5. Modeling transmission lines, cables and transformers
5.2 Cables
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Electromagnetic waves inside of a cable (between the core and the sheath) and outside are different, mainly due to the different value of
permittivities (dielectric constants). For instance, the velocities of which are,:
Therefore, especially for calculating transients of high frequency components, both the inside and the outside should be correctly modeled. As the most simple way, general distributed parameter circuit is applicable, but modeling only the inside. So this method is valid when the sheath voltage is negligible (rigidly grounded). Combination of outside and inside coupled with ideal transformers is possible (see attached Appendix) but today's EMTP sub-routine "Cable Constants" is generally more convenient which can, directly, model various kinds of configurations. From the geometrical configuration's point of view, the following cable system(s) are applicable in the sub-routine.:
Multi phase cable system without enclosing pipe
Features:
Multi phase Cable system enclosed by a conducting pipe
Features:
From electrical point of view like transmission lines, the followings are applicable.:
(Multi stage) lumped PI model
Features:
Distributed parameter circuit model
Features:
Frequency dependent model -- Semlyen model
Features:
An example is attached simulating a single cable system, the dimension of which corresponds to measuring purpose one.


This page is based on Prof. E.Haginomori's lectures in Tokyo Institute of Technology, and edited by Japanese ATP User Group. Copyright (C) Eiichi Haginomori and Japanese ATP User Group.