关于对称短振子的理论

G. Kevanishvili, K.V. Kotetishvili, G.K. Vashadze, D.R. Bolkvadze
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引用次数: 1

摘要

给出了对称短振子的Hallen积分方程的严格解。结果表明,振子轴向电流的线性分布为l(z′)=M/spl径向/(1-(2z′/h)/sup 2/),其中M为已知系数,z′为振子表面观测点的轴向坐标,h为振子的长度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the theory of symmetric short vibrator
The rigorous solution of Hallen's integral equation for a symmetric short vibrator is given. It is shown, that distribution of the linear axial current of the vibrator is presented as l(z')=M/spl radic/(1-(2z'/h)/sup 2/), where M is the known coefficient, z' - the axial coordinate of observation point on the surface of the vibrator, and h - its length.
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