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Chapter 12C apte
Power Amplifiers
DefinitionsDefinitions
In small-signal amplifiers the main factors are:
• Amplification
• Linearity
• Gain
Since large-signal, or power, amplifiers handle relatively large
voltage signals and current levels, the main factors are:
• Efficiency
• Maximum power capability
I d t hi t th t t d i• Impedance matching to the output device
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
22
Amplifier TypesAmplifier Types
Class AClass A
The amplifier conducts through the full 360° of the input. The Q-point is
t th iddl f th l d liset near the middle of the load line.
Class BClass B
The amplifier conducts through 180° of the input The Q point is set atThe amplifier conducts through 180 of the input. The Q-point is set at
the cutoff point.
Class ABClass ABClass ABClass AB
This is a compromise between the class A and B amplifiers. The
amplifier conducts somewhere between 180° and 360° . The Q-point is
located between the mid-point and cutoff.
more…more…
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
33
Amplifier TypesAmplifier Types
Class CClass CClass CClass C
The amplifier conducts less than 180 of the input. The Q-point is located
below the cutoff level.
Class DClass D
This is an amplifier that is biased especially for digital signals.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
44
Class AAmplifierClass AAmplifier
The output of a class A amplifier
conducts for the full 360° of the
cycle.
The Q-point is set at the middle of
th l d li th t th AC i lthe load line so that the AC signal
can swing a full cycle.
Remember that the DC load line
indicates the maximum and minimum
limits set by the DC power supply.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
55
Class B AmplifierClass B Amplifier
A class B amplifier output
only conducts for 180° or
one-half of the AC input
signal.
The Q-point is at 0V on the
load line so that the ACload line, so that the AC
signal can only swing for
one-half cycle.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
66
Class AB AmplifierClass AB Amplifier
This amplifier is a compromise between the
class A and class B amplifier—the Q-point
is above that of the Class B but below theis above that of the Class B but below the
class A.
The output conducts between 180° and
360° f th AC i t i l360° of the AC input signal.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
77
Class CClass C
The output of the class C
conducts for less than 180° of theconducts for less than 180 of the
AC cycle. The Q-point is below
cutoff.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
88
Amplifier EfficiencyAmplifier Efficiency
EfficiencyEfficiency refers to the ratio of output to input power. The lower the amount
f d ti f th lifi th hi h th ffi iof conduction of the amplifier the higher the efficiency.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
99
SeriesSeries--Fed Class AAmplifierFed Class AAmplifier
This is similar to the
small-signal amplifier
except that it will handle
higher voltages. The
transistor used is a high-
ipower transistor.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1010
SeriesSeries--Fed Class AAmplifierFed Class AAmplifier
A small input signal
causes the output voltage
to swing to a maximum ofto swing to a maximum of
Vcc and a minimum of 0V.
The current can also
swing from 0mA to ICSATg CSAT
(VCC/RC)
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1111
SeriesSeries--Fed Class AAmplifierFed Class AAmplifier
The power into the amplifier is from the DC supply. With no input
signal, the DC current drawn is the collector bias current, ICQ.
Input PowerInput Power
g CQ
CQCCi(dc) IVP =
Output PowerOutput Power
C(rms)
2
o(ac)
V
P =
p)-CE(p
2
o(ac)
8R
V
P =or
C
o(ac)
R C
o(ac)
8R
EfficiencyEfficiency
100
P
P
%η
i(ac)
o(ac)
×=
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1212
TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier
This circuit uses a
transformer to couple to
the load. This improves
the efficiency of the Class
A 0%A to 50%.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1313
Transformer ActionTransformer Action
A transformer improves the efficiency because it is able to transform
the voltage, current, and impedance
Voltage RatioVoltage Ratio
1
2
1
2
N
N
V
V
=
Current RatioCurrent Ratio
11
12 NI
Impedance RatioImpedance Ratio
2
1
1
2
N
N
I
I
=
Impedance RatioImpedance Ratio
2
2
2
1
2
1
L
L
a
N
N
R
R
R
R
=⎟⎟
⎠
⎞
⎜⎜
⎝
⎛
==
′
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1414
TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier
DC Load LineDC Load Line
As in all class A amplifiers
th Q i t i t bli h dthe Q-point is established
close to the midpoint of the
DC load line.
