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Radio Frequency Integrated Circuit Design - Webs

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

Solution<br />

We can first compute R p in the usual way, assuming that the inductor is the<br />

sole loss in the system. It is easy to see that at 2 GHz this will be 628.3�.<br />

Next, we also need to know the value of the two capacitors in the resonator.<br />

Noting that there are two capacitors,<br />

C var =<br />

2<br />

� 2 oscL =<br />

1<br />

(2� � 2 GHz) 2 = 2.53 pF<br />

5nH<br />

Now since the transistor limiters will turn on for a voltage of about 0.85V<br />

in a modern bipolar technology, we can assume that the VCO amplitude will<br />

end up being close to this value. Therefore, we can compute the final value for<br />

the resonator current from (8.68).<br />

I tank = V tank<br />

0.635R p<br />

=<br />

1.7V<br />

= 4.26 mA<br />

(0.635)628.3�<br />

We will choose to use the 10:1 ratio for the mirror in order to get the<br />

best dc gain of 10 from this stage. Thus, the current through the mirror transistor<br />

will be 426 �A. We can now compute the values of transconductance and<br />

resistance in the model:<br />

g m5 = I bias<br />

vT<br />

g m6 = I bias<br />

vT<br />

= 426 �A<br />

25 mV<br />

= 4.26 mA<br />

25 mV<br />

= 17.04 mA<br />

V<br />

= 170.4 mA<br />

V<br />

r�5 = � 100<br />

= = 5.87 k�<br />

g m4 17.04 mS<br />

r�6 = � 100<br />

= = 587�<br />

g m4 170.4 mS<br />

Once we have chosen the gain for the current mirror, we also know the<br />

gain from the resonator:<br />

A 2(s) = V tank(0)<br />

I tank(0) =<br />

2 1<br />

� C var<br />

1<br />

s +<br />

R p C var<br />

= 2<br />

� R p = 399 V<br />

A<br />

and since the gain from the mirror will be 10, we can now find the gain required<br />

from the limiters.

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