高湍流、欠膨胀射流的Reynolds平均Navier-Stokes模拟及高喷射压力下的冲击效应

Jacob Riglin, A. Wachtor, R. Morgan, Ryan Holguin, J. Bernardin
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摘要

从燃油喷射到火箭推进,欠膨胀射流有着广泛的应用。本文建立了一个数值模型,研究了高压缸通过窄管向低压缸排气产生的欠膨胀射流形成的流体力学行为和壁面相互作用。采用ANSYS FLUENT显式耦合压力-速度求解器进行轴对称、Reynolds平均Navier - Stokes模拟,以确定孔板下游壁面处的滞止压力。采用1.0 × 10−8 s和5.0 × 10−9 s的时间步长进行瞬态实验。研究了不同的气体,以氢气为主要工作流体,压力比从10到100不等。本文将主要关注压力比为10,20和70的氢气射流。数值结果得到了实验结果和高保真大涡模拟结果的验证。在压力比为10和70时,射流的马赫盘高度、马赫盘宽度和Prandtl-Meyer膨胀风扇角误差均保持在5%以下。在压力比为10,20和70时,远壁中心的峰值停滞压力分别为86,843 Pa, 127,786 Pa和315,843 Pa。当高压区和低压区初始压力比在10 ~ 70之间时,预测的峰值压力与初始压力比呈线性关系。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Reynolds Averaged Navier-Stokes Simulation of Highly Turbulent, Under-Expanded Jets and Effects of Impingement at Elevated Injection Pressure
Under-expanded jets have wide range of application from fuel injection to rocket propulsion. In the present work, a numerical model was generated to investigate the fluid mechanics behavior of under-expanded jet formation and wall interaction of a jet produced by exhausting a high pressure cylinder through a narrow tube into a low pressure cylinder. Axisymmectic, Reynolds Averaged Navier Stokes simulations were conducted employing the ANSYS FLUENT explicit, Coupled Pressure-Velocity solver to determine the stagnation pressure at the wall downstream of the orifice. Transient cases were conducted using timestep sizes of 1.0 × 10−8 s and 5.0 × 10−9 s. Various gases were investigated with Hydrogen being the primary working fluid with pressure ratios ranging from 10 to 100. This paper will focus primarily on the Hydrogen jets for pressure ratios of 10, 20, and 70. Numerical results were validated from both experimental results and higher fidelity Large Eddy Simulation results specifically analyzing the jet formation. Error between Mach disk height, Mach disk width, and Prandtl-Meyer expansion fan angles of the jet for pressure ratios of 10 and 70 were kept below 5%. The peak stagnation pressures at the center of the far wall for pressure ratios of 10, 20, and 70 were observed to be 86,843 Pa, 127,786 Pa, and 315,843 Pa, respectively. The predicted peak pressures show a linear relationship with respect to the initial pressure ratio existing between the high pressure and low pressure regions when the ratios are bounded between 10 and 70.
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