首页> 外文OA文献 >The structure of strong shock waves using the Fokker-Planck model (Shock wave structure in monatomic gases, using Fokker-Planck model for particle collisions and Mott-Smith distribution for shock front)
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The structure of strong shock waves using the Fokker-Planck model (Shock wave structure in monatomic gases, using Fokker-Planck model for particle collisions and Mott-Smith distribution for shock front)

机译:使用Fokker-Planck模型的强冲击波结构(单原子气体中的冲击波结构,使用Fokker-Planck模型进行粒子碰撞,使用Mott-Smith分布进行激波前沿)

摘要

The structure of strong shock waves in monatomic gases is studied using the Fokker-Planck model to represent the particle collisions and the Mott-Smith distribution to describe the distribution function within the shock front. The differential equation governing the variation of the density within the shock is derived by using the13; variational principle. The thickness of the shock front is evaluated numerically for various monatomic gases for Mach numbers varying from 2 to 20, and the variation of the shock thickness with viscosity is also studied for different gases. Several parameters of physical interest within the shock, such as density, temperature, and mean velocity of flow are evaluated numerically, and detailed curves showing their variation within the shock are presented for different Mach numbers. It is found that the temperature rises very steeply, reaches a maximum within a distance less than half the thickness of the shock, and then diminishes slowly to attain its asymptotic downstream values. The variation of the mean velocity is slow for weak shocks, but for higher Mach numbers, the mean velocity diminishes steeply and reaches the downstream values within half the thickness of the shock.13;
机译:使用Fokker-Planck模型来表示粒子碰撞,并使用Mott-Smith分布来描述冲击前沿内的分布函数,从而研究单原子气体中的强冲击波的结构。利用13推导控制冲击内密度变化的微分方程。变分原理。对于各种单原子气体,马赫数在2到20之间变化,对冲击前沿的厚度进行了数值评估,并且还研究了不同气体的冲击厚度随粘度的变化。对冲击波中物理感兴趣的几个参数(例如密度,温度和平均流速)进行了数值评估,并给出了针对不同马赫数的冲击波内其变化的详细曲线。发现温度急剧上升,在小于冲击厚度一半的距离内达到最大值,然后缓慢下降以达到其渐近下游值。对于较弱的冲击,平均速度的变化较慢,但是对于较高的马赫数,平均速度会急剧减小并在冲击厚度的一半以内达到下游值。

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