环形磁芯作为多径磁芯模拟电路

J. Baldwin
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引用次数: 5

摘要

描述了一种类似于多径磁芯的电路。环形核被用来模拟多径核的分支。节点上的磁通守恒是用连接磁芯组的短绕组来模拟的。这保证了给定绕组上磁心的磁通变化总和将消失。通过合理选择绕组匝数和铁芯尺寸来模拟安培定律。推导了用多径核的参数来确定模拟参数的方程。这些规定表明,铁芯的体积必须与相应支路的体积成正比,短路绕组在铁芯上的匝数应与铁芯直径与支路长度的比例成正比,外部供电驱动器的安培匝数也应与该比例成正比。采用单匝耦合环路和不同直径铁芯的模拟电路作为特例进行了讨论。另一种特殊情况采用多匝绕组,但铁芯相同。结果表明,短路绕组中的电流与多径磁芯对应节点的磁势成正比。利用磁芯模拟直接观测节间磁电位差的方法,通过示波器拍摄的三阶laddic节间磁电位差的照片加以说明。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Circuits Employing Toroidal Magnetic Cores as Analogs of Multipath Cores
Circuits which are analogous to multipath magnetic cores are described. Toroidal cores are employed to simulate the branches of the multipath core. The conservation of flux at a node is simulated by means of shorted windings connecting groups of cores. These insure that the sum of the flux changes in the cores on a given winding will vanish. Ampere's law is simulated by proper choice of both number of turns and core dimensions. Equations are derived which determine the parameters of the analog in terms of those of the multipath core. These state that the volume of a core must be proportional to the volume of the corresponding branch, that the number of turns a shorted winding makes on a core should be proportional to the ratio of core diameter to branch length, and that the number of ampere-turns of externally supplied drive should also be proportional to this ratio. Analog circuits employing single-turn coupling loops and cores of different diameters are discussed as a special case. Another special case employs multiturn windings but identical cores. It is shown that the current flowing in a shorted winding is proportional to the magnetic potential of the corresponding node of the multipath core. The use of the core analog for the direct observation of internodal magnetic potential differences is illustrated by means of oscilloscope photographs of the magnetic potential difference between the nodes of a three-rung laddic.
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