Analog Circuits
Day-11
Feedback Amplifiers
Introduction of Feedback Amplifiers:
The phenomenon of feeding a portion of the output signal back to the
input circuit is known as feedback. The effect results in a dependence
between the output and the input and an effective control can be
obtained in the working of the circuit. Feedback is of two types.
• Positive Feedback
• Negative Feedback
Positive or regenerate feedback:
• In positive feedback, the feedback energy (voltage or currents), is in
phase with the input signal and thus aids it. Positive feedback
increases gain of the amplifier also increases distortion, noise and
instability.
• Because of these disadvantages, positive feedback is seldom employed
in amplifiers. But the positive feedback is used in oscillators.
Positive Feedback
Negative or Degenerate feedback:
• In negative feedback, the feedback energy (voltage or current), is out
of phase with the input signal and thus opposes it.
• Negative feedback reduces gain of the amplifier. It also reduce
distortion, noise and instability.
• This feedback increases bandwidth and improves input and output
impedances.
• Due to these advantages, the negative feedback is frequently used in
amplifiers.
NegativeFeedback
Comparison Between Positive and Negative Feed Back:
S.No. Negative Feedback Positive Feedback
1.
2.
3.
4.
5.
6.
Feedback energy is out
phase with their input signal
Gain of the amplifier
decreases
Gain stability increases
Noise and distortion
decreases.
Increase the band width
Used in amplifiers
Feedback energy is in
phase with the input signal.
Gain of the amplifier
increases
Gain stability decreases
Noise and distribution
increases.
Decreases bandwidth
Used in Oscillators
Principle of Feedback Amplifier:
A feedback amplifier generally consists of two parts. They are
the amplifier and the feedback circuit. The feedback circuit usually
consists of resistors. The concept of feedback amplifier can be
understood from the following figure.
Generalized feedback amplifier
In the above figure, the gain of the amplifier is represented as A. The
gain of the amplifier is the ratio of output voltage Vo to the input
voltage Vi. The feedback network extracts a voltage Vf = β Vo from
the output Vo of the amplifier.
This voltage is subtracted for negative feedback, from the signal
voltage Vs. Now,
Vi=Vs−Vf=Vs−βVo
The quantity β = Vf/Vo is called as feedback ratio or feedback
fraction.
The output Vo must be equal to the input voltage (Vs - βVo) multiplied by
the gain A of the amplifier.
Hence,
(Vs−βVo)A=Vo
AVs−AβVo=Vo
AVs=Vo(1+Aβ)
Vo/Vs=A/(1+Aβ)
Therefore, the gain of the amplifier with feedback is given by
Af =A/(1+Aβ)
Effect of negative feedback on amplifier
performance:
The effect of negative feedback on an amplifier is
considered in relation to gain, gain stability,
distortion, noise, input/output impedance and
bandwidth and gain-bandwidth product.
Gain:
The gain of the amplifier with feedback is given by
Af =A/(1+Aβ)
Hence, gain decreases with feedback.
Gain Stability:
An important advantage of negative voltage feedback is that
the resultant gain of the amplifier can be made independent of
transistor parameters or the supply voltage variations,
Af=A/(1+Aβ)
For negative voltage feedback in an amplifier to be effective,
the designer deliberately makes the product Aβ much greater
than unity. Therefore, in the above relation, ‘1’ can be
neglected as compared to Aβ and the expression becomes
Af = A/(1+Aβ) = 1/β
It may be seen that the gain now depends only upon feedback fraction,
β, i.e., on the characteristics of feedback circuit. As feedback circuit is
usually a voltage divider (a resistive network), therefore, it is unaffected
by changes in temperature, variations in transistor parameters and
frequency. Hence, the gain of the amplifier is extremely stable.
Distortion:
A power amplifier will have non-linear distortion because of large signal
variations. The negative feedback reduces the nonlinear distortion. It can be
proved mathematically that:
Df = D/(1+Aβ)
Where D = distortion in amplifier without feedback
Df = distortion in amplifier with negative feedback
It is clear that by applying negative feedback, the distortion is reduced by a
factor (1+Aβ)
Noise :
There are numbers of sources of noise in an amplifier. The noise N can be
reduced by the factor of (1+Aβ), in a similar manner to non-linear distortion,
so that the noise with feedback is given by
However, if it is necessary to increase the gain to its original level by the
addition of another stage, it is quite possible that the overall system will be
