Hideaki Kawai; Joăo Teixeira

2010-04-01T23:59:59.000Z

235

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)"

236

The Partitioning of Acetic, Formic, and Phosphoric Acids Between Liquid Water and Steam  

Science Conference Proceedings (OSTI)

The chemical carryover of impurities and treatment chemicals from the boiler to the steam phase, and ultimately to the low-pressure turbine and condenser, can be quantified based on laboratory experiments preformed over ranges of temperature, pH, and composition. The two major assumptions are that thermodynamic equilibrium is maintained and no deposition, adsorption or decomposition occurs. The most recent results on acetic, formic and phosphoric acids are presented with consideration of the effects of hydrolysis and dimerization reactions. Complications arising from thermal decomposition of the organic acids are discussed. The partitioning constants for these acids and other solutes measured in this program have been incorporated into a simple thermodynamic computer code that calculates the effect of chemical and mechanical carryover on the composition of the condensate formed to varying extents in the water/steam cycle.

Gruszkiewicz, M.S.; Marshall, S.L.; Palmer, D.A.; Simonson, J.M.

1999-06-22T23:59:59.000Z

237

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

238

Radiative effects of supercooled water Summary. Supercooled liquid water layers are visible in lidar imagery as a strongly enhanced return followed by  

E-Print Network (OSTI)

parameters. Hence cloud phase parameterizations in numerical forecast and climate models have tended parameterizations use other model variables (such as vertical velocity) to aid the diagnosis of liquid/ice fraction, suggesting that they are radiatively important. In this chapter, three profiles of liquid and ice extinction

Hogan, Robin

239

Distance-Scaled Water Concentrations versus Mass-Median Drop Size, Temperature, and Altitude in Supercooled Clouds  

Science Conference Proceedings (OSTI)

About 28 000 nautical miles (n mi) of select in-flight measurements of liquid water content (LWC), droplet sizes, temperature, and other variables in supercooled clouds from a variety of research projects over portions of North America, Europe, ...

Richard K. Jeck

2008-07-01T23:59:59.000Z

240

Characterization of water-based liquid scintillator response to gammas and neutrons at varying scintillator-surfactant concentrations  

E-Print Network (OSTI)

Large scale solar neutron and neutrino flux experiments require many tons of bulk liquid organic scintillator to take spectroscopic data of these energetic particles. However, material and chemical concerns make such ...

Chilton, Lauren (Lauren M.)

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.


241

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!

242

Water  

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

Laws Envirosearch Institutional Controls NEPA Activities RCRA RQ*Calculator Water HSS Logo Water Laws Overview of water-related legislation affecting DOE sites Clean...

243

NETL: Coal & Coal Biomass to Liquids - Alternate Hydrogen Production  

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

Coal and CoalBiomass to Liquids Alternate Hydrogen Production In the Alternate Production technology pathway, clean syngas from coal is converted to high-hydrogen-content liquid...

244

Hydrogen Production From Metal-Water Reactions  

E-Print Network (OSTI)

. Current methods of hydrogen storage in automobiles are either too bulky (large storage space for gas phase) or require a high input energy (cooling or pressurization systems for liquid hydrogen), making widespread use abundance, high- energy content, and large surface area, is able to combine with water to produce hydrogen

Barthelat, Francois

245

Deployment and Evaluation of a System for Ground-Based Measurement of Cloud Liquid Water Turbulent Fluxes  

Science Conference Proceedings (OSTI)

Direct interception of windblown cloud water by forests has been dubbed “occult deposition” because it represents a hydrological input that is hidden from rain gauges. Eddy correlation studies of this phenomenon have estimated cloud water fluxes ...

Andrew S. Kowalski; Peter M. Anthoni; Richard J. Vong; Anthony C. Delany; Gordon D. Maclean

1997-06-01T23:59:59.000Z

246

Energy Basics: Solar Liquid Heating  

Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

EERE: Energy Basics Solar Liquid Heating Solar liquid heating systems use a collector with a heat transfer or "working" fluid such as water, antifreeze (usually non-toxic propylene...

