晶格玻尔兹曼模拟现实边界条件对填充相变材料的新型圆柱形外壳体积辐射-传导熔化的影响

Energy Storage Pub Date : 2024-05-15 DOI:10.1002/est2.629
Saeideh Zameni-Ghalati, Reza Mehryar, Gholamreza Imani
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引用次数: 0

摘要

本研究提出了一种新型太阳能潜热蓄热(LHTES)系统,包括填充相变材料(PCM)的圆柱形外壳,该系统可安装在建筑窗户上,以缓解传统填充 PCM 的双层玻璃窗的缺点,如日光阻碍和渗漏。与现有文献相比,本文采用晶格玻尔兹曼法(LBM)模拟了 PCM 在拟议的 LHTES 系统单圆柱体内的体积辐射-传导熔化过程,并考虑了对流边界条件、阴影效应和可变太阳辐射角等更现实的条件。因此,对多个边界条件进行了评估,并研究了圆筒直径、消光系数、散射反照率、太阳角度、阴影效应和自然对流传热系数等参数对熔化率和充电时间的影响。结果表明,对环境对流热损失和阴影等应用条件的考虑会显著影响系统的充电时间。结果表明,在对流边界条件下,h = 4 $$ h=4 $$ 、8 $$ 8 $$ 和 12 W m - 2 K - 1 $$ 12 \mathrm{W}\ {\mathrm{m}}^{-2}\ {\mathrm{K}}^{-1} $$ 的充电时间相对于无阴影效应的绝缘边界条件情况分别增加了 11%、30% 和 50%,相对于有 90° 阴影的绝缘情况分别增加了 38%、91% 和 175%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Lattice Boltzmann simulation of effects of realistic boundary conditions on volumetric radiation-conduction melting of a novel cylindrical enclosure filled with phase change materials

In this research, a novel solar latent heat thermal energy storage (LHTES) system, including the cylindrical enclosures filled with a phase change material (PCM), is proposed, which can be installed on the building windows to alleviate the drawbacks of traditional PCM-filled double-glazed windows, such as daylight hindrance and leakage. The lattice Boltzmann method (LBM) is used to simulate the volumetric radiation-conduction melting of the PCM within a single cylinder of the proposed LHTES system with considering more realistic conditions such as convective boundary condition, shadow effect, and variable solar radiation angle compared with the available works in the literature. As such, several boundary conditions are assessed, and parameters such as cylinder diameter, extinction coefficient, scattering albedo, solar angle, shadow effect, and natural convection heat transfer coefficient are studied on the time history of the melting fraction and charging time. The results revealed that considering the applied conditions, such as convection heat loss to the environment and shadow, significantly affects the charging time of the system. It is shown that the charging time for convective boundary condition with h = 4 $$ h=4 $$ , 8 $$ 8 $$ , and 12 W m 2 K 1 $$ 12\ \mathrm{W}\ {\mathrm{m}}^{-2}\ {\mathrm{K}}^{-1} $$ increases, respectively, by 11%, 30%, and 50% relative to a case with the insulated boundary condition without the shadow effect and 38%, 91%, and 175% compared with the insulated case with a 90° shadow.

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