等离子体物理和高超音速飞行

J. W. Bond
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引用次数: 10

摘要

当一个物体在低于20万英尺的高度,马赫数大于12到15的情况下穿过空气时,环绕物体的激波层中电子的产生对激波空气的某些特性有重大影响。在像20万英尺这样的高度上,电子的影响在更低的马赫数下也能感受到,特别是在电离层,那里的环境电子密度不再可以忽略不计。电子的影响不仅体现在传热、阻力、流场等气动量上,还体现在输运性质、辐射发射和吸收、电磁信号相互作用等物理量上。本论文的主要论点是显示如何,以及在什么条件下,电子产生的高速导弹通过大气的通道显著影响空气动力学和物理量。等离子体可以定义为含有电子的气体,其数量足以严重影响该气体的物理性质。等离子体物理学就是这种气体的物理学。例如,如果导弹以极高的速度飞行,那么高超音速导弹周围的激波层中的空气可能处于等离子状态。我们将首先讨论高超声速轴对称流场的一般结构。接下来将更详细地讨论激波前沿和边界层,重点是电子分布。然后,我们将给出一个分析玻尔兹曼方程和电子散射截面与电子速度分布函数关系的例子。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Plasma Physics and Hypersonic Flight
W an object travels through air at altitudes below something like 200,000 ft and at Mach numbers greater than 12 to 15, the production of electrons in the shocked layer of air which surrounds the object has a significant effect on some of the properties of the shocked air. Above some altitude like 200,000 ft the influence of the electrons is felt at even lower Mach numbers, particularly in the ionosphere where the ambient electron density is no longer negligible. The influence of electrons is felt not only on aerodynamic quantities such as heat transfer, drag and flow field, but also on physical quantities such as transport properties, radiative emission and absorption, and electromagnetic signal interaction. The main thesis of the present paper is to show how, and under what conditions, the electrons produced by the passage of a high speed missile through the atmosphere significantly affect both aerodynamic and physical quantities. A plasma may be defined as a gas containing electrons in sufficient quantity to seriously affect the physical properties of the gas. Plasma physics then is simply the physics of such a gas. For example, the air in the shock layer surrounding a hypersonic missile may be in a plasma state if the missile is traveling at an extremely high velocity. We will first discuss in general terms the structure of a hypersonic axially symmetric flow field. This will be followed by a more detailed discussion of the shock front and boundary layer with emphasis on the electron distribution. We will then show an example of an analysis of the Boltzmann equation and the relationship of the electron scattering cross section and the electron velocity distribution function.
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