noisier that it was at the start. If the increase in gain can be accomplished by
the adjustment of circuit parameters, a definite reduction in noise will result
from the use of negative feedback.
Nf = N/(1+Aβ)
Input / Output Impedance :
The input and output impedances will also improve by a factor of
(1+Aβ), based on feedback connection type.
Bandwidth and Gain-bandwidth Product:
Bandwidth and Gain-bandwidth Product
Each of higher and lower cut-off frequencies will improve by a
factor of (1+Aβ). However, gain-bandwidth product remains
constant.
fhf= fh (1+Aβ)
flf= fl /(1+Aβ)
An important piece of information that can be obtained from a
frequency response curve is the bandwidth of the amplifier. This refers
to the ‘band’ of frequencies for which the amplifier has a useful gain.
Outside this useful band, the gain of the amplifier is considered to be
insufficient compared with the gain at the centre of the bandwidth. The
bandwidth specified for the voltage amplifiers is the range of
frequencies for which the amplifiers gain is greater than 0.707 of the
maximum gain Alternatively, decibels are used to indicate gain, the ratio
of output to input voltage. The useful bandwidth would be described as
extending to those frequencies at which the gain is -3db down compared
to the gain at the mid-band frequency.
Diagram of an emitter follower
Feedback in Emitter Follower Amplifier:
Operation:
For the emitter follower, the input voltage is applied at base and the
resulting a.c. emitter current produces an output voltage (IeRE) across
the emitter resistance. This voltage opposes the input voltage, thus
providing negative feedback (Voltage series). It is called emitter
follower because the output voltage follows the input voltage.
The major characteristics of the emitter follower are:
The voltage gain of an emitter follower is close to 1.
Relatively high current gain and power gain.
High input impedance and low output impedance.
Input and output ac voltages are in phase.
Classification of Basic Amplifiers:
Amplifiers can be classified broadly as,
• Voltage amplifiers.
• Current amplifiers.
• Transconductance amplifiers.
• Transresistance amplifiers.
Voltage Amplifier:
Equivalent circuit of voltage amplifier.
Ri >> Rs and Ro << RL
Current Amplifier:
Ri << Rs and Ro >> RL
Equivalent circuit for current amplifier
Transconductance Amplifier:
Equivalent circuit for transconductance amplifier
Ri >> Rs and Ro >> RL
Transresistance Amplifier:
Ri << Rs and Ro << RL
Equivalent circuit for transresistance amplifier
Sl. No. Type Input Output Ri Ro
1 Voltage Amplifier Voltage Voltage High Low
2 Current Amplifier Current Current Low High
3 Transconductance
Amplifier
Voltage Current High High
4 Transresistance Amplifier Current Voltage Low Low
Summary:
Classification of Feedback Amplifiers:
There are four types of feedback,
• Voltage series feedback.
• Voltage shunt feedback.
• Current shunt feedback.
• Current series feedback
Voltage series feedback. Voltage shunt Feedback
Rif = Ri (1+Aβ)
Rof = Ro / (1+Aβ)
Rif = Ri / (1+Aβ)
Rof = Ro / (1+Aβ)
Current Shunt Feedback Current Series Feedback
Rif = Ri / (1+Aβ)
Rof = Ro (1+Aβ)
Rif = Ri (1+Aβ)
Rof = Ro (1+Aβ)
Effect of feedback on Input Resistance:
Voltage shunt Feedback Current Shunt Feedback
Voltage series feedback. Current series Feedback
Rif = Ri / (1+Aβ) Rif = Ri / (1+Aβ)
Rif = Ri (1+Aβ) Rif = Ri (1+Aβ)
Effect of feedback on Output Resistance:
Voltage shunt Feedback Current Shunt Feedback
Voltage series feedback. Current series Feedback
Rof = Ro / (1+Aβ)
Rof = Ro / (1+Aβ)
Rof = Ro (1+Aβ)
Rof = Ro (1+Aβ)
Sl. No. Type Rif Rof
1 Voltage Shunt
Feedback Amplifier
2 Current Shunt
Feedback Amplifier
3 Voltage Series
Feedback Amplifier
4 Current Series
Feedback Amplifier
Summary:
Rif = Ri / (1+Aβ)
Rif = Ri / (1+Aβ)
Rif = Ri (1+Aβ)
Rif = Ri (1+Aβ)
Rof = Ro / (1+Aβ)
Rof = Ro / (1+Aβ)
Rof = Ro (1+Aβ)
Rof = Ro (1+Aβ)
Current shuntfeedback.
Equivalentcircuit.
Current Series Feedback Voltage Shunt Feedback
GATE Questions and Solutions
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
a159298350984.pdf
14. Match the following
1. 2.
3. 4.
Sol: Trick to remember
The first term shows how the feedback is taken
Voltage is measured in parallel (by voltmeter) - Hence 1st term voltage means, the parallel
connection at the output
Current is measured in series - Hence 1st term current means series connection at the output.
Series connection increases resistance.
Parallel connection decreases resistance .
Answer: 1
End of Presentation

