Nothing Special   »   [go: up one dir, main page]

Unit - 6 Operational Amplifier: Fig.6.1 Symbol of Op-Amp

Download as pdf or txt
Download as pdf or txt
You are on page 1of 12
At a glance
Powered by AI
The key takeaways are that an op-amp can be used as a differential amplifier, inverting amplifier, non-inverting amplifier, voltage follower, adder, integrator and differentiator. An op-amp has high input impedance and low output impedance.

The different configurations of an op-amp are inverting amplifier, non-inverting amplifier, voltage follower, adder, integrator and differentiator.

An inverting amplifier outputs a signal that is 180 degrees out of phase with the input signal, while a non-inverting amplifier outputs a signal that is in phase with the input signal.

Basic Electronics/10ELN15

UNIT -6
OPERATIONAL AMPLIFIER
Op-Amp (operational amplifier) is basically an amplifier available in the IC form. The word
operational is used because the amplifier can be used to perform a variety of mathematical
operations such as addition, subtraction, integration, differentiation etc.
Fig6.1 below shows the symbol of an Op-Amp.
+VCC
V1
Inverting input
V2
Noninverting input
-VEE

Fig.6.1 Symbol of Op-Amp

It has two inputs and one output. The input marked - is known as Inverting input and the input
marked + is known as Non-inverting input.
If a voltage Vi is applied at the inverting input ( keeping the non-inverting input at ground)
as shown below.
Vi
VO
t
t
Vi

VO

Fig.6.2 Op-amp in inverting mode

The output voltage Vo= -AVi is amplified but is out of phase with respect to the input signal by
1800.
SJBIT/ECE Dept

Page 106

Basic Electronics/10ELN15

If a voltage Vi is fed at the non-inverting input ( Keeping the inverting input at ground) as
shown below.
Vo

VO
t

Vi

Fig.6.3 Op-Amp in Non-inverting mode

The output voltage Vo= AVi is amplified and in-phase with the input signal.
If two different voltages V1 and V2 are applied to an ideal Op-Amp as shown below.

V1
VO
V2

Fig.6.4 Ideal Op-Amp

The output voltage will be Vo = A(V1 V2)


i.e the difference of the tow volatages is amplified. Hence an Op-Amp is also called as a High
gain differential amplifier.

SJBIT/ECE Dept

Page 107

Basic Electronics/10ELN15
Note: Op-Amp is 8 pin IC ( named as A 741) with pin details as shown.

OFFSET NULL

NO CONNECTION

+VCC

OUTPUT

INVERTING I/P

A 741

NON INVERTING I/P

-VEE

OFFSET NULL

Fig.6. 5 Pin details of Op-Amp

Block Diagram of an Op-AMP


An Op-Amp consists of four blocks cascaded as shown above

Fig. 6.6 Block diagram of an Op-Amp

Input stage: It consists of a dual input, balanced output differential amplifier. Its function is to
amplify the difference between the two input signals. It provides high differential gain, high input
impedance and low output impedance.
Intermediate stage: The overall gain requirement of an Op-Amp is very high. Since the input
stage alone cannot provide such a high gain. Intermediate stage is used to provide the required
additional voltage gain.
It consists of another differential amplifier with dual input, and unbalanced ( single ended) output

SJBIT/ECE Dept

Page 108

Basic Electronics/10ELN15

Buffer and Level shifting stage


As the Op-Amp amplifies D.C signals also, the small D.C. quiescent voltage level of previous
stages may get amplified and get applied as the input to the next stage causing distortion the final
output.
Hence the level shifting stage is used to bring down the D.C. level to ground potential, when no
signal is applied at the input terminals. Buffer is usually an emitter follower used for impedance
matching.
Output stage- It consists of a push-pull complementary amplifier which provides large A.C.
output voltage swing and high current sourcing and sinking along with low output impedance.

Concept of Virtual ground


We know that , an ideal Op-Amp has perfect balance (ie output will be zero when input voltages
are equal).
Hence when output voltage Vo = 0, we can say that both the input voltages are equal ie V1 = V2.

V1
Vo
Ri
V2

Fig. 6.7(a) Concept of Virtual ground

Since the input impedances of an ideal Op-Amp is infinite ( Ri = ). There is no current flow
between the two terminals.
Hence when one terminal ( say V2 ) is connected to ground (ie V2 = 0) as shown.
VCC

V1 =V2 =0
Ri

VO

V2=0

VEE
Fig. 6.7(b) Concept of Virtual ground

SJBIT/ECE Dept

Page 109

Basic Electronics/10ELN15

Then because of virtual ground V1 will also be zero.


