Power Amplifiers
Classification of Power Amplifiers
 Power amplifiers are classified based on the Q
point
 If the operating point is chosen at the middle of the
load line, it is called Class A amplifier
 If the operating point is chosen at the cut-off point
it is called Class B amplifier
 If the operating point is chosen beyond the cut-off
point it is called Class C amplifier
 It conducts for 3600
Concept Preview
• Efficiency is most important in power amplifiers.
• Poor efficiency means that much of the input
power is converted to heat.
• A class A amplifier conducts for the entire signal
cycle and has the lowest efficiency.
• A class B amplifier conducts for only half of the
signal cycle.
• A class C amplifier conducts for less than half of
the signal cycle.
• A class D amplifier switches between cutoff and
saturation.
Power
Amplifier
PIN
Efficiency =
Input signal
POUT
POUT
PIN
Output signal
HEAT = PIN - POUTHigh efficiency means less heat.
Efficiency
• The dc power supplied to an amplifier is
PIN = VCC xIDC
• Efficiency = POUT/PIN x 100%
• The maximum efficiency for Class A
amplifiers with a dc collector resistance
and a separate load resistance is 25%.
• Class A is usually not acceptable when
watts of power are required.
t
IC
t
IC
t
IC
t
IC
ISAT
A B
C D
The major classes of amplifier operation
Class and efficiency quiz
If POUT = 100 W and PIN = 200 W, the
efficiency is _________. 50%
The efficiency of an ideal amplifier is
__________. 100%
When efficiency is poor, too much of the input
is converted to ________. heat
An amplifier that conducts for the entire cycle
is operating Class _______. A
An amplifier that conducts for half the cycle
is operating Class _______. B
Concept Preview
• Class A amplifiers operate at the center of the load
line and have a large quiescent current flow.
• Class B amplifiers operate at cutoff and have no
quiescent current flow.
• Class B amplifiers are usually operated in push-
pull configurations.
• Class B amplifiers have crossover distortion.
• Class AB reduces crossover distortion.
• Bridge amplifiers provide four times the output
power and eliminate the output coupling capacitor.
Class A amplifier
 The Q point is chosen at the middle of load line
 This will give equal swing on either direction
 Both halves of the input comes at the output
 Hence Class A will give (amplitude) distortionless
output
 It can handle only small signals
 Its efficiency is less
Ic
Vce
Ib = 60μA
Ib = 50μA
Ib = 20μA
Ib = 30μA
Ib = 40μA
10mA
2mA
4mA
6mA
8mA
24 V0 V
Q
A
B
10mA
6mA
4mA
Class A
A large-signal amplifier can also be called a power amplifier.
This class A amplifier has a large quiescent collector current.
C
B
E
VCC = 18 V
RL = 12 ΩRB = 1.2 kΩ
CC
β = 60
ΙΒ =
VCC
RB
18 V
1.2 kΩ
= = 15 mA
IC = β x IB = 60 x 15 mA = 0.9 A
0 2 4 6 8 10 12 14 16 18
0.2
0.4
0.6
0.8
1.0
1.2
1.4
VCE in Volts
IC in A
5 mA
0 mA
25 mA
20 mA
15 mA
10 mA
ISAT =
VCC
RL
18 V
12 Ω
= = 1.5 A
Q
This is a Class A amplifier.
PC = VCE x IC = 7.2 V x 0.9 A = 6.48 W
Class B amplifier
 The Q point is chosen at the cut-off point
 This will give swing only on one direction
 Only one half of the input comes at the output
 Hence Class B will give (amplitude) distorted
output
 It can handle large signals
 Its efficiency is high
 It conducts for 1800
Ic
Vce
Ib = 60μA
Ib = 50μA
Ib = 20μA
Ib = 30μA
Ib = 40μA
10mA
2mA
4mA
6mA
8mA
24 V0 V
Q
10mA
0mA
Class B
0 2 4 6 8 10 12 14 16 18
0.2
0.4
0.6
0.8
1.0
1.2
1.4
VCE in Volts
IC in A
5 mA
0 mA
25 mA
20 mA
15 mA
10 mA
Q
This is a Class B amplifier.
