differential amplifiers

41
Differential Amplifiers

Upload: niabi

Post on 07-Jan-2016

63 views

Category:

Documents


1 download

DESCRIPTION

Differential Amplifiers. Outline. Single-Ended Versus Differential Operation. The transitions disturb the differential by equal amounts, leaving the difference in tact. Immunity to Supply Noise. If VDD changes by ∆V, Vout changes by the same amount. Noise in VDD affects VX and VY, - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Differential Amplifiers

Differential Amplifiers

Page 2: Differential Amplifiers

Outline

Page 3: Differential Amplifiers

Single-Ended Versus Differential Operation

The transitions disturbthe differential by equal amounts, leavingthe difference in tact.

Page 4: Differential Amplifiers

Immunity to Supply Noise

If VDD changes by ∆V, Vout changes bythe same amount.

Noise in VDD affects VX and VY, but not Vx-Vy

Page 5: Differential Amplifiers

Reduction of Coupled Noise

Noise coupled from L3 to L1 and L2 to L1 cancel each other.

Page 6: Differential Amplifiers

Sensitivity to the Common mode level

Excessive lowVin,CM turns offDevices.

Page 7: Differential Amplifiers

Basic Differential Pair

Page 8: Differential Amplifiers

Schematic of Differential Amplifier

Page 9: Differential Amplifiers

Input/Output Characteristics

Independent of Vin,cm

Maximum SlopeThus maximum Gain

Minimum Slope

Page 10: Differential Amplifiers

Range of Vin,cm

Lower bound of Vin,cm:VP should be sufficiently high in order for M3 to actas a current source.Upper bound of Vin, cm

M1 and M2 need to remain in saturation.

Page 11: Differential Amplifiers

Sensitivity to Vin, cm

M3=Linear M3=Linear M3=Linear

M1=M2=Off

M1=M2=Off

M1=M2=Off

M1=M2=On

M1=M2=On

M1=M2=On

M3 in the linear region is modeled as a resistor

Page 12: Differential Amplifiers

Small signal Gain as a function of Vin,

CM

Page 13: Differential Amplifiers

Maximum Allowable Output Swing

The higher the input CM level, the smallerthe allowable output swings.

Page 14: Differential Amplifiers

Transconductance

∆Vin1Represents the maximum differential signal a differentialpair can handle.

Page 15: Differential Amplifiers

Linearity

W/L increasesISS Constant

Constant W/L ISS increases

Page 16: Differential Amplifiers

Determinations of Small Signal Gain

1. CS with resistive source degeneration

2. Thevenin Resistance3. Cascode 4. Superposition Principle

Page 17: Differential Amplifiers

CS with resistive source degeneration

Interpretation: The resistance at the drainDivided by the resistance in the source path

Page 18: Differential Amplifiers

Treat M1 as a CS stage with resistive source degeneration to find VX/Vin

Page 19: Differential Amplifiers

Replace M1 by its Thevenin Equivalent Circuit

If RS is sufficiently large, then the small signal gain of the amplifiercan be obtained using thevenin’s equivalent circuit (see hand out)

Page 20: Differential Amplifiers

Gain of CG

Page 21: Differential Amplifiers

Replace M1 by its Thevenin Equivalent Circuit

Page 22: Differential Amplifiers

Small Signal Gain

Page 23: Differential Amplifiers

Half-Circuit Concept

Page 24: Differential Amplifiers

Conversion of Arbitrary inputs to Differential and Common-Mode Components

Page 25: Differential Amplifiers

Superposition Principle

Page 26: Differential Amplifiers

Schematic of Differential Amplifier

Page 27: Differential Amplifiers

SimulationVin,m=1 mVVout,m=8.735 mVAv=-8.735

Calculations:Gm=1mSro=30.53 KOhmRL=12 KohmAv=-Gm(ro||RL)=-8.615

Page 28: Differential Amplifiers

Common-Mode Response

• Sensitivity of Vout,CM due to Vin,CM

• In the presence of resistor mismatch• In the presence of transistor

mismatch• Common Mood Rejection Ratio

(CMRR)

Page 29: Differential Amplifiers

Sensitivity of Vout,CM due to Vin,CM

Vin,CM ↑, VP ↑, I(RSS) ↑,VX,V↓

Page 30: Differential Amplifiers

Output CM Sensitivity due to Vin, CM

Vout,m=0.285 mV

Vin,cm=1 mV

RL=12 KGm=1.043 mSGds3=58.29 uS

Av, CM(Analytical)=0.343Av, CM(Simulation)=0.285(Excluding gmb, ro)

Page 31: Differential Amplifiers

Common-Mode to Differential Conversion at High Frequencies

Even if the output resistance of the current source is high,the common-mode to differential conversion becomes significantat high frequencies.

Page 32: Differential Amplifiers

Resistor Mismatch

(from CS with resistive source degeneration)

Page 33: Differential Amplifiers

Common Mode to Differential Mode Conversion

Page 34: Differential Amplifiers

Voutp-Voutn

Differential Mode signal at the output: 1.176 uV

Page 35: Differential Amplifiers

Effect of CM Noise in the Presence of Resistor Mismatch

Common Mode to Differential Conversion

Page 36: Differential Amplifiers

Transistor Mismatch

Page 37: Differential Amplifiers

Supply Noise Sensitivity

Page 38: Differential Amplifiers

CMRR

Page 39: Differential Amplifiers

Diode Connected Load

Problem: Difficult to decrease (W/L)P without dropping the common mode voltage of Vout.

Page 40: Differential Amplifiers

Addition of Current Source to Increase Voltage Gain

Reduce gm by reducing current rather than the aspect ratio.Reduce I(M3) and I(M4).

Page 41: Differential Amplifiers

Variable Gain Amplifier