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Chapter 5: FEEDBACK IN AMPLIFIER Dr. Gopika Sood, PG Govt. College For Girls, Sector -11, Chandigarh.

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Presentation on theme: "Chapter 5: FEEDBACK IN AMPLIFIER Dr. Gopika Sood, PG Govt. College For Girls, Sector -11, Chandigarh."— Presentation transcript:

1 Chapter 5: FEEDBACK IN AMPLIFIER Dr. Gopika Sood, PG Govt. College For Girls, Sector -11, Chandigarh

2 OUTLINE  Feedback in Amplifier  Advantages Of Negative Feedback  Stability of gain  Noise reduction  Reduction in Non-linear and Phase Distortion  Effect on Input and Ouput Impedance  Improvement of Frequency Response  Emitter Follower  Operational Amplifier

3 FEEDBACK IN AMPLIFIER FEEDBACK : It is a process in which a portion of the output energy (voltage or current) is transferred to the input of the system. Feedback in amplifier is of two types :  Positive, Direct or regenerative feedback  Negative, Inverse or Degenerative feedback Positive feedback : If the feedback energy is in phase with the input energy, it reinforces or enhances the input signal energy, then it is called positive feedback. Negative feedback : When the feedback energy is in out of phase (180 o phase) with the input energy, it reduces or diminishes the input signal energy, the feedback is called positive feedback. Classification of Feedback Voltage Feedback : It is the feedback in which the feedback energy is proportional to the output voltage of the amplifier. Current feedback : It is the feedback in which the feedback energy is proportional to the output current of the amplifier. Compound feedback : It is the feedback in which the feedback energy is partly proportional to the output voltage of the amplifier and partly proportional to the output current.

4 A - gain of the amplifier with no feedback V o – Output of amplifier V i – Input voltage of amplifier V s – Input signal voltage to the feedback amplifier V f - Feedback voltage A f – Voltage gain with feedback THEORY FOR FEEDBACK

5 The feedback fraction can be written as  = V f /V o V i = V s  V f V i = V s – V f Voltage gain with feedback A f = V o /V i V o = A V i V o = A (V s - V f ) V o (1+A  ) = AV s V o /V s = A/(1+A  ) A f = A/(1+ A  ) THEORY FOR FEEDBACK

6 A f = A/(1+ A  ) The feedback fraction  of output can be positive, negative or real number or a complex function of frequency. The following cases may arise from the above equation  If | 1+A  | > 1, we have |A f | < |A| then feedback is negative feedback which is used in amplifiers  If | 1+A  | = 0, we have |A f | =  implying that amplifier can give the output without input signal, the amplifier becomes an oscillator.  If | 1+A  | |A| then feedback is positive feedback. Feedback causes instability in the oscillations in the operation of the transistor CONDITIONS NECESSARY FOR FEEDBACK

7 ADVANTAGES OF NEGATIVE FEEDBACK Negative feedback produces various advantageous effects to improve the performance of amplifiers  Gain of the amplifier is stabilized against the variations I the values of trnsistor hybrid parameters like h fe  It reduces the non-linear distortion and improves the signal handling capacity of the amplifier  The noise level in the output of the amplifier is reduced  The phase distortion is reduced  The bandwidth of the amplifier is increased and the frequency distortion is reduced  Input and output impedances of the amplifier may be changed by combining the feedback signal with the externally applied signal

8 STABILITY OF GAIN Overall gain of the amplifier is given by A f = A/(1+ A  ) The stability of the gain can be reduced by differentiating the eq log A f = log A – log (1+ A  ) dA f /A f = dA/A ((1+  A -  A)/ /(1+ A  )) = dA/A (1/(1+ A  )) S = (dA f /A f )/(dA/A) = (1/(1+ A  )) Desensitivity, D = 1/S = (1/(1+ A  )) dA f /A f = 1/D (dA/A)

9 REDUCTION IN NON-LINEAR DISTORTION

10 REDUCTION IN NOISE Negative feedback reduces the noise level in the output signal V no = noise output without feedback V n = input noise voltage without feedback A = voltage gain of the internal amplifier V no = AV n V’ no = noise output with feedback V’ n = input noise voltage with feedback V’ n = V n -  V’ no V’ no = AV’ n = A(V n -  V’ no ) V’ no = AV n - A  V’ no V’ no (1+A  ) = AV n V’ no = 1/(1+A  ) AV n

11 IMPROVEMENT IN FREQUENCY RESPONSE

12 REDUCTION IN PHASE DISTORTION


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