PC = VCE x IC = 18 V x 0 A = 0 W
Its quiescent power dissipation is zero.
0 2 4 6 8 10 12 14 16
0.2
0.4
0.6
0.8
1.0
1.2
1.4
5 mA
0 mA
25 mA
20 mA
15 mA
10 mA
ClassB
The collector signal
is too distorted for
linear applications.
C
B
C
B
E
E
+VCC
The complementary-symmetry Class B
push-pull amplifier has acceptable
linearity for some applications.
NPN
PNP
NPN
PNP
Class B
C
B
C
B
E
E
+VCC
Since the base-emitter junction potential
is 0.7 V, there is some crossover distortion.
NPN
PNP
C
B
C
B
E
E
+VCC
Crossover distortion is eliminated
by applying some forward bias
to the transistors (class AB).
NPN
PNP
1.4 V
0 2 4 6 8 10 12 14 16 18
0.2
0.4
0.6
0.8
1.0
1.2
1.4
VCE in Volts
IC in A
Q
The quiescent power dissipation is moderate for class AB.
The efficiency is much better than class A.
Cap. required
+VCC
RL
RL
+VCC
Single-ended amplifier
A bridge-tied load provides four times the output
power for a given supply voltage and load resistance.
+VCC
2
Max.
Max. = VCC
Bridge amplifier
Max. = 2 x VCC
Max.
Class A, B, and AB quiz
Class A amplifiers are biased to operate near
the ________ of the load line. center
Class B amplifiers have their Q-points at
____________. cutoff
The conduction angle for class B is
_________. 180o
To reduce distortion, two class B transistors
are arranged in _____________. push-pull
Class AB is a solution for __________
distortion. crossover
Concept Review
• Class A amplifiers operate at the center of the load
line and have a large quiescent current flow.
• Class B amplifiers operate at cutoff and have no
quiescent current flow.
• Class B amplifiers are usually operated in push-
pull configurations.
• Class B amplifiers have crossover distortion.
• Class AB reduces crossover distortion.
• Bridge amplifiers provide four times the output
power and eliminate the output coupling capacitor.
Repeat Segment
Concept Preview
• Class C amplifiers are biased beyond cutoff for a
small conduction angle and high efficiency.
• Class C amplifiers used tuned tank circuits to
reduce distortion in RF applications.
• Class C amplifiers cannot be used in wideband
applications like audio.
• Class D amplifiers switch between cutoff and
saturation for very high efficiency.
• Class D amplifiers operate at a relatively high
switching frequency and often use PWM.
• Class D can be used in audio applications.
0 2 4 6 8 10 12 14 16 18
0.2
0.4
0.6
0.8
1.0
1.2
1.4
A
B
C
AB
The class of an amplifier
is determined by the bias
which establishes the Q-point.
Class C is established by reverse
biasing the base-emitter junction.
Class C amplifier
 The Q point is chosen at the beyond the cut-off
point
 This will give only a partial swing in one direction
 Only a portion of the input comes at the output
 Hence Class C will give (amplitude) severely
distorted output
 It can handle large signals
 It conducts for less than 1800
Ic
Vce
Ib = 60μA
Ib = 50μA
Ib = 20μA
Ib = 30μA
Ib = 40μA
10mA
2mA
4mA
6mA
8mA
24 V0 V
Q`
10mA
0mA
Class C
Class A
Class B
Class C
Conduction Angles
& theoretical max. efficiencies:
 Class A = 360o
50 %*
 Class B = 180o
78.5 %
 Class AB ≅ 200o
(between A & B)
 Class C ≅ 90o
100 %
*Class A amplifiers are seldom driven to
maximum output and typically provide much
less efficiency.
C
B
E
VCC
RB
CC
VBB
Class C amplifier
VBB reverse biases the base-emitter junction.
Tank circuit
The transistor is
off for most of
the input cycle
and the conduction
angle is small.
VBB
0.7 V
0 A
VBE waveform
IC waveform
VCE waveform
Class C amplifier
waveforms
(with tank circuit)
Low VCE when IC is flowing
C
B
E
VCC
RB
CC
Class C amplifier with signal bias
The base-emitter
junction rectifies
the input signal
and charges CC.
Signal bias increases when the input
signal increases in amplitude.
IB >> 0
Three transistor operating modes:
IB = 0 IB > 0
Cutoff Linear
(PC > 0)
Saturation
PC = 0 in both of these modes
Distortionless amplifier
 Out of the 3 amplifiers, Class C is unsuitable as the
distortion is very heavy
 Class A is the best, as it gives distortionless output
 But Class A cannot handle large signals as
required by the Power Amplifier
 Though Class B gives heavy distortion, it gives out
one half of the signal perfectly
 And Class B can handle large signals
Class A Audio Amplifier
 As we have seen out of the 3 classifications, Class
A is the best, as it does not give any distortion
 Among the configurations, we know that CE is the
best as it gives maximum power gain
 A CE amplifier will have high output impedance
 Unfortunately for an audio amplifier, the output
device is the speaker which has a low impedance
Impedance Matching
 The speaker impedance is typically about 4 Ω
 Hence there is a mismatch between the high Zo of
the amplifier and the low impedance of the speaker
 This will result in loss of gain
 This can be avoided by connecting a transformer at
the output stage
 The primary winding will match the high Zo of the
amplifier while the secondary will match the low
impedance of the speaker
Class A Audio Amplifier
270 K 5.6 K
Re
Rb1
Rb2 Ce
Rc
Vcc
270 K
Re
Rb1
Rb2 Ce
Drawback
 The drawback of this circuit is that it cannot
handle large signals
 In a Class A amplifier, the operating point is
chosen around the middle of the load line
 If the signal exceeds the cut-off point, the output
current stops and any signal with a lower
amplitude will not come at the output
 Similarly, if the signal exceeds the saturation
point, the output current cannot increase any
further, even if the input signal increases
Ic
Vce
Ib = 60μA
Ib = 50μA
Ib = 20μA
Ib = 30μA
Ib = 40μA
10mA
2mA
4mA
6mA
8mA
24 V0 V
Q
A
B Class A
Class B Push-Pull Amplifier
 To avoid this we can use Class B which has a
greater signal handling capacity
 But Class B will give only one half of the signal
 Hence we can use 2 Class B amplifiers
 One for one half and one for the other half
 This type of amplifier is called Push-Pull
Amplifier
Class B Push-Pull
Vcc
T1
T2
T3
TR2
TR1
Push-Pull Circuit
 TR1 and TR2 are output transistors connected
back to back, with their emitters grounded
 The output transformer TR1 couples the push-pull
output to the speaker
 In the Push-Pull arrangement T1 conducts for one
half of the signal & T2 conducts for the other half
 Both are biased in Class B and each gives one half
of the signal & the combined output is coupled to
the speaker
Push-Pull Circuit
 The Driver Transformer TR2 gives 2 out of phase
signals
 During one half, the +ve half forward biases T1
while the –ve half reverse biases T2
 Thus when T1 conducts, T2 is cut-off & vice-
versa
 This way both the transistors conduct alternately
to give the full signal output
Class D Amplifier
 During the +ve half cycle Q1 gets Forward Bias and it
conducts
 During the -ve half cycle Q2 gets Forward Bias and it
conducts
 Thus both the transistors conduct alternately
 The amplifier works for 3600
 No distortion
 100% efficiency
 During the first half T1
conducts
 Ic flows from the
centre-tapping through
T1 to ground
 This half is coupled to
the speaker through
TR1
Working of Push-Pull Circuit
Vcc
T1
T2
T
3
TR2
TR1
 During the second half
T2 conducts
 Ic flows from the
centre-tapping through
T2 to ground
 This half is coupled to
the speaker through
TR1
Working of Push-Pull Circuit
Vcc
T1
T2
T
3
TR2
TR1
Drawbacks
 Though this circuit functions well it has a few
drawbacks
 Transformer coupling affects the quality of
output
 Phase shifting circuit is a must
 Both these drawbacks can be avoided if we use
one pair of PNP and NPN transistors at the
output
T1
T2
Vcc Complementary Symmetry Amplifier
Complementary Symmetry Amplifier