AC Load LineAC Load Line
The saturation point (ICmax)
is at V /R′ and the cutoffis at Vcc/R L and the cutoff
point is at V2 (the secondary
voltage of the transformer).
This increases the maximum
output swing because the
minimum and maximum
values of IC and VCE are
spread further apart
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
spread further apart.
1515
TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier
Signal Swing and Output AC PowerSignal Swing and Output AC Power
The voltage swing:
minCEmaxCE)pp(CE VVV −=−
The current swing:
minCmaxC II −
8
)I)(IV(V
P CminCmaxCEminCEmax
o(ac)
−−
=
The AC power:
8
( )
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1616
TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier
EfficiencyEfficiency
Power input from the DC source:Power input from the DC source:
CQCCi(dc) IVP =
o(ac)i(dc)Q PPP −=
Power dissipated as heat across the transistor:Power dissipated as heat across the transistor:
Note: The larger the input and output signal, the
lower the heat dissipation.
2
VV ⎞⎛
Maximum efficiencyMaximum efficiency::
Note: The larger V and smaller V the
CEminCEmax
CEminCEmax
VV
VV
50%η ⎟⎟
⎠
⎞
⎜⎜
⎝
⎛
+
−
=
Note: The larger VCEmax and smaller VCEmin, the
closer the efficiency approaches the theoretical
maximum of 50%.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1717
Class B AmplifierClass B Amplifier
In class B, the transistor is
biased just off. The AC signal
turns the transistor onturns the transistor on.
The transistor only conducts
when it is turned on by one-
half of the AC cycle.
In order to get a full AC cycle
out of a class B amplifier youout of a class B amplifier, you
need two transistors:
• An npn transistor that provides the
negative half of the AC cycle
• A pnp transistor that provides the
positive half.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1818
Class B Amplifier: EfficiencyClass B Amplifier: Efficiency
The maximum efficiency of a class B is 78.5%..
100
P
)P
%
)dc(i
ac(o
×=η
i
L
2
CC
o(dc)
2R
V
Pmaximum =
For maximum power, VL=VCC
CC
2
CC
CCdcCCi(dc)
2V2V
V)I(maximumVPmaximum =⎟⎟
⎞
⎜⎜
⎛
==
LL
CCdcCCi(dc)
RπRπ
)( ⎟
⎠
⎜
⎝
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
1919
TransformerTransformer--Coupled PushCoupled Push--PullPull
Cl B A lifiCl B A lifiClass B AmplifierClass B Amplifier
The center-tappedThe center tapped
transformer on the input
produces opposite
polarity signals to the
two transistor inputs.
The center-tapped
transformer on the
output combines the two
halves of the AC
f t thwaveform together.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2020
Class B Amplifier PushClass B Amplifier Push--Pull OperationPull Operation
• During the positive
half-cycle of the AChalf-cycle of the AC
input, transistor Q1
(npn) is conducting
and Q2 (pnp) is off.
• During the negative
half-cycle of the AC
input, transistor Q2input, transistor Q2
(pnp) is conducting
and Q1 (npn) is off.
Each transistor produces one-half of an AC cycle. The transformer combines the
two outputs to form a full AC cycle.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2121
Crossover DistortionCrossover Distortion
If the transistors Q1 and Q2 do
t t d ff t tlnot turn on and off at exactly
the same time, then there is a
gap in the output voltage.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2222
QuasiQuasi--Complementary PushComplementary Push--Pull AmplifierPull Amplifier
A Darlington pair and a feedbackA Darlington pair and a feedback
pair combination perform the
push-pull operation. This
increases the output power
capability.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2323
Amplifier DistortionAmplifier Distortion
If the output of an amplifier is not a complete AC sine wave,
then it is distorting the output. The amplifier is non-linear.
