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1 Figure 7.27 A simple but inefficient approach for differential to single-ended conversion.

1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

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Page 1: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

1

Figure 7.27 A simple but inefficient approach for differential to single-ended conversion.

Page 2: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

2

Circuit for a basic MOSFET constant-current source.

Page 3: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

3

Basic MOSFET Current Mirror.

Page 4: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

4

Figure 7.28 The active-loaded MOS differential pair.

Page 5: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

5

Figure 7.28 The circuit at equilibrium assuming perfect matching.

Page 6: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

Assignment # 2

Problems 7.11, 7.14, 7.16, 7.20, 7.21, 7.22, 7.23, 7.31, 7.33, 7.34, 7.36, 7.37, 7.38

Due date: 30th March 2012

Page 7: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

Figure 7.28 The circuit with a differential input signal applied, neglecting the ro of all transistors.

Page 8: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

8

Figure 7.29 Determining the short-circuit transconductance Gm =io/vid of the active-loaded MOS differential pair.

Page 9: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

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Figure 7.30 Circuit for determining Ro. The circled numbers indicate the order of the analysis steps.

Page 10: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

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Figure 7.31 Analysis of the active-loaded MOS differential amplifier to determine its common-mode gain.

Page 11: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

Figure 4.44 (a) Common-source amplifier with a resistance RS in the source lead. (b) Small-signal equivalent circuit with ro neglected.

Page 12: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

12

Common Mode Gain (Acm)

vicmvicm

vovgs3 =-vsg4

1 2

1m1 m2

3 4

3 4

& are negelcted

1 1, 2

g g 2

o o

icmSS

SS

o o o

m m m

r r

vR therefore i

R

r r r

g g g

Page 13: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

13

Common Mode Gain (Acm) & CMRR

vicmvicm

vovgs3 =-vsg4

SS

icm

R

vii

221

3 1 33

4 4 3 1 4 33

4 2 4

1

1

( )

g om

m g m om

o o

v i rg

i g v i g rg

v i i r

Page 14: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

14

1 4 3 2 43

4 3 43

1( )

1( 1)

2

o m o om

icmo m o o

m SS

v i g r i rg

vv g r r

g R

SSmom

SSmoomcm

d

SSmomSS

ocm

om

mSS

o

icm

ocm

RgrgCMRR

RgrrgA

ACMRR

RgrgR

rA

rg

gR

r

v

vA

2||

2

1

1

1

2

11

2

42

33

4

33

44

Common Mode Gain (Acm) & CMRR

Page 15: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

Exercise 7.12

Page 16: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

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The basic BJT current mirror.

Page 17: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

17

A simple BJT current source.

Page 18: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

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Figure 7.32 Active-loaded bipolar differential pair.

Page 19: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

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Figure 7.32 Small-signal equivalent circuit for determining the transconductance Gm=; io/vid.

Page 20: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

20

Differential Gain Ad

vid/2 -vid/2

vo

Page 21: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

21

Differential Gain Ad

3 1 1 3 3 4 1 3

1, 3, 4 e3

3 4 4

4 4 4 1 3

0

2 2 as

Since , the collector curren of will be

2The output current can be f

id idb m o e o m e

o o

b b

idm b m m e

v vv g r r r r g r

r r r r

v v Q

vg v g g r

i

2 4 4 2 4 1 3

1 2 4

33

3

ound from a node equation at the output as

2 2 2/ 2

Since all devices are operating at the same bias current, where

1and

Thu

id id ido m m b o m m m e

Cm m m m m

t t

em m m

v v vi g g v i g g g r

IIg g g g g

V V

rg g g

s om m

id

iG g

v

Page 22: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

22

Figure 7.32 Equivalent circuit for determining the output resistance Ro =vx/ix.

Page 23: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

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Figure 7.33 Analysis of the bipolar active-loaded differential amplifier to determine the common-mode gain.

Page 24: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

24

Figure 7.33 Analysis of the bipolar active-loaded differential amplifier to determine the common-mode gain.

111

11 r

rg

r

rg

rg

grr

m

m

m

me

Page 25: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

25

vicm vicm

vbe3 = -vbe3 vo

i1i2

Common Mode Gain

mmm

ooo

EE

icmEE

oo

ggg

rrr

R

viithereforeR

rr

43

43

11m2m1

21

2 2

g

1,

g

1

negelcted are &

Page 26: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

26

Common Mode Gain

EE

o

icm

ocm

EE

icmoo

mm

EE

icmoo

om

mo

omm

ebbe

oo

eeEEEE

icm

R

r

v

vA

R

vrv

rrg

gR

vrv

rirrg

igv

rrrrrg

irrrg

ivv

rrNeglect

rrRR

vii

3

4

3

4

433

44

42433

14

433433

143033

143

21

2111

2

2

1||||1

2

||||1

,as ||||1

||||||1

&

,2 as 2

Page 27: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

27

Common Mode Gain

EE

o

icm

ocm

EE

icmoo

emEE

icmoo

oemo

eoeeebbe

oo

eeEEEE

icm

R

r

v

vA

R

vrv

rrgR

vrv

rirrigv

rrrrrirrrivv

rrNeglect

rrRR

vii

3

4

3

4

4344

424314

4334314303143

21

2111

2

2

1||2

||

,as ||||||

&

,2as 2

Page 28: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

28

Common Mode Gain

2

2

2111

21||

43

434

3434

m

m

e

em

em

g

g

rr

rrg

rrg

2

2

21

21

2

1

21

21

21

21

21

21

21||||

1

33

34

33

3

43

3

3

34

343

34

rg

gg

rg

r

gr

g

rg

g

rrg

g

m

mm

m

m

m

mm

mm

Page 29: 1 Figure 7.27 A simple but inefficient approach for differential to single- ended conversion

29

Common Mode Rejection Ratio (CMRR)

omd rgA2

1

EE

ocm R

rA

3

4

EEmo

EEom

cm

d Rgr

Rrg

A

ACMRR 3

3

2

1

2

1