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Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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Page 1: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

Differential Amplifiers

ES 330 Electronics II

Chapter 8 Sedra & SmithSection 9.2 on BJT Diff Amps

Page 2: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

Single-Ended Signals versus Double-Ended (i.e., Differential) Signals

2

Page 3: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

The current source is called the tail current.

Differential Pairs – BJT and FET

3

Q1 Q2

Page 4: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

Differential Pair Characteristic

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Page 5: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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Differential Pair Characteristic

Page 6: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

CCY

EECCCX

C

EEC

VV

IRVV

I

II

02

1

Differential Response of a Differential Amplifier (Case 1)

ON

OFF

6

Page 7: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

CCX

EECCCY

C

EEC

VV

IRVV

I

II

01

2

Differential Response of a Differential Amplifier

OFF

ON

7

Page 8: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

Common Mode Response of a Differential Amplifier

8

2

221

21

EECCCYX

EECC

BEBE

IRVVV

III

VV

Page 9: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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Small-Signal Analysis of a Differential Amplifier

II

I

II

I

EEC

EEC

2

2

2

1

Page 10: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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For small changes at inputs, the gm’s are the same, and the respective increase and decrease of IC1 and IC2 are the same, node “P” must stay constant to accommodate these changes. Thus, node “P” is an AC ground, but not a DC ground.

1

2

0limPx

C m

C m

V

I g V

I g V

Virtual Ground in a Differential Amplifier

Page 11: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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Small-Signal Differential Gain

Since the output changes by -2gmVRC and input by 2V, the small signal gain is –gmRC, similar to that of the CE stage. However, for the same gain as in CE stage, DC power dissipation is doubled.

CmCm

v RgV

VRgA

2

2

Vout = VX – VY = -2gmΔVRC

Vin = 2ΔV

Page 12: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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Small Signals and Large Signals

Linear Signal

Clipped Signal

(a) (b)

(c) (d)

Input

Output

TransferCurve

Page 13: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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Small-Signal Model for Differential Amplifier

r0 not included

vout1 vout2

Page 14: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

Since VP is grounded, we can treat the differential pair as two CE “half circuits,” with its gain equal to one half circuit’s single-ended gain.

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From Symmetry We Need Only Analyze a Half Circuit

Cm

inin

outout Rgvv

vv

21

21

vout1 vout2

vout1 vout2

Page 15: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

1 2

1 2

out outm O

in in

v vg r

v v

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Intrinsic Differential Gain of a Differential Amplifier

Note: Resistance associated with these current sources is infinite.Thus, we include output resistors r0.

Page 16: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

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Questions?

Page 17: ES 330 Electronics II Chapter 8 Sedra & Smith · Differential Amplifiers ES 330 Electronics II Chapter 8 Sedra & Smith Section 9.2 on BJT Diff Amps

An Operational Amplifier Example Using Differential Pair at Input

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DifferentialInputs

Output