16. Transmission-Line Equations
Consider the TEM mode in a parallel-plate waveguide shown in the figure below.

The only non-zero field components are
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|
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, we can rewrite Faraday's and Ampere's laws:
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(1) |
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(2) |
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(3) |
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(4) |
via ![]() |
(5) |
via the introduction of the surface current K, ![]() |
(6) |
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(7) |
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(8) |
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(9) |
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(10) |
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(11) |
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(12) |
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(13) |
Wave Equations and Solutions
If we differentiate (12) with respect to z and substitute (13) for the resulted right-hand side, then we can show that the Helmholtz equation governs the electric potential between the two plates.
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(14) |
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(15) |
A simplest solution to (14) is of the form:
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(16) |
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(17) |
In general, along a transmission line, the general solution to (14) includes voltages travelling in both positive and negative z-direction, hence is of the form:
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(18) |
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(19) |
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(20) |
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(21) |
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(22) |
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(23) |
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(24) |
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(25) |
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(26) |
This page was last updated on March 9, 1998.