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226 ANALOG BUILDING BLOCKS AND OPERATIONAL AMPLIFIERS


By defining thecurrent gain GIto be the ratio of the current throughRLto the current through
vS, one gets

GI=

iL
iS

=

Avin/(Ro+RL)
vin/Ri

=

ARi
Ro+RL

(5.1.2)

Thepower gain GP,defined by the ratio of the power delivered to the load to the power given
out by the signal source, is obtained as

GP=

vL^2 /RL
v^2 S/Ri

=

G^2 VRi
RL

=

A^2 RLRi
(Ro+RL)^2

=GVGI (5.1.3)

Note that, for fixed values ofRoandRi,GPis maximized whenRLis chosen equal toRo, and this
corresponds to maximum power transfer to the load. One should also note that the added power
emerging from the output comes from the power source that powers the amplifier, even though
the power-supply connections are usually not shown on the circuit diagram, and that the existence
of power gain does not violate the law of energy conservation.

EXAMPLE 5.1.2
The constants of an amplifier are given byA= 1 ,Ri=10,000, andRo= 100 . It is driven by
a Thévenin source withvTh(t)=VOcosωtandRTh=20,000. The amplifier output is connected
to a 100-load resistance. Find the power amplification, if it is defined as the ratio of the power
delivered to the load to the maximum power available from the Thévenin source.

Solution

The corresponding circuit diagram is shown in Figure E5.1.2. The instantaneous power delivered
toRLis given by

Ro = 100 Ω

RTh = 20,000 Ω

Avin = vin

vin RL^ =
100 Ω

Ri =
10,000 Ω

Signal source Load
Amplifier

vTh =
VO cos ωt

+


+


+


Figure E5.1.2Circuit diagram.

PL(t)=i^2 L(t)RL=

[
Avin(t)
Ro+RL

] 2
RL

The time-averaged powerPLis obtained by representingvin(t) by its phasorV ̄in,

PL=

1
2


∣V ̄in

∣^2 A

(^2) RL
(Ro+RL)^2
Note that the time average of a product of sinusoids is given by

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