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Radio Frequency Integrated Circuit Design - Webs

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

Figure 6.1 Simple transistor amplifiers.<br />

Figure 6.2 The common-emitter amplifier with transistor replaced with its small-signal model.<br />

A vo = vo r�<br />

=−<br />

vi r b + r� g m Z L ≈ Z L<br />

(6.1)<br />

re where re is the small-signal base-emitter diode resistance as seen from the emitter.<br />

Note that r� = �re and g m = 1/re . For low frequencies, the parasitic capacitances<br />

have been ignored and r b has been assumed to be low compared to r� .<br />

The input impedance of the circuit at low frequencies is given by<br />

Z in = r b + r�<br />

(6.2)<br />

However, at RF, C� will provide a low impedance across r� , and C� will<br />

provide a feedback (and feedforward) path. The frequency at which the lowfrequency<br />

gain is no longer valid can be estimated by using Miller’s Theorem<br />

to replace C� with two capacitors C A and C B , as illustrated in Figure 6.3,<br />

where C A and C B are<br />

C A = C�� 1 − vo v�� = C� (1 + g m Z L ) ≈ C� g m Z L (6.3)

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