In electronics, the Miller effect (named after its discoverer John Milton Miller) accounts for the increase in the equivalent input capacitance of an inverting voltage amplifier due to amplification of the effect of capacitance between the amplifier's input and output terminals, and is given by
C M = C ( 1 + A v ) , {\displaystyle C_{\text{M}}=C(1+A_{v}),}
where − A v {\displaystyle -A_{v}} is the voltage gain of the inverting amplifier ( A v {\displaystyle A_{v}} positive), and C {\displaystyle C} is the feedback capacitance. Although the term Miller effect normally refers to capacitance, any impedance connected between the input and another node exhibiting gain can modify the amplifier input impedance via this effect. These properties of the Miller effect are generalized in the Miller theorem. The Miller capacitance due to undesired parasitic capacitance between the output and input of active devices like transistors and vacuum tubes is a major factor limiting their gain at high frequencies.
History When Miller published his work in 1919, he was working on vacuum tube triodes. The same analysis applies to modern devices such as bipolar junction and field-effect transistors.
Derivation
Consider a circuit of an ideal inverting voltage amplifier of gain − A v {\displaystyle -A_{v}} with an impedance Z {\displaystyle Z} connected between its input and output nodes. The output voltage is therefore V o = − A v V i {\displaystyle V_{o}=-A_{v}V_{i}} . Assuming that the amplifier input draws no current, all of the input current flows through Z {\displaystyle Z} , and is therefore given by
I i = V i − V o Z = V i ( 1 + A v ) Z {\displaystyle I_{i}={\frac {V_{i}-V_{o}}{Z}}={\frac {V_{i}(1+A_{v})}{Z}}} . The input impedance of the circuit is
Z i n = V i I i = Z 1 + A v {\displaystyle Z_{in}={\frac {V_{i}}{I_{i}}}={\frac {Z}{1+A_{v}}}} . In the Laplace domain (where s {\displaystyle s} represents complex frequency), if Z {\displaystyle Z} consists of just a capacitor forming a complex impedance Z = 1 s C {\displaystyle Z={\frac {1}{sC}}} , then the circuit's resulting input impedance will be equivalent to that of a larger capacitance C M {\displaystyle C_{M}} :
Z i n = 1 s C ( 1 + A v ) = 1 s C M w h e r e C M = C ( 1 + A v ) {\displaystyle Z_{in}={\frac {1}{sC(1+A_{v})}}={\frac {1}{sC_{M}}}\quad \mathrm {where} \quad C_{M}=C(1+A_{v})} . This Miller capacitance C M {\displaystyle C_{M}} is the physical capacitance C {\displaystyle C} multiplied by the factor ( 1 + A v ) {\displaystyle (1+A_{v})} .
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