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Conjugate natural heat transfer scrutiny in differentially heated cavity partitioned with a conducting solid using the lattice Boltzmann method

机译:使用晶格Boltzmann方法用导电固体分隔的差动加热腔中的共轭自然传热扰动

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In the present paper, we numerically investigated the two-dimensional conjugate heat transfer problems in a unitary computational domain containing both the solid and fluid regions. The physical problem configuration consists of two adiabatic horizontal walls of finite thickness and two vertical walls; the left one is maintained at hot temperature T-h and the right one is maintained at cold temperature T-c. The lattice Boltzmann method (LBM) based on the BGK model has been used to simulate laminar natural convection in the partitioned air-filled cavity with a heat-conducting solid. In the interface boundaries of the heat-conducting solid, the continuity of temperature and heat transfer is considered. A series of numerical simulation is carried out over a wide range of the Rayleigh number (Ra=10(3)-10(6)), the thermal conductivity ratio k(r) and the solid partition thickness (delta=1-95c/o) and its horizontal position. The results show that the partition reduces the heat transfer rate in the cavity. For a centered partition (X-s=0.5), the average Nusselt number decreases almost linearly with partition thickness for delta <= 0.45; however, it increases for delta >= 0.45 due to the confinement in the thin fluid regions. For Ra=10(5), the heat transfer rate decreases with the partition position until a critical value close to 0.325 and rises slightly until X-s=0.5. The critical position value decreases with the Ra number increase and it is close to 0.2 for Ra=10(6) where Nu=3.766. The heat transfer rate is enhanced with the increase in thermal conductivity. Correlations of the average Nusselt numbers are obtained as a function of Rayleigh number.
机译:在本文中,我们在数值上研究了包含固体和流体区域的单一计算结构域中的二维共轭传热问题。物理问题配置由有限厚度和两个垂直墙的两个绝热水平墙组成;左侧保持在热温度T-H处,右侧保持在寒温T-C.基于BGK模型的格子Boltzmann方法(LBM)已被用于用热导热固体模拟分隔的充气腔中的层状自然对流。在导热固体的界面边界中,考虑温度和热传递的连续性。在宽范围的瑞利数(Ra = 10(3)-10(6))上进行一系列数值模拟,导热率K(R)和固体隔板厚度(Delta = 1-95c / o)及其水平位置。结果表明,分区降低了腔中的传热速率。对于居中分区(X-S = 0.5),平均衬布数几乎线性地减小,分隔厚度为Delta <= 0.45;然而,由于薄液位区域的限制,它增加了三角洲> = 0.45。对于RA = 10(5),传热速率随分隔位置而减小,直到接近0.325的临界值并且略微上升,直到X-S = 0.5。临界位置值随着RA = 10(6)的RA = 10(6)接近0.2,其中nu = 3.766。随着导热率的增加,传热速率增强。作为瑞利数的函数获得平均露天数的相关性。

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