More Related Content

PPT
AE UNIT V.ppt
PPTX
Electronic Circuit Analysis UNIT II.pptx
PPT
baocaosu
PDF
E ② chapter one - feedback amplifier
PPTX
Lecture One: semiconductor materials explanation
PPTX
Nunit 2 feedback
PPTX
Operational amplifier FEEDBACK AMPLIFIER.pptx
AE UNIT V.ppt
Electronic Circuit Analysis UNIT II.pptx
baocaosu
E ② chapter one - feedback amplifier
Lecture One: semiconductor materials explanation
Nunit 2 feedback
Operational amplifier FEEDBACK AMPLIFIER.pptx

Similar to a159298350984.pdf (20)

PPTX
PPTX
Unit - V feedback amplifiers and oscillator
PPTX
Feedback_in_Amplifiers_Presentation.pptx
PDF
UNIT-4-FEEDBACK AMPLIFIERS AND OSCILLATORS (1).pdf
PDF
Ee321 lab expt 7_negative_feedback_in_ amplifiers
PDF
Feedback amplifier 2
PPTX
Feedback amplifiers, Power Amplifiers, Oscillators
PDF
Mod3_1_Introduction_to_Feedback_Amplifiers.pdf
PPTX
Feedback Amplifiers & Operational Amplifiers (OPAMP)
PPTX
Negative amplifiers and its types Positive feedback and Negative feedback
PPT
Feedback Amplifier_Nt Pixel
PPT
Ch 2 feedback amplifier
PPT
feedback amplifier
PPT
Deterimining Loop gain in Feedback Amplifiers
PDF
Electronic Circuits
PPTX
Feedbacck Amplifier
PPTX
Feedback amplifiers.pptx
PPTX
Feedback amplifiers
PDF
PPT
Feedback Amplifiers_Introduction in amplifier.ppt
Unit - V feedback amplifiers and oscillator
Feedback_in_Amplifiers_Presentation.pptx
UNIT-4-FEEDBACK AMPLIFIERS AND OSCILLATORS (1).pdf
Ee321 lab expt 7_negative_feedback_in_ amplifiers
Feedback amplifier 2
Feedback amplifiers, Power Amplifiers, Oscillators
Mod3_1_Introduction_to_Feedback_Amplifiers.pdf
Feedback Amplifiers & Operational Amplifiers (OPAMP)
Negative amplifiers and its types Positive feedback and Negative feedback
Feedback Amplifier_Nt Pixel
Ch 2 feedback amplifier
feedback amplifier
Deterimining Loop gain in Feedback Amplifiers
Electronic Circuits
Feedbacck Amplifier
Feedback amplifiers.pptx
Feedback amplifiers
Feedback Amplifiers_Introduction in amplifier.ppt
Ad

