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Radio Frequency Integrated Circuit Design - Webs

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

Example 10.3 Class E Amplifier<br />

<strong>Design</strong> a class E amplifier that delivers 200 mW from a 3-V power supply at<br />

2.4 GHz. Assume an ideal transistor and aim for a Q of 3 for the output circuit.<br />

Specify device ratings and components.<br />

Solution<br />

Using Po ≈ 0.577V 2<br />

CC /R results in R = 26�. The maximum transistor voltage<br />

is vC,max = 3.56 � 3 = 10.68V. If this large voltage is not permissible (and it<br />

is quite likely that it is not), the power supply voltage may need to be reduced.<br />

From (10.28),<br />

I dc = VCC<br />

1.734R =<br />

3<br />

= 66.6 mA<br />

1.734 � 26<br />

ic,peak = 2.861I dc = 190.6 mA<br />

B = 0.1836 0.81Q<br />

R �1 +<br />

Q 2 0.1836 1 + 0.81 � 5<br />

=<br />

+ 4� 26 � 3 2 � = 0.00755<br />

+ 4<br />

Hence C = 0.50 pF. Since Q = 3, C o has a reactance of 78� and is<br />

therefore 0.85 pF. Using (10.27),<br />

X = 1.10Q<br />

Q − 0.67<br />

1.110 � 3<br />

R = 26 = 37.2�<br />

3 − 0.67<br />

L o therefore has a reactance of 37.2 + 78 = 115.2� and is thus 7.64 nH.<br />

Ideally, the RFC should have a reactance of at least 10R and thus should be<br />

at least 17 nH, which would likely need to be an off-chip inductor.<br />

This circuit was simulated using a process with f T that is 25 times higher<br />

than the operating frequency. With numbers calculated as above, and choosing<br />

a transistor size that has optimal f T at about 66 mA, the results in Figure 10.25<br />

were obtained. For simplicity, the input was a ±1.5V pulse waveform through<br />

a 50-� source resistance. In a real circuit, a more realistic input waveform<br />

would have to be used.<br />

It can be seen that the output transistor collector voltage has not gone<br />

down to zero when the transistor switches on. The problem is the parasitic<br />

output capacitance of the very large transistor. As a result, the output power is<br />

only about 77 mW and dc power is of the order of 100 mW. As a first-order<br />

compensation, the capacitor C can be reduced to compensate. With this done,<br />

the results are as shown in Figure 10.26.

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