247

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

248

Influence of wettability on liquid water transport in gas diffusion layer of proton exchange membrane fuel cells (PEMFC)  

E-Print Network (OSTI)

Water management is a key factor that limits PEFC's performance. We show how insights into this problem can be gained from pore-scale simulations of water invasion in a model fibrous medium. We explore the influence of contact angle on the water invasion pattern and water saturation at breakthrough and show that a dramatic change in the invasion pattern, from fractal to compact, occurs as the system changes from hydrophobic to hydrophilic. Then, we explore the case of a system of mixed wettability, i.e. containing both hydrophilic and hydrophobic pores. The saturation at breakthrough is studied as a function of the fraction of hydrophilic pores. The results are discussed in relation with the water management problem, the optimal design of a GDL and the fuel cell performance degradation mechanisms. We outline how the study could be extended to 3D systems, notably from binarised images of GDLs obtained by X ray microtomography.

Hamza Chraibi; L. Ceballos; M. Prat; Michel Quintard; Alexandre Vabre

2009-09-16T23:59:59.000Z

249

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

250

Biodesulfurization of mild gasification liquid products. Final technical report, 1 September, 1992--31 August, 1993  

Science Conference Proceedings (OSTI)

The mild gasification of coal, as being developed at IGT and elsewhere, is a promising new technology that can convert coal to multiple products: gas, solid, and liquids. Mild gasification liquids can be used as feedstock to make transportation fuels and chemicals. However, the sulfur content and aromaticity of mild gasification liquids limits their usefulness and biodesulfurization can potentially decrease both sulfur content and aromaticity. The objective of this project is to investigate and feasibility of using biodesulfurization to upgrade the quality of mild gasification liquids. During this project, it was shown that the middle distillate (360--440 F) fraction of liquids derived from the mild gasification of coal, and unfractionated liquids can be biodesulfurized. Moreover, it was demonstrated that lysed cell preparations and freeze-dried cells can be used to biodesulfurize mild coal gasification liquids. The importance of the finding that freeze-dried biocatalysts can be used to biodesulfurize mild coal gasification liquids is that freeze-dried cells can be produced at one location, stored indefinitely, and then shipped (at reduced weight, volume, and cost) to another location for coal biodesulfurization. Moreover, freeze-dried biocatalysts can be added directly to mild coal gasification liquids with only minimal additions of water so that reactor volumes can be minimized.

Kilbane, J.J. II [Institute of Gas Technology, Chicago, IL (United States)

1993-12-31T23:59:59.000Z

251

Workbook Contents  

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

,"Workbook Contents" ,"From PADD 1 to PADD 2 Movements by Tanker, Pipeline, and Barge" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

252

Workbook Contents  

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

,"Workbook Contents" ,"Price for Natural Gas Pipeline and Distribution Use " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

253

Workbook Contents  

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

,"Workbook Contents" ,"Crude Oil and Petroleum Products Movements by Tanker, Pipeline, and Barge between PAD Districts" ,"Click worksheet name or tab at bottom for data"...

254

Workbook Contents  

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

,"Workbook Contents" ,"U.S. Natural Gas Pipeline Imports by Point of Entry " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

255

Workbook Contents  

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

,"Workbook Contents" ,"U.S. Natural Gas Pipeline Exports by Point of Exit " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

256

Workbook Contents  

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

,"Workbook Contents" ,"Texas Natural Gas Industrial Consumption (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

257

Workbook Contents  

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

,"Workbook Contents" ,"Texas Natural Gas Deliveries to Electric Power Consumers (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

258

Workbook Contents  

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

,"Workbook Contents" ,"Texas Natural Gas Gross Withdrawals (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Late...

259

Workbook Contents  

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

,"Workbook Contents" ,"Texas Natural Gas Marketed Production (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","La...

260

Workbook Contents  

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

,"Workbook Contents" ,"Texas Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet...

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

,"Workbook Contents" ,"Average Commercial Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

262

Workbook Contents  

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

,"Workbook Contents" ,"Nevada Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

263

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Citygate Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

264

Workbook Contents  

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

,"Workbook Contents" ,"U.S. Total Exports " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for" ,"Data...

