加热条件对棱镜腔内共轭自然对流熵产的影响

A. Hasan, Md. Jahid Hasan Sagor, S. Barua, S. Saha
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引用次数: 6

摘要

本文研究了厚底壁柱状壳体内的共轭自然对流换热问题。箱体内充满空气,实心底壁由松木制成,有限厚度t = 0.10L,其中L为箱体底壁长度。三种不同的情况下,如等温,线性和正弦变化的加热条件应用在外壳的底部,以检查热性能和熵的产生在外壳内。采用有限元法求解了控制Navier-Stokes方程和能量方程。在瑞利数103≤Ra≤107范围内进行了参数化模拟,并通过流线图、等温线图和熵等高线图实现了流场和热场的可视化。为了评估上述三种加热条件的影响,还考察了壳体内平均流体温度、厚底壁顶部平均努塞尔数和总熵产的变化。本文研究了厚底壁柱状壳体内的共轭自然对流换热问题。箱体内充满空气,实心底壁由松木制成,有限厚度t = 0.10L,其中L为箱体底壁长度。三种不同的情况下,如等温,线性和正弦变化的加热条件应用在外壳的底部,以检查热性能和熵的产生在外壳内。采用有限元法求解了控制Navier-Stokes方程和能量方程。在瑞利数103≤Ra≤107范围内进行了参数化模拟,并通过流线图、等温线图和熵等高线图实现了流场和热场的可视化。本文还研究了壳体内平均流体温度、厚底壁顶部平均努塞尔数和总熵产的变化规律。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effect of heating condition on entropy generation of conjugate natural convection in a prismatic enclosure
Conjugate natural convection heat transfer inside a prismatic enclosure with thick solid bottom wall has been investigated in the present study. The enclosure is filled with air and the solid bottom wall, made of pine wood, has finite thickness of t = 0.10L, where L is the length of the bottom wall of the enclosure. Three different cases such as isothermal, linear and sinusoidally varying heating conditions are applied at the bottom of the enclosure to examine the thermal performance and entropy generation inside the enclosure. The governing Navier-Stokes and energy equations are solved using finite element method. Parametric simulation is carried out for a range of Rayleigh number, 103 ≤ Ra ≤ 107 and the visualization of flow and thermal fields is presented through streamline, isotherm and entropy contour plots. The variations of average fluid temperature inside the enclosure, the average Nusselt number along the top of the thick bottom wall and the total entropy generation are also examined in order to assess the influence of the above three heating conditions.Conjugate natural convection heat transfer inside a prismatic enclosure with thick solid bottom wall has been investigated in the present study. The enclosure is filled with air and the solid bottom wall, made of pine wood, has finite thickness of t = 0.10L, where L is the length of the bottom wall of the enclosure. Three different cases such as isothermal, linear and sinusoidally varying heating conditions are applied at the bottom of the enclosure to examine the thermal performance and entropy generation inside the enclosure. The governing Navier-Stokes and energy equations are solved using finite element method. Parametric simulation is carried out for a range of Rayleigh number, 103 ≤ Ra ≤ 107 and the visualization of flow and thermal fields is presented through streamline, isotherm and entropy contour plots. The variations of average fluid temperature inside the enclosure, the average Nusselt number along the top of the thick bottom wall and the total entropy generation are also examined in order to ...
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