壁挂式立方体上稀薄气体流动的DSMC模拟

D. Nabapure, R. Murthy
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引用次数: 5

摘要

本文研究了稀薄气体在壁挂式立方体上的流动行为。研究了滑移区和过渡区不同立方体高度(h)为9mm和18mm时的问题。采用直接模拟蒙特卡罗(DSMC)方法对速度场、压力场和温度场进行了数值模拟。雷诺数Re在403 ~ 807之间,克努森数Kn在0.05 ~ 0.103之间。一个典型的冲击波在立方体前面形成。当Kn = 0.05和Kn = 0.103时,涡的再循环长度相对于各自的立方体高度归一化,分别约为1.11和1.95。同样,当Kn = 0.05和Kn = 0.103时,漩涡中心位于上游各自立方体高度的3.33倍和6.11倍左右。在立方体上游观测到的局部温度和压力变化幅度要大两个数量级,这主要归因于强压缩效应。本研究为基准测试铺平了道路,并为理解复杂几何形状上的稀薄气体流动奠定了基础。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
DSMC Simulation of Rarefied Gas Flow Over a Wall Mounted Cube
The present study investigates the flow behavior of the rarefied gas over a wall-mounted cube. The problem is studied for different cube heights (h) of 9mm and 18mm in the slip and transition regimes. The Direct Simulation Monte Carlo (DSMC) method is employed to evaluate the properties such as velocity, pressure and temperature fields. The Reynolds number (Re) ranges from 403 to 807, and the Knudsen number (Kn) is in the range from 0.05 to 0.103. A typical shock wave is formed in front of the cube. The recirculation length of the vortices normalized with respect to the respective cube heights for Kn = 0.05 and Kn = 0.103 are about 1.11 and 1.95 respectively. Similarly, the center of the vortices is located at about 3.33 and 6.11 times the respective cube heights upstream, for Kn = 0.05 and Kn = 0.103. The local temperature and pressure variations observed upstream of the cube are two orders higher in magnitude and are primarily attributed to strong compressibility effects. The present study paves the way for benchmarking, and forms a basis for understanding the rarefied gas flows over complex geometries.
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