N-S/DSMC coupling method using three-dimensional unstructured mesh for complex interfaces
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摘要:
针对近连续流过渡区多尺度绕流问题,学界发展了N-S(Navier-Stokes)/DSMC(direct simulation Monte Carlo)耦合方法,大多数此类求解器面临着耦合界面波动失稳的难题,因此对复杂外形和耦合界面的通用性值得重点研究。鉴于非结构网格面向复杂外形高度的贴体性、优良适应性以及工程领域对过渡流区高效通用型计算方法的需求,提出并实现了一套三维复杂界面四面体非结构网格N-S/DSMC耦合方法用于模拟高超声速过渡流。该方法使用局部克努森数作为连续失效参数划分连续/稀薄区域,并生成三维复杂N-S/DSMC耦合界面,沿分界面两侧分别推进一层或多层界面信息传递单元,基于边界状态法进行信息耦合。该耦合方法无需对复杂不规则分界面作光滑和修型处理,具备对复杂过渡流区工程问题数值模拟的通用性。分别对三维高超声速圆球和钝锥绕流进行模拟,数值结果显示:与参考文献中的DSMC方法相比,激波处数值和壁面特征值基本一致,最大误差不超过8%,但计算效率分别提高了1.74倍和2.28倍,验证了该耦合方法的正确性和高效性。
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关键词:
- N-S/DSMC耦合方法 /
- 四面体非结构网格 /
- 高超声速流 /
- 过渡流区 /
- 复杂界面耦合方法
Abstract:In view of the highly conformable and adaptive nature of unstructured mesh to complex geometries and the demand in engineering for efficient and versatile computational methods, a new implementation of the N-S (Navier-Stokes)/DSMC (direct simulation Monte Carlo) coupling method using tetrahedral unstructured mesh for complex interfaces was presented with the aim of resolving the fluctuations in the positioning of the coupling interfaces in most N-S/DSMC coupling method for multi-scale transitional flows in the near-continuum regime. This implementation utilized local Knudsen number as a continuum breakdown parameter to partition the continuum/rarefied regions and generate three-dimensional complex N-S/DSMC coupling interfaces. Along each side of the interface, one or multiple layers of interface information transfer meshes were advanced, and information coupling was achieved by the state-based approach. According to this method, there was no need for smoothing or reshaping treatments applied to complex irregular interfaces, with the general applicability to numerical simulations of complex transitional flow regions. Simulations of three-dimensional hypersonic flow around a sphere and a blunt cone showed that, compared with the DSMC method, the shock wave and wall characteristics were in close agreement, with a maximum error of less than 8%. At the same time, computational efficiency was improved by 1.74 and 2.28 times, respectively, validating the method’s accuracy and efficiency.
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表 1 两种方法总计算耗时
Table 1. Time consumption of the two methods
h 方法 圆球耗时 钝锥耗时 耦合算法 41.23 27.3 DSMC 71.55 62.12 -
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