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7
Oscillators Lecture 11

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Page 1: Oscillators

Oscillators

Lecture11

Page 2: Oscillators

19

Oscillator Principles •  Types of Oscillators

–  Sinusoidal: Used in AM/FM/Video Circuits to support selection of channels

–  Squares Wave: Clocking/Timing Circuits –  Triangular Wave: TV/Video Timing Circuits –  Rectangular Pulse Waves: Clocking/Timing in Computers

•  Linear Oscillators –  Positive Feedback amplifier circuits which feed back the

proper amplitude and phase to sustain an unlimited output

Page 3: Oscillators

20

The Barkhausen Criterion •  The requirements for oscillation using a feedback circuit:

A

β

Σ

βXo

Xout Xin+ βXout Xin

+ +

0)]()(Im[1)]()(Re[

OR 01)()( percisely, More

. isn oscillatio offrequency the where1)()(

,nonzero be to and 0For )()(1

)(])()[(

==

∠=

==−

=

+=

fAffAf

fAff

fAf

fAffA

ffA

ββ

β

β

β

β

outin

inout

outinout

XX

XX

XXX

Practically, we make β(f)A(f) slightly > 1 (Xout grows) at the frequency of oscillation. (Otherwise, the signal will decay to zero.) This causes clipping eventually but ultimately, a constant amplitude results. (This method enables some wave shaping to yield waveforms other than a sinusoid.)

Page 4: Oscillators

21

Analysis of an Oscillator Ideal Amplifier

Gain = Av

R R C C Feedback Network

CRRCjCR

CRjRCCRj

CjRCjRCj

CjRCjCRj

RCjRCj

RCjRCj

RRCj

R

j

CjRCj

CjRCR

RCjR

CjR

CR

CRCRCR

series

parallel

seriesparallel

parallel

ωωω

ωωω

ωωω

ωωω

ω

ωω

ω

ωωβ

ωω

ω

ωω

β

3]1)[(

3)(1

)1()1(

)1(

1

11

1)(

11)(

111)||(

)()||()||(

2

2

2

+−=

+−=

+++

+

+=

+++

+=

+=+=+

+=

+=

++=

Barkhausen Criterion:Avβ (jω ) =1

AvωCRj[(ωRC)2 −1]+ 3ωCR

=1

3ωCR − AvωCR + j[(ωRC)2 −1] = 0This yields:Avmin = 3

f = 12πRC

Page 5: Oscillators

22

Analysis of an Oscillator Ideal Amplifier

Gain = Av

R1 R2 C1

C2 Feedback Network

1 1

1 1 2 2

11 1

1 11

1

2 22 2 2

2 2

1

1 1

1 2 2

1 1 2

11 2

1 1

1 2 2

( || )( || ) ( )

1( || ) 1 1

11( )

1( ) 11

(1 )( )1

(1

parallel

parallel series

parallel

series

R CR C R C

RR Cj RCj C

Rj R CR C R

j C j CRj RCj R j R C

j RC j CR j RC j Cj RC

R j C j R C

β

ωω

ωω ω

ωβ ω ωω ω

ω ωω

ω ω

=+ +

= =++

++ = + =

+= +++

++=

+ + 2 1 1

2 12

2 2 1 1 2 1 2 2 1 1

)(1 )

(1 ) ( )

j R Cj C R

R C RC j C R R C RC

ωω

ω ω

+

=− + + +

Barkhausen Criterion:Avβ(jω ) =1

Av jωC2R1

(1−ω 2R2C2R1C1) + jω (C2R1 + R2C2 + R1C1)=1

Av jωC2R1 = (1−ω 2R2C2R1C1) + jω (C2R1 + R2C2 + R1C1)

0 = (1−ω 2R2C2R1C1) + jω[AvC2R1 − (C2R1 + R2C2 + R1C1)]

This yields:

Avmin =C2R1 + R2C2 + R1C1

C2R1

f = 1

2π R2C2R1C1

Page 6: Oscillators

23

Wien Bridge Oscillator

•  A non-inverting Amplifier with gain determined by R1 and R2 and the RC feedback network

R R C C Feedback Network

R2

R1

+

-

occur. willclipping and increase willnsoscillatio theof amplitude then the2 If

nsOscillatiofor 2

13

1

amplifier inverting-non For the

12

12

1

2min

1

2

1

21

21

1

RRRR

RRA

RR

RRRA

vRR

Rvv

v

ngnoninverti

ofin

>≥

+==

+=+=∴

+==

Page 7: Oscillators

24

Homework

•  Oscillator Principles – Problems: 9.83-89

•  Wien Bridge Oscillator -  Calculate the conditions (K and frequency) for oscillation for

this circuit.

R

R

C

2C

KRf

Rf

+

_