This distortion can be analyzed using Fourier analysis. In
Fourier analysis, any distorted periodic waveform can be
broken down into frequency components. These
components are harmonics of the fundamental frequency.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2424
HarmonicsHarmonics
Harmonics are integer multiples of a fundamental frequency.
If the fundamental frequency is 5kHz:
1st harmonic 1 x 5kHz
2nd harmonic 2 x 5kHz
3rd harmonic 3 x 5kHz
4th harmonic 4 x 5kHz
etc.
Note that the 1st and 3rd harmonics are called odd harmonicsodd harmonics and the
2nd and 4th are called even harmonicseven harmonics2nd and 4th are called even harmonicseven harmonics.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2525
Harmonic DistortionHarmonic Distortion
According to FourierAccording to Fourier
analysis, if a signal is not
purely sinusoidal, then it
contains harmonics.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2626
Harmonic Distortion CalculationsHarmonic Distortion Calculations
Harmonic distortion (D) can be calculated:
100
A
A
%Ddistortionharmonicnth%
1
n
n ×==
where
An is the amplitude of the fundamental frequency
An is the amplitude of the highest harmonic
The total harmonic distortion (THD) is determined by:
100DDDTHD% 2
3
2
3
2
2 ×+++= L
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2727
Power Transistor Derating CurvePower Transistor Derating Curve
Power transistors dissipate
a lot of power in heat. This
can be destructive to the
amplifier as well as to
surrounding components.
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2828
Class C AmplifiersClass C Amplifiers
A class C amplifier conducts for lessp
than 180°. In order to produce a full
sine wave output, the class C uses a
tuned circuit (LC tank) to provide
the full AC sine wave.
Class C amplifiers are used
i i i i iextensively in radio communications
circuits.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
2929
Class D AmplifierClass D Amplifier
A class D amplifier amplifies
l d i l dpulses, and requires a pulsed
input.
There are many circuits thatThere are many circuits that
can convert a sinusoidal
waveform to a pulse, as well
as circuits that convert aas circuits that convert a
pulse to a sine wave. This
circuit has applications in
digital circuitry.g y
Copyright ©2009 by Pearson Education, Inc.
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Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
3030

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12 power amplifirs

  • 2. DefinitionsDefinitions In small-signal amplifiers the main factors are: • Amplification • Linearity • Gain Since large-signal, or power, amplifiers handle relatively large voltage signals and current levels, the main factors are: • Efficiency • Maximum power capability I d t hi t th t t d i• Impedance matching to the output device Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 22
  • 3. Amplifier TypesAmplifier Types Class AClass A The amplifier conducts through the full 360° of the input. The Q-point is t th iddl f th l d liset near the middle of the load line. Class BClass B The amplifier conducts through 180° of the input The Q point is set atThe amplifier conducts through 180 of the input. The Q-point is set at the cutoff point. Class ABClass ABClass ABClass AB This is a compromise between the class A and B amplifiers. The amplifier conducts somewhere between 180° and 360° . The Q-point is located between the mid-point and cutoff. more…more… Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 33
  • 4. Amplifier TypesAmplifier Types Class CClass CClass CClass C The amplifier conducts less than 180 of the input. The Q-point is located below the cutoff level. Class DClass D This is an amplifier that is biased especially for digital signals. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 44
  • 5. Class AAmplifierClass AAmplifier The output of a class A amplifier conducts for the full 360° of the cycle. The Q-point is set at the middle of th l d li th t th AC i lthe load line so that the AC signal can swing a full cycle. Remember that the DC load line indicates the maximum and minimum limits set by the DC power supply. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 55
  • 6. Class B AmplifierClass B Amplifier A class B amplifier output only conducts for 180° or one-half of the AC input signal. The Q-point is at 0V on the load line so that the ACload line, so that the AC signal can only swing for one-half cycle. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 66