265

Workbook Contents  

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

Contents" ,"Maryland Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

266

Workbook Contents  

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

,"Workbook Contents" ,"Utah Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

267

Workbook Contents  

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

Contents" ,"Tennessee Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

268

Workbook Contents  

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

Contents" ,"Kentucky Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

269

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Industrial Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

270

Workbook Contents  

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

,"Workbook Contents" ,"Alaska Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

271

Workbook Contents  

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

Contents" ,"Utah Natural Gas Residential Consumption (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

272

Workbook Contents  

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

Contents" ,"Missouri Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

273

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Exports Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

274

Workbook Contents  

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

Contents" ,"Oklahoma Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

275

Workbook Contents  

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

Contents" ,"Montana Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

276

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Vehicle Fuel Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data...

277

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Exports (Summary) " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

278

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Consumption " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

279

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Electric Power Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data...

280

Workbook Contents  

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

Contents" ,"Arkansas Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

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

,"Workbook Contents" ,"Natural Gas Imports (Summary) " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

282

Workbook Contents  

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

Contents" ,"Florida Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

283

Workbook Contents  

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

,"Workbook Contents" ,"Average Residential Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

284

Workbook Contents  

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

Contents" ,"Michigan Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

285

Workbook Contents  

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

Contents" ,"Nebraska Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

286

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Wellhead Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

287

Workbook Contents  

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

Contents" ,"Wyoming Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

288

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Imports Price " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for"...

289

Workbook Contents  

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

,"Workbook Contents" ,"Oregon Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

290

Workbook Contents  

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

Contents" ,"Alabama Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

291

Workbook Contents  

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

Contents" ,"Arizona Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

292

Workbook Contents  

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

Contents" ,"Weekly Working Gas in Underground Storage" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

293

Workbook Contents  

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

Contents" ,"Hawaii Natural Gas Residential Consumption (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

294

Workbook Contents  

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

Contents" ,"Kansas Natural Gas Residential Consumption (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

295

Workbook Contents  

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

Contents" ,"Maine Natural Gas Residential Consumption (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

296

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Marketed Production " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data...

297

Workbook Contents  

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

,"Workbook Contents" ,"Kansas Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

298

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Delivered to Consumers " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data...

299

Workbook Contents  

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

,"Workbook Contents" ,"Balancing Item (Bcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest Data for" ,"Data...

300

Workbook Contents  

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

Contents" ,"Colorado Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

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

Contents" ,"California Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

302

Workbook Contents  

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

Contents" ,"Nevada Natural Gas Residential Consumption (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

303

Workbook Contents  

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

Contents" ,"Oregon Natural Gas Residential Consumption (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

304

Workbook Contents  

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

,"Workbook Contents" ,"Texas Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

305

Workbook Contents  

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

Contents" ,"Pennsylvania Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","Latest...

306

Inactive Content  

Science Conference Proceedings (OSTI)

Inactive Content. This page is in the process of being created or has temporarily been inactivated. If you have any questions ...

307

Workbook Contents  

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

,"Workbook Contents" ,"South Dakota Natural Gas Repressuring (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of Series","Frequency","La...

308

Workbook Contents  

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

,"Workbook Contents" ,"South Dakota Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)" ,"Click worksheet name or tab at bottom for data"...

309

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Delivered to Consumers in South Dakota (Including Vehicle Fuel) (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet...

310

Workbook Contents  

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

,"Workbook Contents" ,"Natural Gas Citygate Price in South Dakota (Dollars per Thousand Cubic Feet)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet...

311

Workbook Contents  

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

,"Workbook Contents" ,"South Dakota Natural Gas Withdrawals from Oil Wells (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

312

Workbook Contents  

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

,"Workbook Contents" ,"South Dakota Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)" ,"Click worksheet name or tab at bottom for data"...

313

Workbook Contents  

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

,"Workbook Contents" ,"Percent of Commercial Natural Gas Deliveries in South Dakota Represented by the Price (%)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet...

314

Workbook Contents  

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

,"Workbook Contents" ,"South Dakota Natural Gas Withdrawals from Gas Wells (MMcf)" ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

315

Workbook Contents  

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

,"Workbook Contents" ,"South Dakota Natural Gas Gross Withdrawals from Coalbed Wells (MMcf) " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description","...

316

Workbook Contents  

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

,"Workbook Contents" ,"Percentage of Total Natural Gas Residential Deliveries included in Prices " ,"Click worksheet name or tab at bottom for data" ,"Worksheet...

