2007 Fall: Electronic Circuits 2
CHAPTER 14
Output Stages and
Power Amplifiers
Introduction
In this chapter, we will be covering…
Classification of Output Stages
Class A Output Stage
Class B Output Stage
Class AB Output Stage
Biasing the Class AB Circuit
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14.1 Classification of Output Stages
Output stages are classified according to the collector current waveform when an input signal is applied.
When a sinusoidal input signal is applied,
Class A : biased at a current greater than the amplitude of signal current.
Class B : biased at zero dc current.
Class AB : an intermediate class between A and B.
biased at a nonzero dc current much smaller than the peak current of the sine-wave signal.
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Thermal Issues
Junction temperature
Dissipated power = Psupply – Poutput Æ Need to minimize Pd
51.1 91.9
1.113
T-case (°C) T-junction
(°C) Dissipated
Power (W)
RFIN
RFOUT
33.4 45.3
0.369
T-case (°C) T-junction
(°C) Dissipated
Power (W)
Conduction Angle Dependence under Harmonic Short Termination
Harmonic short termination Ó No harmonic voltage Ó Load resistance
c d e
I
1R
opt= V
DCB class opt
A class
opt
R
R
, −=
, −A class opt AB
class
opt
R
R
, −<
, −RL determines voltage swing
Class and Efficiency
Output Efficiency (Drain/Collector Efficiency)
η ↑ rapidly as class-C
P
dcP
1η
ΔIdeal Case
• All harmonics short- circuited Æ No
distortion
• R
Ldetermines voltage swing
• R
Lalso determines DC power
consumption
14.1 Classification of Output Stages
Collector current waveforms for transistors operating in (a) class A (b) class B (c) class AB
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14.2.1 Transfer Characteristic
The emitter follower – the most popular class A ckt.
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14.2.1 Transfer Characteristic (cont.)
The bias current must be greater than the largest negative load current.
The transfer characteristic is
The positive limit of the linear region is given by
In the negative direction, the limit of the linear region is
1
o I BE
v = −v v
max 1
O CC CE sat
v =V −V
min 2
O L CC CE sat
v = −IR or −V +V
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14.2.2 Signal Waveforms
For sine-wave input, neglecting VCEsat, the output voltage can
swing from –VCC to +VCC with the quiescent value being zero.
Since vCE1 = VCC-vo,
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14.2.2 Signal Waveforms (cont.)
Assuming that the bias current is selected to allow a maximum negative load current of Vcc/RL,
The instantaneous power dissipation in Q1, pD1=vCE1·iC1
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14.2.3 Power Dissipation
The maximum instantaneous power dissipation in Q
1= V
CC·I
= The quiescent power dissipation in Q
1.
The emitter follower transistor dissipates the largest amount of power when vo=0: The transistor Q1 must be able to withstand a continuous power dissipation of VCC·I.
The power dissipation in Q1 depends on the value of RL: When RL=0, a very large current may flow through Q1: short circuit protection is needed.
The maximum instantaneous power dissipation in Q
2=2·V
CC·I
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14.2.4 Power-Conversion Efficiency
Power-Conversion Efficiency of an output stage is defined as
For the emitter follower, the average load power will be
The average (positive + negative) supply power is,
Thus, the PCE is,
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( ) ( )
L S
Load power P Supply power P η =
2 2
ˆ ˆ
( / 2) 1 2
o o
L
L L
V V
P = R = R
S 2 CC
P = V I
ˆ 2 ˆ ˆ
1 1
4 4
o o o
L CC L CC
V V V
IR V IR V
η = =
14.2.4 Power-Conversion Efficiency (cont.)
The maximum efficiency is 25%, obtained when
Because 25% is a rather low figure, the class A output stage is rarely used in high-power applications (>1W).
In practice the output voltage swing is limited to lower values to avoid transistors saturation and associated nonlinear distortion. Thus the efficiency achieved is usually in the 10% to 20% range.
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ˆ
o CC LV = V = IR
14.3 Class B Output Stage
The class B output stage consists of a complementary pare of transistors connected in such a way that both cannot conduct simultaneously.
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Figure 14.5 A class B output stage.