 This circuit uses one NPN transistor & one PNP
transistor at the output stage
 During the +ve half, T1(NPN) base gets forward bias &
it conducts while T2 (PNP) gets reverse biased and does
not conduct
 This gives one half of the signal at the speaker coupled
to the emitter
Complementary Symmetry Amplifier
 During the other half, T2 gets forward bias
and conducts while T1 gets reverse biased and
does not conduct
 Thus T1 & T2 conduct alternately giving a
distortionless output
 This circuit does not require a phase shifter
Cross – over distortion
 Class B Push-Pull amplifier has one limitation
 As the phase of the signal changes from +ve to –ve
(or vice-versa) one transistor stops conducting
while the other begins conducting
 But the transistor cannot conduct instantaneously
as it requires a minimum Vbe before it starts
conducting
 Thus as the signal crosses over zero, a distortion
occurs
 This is called Cross over distortion
Cross – over distortion
Vbe
-Vbe
Class AB amplifier
 This circuit overcomes cross-over distortion
 Biasing is done such that even if there is no input
signal, a small current keeps the output transistor
conducting
 This circuit uses 2 diodes whose characteristics
matches with that of the BE junction of the output
transistors
 Biasing resistors R1 & R2 are also identical values
T1
T2
Vcc Class AB amplifier
R1
R2
D1
D2
Symmetrical components
 Since R1 & D1 are identical to R2 & D2, the diode
junction as well as the output point will be at half
the supply voltage
 Because of symmetry both T1 & T2 will conduct
equally
 Even when there is no input signal, there will be a
current Icq = (I/2 Vcc – 0.6) / R1
 This will keep the output transistors conducting
Elimination of cross-over distortion
 Normally, during cross-over there will not be any
output till the non-conducting transistor gets the
minimum Vbe
 This causes distortion
 This has been eliminated here, since the 0.6 V
across the diodes keep the transistors on and gives
a continuous output signal without producing
cross-over distortion
Thermal stability
 In addition, the two diodes also provide thermal
stability
 They prevent the output transistors going to
Thermal Run Away
 When the output current is high, heat dissipation is
more
 The increase in temperature produces more charge
carrier in the BE junction of T1 & T2
 This increases Ib & hence Ic
 This in turn increases the power dissipation &
hence the heat
 This chain goes on till too much current flows and
destroys the transistors
 This is called Thermal Run Away
 This is arrested by the diodes in the output circuit
 When the charge carriers increase in the B-E
junction of T1 & T2, a similar increase takes place
in D1 & D2, due to matching characteristics
 This increase in the diode current, produces more
drop across R1 & R2 and brings down the forward
bias at the base of T1 & T2
 Thus the 2 diodes prevent cross-over distortion as
well as provide thermal stability
A switch-mode amplifier uses a
rectangular input signal to drive the
transistor rapidly between cutoff and
saturation. The efficiency is very high.
C
B
E
RB
They are also
called Class D
amplifiers.
If the switching frequency is a good deal higher
than the signal frequency, a Class D amplifier is
capable of linear amplification. Pulse-width
modulation and a low-pass filter are often used.
PWM Signal
Input Signal
PWM LPF
The low-pass filter rejects
the switching frequency.
Class C and D quiz
Class C amplifiers use _______ circuits to
restore sinusoidal signals. tank
The base-emitter junction in a class C
amplifier is ________ biased. reverse
The theoretical maximum efficiency for
class C is ___________. 100%
Class D amplifiers are also known as
__________ amplifiers. switch-mode
Class D amplifiers employ a varying duty-
cycle known as _________. PWM
Concept Review
• Class C amplifiers are biased beyond cutoff for a
small conduction angle and high efficiency.
• Class C amplifiers used tuned tank circuits to
reduce distortion in RF applications.
• Class C amplifiers cannot be used in wideband
applications like audio.
• Class D amplifiers switch between cutoff and
saturation for very high efficiency.