  • 7. Class AB AmplifierClass AB Amplifier This amplifier is a compromise between the class A and class B amplifier—the Q-point is above that of the Class B but below theis above that of the Class B but below the class A. The output conducts between 180° and 360° f th AC i t i l360° of the AC input signal. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 77
  • 8. Class CClass C The output of the class C conducts for less than 180° of theconducts for less than 180 of the AC cycle. The Q-point is below cutoff. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 88
  • 9. Amplifier EfficiencyAmplifier Efficiency EfficiencyEfficiency refers to the ratio of output to input power. The lower the amount f d ti f th lifi th hi h th ffi iof conduction of the amplifier the higher the efficiency. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 99
  • 10. SeriesSeries--Fed Class AAmplifierFed Class AAmplifier This is similar to the small-signal amplifier except that it will handle higher voltages. The transistor used is a high- ipower transistor. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1010
  • 11. SeriesSeries--Fed Class AAmplifierFed Class AAmplifier A small input signal causes the output voltage to swing to a maximum ofto swing to a maximum of Vcc and a minimum of 0V. The current can also swing from 0mA to ICSATg CSAT (VCC/RC) Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1111
  • 12. SeriesSeries--Fed Class AAmplifierFed Class AAmplifier The power into the amplifier is from the DC supply. With no input signal, the DC current drawn is the collector bias current, ICQ. Input PowerInput Power g CQ CQCCi(dc) IVP = Output PowerOutput Power C(rms) 2 o(ac) V P = p)-CE(p 2 o(ac) 8R V P =or C o(ac) R C o(ac) 8R EfficiencyEfficiency 100 P P %η i(ac) o(ac) ×= Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1212
  • 13. TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier This circuit uses a transformer to couple to the load. This improves the efficiency of the Class A 0%A to 50%. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1313
  • 14. Transformer ActionTransformer Action A transformer improves the efficiency because it is able to transform the voltage, current, and impedance Voltage RatioVoltage Ratio 1 2 1 2 N N V V = Current RatioCurrent Ratio 11 12 NI Impedance RatioImpedance Ratio 2 1 1 2 N N I I = Impedance RatioImpedance Ratio 2 2 2 1 2 1 L L a N N R R R R =⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ == ′ Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1414
  • 15. TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier DC Load LineDC Load Line As in all class A amplifiers th Q i t i t bli h dthe Q-point is established close to the midpoint of the DC load line. AC Load LineAC Load Line The saturation point (ICmax) is at V /R′ and the cutoffis at Vcc/R L and the cutoff point is at V2 (the secondary voltage of the transformer). This increases the maximum output swing because the minimum and maximum values of IC and VCE are spread further apart Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky spread further apart. 1515
  • 16. TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier Signal Swing and Output AC PowerSignal Swing and Output AC Power The voltage swing: minCEmaxCE)pp(CE VVV −=− The current swing: minCmaxC II − 8 )I)(IV(V P CminCmaxCEminCEmax o(ac) −− = The AC power: 8 ( ) Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1616
  • 17. TransformerTransformer--Coupled Class AAmplifierCoupled Class AAmplifier EfficiencyEfficiency Power input from the DC source:Power input from the DC source: CQCCi(dc) IVP = o(ac)i(dc)Q PPP −= Power dissipated as heat across the transistor:Power dissipated as heat across the transistor: Note: The larger the input and output signal, the lower the heat dissipation. 2 VV ⎞⎛ Maximum efficiencyMaximum efficiency:: Note: The larger V and smaller V the CEminCEmax CEminCEmax VV VV 50%η ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ + − = Note: The larger VCEmax and smaller VCEmin, the closer the efficiency approaches the theoretical maximum of 50%. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1717
  • 18. Class B AmplifierClass B Amplifier In class B, the transistor is biased just off. The AC signal turns the transistor onturns the transistor on. The transistor only conducts when it is turned on by one- half of the AC cycle. In order to get a full AC cycle out of a class B amplifier youout of a class B amplifier, you need two transistors: • An npn transistor that provides the negative half of the AC cycle • A pnp transistor that provides the positive half. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1818
