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Radio Frequency Integrated Circuit Design - Webs

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

The same type of analysis can be performed on the network in Figure<br />

4.16(a). In this case,<br />

R eq ≈ R�C 1 + C 2<br />

C � 1<br />

2<br />

C eq ≈� 1<br />

+<br />

C 1<br />

1<br />

C 2� −1<br />

4.6 The Concept of Mutual Inductance<br />

(4.17)<br />

(4.18)<br />

Any two coupled inductors that affect each other’s magnetic fields and transfer<br />

energy back and forth form a transformer. How tightly they are coupled together<br />

affects how efficiently they transfer energy back and forth. The amount of<br />

coupling between two inductors can be quantified by defining a coupling factor<br />

k, which can take on any value between one and zero. Another way to describe<br />

the coupling between two inductors is with mutual inductance. For two coupled<br />

inductors of value L p and L s , coupling factor k and the mutual inductance M<br />

as shown in Figure 4.17 are related by<br />

k = M<br />

√ L p L s<br />

(4.19)<br />

The relationship between voltage and current for two coupled inductors<br />

can be written out as follows [3]:<br />

Figure 4.17 A basic transformer structure.<br />

Vp = j�L p I p + j�MI s<br />

Vs = j�Ls Is + j�MIp<br />

(4.20)

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