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Propagation coefficient for the current distribution along a cylindrical antenna immersed in a warm plasma

机译:沿圆柱天线浸没在热等离子体中的电流分布的传播系数

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摘要

A perfectly conducting, infinitely long cylindrical wire of radius a surrounded by an insulating layer of a cylindrical sheath of free space of radius b is immersed in a homogeneous, warm plasma of infinite extent. Using the linearised plasma theory and approximate boundary conditions, the dispersion equation for the propagation coefficient along the wire is derived. The numerical solution of the dispersion equation for a wide range of values for the radius of the cylindrical wire and the width of the insulating sheath shows that the propagation coefficient along the cylindrical wire is close to that of the plasma mode in an unbounded plasma, in the frequency range for which the electromagnetic and the plasma space waves are excited, that is for frequencies above the plasma frequency. It is therefore concluded that, for a finite antenna immersed in a warm plasma without or with an insulating sheath, it is appropriate to include in the approximation for the current distribution along the antenna a part which has the propagation coefficient of the order of magnitude of the plasma wave.
机译:由半径为b的自由空间的圆柱形护套的绝缘层包围的,半径为a的完美导电的无限长圆柱线浸入无限量的均匀,温暖的等离子体中。利用线性化等离子体理论和近似边界条件,得出沿导线的传播系数的色散方程。对于圆柱形导线的半径和绝缘护套的宽度的宽范围值的色散方程的数值解表明,在无边界等离子体中,沿着圆柱形导线的传播系数接近于等离子体模式的传播系数。电磁波和等离子体空间波所激发的频率范围,即高于等离子体频率的频率。因此得出结论,对于浸没在带有或不带有绝缘护套的温暖等离子体中的有限天线,在沿天线的电流分布的近似值中,宜包括一个传播系数约为数量级的部分。等离子波。

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