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Title: Computational Fluid Dynamics Library

Abstract

CFDLib05 is the Los Alamos Computational Fluid Dynamics LIBrary. This is a collection of hydrocodes using a common data structure and a common numerical method, for problems ranging from single-field, incompressible flow, to multi-species, multi-field, compressible flow. The data structure is multi-block, with a so-called structured grid in each block. The numerical method is a Finite-Volume scheme employing a state vector that is fully cell-centered. This means that the integral form of the conservation laws is solved on the physical domain that is represented by a mesh of control volumes. The typical control volume is an arbitrary quadrilateral in 2D and an arbitrary hexahedron in 3D. The Finite-Volume scheme is for time-unsteady flow and remains well coupled by means of time and space centered fluxes; if a steady state solution is required, the problem is integrated forward in time until the user is satisfied that the state is stationary.

Authors:
; ; ;
Publication Date:
Research Org.:
Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)
Sponsoring Org.:
DOE/DP; USDOD
OSTI Identifier:
1230634
Report Number(s):
CFDLib05; 000663SUN0002
DOE Contract Number:  
W-7405-ENG-36
Resource Type:
Software
Software Revision:
02
Software Package Number:
000663
Software Package Contents:
Software Abstract; Program note for CFDLib05; LA-UR-93-3922; Media Includes Media Directory, Source Code, Auxiliary Material; Compilation Instructions, Linking Instructions; Object Module; Sample Problem Input and Output;\ 1 CD ROM
Software CPU:
SUN00
Open Source:
No
Source Code Available:
Yes
Other Software Info:
The following codes are included in this package: CAVEAT and, compressible, single-velocity, explicit Godunov hydro, van Leer advection, mixed-cell interface tracking, numerous physics packages (HE burn, compressible turbulence transport, etc.). CCMAC, incompressible, single-fluid, ALE, semi-implicit, TVD hydro. CCICE, compressible, single-fluid, ALE semi-implicit, TVD hydro. MSMAC, incompressible, multi-species, ALE, semi-implicit, TVD hydro. MSICE, compressible, multi-species, ALE, implicit, TVD hydro, optional N-species, M-reaction, gas-phase finite-rate chemical kinetics. MFMAC, incompressible, multiphase, ALE, semi-implicit, TVD hydro. MFICE, compressible, multiphase, ALE semi-implicit, TVD hydro. MFMHD, compressible, multifluid, magnetohydrodynamic, semi-implicit, TVD hydro, Lagrangean or Eulerian, N-species, M-reaction gas-phase chemical kinetics, global remapping. CFDSET, general interactive mesh generator.
Country of Publication:
United States

Citation Formats

Kashiwa, B. A., Padial, N. T., Rauenzahn, R. M., and VanderHeyden, & W.B. Computational Fluid Dynamics Library. Computer software. Vers. 02. DOE/DP; USDOD. 4 Mar. 2005. Web.
Kashiwa, B. A., Padial, N. T., Rauenzahn, R. M., & VanderHeyden, & W.B. (2005, March 4). Computational Fluid Dynamics Library (Version 02) [Computer software].
Kashiwa, B. A., Padial, N. T., Rauenzahn, R. M., and VanderHeyden, & W.B. Computational Fluid Dynamics Library. Computer software. Version 02. March 4, 2005.
@misc{osti_1230634,
title = {Computational Fluid Dynamics Library, Version 02},
author = {Kashiwa, B. A. and Padial, N. T. and Rauenzahn, R. M. and VanderHeyden, & W.B.},
abstractNote = {CFDLib05 is the Los Alamos Computational Fluid Dynamics LIBrary. This is a collection of hydrocodes using a common data structure and a common numerical method, for problems ranging from single-field, incompressible flow, to multi-species, multi-field, compressible flow. The data structure is multi-block, with a so-called structured grid in each block. The numerical method is a Finite-Volume scheme employing a state vector that is fully cell-centered. This means that the integral form of the conservation laws is solved on the physical domain that is represented by a mesh of control volumes. The typical control volume is an arbitrary quadrilateral in 2D and an arbitrary hexahedron in 3D. The Finite-Volume scheme is for time-unsteady flow and remains well coupled by means of time and space centered fluxes; if a steady state solution is required, the problem is integrated forward in time until the user is satisfied that the state is stationary.},
doi = {},
url = {https://www.osti.gov/biblio/1230634}, year = {Fri Mar 04 00:00:00 EST 2005},
month = {Fri Mar 04 00:00:00 EST 2005},
note =
}

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