The Miller Theorem , named after John Milton Miller , deals with the separation of impedances in electrical networks . If there are two networks ( two-pole ) that are connected via a real impedance Z , this impedance can be virtually broken down so that both networks can be viewed separately. The Miller theorem is the generalization of the Miller effect .
The decomposition into Z 1 and Z 2 is correct if both networks see the same impedances after the decomposition as before.
The two tensions are about gain
linked, which then results in the decomposed impedances Z 1 and Z 2 :
results.
It should be noted that for a gain M greater than one, the impedance Z 1 is negative when Z is positive. With an inverting amplifier M less than minus −1, the impedance Z 1 is significantly
reduced compared to Z.
Derivation
The voltage U Z across the impedance Z results from the difference between the terminal voltages , the substitution by M giving the conversion listed.
At the same time applies to the "seen" impedance Z 1 :
By equating it follows:
and by equivalence conversion we finally get:
.
The same applies to the "seen" impedance Z 2 :
literature
Richard C. Li: RF Circuit Design . In: Information and Communication Technology . 2nd Edition. Wiley, 2012, ISBN 978-1-118-12849-7 .