TWO-EQUATION MODEL FOR HEAT TRANSPORT IN WALL TURBULENT SHEAR FLOWS.
被引:0
作者:
Nagano, Y.
论文数: 0引用数: 0
h-index: 0
机构:
Nagoya Inst of Technology, Nagoya, Japan, Nagoya Inst of Technology, Nagoya, JapanNagoya Inst of Technology, Nagoya, Japan, Nagoya Inst of Technology, Nagoya, Japan
Nagano, Y.
[1
]
Kim, C.
论文数: 0引用数: 0
h-index: 0
机构:
Nagoya Inst of Technology, Nagoya, Japan, Nagoya Inst of Technology, Nagoya, JapanNagoya Inst of Technology, Nagoya, Japan, Nagoya Inst of Technology, Nagoya, Japan
Kim, C.
[1
]
机构:
[1] Nagoya Inst of Technology, Nagoya, Japan, Nagoya Inst of Technology, Nagoya, Japan
来源:
Journal of Heat Transfer
|
1988年
/
110卷
/
03期
关键词:
FLOW OF FLUIDS - Turbulent - TEMPERATURE DISTRIBUTION;
D O I:
暂无
中图分类号:
学科分类号:
摘要:
A new proposal for closing the energy equation is presented at the two-equation level of turbulence modeling. The eddy diffusivity concept is used in modeling. However, just as the eddy viscosity is determined from solutions of the k and epsilon equations, so the eddy diffusivity for heat is given as functions of temperature variance t OVER BAR **2 and the dissipation rate of temperature fluctuations epsilon //t, together with k and epsilon . Thus, the proposed model does not require any questionable assumptions for the 'turbulent Prandtl number. ' Modeled forms of the t OVER BAR **2 and epsilon //t equations are developed to account for the physical effects of molecular Prandtl number and near-wall turbulence. The model is tested by application to a flat-plate boundary layer, the thermal entrance region of a pipe, and the turbulent heat transfer in fluids over a wide range of the Prandtl number.