Abstract
One of the most significant coupling paths for electromagnetic interference into systems is via cables [1], This may be cable to cable coupling within a bundle of conductors or coupling from an illuminating electromagnetic field [2]–[4], These coupling effects may be enhanced by non-ideal cable terminations such as pigtail connections of shields or by crosstalk within connectors [5], In addition, imperfect cable shields allow coupling via transfer impedance and transfer admittance [6][7].
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