Abstract
This chapter deals with the explanation of ideal multiconductor transmission lines. Ideal two-conductor transmission lines can be characterized as two-ports in the time domain, and their behavior can be represented through simple equivalent lumped circuits of Thévenin and Norton type. This chapter extends these findings to ideal multiconductor transmission lines by using the matrix theory. The ideal multiconductor line equation is diagonalized, the concept of propagation mode is introduced, and the d’Alembert solution to these equations is extended. Using this solution the characteristic relation of the 2n-port representing a generic ideal multiconductor line is determinded followed by an introduction to equivalent circuits of Thévenin and Norton type.
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