317

Liquid-Liquid Extraction Processes  

E-Print Network (OSTI)

Liquid-liquid extraction is the separation of one or more components of a liquid solution by contact with a second immiscible liquid called the solvent. If the components in the original liquid solution distribute themselves differently between the two liquid phases, separation will result. This is the principle upon which separation by liquid-liquid extraction is based, and there are a number of important applications of this concept in industrial processes. This paper will review the basic concepts and applications as well as present future directions for the liquid-liquid extraction process.

Fair, J. R.; Humphrey, J. L.

1983-01-01T23:59:59.000Z

318

On the Calibration and Performance of an Instrument for Measuring Total Water Mixing Ratio in Cloud  

Science Conference Proceedings (OSTI)

An instrument which measures the total water mixing ratio in cloud has been calibrated to an accuracy of ±0.1 g kg?1 in the presence of liquid water contents ranging up to 7 g kg?1. Evaporation occurs in a labyrinth of heated plates and the ...

C. E. Coulman; M. A. Parker

1982-05-01T23:59:59.000Z

319

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. â—Ź Model simulated large scale features match well with observations. â—Ź 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. â—Ź Model overestimates high clouds, especially in warm seasons. â—Ź Model makes close estimation for middle clouds. â—Ź Model underestimates low clouds in warm seasons, especially in

320

Reply to Comment on"Isotope and Temperature Effects in Liquid Water Probed by X-ray Absorption and Resonant X-ray Emission Spectroscopy"  

Science Conference Proceedings (OSTI)

In Ref. [1], we present and analyze experimental high resolution x-ray emission spectra (XES) of liquid water which exhibit a splitting of the 1b1 line into two components. We also suggest a qualitative model to explain the experimental spectra which, even though tentative (as clearly stated in the summary of Ref. [1]), is able to explain ALL available experimental data. In the preceding Comment, Pettersson et al. [3]claim that a spectrum with two similarly sharp 1b1 features both from a dissociated product (d2) and from the intact molecule (d1) would be"unphysical and unsubstantiated" since"the path connecting initial and final structure" is not taken into account. In the meantime, we have collected new data [2], which further support and strengthen our model.

Heske, C.; Zharnikov, M.; Weinhardt, L.; Blum, M.; Weigand, M.; Zubavichus, Y.; Bar, M.; Maier, F.; Denlinger, J. D.; Fuchs, O.; Grunze, M.; Umbach, E.

2008-05-14T23:59:59.000Z

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.


321

Workbook Contents  

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

,"Workbook Contents" ,"U.S. Price of Natural Gas Pipeline Exports by Point of Exit " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

322

Workbook Contents  

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

,"Workbook Contents" ,"U.S. Price of Natural Gas Pipeline Imports by Point of Entry " ,"Click worksheet name or tab at bottom for data" ,"Worksheet Name","Description"," Of...

323

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 9:14:27 AM" "Back to Contents","Data 1: Wisconsin Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"...

324

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 9:13:24 AM" "Back to Contents","Data 1: Wisconsin Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic...

325

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 5:40:28 AM" "Back to Contents","Data 1: Wisconsin Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010WI2" "Date","Wisconsin...

326

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 5:43:56 AM" "Back to Contents","Data 1: Wisconsin Natural Gas Industrial Consumption (MMcf)" "Sourcekey","N3035WI2" "Date","Wisconsin...

327

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 5:45:05 AM" "Back to Contents","Data 1: Wisconsin Natural Gas Deliveries to Electric Power Consumers (MMcf)" "Sourcekey","N3045WI2"...

328

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 5:45:04 AM" "Back to Contents","Data 1: Wisconsin Natural Gas Deliveries to Electric Power Consumers (MMcf)" "Sourcekey","N3045WI2"...

329

Spectral Content  

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

Spectral Content of the NLC Bunch Train due to Long Range Wakefields Peter Tenenbaum LCC-Note-0015 10-May-1999 Abstract The functional specifications of the sub-train position...

330

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:41:19 AM" "Back to Contents","Data 1: Natural...

331

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"1092013 12:45:25 PM" "Back to Contents","Data 1: Natural...

332

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:47:49 AM" "Back to Contents","Data 1: Oklahoma...

