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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
 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
                                             
                                             
                   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