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Radio Frequency Integrated Circuit Design - Webs

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80 <strong>Radio</strong> <strong>Frequency</strong> <strong>Integrated</strong> <strong>Circuit</strong> <strong>Design</strong><br />

Example 4.5 Equivalent Impedance of Transformer Networks<br />

Referring to the diagram of Figure 4.20, find the equivalent impedance of each<br />

structure, noting the placement of the dots.<br />

Solution<br />

For each structure we apply a test voltage and see what current flows. In the<br />

first case, the current flows into the side with the dot of each inductor. In this<br />

case, the flux from each structure is added. If we apply a voltage V to the circuit<br />

on the left in Figure 4.20, then V /2 appears across each inductor. Therefore,<br />

for each inductor,<br />

V<br />

2<br />

= j�LI + j�MI<br />

We can solve for the impedance by<br />

Z = V<br />

I<br />

= 2j�(L + M )<br />

Thus, since Z = j�Leq, we can solve for L eq:<br />

L eq = 2L + 2M<br />

In the second case for the circuit on the right in Figure 4.20, the dots<br />

are placed in such a way that the flux is reduced. We repeat the analysis:<br />

V<br />

2<br />

= j�LI − j�MI<br />

Z = V<br />

= 2j�(L − M )<br />

I<br />

L eq = 2L − 2M<br />

Figure 4.20 <strong>Circuit</strong>s to find the equivalent impedance.

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