Feedback Concept
Depending on the relative polarity of the signal being fed back into a circuit,
feedback is classified as
 Positive feedback.
 Negative feedback.
 Negative feedback results in decreased voltage gain, for which a number of
circuit features are improved .
 Positive feedback drives a circuit into oscillation as in various types of oscillator
circuits.
Negative Feedback Properties
• Since Negative feedback reduces the transfer gain, why it is used?
– The answer is that many desirable characteristics are obtained for the price of gain
reduction.
• A negative feedback
Desensitizes the gain of an amplifier
-Make the gain less sensitive to circuit and temperature variations
Reduces nonlinear distortion
-Make the output proportional to input
Reduces the effect of noise
-Minimize the contribution of output unwanted signals
Controls the input and output impedances
-Raise or lower the input and output impedances
Extends the bandwidth of the amplifier
-Increases the bandwidth
Feedback – a historical perspective
• All Op-amp circuits employ negative feedback.
• In a CE amplifier, introducing an emitter resistor RE,
improves the stability but decreases the gain. This is
due to a negative feedback.
Negative Feedback Applications
Basic configuration of a feed-back amplifier
• Si  the primary input.
• S the error signal.
• A  open loop gain of the amplifier.
• So the output.
•   Feedback factor
• Sfb  Feedback signal
General Feedback Structure
Basic configuration of a feed-back amplifier
• The -ve sign at the summing node () indicates that Sfb is subtracted
from the input, which in turn becomes the new input to the
amplifier, which is amplified and delivered to the load, while a part
of it is fed back.
Ideal Closed Loop Signal Gain
• So = AS → (1); where S is the error signal.
• Sfb =  So → (2)
• At the summing node we have S = Si − Sfb;
Ideal Closed Loop Signal Gain
•  (1) →So = A(Si − Sfb)
• So = ASi – ASfb
• So = ASi – ASo from (2)
• Rearranging - i.e. – So to one side and Si to the other
• So+A So = ASi
• (1+A )So = ASi ;
• The closed loop gain Af = So/Si = A/(1+A)
• Af ≈ 1/ as A >> 1 ( For Negative Feedback)
• Define A  loop gain
• 1+A desensitivity factor.
Properties of Negative feedback
• Gain Desensitivity: Defines how the change in open loop gain (A)
affects the change in closed loop gain (Af).
Af = A/(1+A) → (1)
• Assume  is constant, taking differentials on both sides
→ (2)
• Dividing (2) by (1)
• The percentage change in gain Af is smaller than the percentage
change in A by the factor (1+A). Hence the name desensitivity
factor.
Copyright © 2017 McGraw-Hill Education. All rights reserved. No reproduction or distribution without the prior written consent of McGraw-Hill Education. 1
Properties of Feedback Circuits
• Bandwidth Modification:
• Suppose the feedforward amplifier above has a one-
pole transfer function
• A0 is the low-frequency gain and ω0 is the 3-dB
bandwidth
• Transfer function of the closed-loop system is
Copyright © 2017 McGraw-Hill Education. All rights reserved. No reproduction or distribution without the prior written consent of McGraw-Hill Education. 2
Properties of Feedback Circuits
• Bandwidth Modification:
• The closed-loop gain at low frequencies is reduced
by a factor of , and the 3-dB bandwidth is
increased by the same factor, revealing a pole at
ssssss
• If A is large enough, closed-loop gain remains
approximately equal to 1/β even if A experiences
substantial variations
• At high frequencies, A drops so that βA is
comparable to unity and closed-loop gain falls below
1/β
Copyright © 2017 McGraw-Hill Education. All rights reserved. No reproduction or distribution without the prior written consent of McGraw-Hill Education. 3
Effect of Feedback on Noise
• Feedback does not improve noise performance of
circuits
• In Fig. (a), the open-loop amplifier A1 is characterized
by only an input-referred noise voltage and the
feedback network is assumed to be noiseless
• We have (Vin – βVout + Vn)A1 = Vout, and hence
• Circuit can be modified as in Fig. (b), input-referred
noise is still Vn
Properties of Negative feedback
• Reduction in Nonlinear Distortion:

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Mod3_1_Introduction_to_Feedback_Amplifiers.pdf

  • 1. Feedback Concept Depending on the relative polarity of the signal being fed back into a circuit, feedback is classified as  Positive feedback.  Negative feedback.  Negative feedback results in decreased voltage gain, for which a number of circuit features are improved .  Positive feedback drives a circuit into oscillation as in various types of oscillator circuits.
