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Radio Frequency Integrated Circuit Design - Webs

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

behave in an application when loaded with impedances other than 50�. It<br />

would be more useful to extract an inductance and Q for both windings and<br />

plot the coupling (k factor) or mutual inductance for the structure instead.<br />

These properties have the advantage that they do not depend on the system<br />

reference impedance.<br />

In the following narrowband model, all the losses are grouped into a<br />

primary and secondary resistance as shown in Figure 5.30.<br />

The model parameters can be found from the Z parameters starting with<br />

V1<br />

I1 | = Z 11 = R p + j�(L p − M ) + j�M = R p + j�L p<br />

I2 =0<br />

Similarly,<br />

Z 22 = R s + j�Ls<br />

(5.30)<br />

(5.31)<br />

Thus, the inductance of the primary and secondary and the primary and<br />

secondary Q can be defined as<br />

L s = Im(Z 22)<br />

j�<br />

L p = Im(Z 11)<br />

j�<br />

Q s = Im(Z 22)<br />

Re(Z 22)<br />

Q p = Im(Z 11)<br />

Re(Z 11)<br />

Figure 5.30 Narrowband equivalent model for a transformer.<br />

(5.32)<br />

(5.33)<br />

(5.34)<br />

(5.35)

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