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Spanwise Heat Transport in Turbulent Channel Flow With Prandtl Numbers Ranging From 0.025 to 5.0

机译:Prandtl数在0.025到5.0之间的湍流通道中的横向传热

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摘要

The near-wall turbulent heat transport of the three orthogonal directions was directly solved for the Prandtl numbers ranging from 0.025 to 5.0 to validate the algebraic models of the turbulent heat flux. Two kinds of thermal situations were considered in the low Reynolds number turbulent flow: (a) the case with a uniform heat flux in the spanwise direction (UHF) and (b) the case with the mean spanwise temperature gradient (STG). Among the turbulent heat flux models tested, the model of Rogers preferably predicted over the treated range of the Prandtl numbers, but it failed to reproduce the low Prandtl number effects very accurately. This paper revealed that the coefficient of the Rotta model can be modified to include the low Prandtl number effects by means of the correlation between the exact coefficient suggested by DNS and the Prandtl number.
机译:直接求解三个正交方向的近壁湍流传热,其Prandtl数范围为0.025至5.0,以验证湍流通量的代数模型。在低雷诺数湍流中考虑了两种热态:(a)在翼展方向(UHF)上具有均匀热通量的情况,以及(b)在翼展方向上具有平均温度梯度(STG)的情况。在测试的湍流通量模型中,Rogers模型最好在已处理的Prandtl数范围内进行预测,但未能非常准确地再现低Prandtl数效应。本文揭示了可以通过DNS建议的精确系数与Prandtl数之间的相关性,将Rotta模型的系数修改为包括低Prandtl数效应。

著录项

  • 来源
    《Journal of Heat Transfer》 |2012年第4期|p.51-58|共8页
  • 作者单位

    Department of Mechanical and Production Engineering, Niigata University, Ikarashi 2-nocho 8050, Niigata 950-2181, Japan;

    Department of Mechanical and Production Engineering, Niigata University, Ikarashi 2-nocho 8050, Niigata 950-2181, Japan;

    Graduate School of Science and Technology, Niigata University, Ikarashi 2-nocho 8050, Niigata 950-2181, Japan;

    Graduate School of Science and Technology, Niigata University, Ikarashi 2-nocho 8050, Niigata 950-2181, Japan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    turbulent heat transfer; prandtl number; turbulent heat flux model; direct numerical simulation;

    机译:湍流传热普朗特号码湍流通量模型直接数值模拟;
  • 入库时间 2022-08-18 00:25:13

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