喷嘴几何形状对高压气体泄漏射流近场流动特性的影响

Xiaopeng Li, Fakun Zhuang, R. Zhou, Yian Wang, Libo Wang, Guoshan Xie
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引用次数: 0

摘要

对同一喷嘴压力比为5.60但不同喷嘴发出的高压射流进行了三维大涡模拟。采用圆形、椭圆形、方形和矩形四种不同的喷嘴几何形状,研究了喷嘴几何形状对近场射流特性的影响。一个高分辨率、六面体和块结构网格包含大约3180万个计算单元。利用基于OpenFOAM c++库开发的可压缩流求解器astroFoam进行仿真。将时间平均的近场激波结构和平均轴向密度与实验数据进行了比较,验证了LES结果的保真性,得到了合理的一致性。结果表明,射流的近场流场结构存在显著差异。特别是,圆形和方形射流对应于三维螺旋失稳模式,而椭圆和矩形射流在其小轴平面上具有二维横向失稳模式。圆形射流和方形射流在马赫盘后存在亚音速流区,而椭圆射流和矩形射流没有亚音速流区。圆形射流中的拦截激波起源于喷嘴出口附近,在横截面上呈圆形。方形射流中的拦截激波首先产生于喷嘴出口的四个角,然后沿喷嘴出口下游一段距离的长轴平面观察到。然而,对于椭圆和矩形射流,在长轴平面上可以观察到拦截激波的形成,而在短轴平面上则没有。此外,基于LES模型计算了不同射流的实际质量流量和流量系数,并探讨了它们之间的差异。
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 Nozzle Geometry on the Near-Field Flow Characteristics of High-Pressure Gas Leak Jets
Three-dimensional large eddy simulations of high-pressure jets at the same nozzle pressure ratio of 5.60 but issuing from different nozzles are conducted. Four different nozzle geometries, i.e., the circular, elliptic, square, and rectangular nozzles, are used to investigate the effect of the nozzle geometry on the near-field jet flow behavior. A high-resolution, hexahedral, and block-structured grid containing about 31.8 million computational cells is applied. The compressible flow solver, astroFoam, which is developed based on the OpenFOAM C++ library, is used to perform the simulations. The time-averaged near-field shock structures and the mean axial density are compared with the experiment data to validate the fidelity of the LES results, and the reasonable agreement is observed. The results indicate that the remarkable differences exist in the near-field flow structures of the jets. In particular, the circular and square jets correspond to a three-dimensional helical instability mode, while the elliptic and rectangular jets have a two-dimensional lateral instability in their minor axis planes. A subsonic flow zone exists after the Mach disk in the circular and square jets, but is lacking in the elliptic and rectangular jets. The intercepting shocks in the circular jet originate near the nozzle exit, and appear to be circular in cross-section. The intercepting shocks in the square jet originate at the four corners of the nozzle exit at first, and then are observed along the major axis plane some distance downstream of the nozzle exit. However, the formation of the intercepting shock is observed in the major axis planes but is lacking in the minor axis planes for the elliptic and rectangular jets. In addition, the real mass flow rates and discharge coefficients for different jets are computed based on the LES modeling, and their differences are explored.
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