  • 2. Negative Feedback Properties • Since Negative feedback reduces the transfer gain, why it is used? – The answer is that many desirable characteristics are obtained for the price of gain reduction. • A negative feedback Desensitizes the gain of an amplifier -Make the gain less sensitive to circuit and temperature variations Reduces nonlinear distortion -Make the output proportional to input Reduces the effect of noise -Minimize the contribution of output unwanted signals Controls the input and output impedances -Raise or lower the input and output impedances Extends the bandwidth of the amplifier -Increases the bandwidth
  • 3. Feedback – a historical perspective • All Op-amp circuits employ negative feedback. • In a CE amplifier, introducing an emitter resistor RE, improves the stability but decreases the gain. This is due to a negative feedback. Negative Feedback Applications
  • 4. Basic configuration of a feed-back amplifier • Si  the primary input. • S the error signal. • A  open loop gain of the amplifier. • So the output. •   Feedback factor • Sfb  Feedback signal General Feedback Structure
  • 5. Basic configuration of a feed-back amplifier • The -ve sign at the summing node () indicates that Sfb is subtracted from the input, which in turn becomes the new input to the amplifier, which is amplified and delivered to the load, while a part of it is fed back.
  • 6. Ideal Closed Loop Signal Gain • So = AS → (1); where S is the error signal. • Sfb =  So → (2) • At the summing node we have S = Si − Sfb;
  • 7. Ideal Closed Loop Signal Gain •  (1) →So = A(Si − Sfb) • So = ASi – ASfb • So = ASi – ASo from (2) • Rearranging - i.e. – So to one side and Si to the other • So+A So = ASi • (1+A )So = ASi ; • The closed loop gain Af = So/Si = A/(1+A) • Af ≈ 1/ as A >> 1 ( For Negative Feedback) • Define A  loop gain • 1+A desensitivity factor.
  • 8. Properties of Negative feedback • Gain Desensitivity: Defines how the change in open loop gain (A) affects the change in closed loop gain (Af). Af = A/(1+A) → (1) • Assume  is constant, taking differentials on both sides → (2) • Dividing (2) by (1) • The percentage change in gain Af is smaller than the percentage change in A by the factor (1+A). Hence the name desensitivity factor.
  • 9. Copyright © 2017 McGraw-Hill Education. All rights reserved. No reproduction or distribution without the prior written consent of McGraw-Hill Education. 1 Properties of Feedback Circuits • Bandwidth Modification: • Suppose the feedforward amplifier above has a one- pole transfer function • A0 is the low-frequency gain and ω0 is the 3-dB bandwidth • Transfer function of the closed-loop system is
  • 10. Copyright © 2017 McGraw-Hill Education. All rights reserved. No reproduction or distribution without the prior written consent of McGraw-Hill Education. 2 Properties of Feedback Circuits • Bandwidth Modification: • The closed-loop gain at low frequencies is reduced by a factor of , and the 3-dB bandwidth is increased by the same factor, revealing a pole at ssssss • If A is large enough, closed-loop gain remains approximately equal to 1/β even if A experiences substantial variations • At high frequencies, A drops so that βA is comparable to unity and closed-loop gain falls below 1/β
  • 11. Copyright © 2017 McGraw-Hill Education. All rights reserved. No reproduction or distribution without the prior written consent of McGraw-Hill Education. 3 Effect of Feedback on Noise • Feedback does not improve noise performance of circuits • In Fig. (a), the open-loop amplifier A1 is characterized by only an input-referred noise voltage and the feedback network is assumed to be noiseless • We have (Vin – βVout + Vn)A1 = Vout, and hence • Circuit can be modified as in Fig. (b), input-referred noise is still Vn
  • 12. Properties of Negative feedback • Reduction in Nonlinear Distortion: