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Lecture 3 Operational Amplifiers—Non- ideal behavior 1

Lecture 3 Operational AmplifiersNon-ideal behavior 1

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Page 1: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Lecture 3Operational Amplifiers—Non-ideal

behavior

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Page 2: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Goals

• Study non-ideal op amp behavior.

• Demonstrate circuit analysis techniques for non-ideal op amps.

• Understand frequency response limitations of op amp circuits.

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Page 3: Lecture 3 Operational AmplifiersNon-ideal behavior 1

vi2 = 0

v+ = 0 = v-, vo(1) = -R2.vi1 (inverting amplifier) R1

Vi1 = 0

V+ = R4. vi2, vo(2) = (1+ R2/R1) . R4.vi2 R3 + R4 R3+R4

non-inverting amplifier

vo = vo(1) + vo(2)

= (1+ R2). R4 vi2 - R2.Vi1

R1 R3 + R4 R1

Difference Amplifier

Assume an ideal op-ampUse the superposition theory

Page 4: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Difference Amplifiers

In order to provide equal gain for both inputs vo = -R2/R1 (v1 – v2)

(1 + R2 ) . R4 = R2

R1 R3 + R4 R1

R4/R3 = R2/R1 Balance Condition

Page 5: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Difference Amplifier

• Also called a differential subtractor, amplifies difference between input signals.

• Rin2 is series combination of R1 and R2 because i+ is zero.

• For v2=0, Rin1= R1, as the circuit reduces to an inverting amplifier.

• For general case, i1 is a function of both v1 and v2.

)2

v1

(v

1

2v R

Ro

For R2= R1)

2v

1(vv o

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Page 6: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Difference Amplifier

vicm, and vid are another representation for the inputs

vo = Ad vid + Acmvicm

Differential gain

Common-modegain

For the ideal case, vo = -R2/R1(v1 – v2) = (-R2/R1).vid + 0

Ad = -R2/R1, and Acm = 0

If balance condition is not satisfied, (R4/R3≠ R2/R1) Then Acm ≠ 0

vid = v1 – v2 differential input voltagevicm = (v1 + v2)/2 Common-mode input voltage

Define

Page 7: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Figure of meritThe Common-mode rejection ratioCMRR = 20.LOG |Ad| in dB , For Acm = 0, CMRR = 8

|Acm|

V id

1 2

4

3

v1

v2

+

-

Ad = vo / vid

1 2

4

3

Acm = vo / vicm

Vicm

+

Figure of meritThe Common-mode rejection ratioCMRR = 20.LOG |Ad| in dB , For Acm = 0, CMRR = 8

|Acm|

V id

1 2

4

3

v1

v2

+

-

Ad = vo / vid

1 2

4

3

Acm = vo / vicm

Vicm

+

Difference Amplifier FOM

Page 8: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Integrator

• Feedback resistor R2 in the inverting amplifier is replaced by capacitor C.

• The circuit uses frequency-dependent feedback.

Rsv

si dt

odvCci

Since ic= is

)0()0(

)0(0

)(1)(

1

cVov

ovdt

svRC

tov

dsvRCodv

Voltage at the circuit’s output at time t is given by the initial capacitor voltage integral of the input signal from start of

integration interval, here, t=0.Integration of an input step signal results in a ramp at the output.

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Page 9: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Differentiator

• Input resistor R1 in the inverting amplifier is replaced by capacitor C.

• Derivative operation emphasizes high-frequency components of input signal, hence is less often used than the integrator.

Rov

Ri dt

sdvCsi

Since iR= is

dtsdv

RCov

Output is scaled version of derivative of input voltage.

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Page 10: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Operational Amplifier Complete Model

Represented by:

A= open-circuit voltage gain

vid = (v+-v-) = differential input signal voltage

Rid = amplifier input resistance

Ro = amplifier output resistance

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Page 11: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Non-ideal Operational Amplifier

• Various error terms arise in practical operational amplifiers due to non-ideal behavior.

• Some of the non-ideal characteristics include:

– √ Finite open-loop gain that causes gain error

– Nonzero output resistance

– Finite input resistance

– Finite CMRR

– Common-mode input resistance

– √ DC error sources

– √ Output voltage and current limits

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Page 12: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Vo

+VS

-VS

-+

+

-

A VinV+

V-

Vin = V+ - V-

vo = A (v+ - v-) = A.vin

|v+ - v- | > 0

Finite Open-loop Gain

Example 1, Inverting Amplifier

S

SV-

V+

i

i

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Page 13: Lecture 3 Operational AmplifiersNon-ideal behavior 1

in

f

in

out

in

in

f

in

out

in

in

inffout

in

in

in

out

f

out

f

out

outout

in

in

in

-

f

-

f

out

f

out-

in

in

-

R

R

v

vA

ARA

R

R

v

v p gain Closed loo

R

v

ARARRv

R

v

AR

v

AR

v

R

v

Avv)-vA(v,vv

R

v

R

v

R

v

R

v

R

- vv

R

vv i

, V

inite pedance ise input imtill assum, We can s i i

,

111

111

,0

0

inf0

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Page 14: Lecture 3 Operational AmplifiersNon-ideal behavior 1

DC Error Sources: Input-Offset Voltage

AoV

OSV

vo=A(v+-v-), if v+ = v-

Then vo = 0 (Ideal case)

For real op-amp an input dc offset exists that can saturates the output.

We can bring the output back to zero by applying an external voltage equal in magnitude but opposite in direction to the offset voltage

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Page 15: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Finding the error in the output voltage produced by the offset (vos)

osoe

os

vR

Rv

vvv

)1

21(

Consider only the offset voltage. i.e set any input signal to zeroVoe = output error due to vos

If an input signal is connected to R1Total output =

osi vR

Rv

R

Rvo )1(

1

2

1

2

Desired output error

FOR LF351, vos = 5mV (typical)

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Page 16: Lecture 3 Operational AmplifiersNon-ideal behavior 1

DC Error Sources: Input-Offset Voltage (Example)

Problem: Find quiescent dc voltage at output.

Given data: R1 =1.2 k, R2 = 99 k

Assumptions: Ideal op amp except for nonzero offset voltage.

mV3OS

V

Output voltage is given by

Actual sign of VOS is unknown as only upper bound is given.Note: Offset voltage of most IC op amps can be manually adjusted by adding a potentiometer as shown.

V25.0)003.0(1.2k99k1

OSV

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Page 17: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Bias currents IB1 and IB2 ( base currents in BJTs or gate currents in MOSFETs or JFETs) are similar in value with directions depending on internal amplifier circuit type

21

12

2

BBos

BBB

III

III

+-IB

IB

Ios/2

IB2

IB1

Ideal -opamp

Equivalent circuit model

Sign of offset current is unknown as only upper bound is given.

DC Error Sources: Input-Bias and Offset Currents

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Page 18: Lecture 3 Operational AmplifiersNon-ideal behavior 1

DC Error Sources: Input-Bias and Offset Currents

In inverting amplifier shown, IB1

shorted out by ground connection. Since,inverting input is at virtual ground, amplifier output is forced to supply IB2 through R2 .

22R

BIoV

18

Set vin=0, v- = v+ = 0 (virtual gnd)i1=0, i2=IB2

i1

i2

This poses a limitation on the value of R2

Page 19: Lecture 3 Operational AmplifiersNon-ideal behavior 1

Numerical Example

nAInAI

OR

nAInAI

nAII

nAIII

nAInAIgiven

BB

BB

BB

BBB

osB

95 ,105

105 ,95

10

2002

10 ,100

12

12

21

21

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Page 20: Lecture 3 Operational AmplifiersNon-ideal behavior 1

DC Error Sources: Input-Bias and Offset Currents - Bias Current Compensation

Bias current compensation resistor RB is used in series with non-inverting input. Output due to IB1 alone is

1

211 R

R

BRB

IoV

By superposition,

if .

Since, offset current is typically 5.10 times smaller than individual bias currents, dc output voltage error can be reduced by using bias compensation.

22)

12(

1

21122

ROS

IRB

IB

I

R

R

BRB

IRB

IToV

2//

121

21 RRRR

RR

BR

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Page 21: Lecture 3 Operational AmplifiersNon-ideal behavior 1

DC Error Sources: Input-Bias and Offset Currents - Errors in Integrator

At t<0, reset switch is closed, circuit becomes a voltage-follower,

OSVoV

At t=0, reset switch is opened, circuit starts integrating its own offset voltage and bias current. Using superposition analysis,

Output becomes ramp with slope determined by VOS and IB2 and saturates at one of the power supplies.

tCB

It

RCOS

V

OSVtov 2)(

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