Applications of Op-Amp
An Op-Amp can be used as
1. Inverting Amplifer
2. Non-Iverting Amplifer
3. Voltage follower
4. Adder ( Summer)
5. Integrator
6. Differentiator
Definitions
1. Slewrate(S): It is defined as The rate of change of output voltage per unit time
s

dVO
dt

volts / sec

Ideally slew rate should be as high as possible.But its typical value is s=0. V/-sec.
2. Common Mode Rejection Ratio(CMRR): It is defined as The ratio of differential
voltage gain to common-mode voltage gain.
CMRR

Ad
ACM

Ideally CMRR is infinite, but its typical value is CMRR = 90 dB


3. Open Loop Voltage Gain (AV): It is the ration of output voltage to input voltage in the
absence of feed back.
Its typical value is AV = 2x105
4. Input Impedance (Ri):It is defined as The impedance seen by the input(source) applied
to one input terminal when the other input terminal is connected to ground.
Ri M
5. Output Impedance (RO): It is defined as The impedance given by the output (load) for
a particular applied input.
Ro 7

SJBIT/ECE Dept

Page 110

Basic Electronics/10ELN15

Note: Typical values given above are for Op-Amp IC=A741


Characteristics of an Ideal Op-Amp
An ideal Op-Amp has the following characteristics.
1. Infinite voltage gain ( ie AV =)
2. Infinite input impedance (Ri = )
3. Zero output impedance(Ro =0)
4. Infinite Bandwidth (B.W. = C
5. Infinite Common mode rejection ratio (ie CMRR =)
6. Infinite slew rate (ie S=)
7. Zero power supply rejection ratio ( PSRR =0)ie output voltage is zero when power supply
VCC =0
8. Zero offset voltage(ie when the input voltages are zero, the output voltage will also be
zero)
9. Perfect balance (ie the output voltage is zero when the input voltages at the two input
terminals are equal)
10. The characteristics are temperature independent.

Inverting Amplifier
An inverting amplifier is one whose output is amplified and is out of phase by 180 0 with
respect to the input
Rf
i2
R1
V1

i1

G=0
VO

Fig.6.8 Inverting Amplifier

SJBIT/ECE Dept

Page 111

Basic Electronics/10ELN15
The point G is called virtual ground and is equal to zero.
By KCL we have
i1 i2
Vi 0
R1

Vi
R1

VO

Where

0 Vo
Rf

Vo
Rf

Rf
R1
Rf
R1

Vi

is the gain of the amplifier and negative sign indicates that the output is inverted

with respect to the input.


VO
Vi

Fig.6. 9 Waveforms of Inverting Amplifers

Non- Inverting Amplifier


A non-inverting amplifier is one whose output is amplified and is in-phase with the input.
Rf
i2
R1
V1

i1

G=Vi
VO
Vi

Fig.6.10 Non Inverting Amplifiers

By KCL we have

i1
SJBIT/ECE Dept

i2
Page 112

Basic Electronics/10ELN15

Vi

Vi

VO

R1
Vi
R1

Rf
VO Vi
Rf
Rf

V0 Vi
Vi

VO
Vi
VO
Vi

Rf

R1
Rf

V0

R1

Ri
Rf

Where 1

R1

Vi

Rf
R1

is the gain of the amplifier and + sign indicates that the output is in-

phase with the input.


Voltage follower

VO
Vi

VO

Vi

Fig. 6.11 Voltage follower

Voltage follower is one whose output is equal to the input.


The voltage follower configuration shown above is obtained by short circuiting R f and open
circuiting R1 connected in the usual non-inverting amplifier.
SJBIT/ECE Dept

Page 113

Basic Electronics/10ELN15
Thus all the output is fed back to the inverting input of the op-Amp.
Consider the equation for the output of non-inverting amplifer

Rf

V0

Vi

R1

When Rf = 0 short circuiting


R1= open circuiting

VO

VO

Vi

Vi

Therefore the output voltage will be equal and in-phase with the input voltage. Thus voltage
follower is nothing but a non-inverting amplifier with a voltage gain of unity.
Inverting Adder
Inverting adder is one whose output is the inverted sum of the constituent inputs

R1
Rf
V1

i1
If
R2

V2

i2

G=0
VO

V3

R3

i3

Fig.6.12. Inverting Adder

By KCL we have

if

i1

i2

i3

0 VO
Rf
SJBIT/ECE Dept

V1 0
R1

V2 0
R2

V3 0
R3
Page 114

Basic Electronics/10ELN15

VO
Rf

V1
R1
VO

V2
R2
Rf

V1
R1

V3
R3
V2
R2

V3
R3

If R1 = R2 = R3 =R then

VO

Rf
R

V1 V2 V3

If Rf = R then
VO = -[ V1 + V2 + V3 ]
Hence it can be observed that the output is equal to the inverted sum of the inputs.
Integrator
C
i2
R1
V1

i1

G=0
VO

Fig, 6.13 Integrator

An integrator is one whose output is the integration of the input.,


By KCL we have,
i1 i2
1

SJBIT/ECE Dept

Page 115

Basic Electronics/10ELN15
From the above figure we have
0

Vi

i1

Vi
R

and similarly we have


0

1
C

VO

1
C

VO

dVO
dt

i 2 dt

i 2 dt

1
i2
C

i.e. i 2

dVO
dt

substituing 2 and 3 in 1 we have


Vi
R

dVO
dt

dVO
dt
1
Vi
RC

VO

1
RC

Vi dt

Differentiator
A differentiator is one whose output is the differentiation of the input
R
i2

V1

i1

G=0
VO

By KCL we have

SJBIT/ECE Dept

Page 116

Basic Electronics/10ELN15
i1

i2

From the above figure we have


1
i1 dt
C

Vi

dVi
dt

i1

1
i1
C

C.

dVi
dt

and similarly we have

i2

0 VO
R

VO
R

substituting 2 and 3 in 1 we have

dVi
dt

VO
R

VO

RC

SJBIT/ECE Dept

dV
dt

Page 117

You might also like