K
Kristine Hyvang
Guest
When there is an impedance connecting the input side to the output side
across an amplifier, there is an expression saying :
Zmiller,in = ZF/(1-Av)
where ZF is the impedance connecting input to output, and Av is the voltage
gain from input to output. Now the Millers impedance is from input to ground
(without any impedance connecting the input to the output), and the model
looks different. That's allright.
but.......
when looking on the output side,
Zmiller,out=(Zf*Av)/(Av-1) (according to the book)
......what I don't grasp is the denominator .... Av-1.
When I analyze this I get:
ZFmiller,out=(Zf*Av)/ (1-Av)
models :
Impedance connecting input and output:
IF------->
-------------------ZF---------------------
---
|
|
|
|
|
|
Vin-------------
Av -------------------Vout
gnd-----------------------------------------gnd
Millers impedance:
Vin -----------
v -------------------Vout
|
|
|
|
Zmiller,in
ZMiller,out
|
|
|
|
gnd-----------------------------------------gnd
If I add a minus to the ZMiller,out-expression it adds up,
but that means that the current enters the amplifier from both ends, and
that doesn't make sense !
Or is this a definition of input- and output- impedances..........that the
current allways enters the amplifier from both ends ?
across an amplifier, there is an expression saying :
Zmiller,in = ZF/(1-Av)
where ZF is the impedance connecting input to output, and Av is the voltage
gain from input to output. Now the Millers impedance is from input to ground
(without any impedance connecting the input to the output), and the model
looks different. That's allright.
but.......
when looking on the output side,
Zmiller,out=(Zf*Av)/(Av-1) (according to the book)
......what I don't grasp is the denominator .... Av-1.
When I analyze this I get:
ZFmiller,out=(Zf*Av)/ (1-Av)
models :
Impedance connecting input and output:
IF------->
-------------------ZF---------------------
---
|
|
|
|
|
|
Vin-------------
Av -------------------Vout
gnd-----------------------------------------gnd
Millers impedance:
Vin -----------
v -------------------Vout
|
|
|
|
Zmiller,in
ZMiller,out
|
|
|
|
gnd-----------------------------------------gnd
If I add a minus to the ZMiller,out-expression it adds up,
but that means that the current enters the amplifier from both ends, and
that doesn't make sense !
Or is this a definition of input- and output- impedances..........that the
current allways enters the amplifier from both ends ?