• Class D amplifiers operate at a relatively high
switching frequency and often use PWM.
• Class D can be used in audio applications.
Repeat Segment

267182869 large-signal-amplifiers-ppt

  • 1.
  • 2.
    Classification of PowerAmplifiers  Power amplifiers are classified based on the Q point  If the operating point is chosen at the middle of the load line, it is called Class A amplifier  If the operating point is chosen at the cut-off point it is called Class B amplifier  If the operating point is chosen beyond the cut-off point it is called Class C amplifier  It conducts for 3600
  • 3.
    Concept Preview • Efficiencyis most important in power amplifiers. • Poor efficiency means that much of the input power is converted to heat. • A class A amplifier conducts for the entire signal cycle and has the lowest efficiency. • A class B amplifier conducts for only half of the signal cycle. • A class C amplifier conducts for less than half of the signal cycle. • A class D amplifier switches between cutoff and saturation.
  • 4.
    Power Amplifier PIN Efficiency = Input signal POUT POUT PIN Outputsignal HEAT = PIN - POUTHigh efficiency means less heat.
  • 5.
    Efficiency • The dcpower supplied to an amplifier is PIN = VCC xIDC • Efficiency = POUT/PIN x 100% • The maximum efficiency for Class A amplifiers with a dc collector resistance and a separate load resistance is 25%. • Class A is usually not acceptable when watts of power are required.
  • 6.
    t IC t IC t IC t IC ISAT A B C D Themajor classes of amplifier operation
  • 7.
    Class and efficiencyquiz If POUT = 100 W and PIN = 200 W, the efficiency is _________. 50% The efficiency of an ideal amplifier is __________. 100% When efficiency is poor, too much of the input is converted to ________. heat An amplifier that conducts for the entire cycle is operating Class _______. A An amplifier that conducts for half the cycle is operating Class _______. B
  • 8.
    Concept Preview • ClassA amplifiers operate at the center of the load line and have a large quiescent current flow. • Class B amplifiers operate at cutoff and have no quiescent current flow. • Class B amplifiers are usually operated in push- pull configurations. • Class B amplifiers have crossover distortion. • Class AB reduces crossover distortion. • Bridge amplifiers provide four times the output power and eliminate the output coupling capacitor.
  • 9.
    Class A amplifier The Q point is chosen at the middle of load line  This will give equal swing on either direction  Both halves of the input comes at the output  Hence Class A will give (amplitude) distortionless output  It can handle only small signals  Its efficiency is less
  • 10.
    Ic Vce Ib = 60μA Ib= 50μA Ib = 20μA Ib = 30μA Ib = 40μA 10mA 2mA 4mA 6mA 8mA 24 V0 V Q A B 10mA 6mA 4mA Class A
  • 11.
    A large-signal amplifiercan also be called a power amplifier. This class A amplifier has a large quiescent collector current. C B E VCC = 18 V RL = 12 ΩRB = 1.2 kΩ CC β = 60 ΙΒ = VCC RB 18 V 1.2 kΩ = = 15 mA IC = β x IB = 60 x 15 mA = 0.9 A
  • 12.
    0 2 46 8 10 12 14 16 18 0.2 0.4 0.6 0.8 1.0 1.2 1.4 VCE in Volts IC in A 5 mA 0 mA 25 mA 20 mA 15 mA 10 mA ISAT = VCC RL 18 V 12 Ω = = 1.5 A Q This is a Class A amplifier. PC = VCE x IC = 7.2 V x 0.9 A = 6.48 W
  • 13.
    Class B amplifier The Q point is chosen at the cut-off point  This will give swing only on one direction  Only one half of the input comes at the output  Hence Class B will give (amplitude) distorted output  It can handle large signals  Its efficiency is high  It conducts for 1800
  • 14.
    Ic Vce Ib = 60μA Ib= 50μA Ib = 20μA Ib = 30μA Ib = 40μA 10mA 2mA 4mA 6mA 8mA 24 V0 V Q 10mA 0mA Class B
  • 15.
