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Radio Frequency Integrated Circuit Design - Webs

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The Use and <strong>Design</strong> of Passive <strong>Circuit</strong> Elements in IC Technologies<br />

In this case, the substrate capacitance and resistance from both halves of<br />

the inductor are in series. When the inductor is excited in this mode, it ‘‘sees’’<br />

less loss and will give a higher Q. Thus, the differential Q is usually higher than<br />

the single-ended Q. The self-resonance of the inductor in this mode will also<br />

be higher than the self-resonance frequency looking from either side to ground.<br />

Also, the frequency at which the differential Q peaks is usually higher than for<br />

the single-ended excitation. Care must be taken, therefore, when optimizing an<br />

inductor for a given frequency, to keep in mind its intended configuration in<br />

the circuit.<br />

Important note: Every inductor has a differential Q and a single-ended<br />

Q regardless of its layout. Which Q should be used in analysis depends on how<br />

the inductor is used in a circuit.<br />

5.16 Some Notes About the Proper Use of Inductors<br />

<strong>Design</strong>ers are very hesitant to place a nonsymmetric regular inductor across a<br />

differential circuit. Instead, two regular inductors are usually used. In this case,<br />

the center of the two inductors is effectively ac grounded and the effective Q<br />

for the two inductors is equal to their individual single-ended Qs. To illustrate<br />

this point, take a simplified model of an inductor with only substrate loss, as<br />

shown in Figure 5.18. In this case, the single-ended Q is given by<br />

and the differential Q is given by<br />

Q SE = R<br />

�L<br />

Q diff = 2R<br />

�L<br />

117<br />

(5.22)<br />

(5.23)<br />

Now if two inductors are placed in series as shown in Figure 5.19, the<br />

differential Q of the overall structure is given by<br />

Figure 5.18 Simplified inductor model with only substrate loss.

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