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首页> 外文期刊>Journal of Heat Transfer >Investigation of the Wall Scalar Fluctuations Effect on Passive Scalar Turbulent Fields at Several Prandtl Numbers by Means of Direct Numerical Simulations
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Investigation of the Wall Scalar Fluctuations Effect on Passive Scalar Turbulent Fields at Several Prandtl Numbers by Means of Direct Numerical Simulations

机译:直接数值模拟研究壁面标量涨落对被动标量湍流场在几个Prandtl数上的影响

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摘要

We investigate the effect of the wall-scalar fluctuations on passive scalar turbulent fields for a moderate Reynolds number R-s = 395 and for several Prandtl numbers ranging from the very low value P-r = 0.01 to the high value P-r = 10 by means of direct numerical simulation (DNS) simulations. Several cases of plane channel flows are considered. Case I is a channel flow heated on both walls with a constant imposed heat flux q(w). We consider for this case two different types of boundary conditions. For the first one, the isoscalar boundary condition theta(w) = 0 is imposed at the wall implying that its fluctuation and therefore its rms scalar fluctuations theta(rms) = root is not affected by the scalar fluctuations at the wall. But owing to the different boundary conditions applied at the wall, significant differences in the evolution of the rms scalar fluctuations hrms are observed in the immediate vicinity of the wall. Surprisingly, the maximum theta(rms) intensity remains almost unchanged in the near wall region whatever the type of boundary condition is applied at the wall. In addition, the turbulent heat fluxes that play a major role in heat transfer are found to be independent of the wall scalar fluctuations. This study demonstrates that the impact of the wall scalar fluctuations is appreciable mainly in the near wall region. This outcome must be taken into account when simulating industrial flows with thermal boundary conditions involving different fluid/solid combinations.
机译:通过直接数值模拟,我们研究了壁标量波动对被动标量湍流场的影响,其中中等雷诺数Rs = 395以及从极低值Pr = 0.01到较高值Pr = 10的几个Prandtl数(DNS)模拟。考虑了平面通道流动的几种情况。情况一是在两壁上以恒定的施加的热通量q(w)加热的通道流。对于这种情况,我们考虑两种不同类型的边界条件。对于第一个,在壁上施加等量边界条件theta(w)= 0,这意味着壁面的波动以及均方根标量波动theta(rms)=根不受壁上标量波动的影响。但是由于在墙壁上施加的边界条件不同,在墙壁的紧邻区域内观察到rms标量波动hrms的演变存在显着差异。出乎意料的是,无论在壁上施加何种边界条件,最大θ(rms)强度在近壁区域几乎保持不变。此外,发现在热传递中起主要作用的湍流与壁标量波动无关。这项研究表明,壁标量波动的影响主要在壁附近区域是可观的。在模拟涉及不同流体/固体组合的热边界条件的工业流时,必须考虑到这一结果。

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  • 来源
    《Journal of Heat Transfer》 |2019年第12期|122002.1-122002.9|共9页
  • 作者单位

    Univ Paris Saclay Dept Computat Fluid Dynam ONERA F-92322 Chatillon France;

  • 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
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