333

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:47:48 AM" "Back to Contents","Data 1: Ohio...

334

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:40:49 AM" "Back to Contents","Data 1: Natural...

335

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:47:39 AM" "Back to Contents","Data 1: Indiana...

336

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:41:58 AM" "Back to Contents","Data 1: Natural...

337

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:44:37 AM" "Back to Contents","Data 1: Nebraska...

338

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:50:33 AM" "Back to Contents","Data 1:...

339

Workbook Contents  

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

2:08:06 PM" "Back to Contents","Data 1: Price of Liquefied U.S. Natural Gas Exports to Brazil (Dollars per Thousand Cubic Feet)" "Sourcekey","NGMEPG0PNGNUS-NBRDMCF"...

340

Workbook Contents  

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

2:08:07 PM" "Back to Contents","Data 1: Price of Liquefied U.S. Natural Gas Exports to Brazil (Dollars per Thousand Cubic Feet)" "Sourcekey","NGMEPG0PNGNUS-NBRDMCF"...

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

132014 2:06:54 PM" "Back to Contents","Data 1: Liquefied U.S. Natural Gas Exports to Brazil (MMcf)" "Sourcekey","NGMEPG0ENGNUS-NBRMMCF" "Date","Liquefied U.S. Natural Gas...

342

Workbook Contents  

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

312013 3:21:41 PM" "Back to Contents","Data 1: Natural Gas Gross Withdrawals from Shale Gas Wells (Summary) " "Sourcekey","NGMEPG0FGSNUSMMCF","NGMEPG0FGSR3FMMMCF","NG...

343

Workbook Contents  

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

312013 3:21:40 PM" "Back to Contents","Data 1: Natural Gas Gross Withdrawals from Shale Gas Wells (Summary) " "Sourcekey","NGMEPG0FGSNUSMMCF","NGMEPG0FGSR3FMMMCF","NG...

344

Workbook Contents  

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

4:58:30 PM" "Back to Contents","Data 1: Liquefied U.S. Natural Gas Exports to South Korea (MMcf)" "Sourcekey","NGMEPG0ENGNUS-NKSMMCF" "Date","Liquefied U.S. Natural Gas...

345

Workbook Contents  

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

2:08:11 PM" "Back to Contents","Data 1: Alaska Liquefied Natural Gas Exports Price to China (Dollars per Thousand Cubic Feet)" "Sourcekey","NGMEPG0PNGSAK-NCHDMCF"...

346

Workbook Contents  

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

2:08:07 PM" "Back to Contents","Data 1: Price of Liquefied U.S. Natural Gas Exports to China (Dollars per Thousand Cubic Feet)" "Sourcekey","NGMEPG0PNGNUS-NCHDMCF"...

347

Workbook Contents  

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

132014 2:06:55 PM" "Back to Contents","Data 1: Liquefied U.S. Natural Gas Exports to China (MMcf)" "Sourcekey","NGMEPG0ENGNUS-NCHMMCF" "Date","Liquefied U.S. Natural Gas...

348

Workbook Contents  

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

2:08:12 PM" "Back to Contents","Data 1: Alaska Liquefied Natural Gas Exports Price to China (Dollars per Thousand Cubic Feet)" "Sourcekey","NGMEPG0PNGSAK-NCHDMCF"...

349

Workbook Contents  

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

,,"(202) 586-8800",,,"11252013 9:01:19 AM" "Back to Contents","Data 1: Total Crude Oil and Products Imports from All Countries" "Sourcekey","MTTIPP11","MTTIPP21","MTTIPP31",...

350

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 5:41:31 AM" "Back to Contents","Data 1:...

351

Workbook Contents  

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

,"Source:","Energy Information Administration" ,"For Help, Contact:","infoctr@eia.doe.gov" ,,"(202) 586-8800",,,"9302013 6:13:51 AM" "Back to Contents","Data 1:...

352

Workbook Contents  

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

,,"(202) 586-8800",,,"172014 2:58:22 PM" "Back to Contents","Data 1: Federal Offshore--Gulf of Mexico Natural Gas Gross Withdrawals (MMcf)" "Sourcekey","N9010FX2"...

