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Radio Frequency Integrated Circuit Design - Webs

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Figure 10.24 Class E waveforms.<br />

Power Amplifiers<br />

The fundamental frequency component of vC (� )isv 1(� ). This is applied<br />

to R + jX to determine output current, voltage, and power. Here jX is the<br />

residual impedance of the series combination of L o and C o , which are tuned<br />

to be slightly away from resonance at f 0.<br />

For lossless components (as in the assumptions), the only loss is due to<br />

the discharge of C when the switch turns on. If the components are selected<br />

so that vC just reaches zero as the switch turns on, no energy is lost and the<br />

efficiency is 100%. In practice, because the assumptions do not strictly hold<br />

and because components will not be ideal, the voltage will not be at zero and<br />

so energy will be lost. However, with careful design, efficiencies in the 80%<br />

range are feasible.<br />

10.7.2 Class E Equations<br />

It is necessary to choose B and X for the correct resonance to make sure vC = 0<br />

as the switch turns on, and to make sure that d [vC (� )]/d� = 0 so that there<br />

is no current flowing into the capacitor.<br />

Setting vC (� ) and d[v C (� )]/d� to0at� = �/2 + y results in<br />

371

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