Amplifier Design 707
The angle of the first factor is
while the angle of the second factor is
therefore, the total phase shift is
Make a graph of I versus in order to
complete the Bode diagram. This graph also appears in
Fig. 20-7.
20.2.2 Feedback Theory
Fig. 20-8 represents a generalized feedback loop based
on a voltage amplifier. In the absence of feedback, with
the loop open, the amplifier has a transfer function A.
The feedback path has a transfer function B, the input
signal from the outside world is Vin and the signal
supplied as an output is V 0. When the loop is closed, the
input signal is combined with the feedback signal in the
indicated junction to form an error signal Ve. The
process that occurs in the junction may be either addi-
tion or subtraction, depending on the nature of A, B, and
the type of feedback (positive or negative) desired. In
any event the signal actually supplied to the amplifier
when the loop is closed is Ve.
The system contained within the dotted enclosure of
Fig. 20-8 has a rather different transfer function from
that of the amplifier operated under open loop condi-
tions. The closed loop transfer function denoted by Ac^ is
derived as follows:
(20-7)
(20-8)
(20-9)
A and B, in general, are complex functions of the
steady-state frequency of operation. The absolute
magnitude of the denominator of Eq. 20-9 is called the
gain reduction factor. The feedback is called negative
when
(20-10)
and is positive when
Figure 20-7. Bode diagram for simple ac amplifier.
A S
S
Z 0
4
+------
----------------
10 Z 0
S+Z 0
= u---------------
jZ
jZ
Z 0
4
+------
-------------------
10 Z 0
jZZ+ 0
= u-------------------
90 o
45 o
0
45 o
90 o
1.0 10
0.1 1.0 10
20 dB
0 dB
S
2
---tan
1– 4 Z
Z 0
- ©¹§·------ -
tan1– Z
Z 0
------
©¹
- §·
I S
2
---tan
1– 4 Z
Z 0
–t©¹§·------ -an1– Z
Z 0
= – ©¹§·------
log ZZe 0
Figure 20-8. Generalized feedback loop.
B
A
BV 0
Ve
Vin Vout
Ve Vin+= BV 0
V 0 =AVe
AVin+= ABV 0
Ac
V 0
Vin
=-------
A
1 – AB
----------------.=
1 –>1AB