353

Workbook Contents  

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

AM" "Back to Contents","Data 1: Percent of Commercial Natural Gas Deliveries in Pennsylvania Represented by the Price (%)" "Sourcekey","N3020PA4" "Date","Percent of Commercial...

354

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 9:13:15 AM" "Back to Contents","Data 1: Pennsylvania Price of Natural Gas Delivered to Residential Consumers (Dollars per Thousand Cubic Feet)"...

355

Workbook Contents  

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

,,"(202) 586-8800",,,"9302013 9:14:13 AM" "Back to Contents","Data 1: Pennsylvania Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"...

356

Workbook Contents  

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

586-8800",,,"9302013 9:16:27 AM" "Back to Contents","Data 1: Natural Gas Citygate Price in Pennsylvania (Dollars per Thousand Cubic Feet)" "Sourcekey","N3050PA3"...

357

Workbook Contents  

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

586-8800",,,"9302013 9:16:28 AM" "Back to Contents","Data 1: Natural Gas Citygate Price in Pennsylvania (Dollars per Thousand Cubic Feet)" "Sourcekey","N3050PA3"...

358

Workbook Contents  

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

,,"(202) 586-8800",,,"172014 2:49:36 PM" "Back to Contents","Data 1: Idaho Price of Natural Gas Sold to Commercial Consumers (Dollars per Thousand Cubic Feet)"...

359

Workbook Contents  

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

,,"(202) 586-8800",,,"172014 2:48:16 PM" "Back to Contents","Data 1: Idaho Natural Gas Residential Consumption (MMcf)" "Sourcekey","N3010ID2" "Date","Idaho...

360

Workbook Contents  

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

72014 2:54:14 PM" "Back to Contents","Data 1: Natural Gas Citygate Price in Idaho (Dollars per Thousand Cubic Feet)" "Sourcekey","N3050ID3" "Date","Natural Gas Citygate...

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

72014 2:54:52 PM" "Back to Contents","Data 1: Natural Gas Delivered to Consumers in Idaho (Including Vehicle Fuel) (MMcf)" "Sourcekey","N3060ID2" "Date","Natural Gas Delivered...

362

Workbook Contents  

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

,,"(202) 586-8800",,,"172014 2:53:12 PM" "Back to Contents","Data 1: Idaho Natural Gas Deliveries to Electric Power Consumers (MMcf)" "Sourcekey","N3045ID2"...

363

Workbook Contents  

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

72014 2:54:13 PM" "Back to Contents","Data 1: Natural Gas Citygate Price in Idaho (Dollars per Thousand Cubic Feet)" "Sourcekey","N3050ID3" "Date","Natural Gas Citygate...

364

Workbook Contents  

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

2:49:37 PM" "Back to Contents","Data 1: Percent of Commercial Natural Gas Deliveries in Idaho Represented by the Price (%)" "Sourcekey","N3020ID4" "Date","Percent of Commercial...

365

Workbook Contents  

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

,,"(202) 586-8800",,,"172014 2:51:34 PM" "Back to Contents","Data 1: Idaho Natural Gas Industrial Consumption (MMcf)" "Sourcekey","N3035ID2" "Date","Idaho...

366

Workbook Contents  

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

72014 2:54:53 PM" "Back to Contents","Data 1: Natural Gas Delivered to Consumers in Idaho (Including Vehicle Fuel) (MMcf)" "Sourcekey","N3060ID2" "Date","Natural Gas Delivered...

367

A TOUGH2 equation-of-state module for the simulation of two-phase flow of air, water, and a miscible gelling liquid  

SciTech Connect

The injection of grout into the subsurface can be used to encapsulate contaminated regions of an aquifer, or to form underground barriers for the isolation of contaminant sources and to prevent the spreading of existing plumes. This requires identifying grouts, or barrier fluids, which when injected into the subsurface exhibit a large increase in viscosity and eventually solidify, sealing the permeable zones in the aquifer. Simulation and modeling analysis are indispensable tools for designing the injection and predicting the performance of the barrier. In order to model flow and transport in such systems, the thermophysical properties of the fluid mixtures have to be provided, and the governing mass- and energy-balance equations for multiphase flow in porous media have to be solved numerically. The equation-of-state module EOS11 described herein is an extension of the EOS7 module of the TOUGH2 code for flow of saline water and air. In the modeling approach, the chemical grout is treated as a miscible fluid the viscosity of which is a function of time and concentration of the gelling agent in the pore water. If a certain high viscosity is reached and the movement of the grout plume ceases, the gel is assumed to solidify, leading to a new porous medium with changed soil characteristics, i.e. reduced porosity and permeability, increased capillary strength for a given water content, and changed initial saturation distribution.