    0 2 46 8 10 12 14 16 18 0.2 0.4 0.6 0.8 1.0 1.2 1.4 VCE in Volts IC in A 5 mA 0 mA 25 mA 20 mA 15 mA 10 mA Q This is a Class B amplifier. PC = VCE x IC = 18 V x 0 A = 0 W Its quiescent power dissipation is zero.
  • 16.
    0 2 46 8 10 12 14 16 0.2 0.4 0.6 0.8 1.0 1.2 1.4 5 mA 0 mA 25 mA 20 mA 15 mA 10 mA ClassB The collector signal is too distorted for linear applications.
  • 17.
    C B C B E E +VCC The complementary-symmetry ClassB push-pull amplifier has acceptable linearity for some applications. NPN PNP
  • 18.
  • 19.
    C B C B E E +VCC Since the base-emitterjunction potential is 0.7 V, there is some crossover distortion. NPN PNP
  • 20.
    C B C B E E +VCC Crossover distortion iseliminated by applying some forward bias to the transistors (class AB). NPN PNP 1.4 V
  • 21.
    0 2 46 8 10 12 14 16 18 0.2 0.4 0.6 0.8 1.0 1.2 1.4 VCE in Volts IC in A Q The quiescent power dissipation is moderate for class AB. The efficiency is much better than class A.
  • 22.
    Cap. required +VCC RL RL +VCC Single-ended amplifier Abridge-tied load provides four times the output power for a given supply voltage and load resistance. +VCC 2 Max. Max. = VCC Bridge amplifier Max. = 2 x VCC Max.
  • 23.
    Class A, B,and AB quiz Class A amplifiers are biased to operate near the ________ of the load line. center Class B amplifiers have their Q-points at ____________. cutoff The conduction angle for class B is _________. 180o To reduce distortion, two class B transistors are arranged in _____________. push-pull Class AB is a solution for __________ distortion. crossover
  • 24.
    Concept Review • ClassA amplifiers operate at the center of the load line and have a large quiescent current flow. • Class B amplifiers operate at cutoff and have no quiescent current flow. • Class B amplifiers are usually operated in push- pull configurations. • Class B amplifiers have crossover distortion. • Class AB reduces crossover distortion. • Bridge amplifiers provide four times the output power and eliminate the output coupling capacitor. Repeat Segment
  • 25.
    Concept Preview • ClassC amplifiers are biased beyond cutoff for a small conduction angle and high efficiency. • Class C amplifiers used tuned tank circuits to reduce distortion in RF applications. • Class C amplifiers cannot be used in wideband applications like audio. • Class D amplifiers switch between cutoff and saturation for very high efficiency. • Class D amplifiers operate at a relatively high switching frequency and often use PWM. • Class D can be used in audio applications.
  • 26.
    0 2 46 8 10 12 14 16 18 0.2 0.4 0.6 0.8 1.0 1.2 1.4 A B C AB The class of an amplifier is determined by the bias which establishes the Q-point. Class C is established by reverse biasing the base-emitter junction.
  • 27.
    Class C amplifier The Q point is chosen at the beyond the cut-off point  This will give only a partial swing in one direction  Only a portion of the input comes at the output  Hence Class C will give (amplitude) severely distorted output  It can handle large signals  It conducts for less than 1800
  • 28.
    Ic Vce Ib = 60μA Ib= 50μA Ib = 20μA Ib = 30μA Ib = 40μA 10mA 2mA 4mA 6mA 8mA 24 V0 V Q` 10mA 0mA Class C
  • 29.
  • 30.
    Conduction Angles & theoreticalmax. efficiencies:  Class A = 360o 50 %*  Class B = 180o 78.5 %  Class AB ≅ 200o (between A & B)  Class C ≅ 90o 100 % *Class A amplifiers are seldom driven to maximum output and typically provide much less efficiency.
  • 31.
    C B E VCC RB CC VBB Class C amplifier VBBreverse biases the base-emitter junction. Tank circuit The transistor is off for most of the input cycle and the conduction angle is small.
  • 32.
    VBB 0.7 V 0 A VBEwaveform IC waveform VCE waveform Class C amplifier waveforms (with tank circuit) Low VCE when IC is flowing
  • 33.
