Btrend
Advanced Member level 1
u are probably wrong.
1. consider the simpe single pole model of OP, a high impedance Vin, a gm , Ro, and the loading Cap , CL
2. the transfer function:
A(s)=Vo(s)/Vi(s)=gm*(Ro||CL)=gm*Ro/(s/ω0+1)=A0/(s/ω0+1)
where ω0=1/(Ro*CL) is the cut-off frequency (i.e. -3dB frequency, or bandwidth of the open loop OP) and A0=gm*R0
3. unit gain frequency calcualtion:
let |A(s)|=1 ,
===> 1=A0/(ωu/ω0+1)
===> because ωu >> ω0
===> 1~=A0*ω0/ωu
===> ωu=A0*ω0=gm*Ro/(Ro*CL)=gm/CL
4. u can also check these derivation from some text book, such as John Martin's book.
1. consider the simpe single pole model of OP, a high impedance Vin, a gm , Ro, and the loading Cap , CL
2. the transfer function:
A(s)=Vo(s)/Vi(s)=gm*(Ro||CL)=gm*Ro/(s/ω0+1)=A0/(s/ω0+1)
where ω0=1/(Ro*CL) is the cut-off frequency (i.e. -3dB frequency, or bandwidth of the open loop OP) and A0=gm*R0
3. unit gain frequency calcualtion:
let |A(s)|=1 ,
===> 1=A0/(ωu/ω0+1)
===> because ωu >> ω0
===> 1~=A0*ω0/ωu
===> ωu=A0*ω0=gm*Ro/(Ro*CL)=gm/CL
4. u can also check these derivation from some text book, such as John Martin's book.