Finsterle, S.; Moridis, G.J.; Pruess, K. [Lawrence Berkeley Lab., CA (United States). Earth Sciences Div.

1994-05-01T23:59:59.000Z

368

Isotope and Temperature Effects in Liquid Water Probed by X-RayAbsorption and Resonant X-Ray Emission Spectroscopy  

DOE Green Energy (OSTI)

High-resolution x-ray absorption and emission spectra ofliquid water exhibit a strong isotope effect. Further, the emissionspectra show a splitting of the 1b1 emission line, a weak temperatureeffect, and a pronounced excitation-energy dependence. They can bedescribed as a superposition of two independent contributions. Bycomparing with gasphase, ice, and NaOH/NaOD, we propose that the twocomponents are governed by the initial state hydrogen bondingconfiguration and ultrafast dissociation on the time scale of the O 1score hole decay.

Fuchs, O.; Zharnikov, M.; Weinhardt, L.; Blum, M.; Weigand, M.; Zubavichus, Y.; Bar, M.; Maier, F.; Denlinger, J.D.; Heske, C.; Grunze,M.; Umbach, E.

2007-03-10T23:59:59.000Z

369

Indirect thermal liquefaction process for producing liquid fuels from biomass  

DOE Green Energy (OSTI)

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

370

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"

371

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

372

Estimating Seasonal Changes in Volumetric Soil Water Content at Landscape Scales in a Savanna Ecosystem Using Two-Dimensional Resistivity Profiling  

Science Conference Proceedings (OSTI)

Water distributed in deep soil reservoirs is an important factor determining the ecosystem structure of water-limited environments, such as the seasonal tropical savannas of South America. In this study a two-dimensional (2D) geoelectrical ...

Diana C. Garcia-Montiel; Michael T. Coe; Meyr P. Cruz; Joice N. Ferreira; Euzebio M. da Silva; Eric A. Davidson

2008-03-01T23:59:59.000Z

373

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

374

POLICY CONTENT  

E-Print Network (OSTI)

March 31, 1999. It lists in alphabetical order the National Customs Rulings (NCR) that were made since the Memorandum was published. 2. Appendix B – Supplement 1 is a supplement to Appendix B of Memorandum D11-11-2. It presents the policy content of the more recent NCRs, which are listed by numerical order of tariff items for greater ease of reference.

Um D; National Customs Rulings (ncrs

1999-01-01T23:59:59.000Z

375

Workbook Contents  

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

586-8800",,,"12122013 6:56:58 PM" "Back to Contents","Data 1: U.S. Liquefied Natural Gas Imports by Point of Entry " "Sourcekey","N9103US2","NGAEPG0IMLYCAM-Z00MMCF","NAEP...

376

INEEL Liquid Effluent Inventory  

Science Conference Proceedings (OSTI)

The INEEL contractors and their associated facilities are required to identify all liquid effluent discharges that may impact the environment at the INEEL. This liquid effluent information is then placed in the Liquid Effluent Inventory (LEI) database, which is maintained by the INEEL prime contractor. The purpose of the LEI is to identify and maintain a current listing of all liquid effluent discharge points and to identify which discharges are subject to federal, state, or local permitting or reporting requirements and DOE order requirements. Initial characterization, which represents most of the INEEL liquid effluents, has been performed, and additional characterization may be required in the future to meet regulations. LEI information is made available to persons responsible for or concerned with INEEL compliance with liquid effluent permitting or reporting requirements, such as the National Pollutant Discharge Elimination System, Wastewater Land Application, Storm Water Pollution Prevention, Spill Prevention Control and Countermeasures, and Industrial Wastewater Pretreatment. The State of Idaho Environmental Oversight and Monitoring Program also needs the information for tracking liquid effluent discharges at the INEEL. The information provides a baseline from which future liquid discharges can be identified, characterized, and regulated, if appropriate. The review covered new and removed buildings/structures, buildings/structures which most likely had new, relocated, or removed LEI discharge points, and at least 10% of the remaining discharge points.

