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首页> 外文期刊>Journal of Heat Transfer >Direct Numerical Simulation of Turbulent Heat Transfer Across a Mobile, Sheared Gas-Liquid Interface
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Direct Numerical Simulation of Turbulent Heat Transfer Across a Mobile, Sheared Gas-Liquid Interface

机译:流动,剪切气液界面中湍流传热的直接数值模拟

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The impact of interfacial dynamics on turbulent heat transfer at a deformable, sheared gas-liquid interface is studied using Direct Numerical Simulation (DNS). The flow system comprises a gas and a liquid phase flowing in opposite directions. The governing equations for the two fluids are alternately solved in separate domains and then coupled at the interface by imposing continuity of velocity and stress. The deformations of the interface fall in the range of capillary waves of waveslope ak=0.01 (wave amplitude a times wavenumber k), and very small phase speed-to-friction velocity ratio, c/u_*. The influence of low-to-moderate molecular Prandtl numbers (Pr) on the transport in the immediate vicinity of the interface is examined for the gas phase, and results are compared to existing wall-bounded flow data. The shear-based Reynolds number Re_* is 171 and Prandtl numbers of 1, 5, and 10 were studied. The effects induced by changes in Pr in both wall-bounded flow and over a gas-liquid interface were analyzed by comparing the relevant statistical flow properties, including the budgets for the temperature variance and the turbulent heat fluxes. Overall, Pr was found to affect the results in very much the same way as in most of the available wall flow data. The intensity of the averaged normal heat flux at high Prandtl numbers is found to be slightly greater near the interface than at the wall. Similar to what is observed in wall flows, for Pr = 1 the turbulent viscosity and diffusivity are found to asymptote with z~(+3), where z~+ is the distance to the interface, and with z~(+n), where n>3 for Pr=5 and 10. This implies that the gas phase perceives deformable interfaces as impermeable walls for small amplitude waves with wavelengths much larger than the diffusive sublayers. Moreover, high-frequency fluctuating fields are shown to play a minor role in transferring heat across the interface, with a marked filtering effect of Pr. A new scaling law for the normalized heat transfer coefficient, K~+ has been derived with the help of the DNS data. This law, which could be used in the range of Pr = 1 to 10 for similar flow conditions, suggests an approximate Pr~(-3/5) relationship, lying between the Pr~(-1/2) dependence for free surfaces and the Pr~(-2/3) law for immobile interfaces and much higher Prandtl numbers. A close inspection of the transfer rates reveals a strong and consistent relationship between K~+, the frequency of sweeps impacting the interface, the interfacial velocity streaks, and the interfacial shear stress.
机译:使用直接数值模拟(DNS)研究了界面动力学对在可变形的剪切气液界面处湍流传热的影响。该流动系统包括沿相反方向流动的气相和液相。两种流体的控制方程在单独的域中交替求解,然后通过施加速度和应力的连续性在界面处耦合。界面的变形落在毛细波的范围之内,毛细波的波幅为ak = 0.01(波幅a乘以波数k),并且相速度与摩擦速度之比非常小c / u_ *。检查了气相的中低分子普朗特数(Pr)对界面附近传输的影响,并将结果与​​现有的边界流数据进行了比较。基于剪切的雷诺数Re_ *为171,研究了1、5和10的普朗特数。通过比较相关的统计流量特性,包括温度变化和湍流通量的预算,来分析Pr在壁边界流量和气液界面上的变化所引起的影响。总的来说,发现Pr对结果的影响与大多数现有壁流数据几乎相同。发现在高Prandtl数下,平均法向热通量的强度在界面附近比壁处略大。类似于在壁流中观察到的情况,对于Pr = 1,发现湍流粘度和扩散率随z〜(+3)渐近,其中z〜+是到界面的距离,而z〜(+ n),其中,对于Pr = 5和10,n> 3。这意味着对于波长比扩散子层大得多的小振幅波,气相将可变形界面感知为不可渗透的壁。此外,显示出高频波动场在通过界面传热方面起次要作用,Pr的过滤效果显着。借助DNS数据,得出了归一化传热系数K〜+的新缩放定律。对于相似的流动条件,该定律可以在Pr = 1到10的范围内使用,它提出了近似的Pr〜(-3/5)关系,介于自由表面的Pr〜(-1/2)依赖性和固定接口的Pr〜(-2/3)定律和更高的Prandtl数。对传输速率的仔细检查发现,K〜+,冲击界面的扫描频率,界面速度条纹和界面剪切应力之间存在牢固且一致的关系。

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