Unit - 6 Operational Amplifier: Fig.6.1 Symbol of Op-Amp
Unit - 6 Operational Amplifier: Fig.6.1 Symbol of Op-Amp
Unit - 6 Operational Amplifier: Fig.6.1 Symbol of Op-Amp
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
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
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
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
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
-VEE
OFFSET NULL
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
V1
Vo
Ri
V2
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
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
SJBIT/ECE Dept
Page 110
Basic Electronics/10ELN15
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
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
i1
G=Vi
VO
Vi
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-
VO
Vi
VO
Vi
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
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
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
SJBIT/ECE Dept
Page 115
Basic Electronics/10ELN15
From the above figure we have
0
Vi
i1
Vi
R
1
C
VO
1
C
VO
dVO
dt
i 2 dt
i 2 dt
1
i2
C
i.e. i 2
dVO
dt
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
Vi
dVi
dt
i1
1
i1
C
C.
dVi
dt
i2
0 VO
R
VO
R
dVi
dt
VO
R
VO
RC
SJBIT/ECE Dept
dV
dt
Page 117