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Radio Frequency Integrated Circuit Design - Webs

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

Thus, we can see from this example that a −Gm oscillator can start with<br />

half as much collector current in each transistor as a Colpitts oscillator under<br />

the same loading conditions.<br />

8.9 Comments on Oscillator Analysis<br />

It has been shown that closed-loop analysis agrees exactly with the open-loop<br />

analysis. It can also be shown that analysis by negative resistance produces<br />

identical results. This analysis can be extended. For example, in a negative<br />

resistance oscillator, it is possible to determine if oscillations will be stable as<br />

shown by Kurokawa [1], with detailed analysis shown by [2]. However, what<br />

does it mean to have an exact analysis? Does this allow one to predict the<br />

frequency exactly? The answer is no. Even if one could take into account<br />

RF model complexities including parasitics, temperature, process, and voltage<br />

variations, the nonlinearities of an oscillator would still change the frequency.<br />

These nonlinearities are required to limit the amplitude of oscillation, so they<br />

are a built-in part of an oscillator. Fortunately, for a well-designed oscillator,<br />

the predicted results will give a reasonable estimate of the performance. Then,<br />

to refine the design, it is necessary to simulate the circuit.<br />

Example 8.5 Oscillator <strong>Frequency</strong> Shifts and Open-Loop Gain<br />

Explore the predicted frequency with the actual frequency of oscillation by<br />

doing open-loop and closed-loop simulation of an oscillator. Compare the results<br />

to the simple formula. This example can also be used to explore the amplitude<br />

of oscillation and its relationship to the open-loop gain.<br />

Solution<br />

For this example, the previously found capacitor and inductor values are used<br />

in the circuit shown in Figure 8.20.<br />

Loop gain can be changed by adjusting g m or the tank resistance R p . Both<br />

will also affect frequency somewhat. R p will affect �c through Q L and g m will<br />

affect �c indirectly, since re = 1/g m . In this case, we varied both R p and g m .<br />

Results are plotted in Figure 8.21.<br />

It can be seen from Figure 8.21(a) that the open-loop simulations consistently<br />

predict higher oscillating frequencies than the closed-loop simulations.<br />

Thus, nonlinear behavior results in the frequency being decreased. We note<br />

that the initial frequency estimate using the inductor and capacitor values and<br />

adding an estimate for the parasitic capacitance results in a good estimate of<br />

final closed-loop oscillating frequency. In fact, this estimate of frequency is<br />

better than the open-loop small-signal prediction of frequency. It can also be<br />

seen from Figure 8.21(b) that output signal amplitude is related to the openloop<br />

gain, and as expected, as gain drops to 1 or less, the oscillations stop.

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