Wray-Agarwal(WA) Turbulence Model
From CFD-Wiki
(Difference between revisions)
(→WA Model) |
(→References) |
||
Line 104: | Line 104: | ||
==References== | ==References== | ||
- | *{{reference-paper|author=X. Han, T. J. Wray, and R. K. Agarwal | + | *{{reference-paper|author=X. Han, T. J. Wray, and R. K. Agarwal|year=2017|title=Application of a New DES Model Based on Wray-Agarwal Turbulence Model for Simulation of Wall-Bounded Flows with Separation|rest= AIAA Paper 2017-3966, June 2017}} |
[[Category:Turbulence models]] | [[Category:Turbulence models]] |
Revision as of 21:22, 22 January 2021
Contents |
Introduction
The Wray-Agarwal (WA 2017m) model is a one-equation linear eddy viscosity model that was derived from two-equation closure. It combines the most desirable characteristics of the one-equation model and one-equation model, analogous to the SST model which combines best features of two-equation and models.
WA Model (WA 2017m)
The turbulent eddy viscosity is given by:
The model solves for the variable using the following equation:
Where:
and d is the minimum distance to the nearest wall.
The model constants are:
Boundary Conditions
Solid smooth wall:
Freestream:
References
- X. Han, T. J. Wray, and R. K. Agarwal (2017), "Application of a New DES Model Based on Wray-Agarwal Turbulence Model for Simulation of Wall-Bounded Flows with Separation", AIAA Paper 2017-3966, June 2017.