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Experiment 5 — Coupler Design.

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Z 0<br />

Z 0<br />

Through wave<br />

R 2<br />

Z 0<br />

Sampled wave<br />

R 1<br />

Figure 3 - Resistor divider non-directional coupler.<br />

The transmission lines are not electromagnetically coupled and the coupling<br />

equations are derived from the lumped circuit calculation of the resistor<br />

divider.<br />

3.2 Coupled Line Directional <strong>Coupler</strong><br />

3.2.1 A Single Section <strong>Coupler</strong><br />

There are two modes of current flow in an electromagnetic situation. The first<br />

is one current flowing down one conductor with a contra-flow current back<br />

up the other conductor caused by displacement current coupling between<br />

the two conductors. This is termed the ’odd mode’ current, and it has an<br />

associated odd mode characteristic impedance, styled Z 0o .<br />

Theothermodeisonecurrentflows by displacement current between<br />

each center conductor carrying the same polarity, and the ground that is<br />

common between them. Hence this is called the ’even mode’ current, and it<br />

has an associated even mode characteristic impedance, styled Z 0e .Figure4<br />

shows the polarity of the lines of each mode.<br />

For a single section coupler the even and odd mode characteristic impedances<br />

are defined as:<br />

6

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