A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic Cases

In our work in 2008, we evaluated the aptitude of the code Neptune_CFD to reproduce the incidence of a structure topped by vanes on a boiling layer, within the framework of the Neptune project. The objective was to reproduce the main effects of the spacer grids. The turbulence of the liquid phase wa...

Full description

Bibliographic Details
Main Authors: S. Mimouni, F. Archambeau, M. Boucker, J. Laviéville, C. Morel
Format: Article
Language:English
Published: Hindawi Limited 2009-01-01
Series:Science and Technology of Nuclear Installations
Online Access:http://dx.doi.org/10.1155/2009/792395
id doaj-26d214a517464d89be012463913ee4df
record_format Article
spelling doaj-26d214a517464d89be012463913ee4df2020-11-24T22:21:02ZengHindawi LimitedScience and Technology of Nuclear Installations1687-60751687-60832009-01-01200910.1155/2009/792395792395A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic CasesS. Mimouni0F. Archambeau1M. Boucker2J. Laviéville3C. Morel4Electricité de France R&D Division, 6 Quai Watier, 78400 Chatou, FranceElectricité de France R&D Division, 6 Quai Watier, 78400 Chatou, FranceElectricité de France R&D Division, 6 Quai Watier, 78400 Chatou, FranceElectricité de France R&D Division, 6 Quai Watier, 78400 Chatou, FranceCommissariat à l'Energie Atomique, 17 rue des Martyrs, 38000 Grenoble, FranceIn our work in 2008, we evaluated the aptitude of the code Neptune_CFD to reproduce the incidence of a structure topped by vanes on a boiling layer, within the framework of the Neptune project. The objective was to reproduce the main effects of the spacer grids. The turbulence of the liquid phase was modeled by a first-order K-ε model. We show in this paper that this model is unable to describe the turbulence of rotating flows, in accordance with the theory. The objective of this paper is to improve the turbulence modeling of the liquid phase by a second turbulence model based on a Rij-ε approach. Results obtained on typical single-phase cases highlight the improvement of the prediction for all computed values. We tested the turbulence model Rij-ε implemented in the code versus typical adiabatic two-phase flow experiments. We check that the simulations with the Reynolds stress transport model (RSTM) give satisfactory results in a simple geometry as compared to a K-ε model: this point is crucial before calculating rod bundle geometries where the K-ε model may fail.http://dx.doi.org/10.1155/2009/792395
collection DOAJ
language English
format Article
sources DOAJ
author S. Mimouni
F. Archambeau
M. Boucker
J. Laviéville
C. Morel
spellingShingle S. Mimouni
F. Archambeau
M. Boucker
J. Laviéville
C. Morel
A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic Cases
Science and Technology of Nuclear Installations
author_facet S. Mimouni
F. Archambeau
M. Boucker
J. Laviéville
C. Morel
author_sort S. Mimouni
title A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic Cases
title_short A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic Cases
title_full A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic Cases
title_fullStr A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic Cases
title_full_unstemmed A Second-Order Turbulence Model Based on a Reynolds Stress Approach for Two-Phase Flow—Part I: Adiabatic Cases
title_sort second-order turbulence model based on a reynolds stress approach for two-phase flow—part i: adiabatic cases
publisher Hindawi Limited
series Science and Technology of Nuclear Installations
issn 1687-6075
1687-6083
publishDate 2009-01-01
description In our work in 2008, we evaluated the aptitude of the code Neptune_CFD to reproduce the incidence of a structure topped by vanes on a boiling layer, within the framework of the Neptune project. The objective was to reproduce the main effects of the spacer grids. The turbulence of the liquid phase was modeled by a first-order K-ε model. We show in this paper that this model is unable to describe the turbulence of rotating flows, in accordance with the theory. The objective of this paper is to improve the turbulence modeling of the liquid phase by a second turbulence model based on a Rij-ε approach. Results obtained on typical single-phase cases highlight the improvement of the prediction for all computed values. We tested the turbulence model Rij-ε implemented in the code versus typical adiabatic two-phase flow experiments. We check that the simulations with the Reynolds stress transport model (RSTM) give satisfactory results in a simple geometry as compared to a K-ε model: this point is crucial before calculating rod bundle geometries where the K-ε model may fail.
url http://dx.doi.org/10.1155/2009/792395
work_keys_str_mv AT smimouni asecondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT farchambeau asecondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT mboucker asecondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT jlavieville asecondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT cmorel asecondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT smimouni secondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT farchambeau secondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT mboucker secondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT jlavieville secondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
AT cmorel secondorderturbulencemodelbasedonareynoldsstressapproachfortwophaseflowpartiadiabaticcases
_version_ 1725772608742359040