Small signal amplifiers
Download
Report
Transcript Small signal amplifiers
Power Amplifiers
Unit – 4.1
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
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
B
Ib = 60μA
10mA
Ib = 50μA
8mA
Q
6mA
Ib = 40μA
Ib = 30μA
4mA
Ib = 20μA
2mA
A
0V
24 V
Vce
Class A
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
Ib = 60μA
10mA
Ib = 50μA
8mA
Ib = 40μA
6mA
Ib = 30μA
4mA
Ib = 20μA
2mA
Q
0V
Class B
24 V
Vce
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
Ib = 60μA
10mA
Ib = 50μA
8mA
Ib = 40μA
6mA
Ib = 30μA
4mA
Ib = 20μA
2mA
Q`
0V
Class C
24 V
Vce
Class A
Class B
Class C
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
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
The
Class A Audio Amplifier
Vcc
Rb1
270 K
Rb2
Rb1
Rc
5.6 K
Re
270 K
Ce
Rb2
Re
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
Class A
B
Ib = 60μA
10mA
Ib = 50μA
8mA
Q
6mA
Ib = 40μA
Ib = 30μA
4mA
Ib = 20μA
2mA
A
0V
24 V
Vce
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
Vcc
T1
TR1
TR2
T3
T2
Class B Push-Pull
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 & viceversa
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
Working of Push-Pull Circuit
Vcc
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
T1
TR2
T
3
T2
TR1
Working of Push-Pull Circuit
Vcc
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
T1
TR2
T
3
T2
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
Vcc
Complementary Symmetry Amplifier
T1
T2
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
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