    C B E VCC RB CC Class C amplifierwith signal bias The base-emitter junction rectifies the input signal and charges CC. Signal bias increases when the input signal increases in amplitude.
  • 34.
    IB >> 0 Threetransistor operating modes: IB = 0 IB > 0 Cutoff Linear (PC > 0) Saturation PC = 0 in both of these modes
  • 35.
    Distortionless amplifier  Outof the 3 amplifiers, Class C is unsuitable as the distortion is very heavy  Class A is the best, as it gives distortionless output  But Class A cannot handle large signals as required by the Power Amplifier  Though Class B gives heavy distortion, it gives out one half of the signal perfectly  And Class B can handle large signals
  • 36.
    Class A AudioAmplifier  As we have seen out of the 3 classifications, Class A is the best, as it does not give any distortion  Among the configurations, we know that CE is the best as it gives maximum power gain  A CE amplifier will have high output impedance  Unfortunately for an audio amplifier, the output device is the speaker which has a low impedance
  • 37.
    Impedance Matching  Thespeaker impedance is typically about 4 Ω  Hence there is a mismatch between the high Zo of the amplifier and the low impedance of the speaker  This will result in loss of gain  This can be avoided by connecting a transformer at the output stage  The primary winding will match the high Zo of the amplifier while the secondary will match the low impedance of the speaker
  • 38.
    Class A AudioAmplifier 270 K 5.6 K Re Rb1 Rb2 Ce Rc Vcc 270 K Re Rb1 Rb2 Ce
  • 39.
    Drawback  The drawbackof this circuit is that it cannot handle large signals  In a Class A amplifier, the operating point is chosen around the middle of the load line  If the signal exceeds the cut-off point, the output current stops and any signal with a lower amplitude will not come at the output  Similarly, if the signal exceeds the saturation point, the output current cannot increase any further, even if the input signal increases
  • 40.
    Ic Vce Ib = 60μA Ib= 50μA Ib = 20μA Ib = 30μA Ib = 40μA 10mA 2mA 4mA 6mA 8mA 24 V0 V Q A B Class A
  • 41.
    Class B Push-PullAmplifier  To avoid this we can use Class B which has a greater signal handling capacity  But Class B will give only one half of the signal  Hence we can use 2 Class B amplifiers  One for one half and one for the other half  This type of amplifier is called Push-Pull Amplifier
  • 42.
  • 43.
    Push-Pull Circuit  TR1and TR2 are output transistors connected back to back, with their emitters grounded  The output transformer TR1 couples the push-pull output to the speaker  In the Push-Pull arrangement T1 conducts for one half of the signal & T2 conducts for the other half  Both are biased in Class B and each gives one half of the signal & the combined output is coupled to the speaker
  • 44.
    Push-Pull Circuit  TheDriver Transformer TR2 gives 2 out of phase signals  During one half, the +ve half forward biases T1 while the –ve half reverse biases T2  Thus when T1 conducts, T2 is cut-off & vice- versa  This way both the transistors conduct alternately to give the full signal output
  • 45.
    Class D Amplifier During the +ve half cycle Q1 gets Forward Bias and it conducts  During the -ve half cycle Q2 gets Forward Bias and it conducts  Thus both the transistors conduct alternately  The amplifier works for 3600  No distortion  100% efficiency
  • 46.
     During thefirst half T1 conducts  Ic flows from the centre-tapping through T1 to ground  This half is coupled to the speaker through TR1 Working of Push-Pull Circuit Vcc T1 T2 T 3 TR2 TR1
  • 47.
     During thesecond half T2 conducts  Ic flows from the centre-tapping through T2 to ground  This half is coupled to the speaker through TR1 Working of Push-Pull Circuit Vcc T1 T2 T 3 TR2 TR1
  • 48.
    Drawbacks  Though thiscircuit functions well it has a few drawbacks  Transformer coupling affects the quality of output  Phase shifting circuit is a must  Both these drawbacks can be avoided if we use one pair of PNP and NPN transistors at the output
  • 49.
  • 50.