  • 19. Class B Amplifier: EfficiencyClass B Amplifier: Efficiency The maximum efficiency of a class B is 78.5%.. 100 P )P % )dc(i ac(o ×=η i L 2 CC o(dc) 2R V Pmaximum = For maximum power, VL=VCC CC 2 CC CCdcCCi(dc) 2V2V V)I(maximumVPmaximum =⎟⎟ ⎞ ⎜⎜ ⎛ == LL CCdcCCi(dc) RπRπ )( ⎟ ⎠ ⎜ ⎝ Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 1919
  • 20. TransformerTransformer--Coupled PushCoupled Push--PullPull Cl B A lifiCl B A lifiClass B AmplifierClass B Amplifier The center-tappedThe center tapped transformer on the input produces opposite polarity signals to the two transistor inputs. The center-tapped transformer on the output combines the two halves of the AC f t thwaveform together. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2020
  • 21. Class B Amplifier PushClass B Amplifier Push--Pull OperationPull Operation • During the positive half-cycle of the AChalf-cycle of the AC input, transistor Q1 (npn) is conducting and Q2 (pnp) is off. • During the negative half-cycle of the AC input, transistor Q2input, transistor Q2 (pnp) is conducting and Q1 (npn) is off. Each transistor produces one-half of an AC cycle. The transformer combines the two outputs to form a full AC cycle. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2121
  • 22. Crossover DistortionCrossover Distortion If the transistors Q1 and Q2 do t t d ff t tlnot turn on and off at exactly the same time, then there is a gap in the output voltage. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2222
  • 23. QuasiQuasi--Complementary PushComplementary Push--Pull AmplifierPull Amplifier A Darlington pair and a feedbackA Darlington pair and a feedback pair combination perform the push-pull operation. This increases the output power capability. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2323
  • 24. Amplifier DistortionAmplifier Distortion If the output of an amplifier is not a complete AC sine wave, then it is distorting the output. The amplifier is non-linear. This distortion can be analyzed using Fourier analysis. In Fourier analysis, any distorted periodic waveform can be broken down into frequency components. These components are harmonics of the fundamental frequency. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2424
  • 25. HarmonicsHarmonics Harmonics are integer multiples of a fundamental frequency. If the fundamental frequency is 5kHz: 1st harmonic 1 x 5kHz 2nd harmonic 2 x 5kHz 3rd harmonic 3 x 5kHz 4th harmonic 4 x 5kHz etc. Note that the 1st and 3rd harmonics are called odd harmonicsodd harmonics and the 2nd and 4th are called even harmonicseven harmonics2nd and 4th are called even harmonicseven harmonics. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2525
  • 26. Harmonic DistortionHarmonic Distortion According to FourierAccording to Fourier analysis, if a signal is not purely sinusoidal, then it contains harmonics. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2626
  • 27. Harmonic Distortion CalculationsHarmonic Distortion Calculations Harmonic distortion (D) can be calculated: 100 A A %Ddistortionharmonicnth% 1 n n ×== where An is the amplitude of the fundamental frequency An is the amplitude of the highest harmonic The total harmonic distortion (THD) is determined by: 100DDDTHD% 2 3 2 3 2 2 ×+++= L Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2727
  • 28. Power Transistor Derating CurvePower Transistor Derating Curve Power transistors dissipate a lot of power in heat. This can be destructive to the amplifier as well as to surrounding components. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2828
  • 29. Class C AmplifiersClass C Amplifiers A class C amplifier conducts for lessp than 180°. In order to produce a full sine wave output, the class C uses a tuned circuit (LC tank) to provide the full AC sine wave. Class C amplifiers are used i i i i iextensively in radio communications circuits. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 2929
  • 30. Class D AmplifierClass D Amplifier A class D amplifier amplifies l d i l dpulses, and requires a pulsed input. There are many circuits thatThere are many circuits that can convert a sinusoidal waveform to a pulse, as well as circuits that convert aas circuits that convert a pulse to a sine wave. This circuit has applications in digital circuitry.g y Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky 3030