More from VIT VELLORE (12)

PDF
08031887.pdf
PDF
M 3 iot
PDF
M 3.1 reuse
PDF
M1. io t
PDF
M 4 iot..
PDF
baseband system
PDF
line codes
PDF
PDF
Siw cavity backed antennas
PDF
SUBSTRATE INTEGRATED WAVEGUIDE BASED ANTENNA AND ARRAY ----REVIEW
PDF
QUANTIZATION ERROR AND NOISE
PDF
01031925
08031887.pdf
M 3 iot
M 3.1 reuse
M1. io t
M 4 iot..
baseband system
line codes
Siw cavity backed antennas
SUBSTRATE INTEGRATED WAVEGUIDE BASED ANTENNA AND ARRAY ----REVIEW
QUANTIZATION ERROR AND NOISE
01031925
Ad

Recently uploaded (20)

PDF
ST MNCWANGO P2 WIL (MEPR302) FINAL REPORT.pdf
PPTX
CS6006 - CLOUD COMPUTING - Module - 1.pptx
PDF
Research on ultrasonic sensor for TTU.pdf
PPTX
AI-Reporting for Emerging Technologies(BS Computer Engineering)
PPTX
Soft Skills Unit 2 Listening Speaking Reading Writing.pptx
PPTX
DATA STRCUTURE LABORATORY -BCSL305(PRG1)
PPTX
22ME926Introduction to Business Intelligence and Analytics, Advanced Integrat...
PDF
CELDAS DE COMBUSTIBLE TIPO MEMBRANA DE INTERCAMBIO PROTÓNICO.pdf
PDF
IAE-V2500 Engine Airbus Family A319/320
DOCX
An investigation of the use of recycled crumb rubber as a partial replacement...
PPTX
ARCHITECTURE AND PROGRAMMING OF EMBEDDED SYSTEMS
PDF
Cryptography and Network Security-Module-I.pdf
PDF
Artificial Intelligence_ Basics .Artificial Intelligence_ Basics .
PDF
ECT443_instrumentation_Engg_mod-1.pdf indroduction to instrumentation
PPT
UNIT-I Machine Learning Essentials for 2nd years
PPTX
Agentic Artificial Intelligence (Agentic AI).pptx
PDF
Beginners-Guide-to-Artificial-Intelligence.pdf
PDF
Software defined netwoks is useful to learn NFV and virtual Lans
PDF
LS-6-Digital-Literacy (1) K12 CURRICULUM .pdf
PPTX
INTERNET OF THINGS - EMBEDDED SYSTEMS AND INTERNET OF THINGS
ST MNCWANGO P2 WIL (MEPR302) FINAL REPORT.pdf
CS6006 - CLOUD COMPUTING - Module - 1.pptx
Research on ultrasonic sensor for TTU.pdf
AI-Reporting for Emerging Technologies(BS Computer Engineering)
Soft Skills Unit 2 Listening Speaking Reading Writing.pptx
DATA STRCUTURE LABORATORY -BCSL305(PRG1)
22ME926Introduction to Business Intelligence and Analytics, Advanced Integrat...
CELDAS DE COMBUSTIBLE TIPO MEMBRANA DE INTERCAMBIO PROTÓNICO.pdf
IAE-V2500 Engine Airbus Family A319/320
An investigation of the use of recycled crumb rubber as a partial replacement...
ARCHITECTURE AND PROGRAMMING OF EMBEDDED SYSTEMS
Cryptography and Network Security-Module-I.pdf
Artificial Intelligence_ Basics .Artificial Intelligence_ Basics .
ECT443_instrumentation_Engg_mod-1.pdf indroduction to instrumentation
UNIT-I Machine Learning Essentials for 2nd years
Agentic Artificial Intelligence (Agentic AI).pptx
Beginners-Guide-to-Artificial-Intelligence.pdf
Software defined netwoks is useful to learn NFV and virtual Lans
LS-6-Digital-Literacy (1) K12 CURRICULUM .pdf
INTERNET OF THINGS - EMBEDDED SYSTEMS AND INTERNET OF THINGS