    Complementary Symmetry Amplifier This circuit uses one NPN transistor & one PNP transistor at the output stage  During the +ve half, T1(NPN) base gets forward bias & it conducts while T2 (PNP) gets reverse biased and does not conduct  This gives one half of the signal at the speaker coupled to the emitter
  • 51.
    Complementary Symmetry Amplifier During the other half, T2 gets forward bias and conducts while T1 gets reverse biased and does not conduct  Thus T1 & T2 conduct alternately giving a distortionless output  This circuit does not require a phase shifter
  • 52.
    Cross – overdistortion  Class B Push-Pull amplifier has one limitation  As the phase of the signal changes from +ve to –ve (or vice-versa) one transistor stops conducting while the other begins conducting  But the transistor cannot conduct instantaneously as it requires a minimum Vbe before it starts conducting  Thus as the signal crosses over zero, a distortion occurs  This is called Cross over distortion
  • 53.
    Cross – overdistortion Vbe -Vbe
  • 54.
    Class AB amplifier This circuit overcomes cross-over distortion  Biasing is done such that even if there is no input signal, a small current keeps the output transistor conducting  This circuit uses 2 diodes whose characteristics matches with that of the BE junction of the output transistors  Biasing resistors R1 & R2 are also identical values
  • 55.
    T1 T2 Vcc Class ABamplifier R1 R2 D1 D2
  • 56.
    Symmetrical components  SinceR1 & D1 are identical to R2 & D2, the diode junction as well as the output point will be at half the supply voltage  Because of symmetry both T1 & T2 will conduct equally  Even when there is no input signal, there will be a current Icq = (I/2 Vcc – 0.6) / R1  This will keep the output transistors conducting
  • 57.
    Elimination of cross-overdistortion  Normally, during cross-over there will not be any output till the non-conducting transistor gets the minimum Vbe  This causes distortion  This has been eliminated here, since the 0.6 V across the diodes keep the transistors on and gives a continuous output signal without producing cross-over distortion
  • 58.
    Thermal stability  Inaddition, the two diodes also provide thermal stability  They prevent the output transistors going to Thermal Run Away  When the output current is high, heat dissipation is more  The increase in temperature produces more charge carrier in the BE junction of T1 & T2
  • 59.
     This increasesIb & hence Ic  This in turn increases the power dissipation & hence the heat  This chain goes on till too much current flows and destroys the transistors  This is called Thermal Run Away  This is arrested by the diodes in the output circuit
  • 60.
     When thecharge carriers increase in the B-E junction of T1 & T2, a similar increase takes place in D1 & D2, due to matching characteristics  This increase in the diode current, produces more drop across R1 & R2 and brings down the forward bias at the base of T1 & T2  Thus the 2 diodes prevent cross-over distortion as well as provide thermal stability
  • 61.
    A switch-mode amplifieruses a rectangular input signal to drive the transistor rapidly between cutoff and saturation. The efficiency is very high. C B E RB They are also called Class D amplifiers.
  • 62.
    If the switchingfrequency is a good deal higher than the signal frequency, a Class D amplifier is capable of linear amplification. Pulse-width modulation and a low-pass filter are often used. PWM Signal Input Signal
  • 63.
    PWM LPF The low-passfilter rejects the switching frequency.
  • 64.
    Class C andD quiz Class C amplifiers use _______ circuits to restore sinusoidal signals. tank The base-emitter junction in a class C amplifier is ________ biased. reverse The theoretical maximum efficiency for class C is ___________. 100% Class D amplifiers are also known as __________ amplifiers. switch-mode Class D amplifiers employ a varying duty- cycle known as _________. PWM
  • 65.
    Concept Review • ClassC amplifiers are biased beyond cutoff for a small conduction angle and high efficiency. • Class C amplifiers used tuned tank circuits to reduce distortion in RF applications. • Class C amplifiers cannot be used in wideband applications like audio. • Class D amplifiers switch between cutoff and saturation for very high efficiency. • Class D amplifiers operate at a relatively high switching frequency and often use PWM. • Class D can be used in audio applications. Repeat Segment