Heat Transfer, Volume 6 2002
DOI: 10.1115/imece2002-33098
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A Multi-Mechanics Approach to Computational Heat Transfer

Abstract: We present a turbulent combustion code for modeling heat transfer in fires that arise in accident scenarios. The code is a component of a multi-mechanics framework and is based on a domain-decomposition, message-passing approach to parallel computing. The turbulent combustion code is based on a vertex-centered, finite-volume scheme for 3D unstructured meshes. The multi-mechanics nature of the frameworks allows us to couple to a conduction heat transfer code for conjugate heat transfer problems or a participati… Show more

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Cited by 25 publications
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“…The soot radiation flux is a key threat to the safety and security of personnel and infrastructure and is a dominant concern for risk assessment and analysis. New computational models are currently being developed for the Advanced Simulation and Computing (ASC) code FUEGO [2][3][4] at Sandia National…”
Section: Introductionmentioning
confidence: 99%
“…The soot radiation flux is a key threat to the safety and security of personnel and infrastructure and is a dominant concern for risk assessment and analysis. New computational models are currently being developed for the Advanced Simulation and Computing (ASC) code FUEGO [2][3][4] at Sandia National…”
Section: Introductionmentioning
confidence: 99%
“…The computational domain was discretized into 6x10 5 elements with nonuniform size (finer mesh at end of tube, z=0). The boundary condition for the jet exit was a uniform velocity of 2.96x10 4 cm/s at the end of the tube. The outer boundaries of the rectangular domain were defined as open boundaries with a constant pressure boundary condition.…”
Section: Incompressible Turbulent H 2 -Air Jet Flamementioning
confidence: 99%
“…A constant pressure boundary condition was applied around the circumference and at the open end of the cylinder. Results were computed on two hexagonal element meshes (5.9x10 4 and 4.8x10 5 elements where the refined mesh is obtained by dividing each coarse mesh element into 8 smaller elements) that expanded in both the axial and radial directions from the jet. Results were obtained for the standard k-ε and RNG k-ε turbulence models and for two convection operators, the 1st order upwind scheme and MUSCL scheme [4].…”
Section: Unignited Incompressible Turbulent Air Jetmentioning
confidence: 99%
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