Shielding Effectiveness of Typical Cables from 1 MHz to 1000 MHz

M. Dinallo, L. Hoeft, J. Hofstra, D. Thomas
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引用次数: 4

Abstract

Cable shields frequently have two specifica­ tions: one for EMP, and one for EMC. From 0 to 100 MHz, the total transfer impedance of a cable can be measured in a straightforward manner since the cable is electrically small over most of this range. Consequently, transfer impedance is frequently used as the measure of shielding quality of a cable for EMP shielding analysis. Beyond 100 MHz the cable length is not electrically small and it becomes dif­ ficult to reduce measured data. Consequently, some form of shielding effectiveness is often used to specify the shielding quality of cables forEMC analysis. Two alternative definitions of shielding effectiveness (the ratio of power flow out of the interior of the cable to the power flowing on the shield (SEP) and the ratio of current flowing out of the interior of the cable to that flowing on the shield (SEI)), transmission line theory, Ohm's Taw and the transfer impedance parameters (resistance and mutual inductance) were used to calculate shielding effectiveness Up to 10 GHz, The results show that, below a few MHz, the shielding effectiveness was independent of frequency and dependent on cable length. Above a few tens of MHz, when the cable becomes electrically long, the shielding effective­ ness reaches a minimum value which is directly pro­ portional to the shield's mutual inductance and becomes a maximum at the cable electrical length resonances. The high frequency limit of the shield­ ing effectiveness is independent of cable length. The two definitions of shield effectiveness differ by a factor related to the external impedance. Measured data for the shielding effectiveness (the ratio of center conductor to shield current) of several shielded twisted pairs and cable assemblies, from 1 MHz to 1000 MHz using a quadraxial test fixture, will be presented. The measured results agree reasonably well with the theory. The effect of a single aperture was also studied, and measurements show the shielding effectiveness of cables with this type of leakage is particularly poor at the UHF frequencies.
典型电缆在1mhz ~ 1000mhz范围内的屏蔽效果
电缆屏蔽层通常有两种规格:一种用于EMP,一种用于EMC。从0到100 MHz,电缆的总传输阻抗可以用一种直接的方式测量,因为电缆在这个范围的大部分是电小的。因此,在电磁脉冲屏蔽分析中,传输阻抗经常被用作电缆屏蔽质量的度量。超过100兆赫的电缆长度在电气上并不小,因此很难减少测量数据。因此,在forEMC分析中,经常使用某种形式的屏蔽效能来指定电缆的屏蔽质量。采用两种不同的屏蔽效能定义(电缆内部流出功率与屏蔽层流过功率之比(SEP)和电缆内部流出电流与屏蔽层流过电流之比(SEI))、传输线理论、欧姆定律和传输阻抗参数(电阻和互感)来计算10 GHz以下的屏蔽效能。屏蔽效果与频率无关,而与电缆长度有关。在几十MHz以上,当电缆变长时,屏蔽效能达到与屏蔽互感成正比的最小值,在电缆电长共振处达到最大值。屏蔽效能的高频极限与电缆长度无关。屏蔽效能的两种定义因与外部阻抗有关的因素而不同。将介绍几种屏蔽双绞线和电缆组件的屏蔽效能(中心导体与屏蔽电流的比率)的测量数据,使用二次测试夹具,从1 MHz到1000 MHz。实测结果与理论相当吻合。对单孔径的影响也进行了研究,测量结果表明,这种泄漏类型的电缆在UHF频率下的屏蔽效果特别差。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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