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Radio Frequency Integrated Circuit Design - Webs

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

Table 10.1<br />

PA Class A, AB, B, C Conduction Angle and Efficiency<br />

Conduction Efficiency Ouput Power<br />

Class Angle (�) (max theoretical) (%) (normalized)<br />

A 360 50 1<br />

AB 360–180 50–78.5 Nearly constant about 1<br />

(theory: max of 1.15 at 240°)<br />

B 180 78.5 1<br />

C 180–0 78.5–100 1 at 180°, 0at0°<br />

To obtain high efficiency, power loss in the transistor must be minimized,<br />

and this means that current should be minimum while voltage is high, and<br />

voltage should be minimum while current is high. It can be seen in Figures<br />

10.7 and 10.8 that for all waveforms, maximum voltage is aligned with minimum<br />

current, and maximum current is aligned with minimum voltage. It can further<br />

be seen that for class B and class C, the current is set to zero for part of the<br />

cycle where the voltage is high. This leads to increased efficiency; however,<br />

there will still be some loss, since there is an overlap of nonzero voltage and<br />

current. Other classes of amplifiers, to be described in later sections, namely,<br />

classes D, E, F, and S, are designed such that the voltage across the transistor<br />

is also nonlinear, leading to higher efficiencies, in some cases up to 100%. A<br />

different way to improve efficiency, while potentially maintaining linearity, is<br />

to power a linear amplifier from a variable or switched power supply. This is<br />

the basis for class G and H designs. All of the above amplifiers will be discussed<br />

in more detail in Sections 10.6 to 10.9.<br />

Figure 10.9 shows a simplified power amplifier and a plot of transistor<br />

current versus time for the various classes. The different classes can be obtained<br />

with the same circuit by adjusting the input bias circuit. For example, in class<br />

A, if the maximum current is Imax, the amplifier is set to have a nominal bias<br />

of half of Imax so that current swings from nearly 0 to Imax. For class B, the<br />

bias is set so that the transistor is nominally at the edge of conduction so that<br />

positive input swing will cause the transistor to conduct, while negative input<br />

will guarantee the transistor is off. Thus, the transistor will conduct half the<br />

time.<br />

10.5.1 Class A, B, and C Analysis<br />

Except for class A, the current through the transistor is not sinusoidal, but may<br />

be modeled as a biased sinusoid as shown in Figure 10.10.<br />

The collector current can be expressed as

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