Major, C.A.

1997-06-01T23:59:59.000Z

377

An Educational Resource Based on Water and Health as a Teaching Aid in French Primary Schools Part I: Identification of Needs and Content  

E-Print Network (OSTI)

Abstract: It is a commonplace that water is essential for life, but to what extent is the general public, and children in particular, aware of how water affects health? The aim of this review was to consider the relationship between water and health under three main headings: the importance of hydration for children, dietary intake of water, and water as an essential factor in hygiene contributing to good health. The literature was reviewed to provide a rationale for the implementation of teaching about water and health in French primary schools under three main areas: (i) the importance of hydration for school children and water promotion in primary schools; (ii) the problem of overweight/obesity and the need to adopt healthy drinking habits as defined in French nutritional policy; (iii) the survey of the quality of drinking water in France and its relationship with good hygiene practices. There are currently few educational resources in France on water and health that teachers can use in the classroom. This review gives reasons why a “Water and Health ” learning resource is a useful tool and shows how it can be developed within the constraints imposed by the school syllabus and in accordance with French nutritional and environmental policy. Educ. Sci. 2013, 3 301

Chantal Savanovitch; Marie-pierre Sauvant-rochat

2013-01-01T23:59:59.000Z

378

Enantioselective Liquid-Liquid Extraction Centrifugal Contactor Separators  

E-Print Network (OSTI)

to determine the effective wetted area and local liquid holdup for an air-water contactor containing structured communication errors. 2.3. Air-Water Contactor. The air-water column used for the imaging studies, shown and the other for vapor flow into the contactor. The column base is simply clamped to the turntable. Four

Groningen, Rijksuniversiteit

379

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

380

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"

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,"6/30/1981" 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"

382

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"

383

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"

384

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"

385

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"

386

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"

387

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"

388

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"

389

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"

390

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"

391

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"

392

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"

393

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"

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:","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) "

395

July/August 2012 Table of Contents  

Science Conference Proceedings (OSTI)

July/August 2012 Table of Contents Inform Magazine Inform Archives News July/August 2012 Oilseeds and food, water, and energy security ...

396

Best Practice for Energy Efficient Cleanrooms: Cooling tower and condenser water optimization  

E-Print Network (OSTI)

condenser water optimization Tengfang Xu Contents HVAC WATERHVAC Water Systems Cooling tower and condenser water optimization

Xu, Tengfang

2005-01-01T23:59:59.000Z

397

Emergency Operations Table of Contents  

E-Print Network (OSTI)

Table of Contents..................................................................................................... ii

unknown authors

2012-01-01T23:59:59.000Z

398

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

399

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)"

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:","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

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.


401

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

402

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

403

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

404

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

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:","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)"

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:","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)"

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:","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)"

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:","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)"

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:","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)"

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:","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)"

411

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)"

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:","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

413

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

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:","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)"

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:","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

416

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)"

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:","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)"

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:","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

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:","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

420

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

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:","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

422

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

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:","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

424

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

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:","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 (%)"

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:","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

427

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

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:","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

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:","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

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:","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

431

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

432

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

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:","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

434

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

435

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"

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:","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)"

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:","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

438

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

439

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

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:","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)"

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

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

442

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

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:","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

444

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

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:","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

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:","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

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:","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

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:","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

449

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

450

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"

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:","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) "

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:","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)"

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:","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)"

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:","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)"

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:","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

456

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)"

457

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"

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:","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

459

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)"

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:","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)"

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:","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)"

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:","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

463

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

464

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

465

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

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:","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

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:","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

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:","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

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:","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

470

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)"

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:","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)"

472

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

473

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

474

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

475

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 (%)"

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:","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)"

477

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)"

478

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

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:","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

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:","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

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

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 (%)"

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:","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)"

483

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

484

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)"

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:","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)"

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:","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

487

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

488

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

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:","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)"

490

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

491

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)"

492

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

493

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)"

494

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

495

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)"

496

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

497

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

498

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

499

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

500

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