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Radio Frequency Integrated Circuit Design - Webs

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Power Amplifiers<br />

Solution<br />

The first thing to note is that the current extremes I max and I min will still be<br />

approximately the same as they were for the class A amplifier even though<br />

current will flow for a smaller percentage of the time. Examination of Figure<br />

10.14 shows that the output fundamental current will be roughly constant for<br />

any conduction angle between 180° and 360°. Thus, it would seem that it<br />

should be possible to reduce the nominal current through this amplifier and<br />

achieve roughly the same output power by driving the amplifier into compression.<br />

In practice, with reduced bias, the achievable output power is reduced, as<br />

shown by simulation results summarized in Table 10.2.<br />

It can be seen that by reducing the bias current to 105 mA, approximately<br />

the same results are obtained as for the class A amplifier. However, there are<br />

a few important differences. Because the amplifier is driven into compression,<br />

the efficiency is now 57.2% and the amplifier is now nonlinear. If instead the<br />

same amplifier is used as in Example 10.1, a bias current of 147 mA, output<br />

power is increased to 24.1 dBm and efficiency is increased to 58.9%. Timedomain<br />

waveforms for this case can be seen in Figure 10.21. It can be seen<br />

that waveforms do not match simple theory in that voltage is not sinusoidal<br />

and current goes negative due to transistor capacitance. By considering the<br />

positive portion of the current, the conduction angle for a 14-dBm input is<br />

estimated to be about 260° (� = 130°), and from Figure 10.11, efficiency is<br />

expected to be about 60%, which is close to the simulated value.<br />

10.6 Class D Amplifiers<br />

Two examples of class D amplifiers are shown in Figure 10.22. The two<br />

transistors alternately switch the output to ground or to VCC . The output filter,<br />

consisting of L o and C o , is tuned to the fundamental frequency. This serves<br />

to remove the dc component and the harmonics, resulting in a sine wave at<br />

the output. While class D amplifiers can have high efficiency and have been<br />

Table 10.2<br />

Simulation Results for Class AB Power Amplifier Example<br />

P in<br />

I bias Opt PAE (opt PAE) P out Compression<br />

(mA) (%) (dBm) (opt PAE) (dB) � opt<br />

63 55.8 12 20.7 2.5 11.5 + j 18.7<br />

105 57.2 13 22.6 3.2 12.2 + j 14.3<br />

147 58.9 14 24.1 3.7 13.1 + j 10.3<br />

367

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