Q2 (a) The closed loop gain of an oscillator is given by: RG ' (1+ j@R,C,)– @³LC,(1+ j@R,C,)+ j@R,C, A =-gm Using the Barkhausen Criteria, determine its resonant frequency. Given: RG (1+ j@R,C,)– w³ LC, (1+ j@R,C,)+ j@R,C, RG '1-w²LC, + jw(R,(C, +C,)– W²LR,C,C,) A =-gm 21+ j0 ニーgm Barkhausen Criteria states: For oscillation, this gain should be 21+j0 All imagery terms should be zero, therefore R,(C, +C;)–W²LR.C,C, = 0 C+C, w = LC,C, Draw the circuit diagram of one implementation of a Hartley oscillator using NMOS amplifier. (b) VDD R1 2 {L1 C CD CG W Z Vout R2 RS CS VSS
Q2 (a) The closed loop gain of an oscillator is given by: RG ' (1+ j@R,C,)– @³LC,(1+ j@R,C,)+ j@R,C, A =-gm Using the Barkhausen Criteria, determine its resonant frequency. Given: RG (1+ j@R,C,)– w³ LC, (1+ j@R,C,)+ j@R,C, RG '1-w²LC, + jw(R,(C, +C,)– W²LR,C,C,) A =-gm 21+ j0 ニーgm Barkhausen Criteria states: For oscillation, this gain should be 21+j0 All imagery terms should be zero, therefore R,(C, +C;)–W²LR.C,C, = 0 C+C, w = LC,C, Draw the circuit diagram of one implementation of a Hartley oscillator using NMOS amplifier. (b) VDD R1 2 {L1 C CD CG W Z Vout R2 RS CS VSS
Introductory Circuit Analysis (13th Edition)
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Publisher:Robert L. Boylestad
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
Transcribed Image Text:Q2
(a)
The closed loop gain of an oscillator is given by:
RG
A =-8m
'(1 + j@R,C,)- @°LC,(1+ jwR,C,)+ jwR,C,
Using the Barkhausen Criteria, determine its resonant frequency.
Draw the circuit diagram of one implementation of a Hartley oscillator using NMOS
amplifier.
(b)

Transcribed Image Text:Q2 (a)
The closed loop gain of an oscillator is given by:
RG
(1+ j@R,C,)– @³LC (1+ j@R,C, )+ j@R,C,
A =-gm
Using the Barkhausen Criteria, determine its resonant frequency.
Given:
RG
(1+ j@R,C,)- o²LC, (1+ j@R,C,)+ j@R,C,
RG
-B 1- W°LC, + jw(Rc(C, +C,)-w*LR,C,C,)
A =-gm
21+ j0
Barkhausen Criteria states:
For oscillation, this gain should be >1+j0
All imagery terms should be zero, therefore
R,(C, +C,)–W²LR.C,C, = 0
C +C,
wi =
LC,C,
%3D
Draw the circuit diagram of one implementation of a Hartley oscillator using
NMOS amplifier.
(b)
VDD
L2{
L1
R1 3
CD
CG
W M1
Vout
R2 E
RS
CS
VsS
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