a159298350984.pdf

  • 3. Introduction of Feedback Amplifiers: The phenomenon of feeding a portion of the output signal back to the input circuit is known as feedback. The effect results in a dependence between the output and the input and an effective control can be obtained in the working of the circuit. Feedback is of two types. • Positive Feedback • Negative Feedback
  • 4. Positive or regenerate feedback: • In positive feedback, the feedback energy (voltage or currents), is in phase with the input signal and thus aids it. Positive feedback increases gain of the amplifier also increases distortion, noise and instability. • Because of these disadvantages, positive feedback is seldom employed in amplifiers. But the positive feedback is used in oscillators.
  • 6. Negative or Degenerate feedback: • In negative feedback, the feedback energy (voltage or current), is out of phase with the input signal and thus opposes it. • Negative feedback reduces gain of the amplifier. It also reduce distortion, noise and instability. • This feedback increases bandwidth and improves input and output impedances. • Due to these advantages, the negative feedback is frequently used in amplifiers.
  • 8. Comparison Between Positive and Negative Feed Back: S.No. Negative Feedback Positive Feedback 1. 2. 3. 4. 5. 6. Feedback energy is out phase with their input signal Gain of the amplifier decreases Gain stability increases Noise and distortion decreases. Increase the band width Used in amplifiers Feedback energy is in phase with the input signal. Gain of the amplifier increases Gain stability decreases Noise and distribution increases. Decreases bandwidth Used in Oscillators
  • 9. Principle of Feedback Amplifier: A feedback amplifier generally consists of two parts. They are the amplifier and the feedback circuit. The feedback circuit usually consists of resistors. The concept of feedback amplifier can be understood from the following figure.
  • 11. In the above figure, the gain of the amplifier is represented as A. The gain of the amplifier is the ratio of output voltage Vo to the input voltage Vi. The feedback network extracts a voltage Vf = β Vo from the output Vo of the amplifier. This voltage is subtracted for negative feedback, from the signal voltage Vs. Now, Vi=Vs−Vf=Vs−βVo The quantity β = Vf/Vo is called as feedback ratio or feedback fraction.
  • 12. The output Vo must be equal to the input voltage (Vs - βVo) multiplied by the gain A of the amplifier. Hence, (Vs−βVo)A=Vo AVs−AβVo=Vo AVs=Vo(1+Aβ) Vo/Vs=A/(1+Aβ) Therefore, the gain of the amplifier with feedback is given by Af =A/(1+Aβ)
  • 13. Effect of negative feedback on amplifier performance: The effect of negative feedback on an amplifier is considered in relation to gain, gain stability, distortion, noise, input/output impedance and bandwidth and gain-bandwidth product.
  • 14. Gain: The gain of the amplifier with feedback is given by Af =A/(1+Aβ) Hence, gain decreases with feedback.
  • 15. Gain Stability: An important advantage of negative voltage feedback is that the resultant gain of the amplifier can be made independent of transistor parameters or the supply voltage variations, Af=A/(1+Aβ) For negative voltage feedback in an amplifier to be effective, the designer deliberately makes the product Aβ much greater than unity. Therefore, in the above relation, ‘1’ can be neglected as compared to Aβ and the expression becomes
  • 16. Af = A/(1+Aβ) = 1/β It may be seen that the gain now depends only upon feedback fraction, β, i.e., on the characteristics of feedback circuit. As feedback circuit is usually a voltage divider (a resistive network), therefore, it is unaffected by changes in temperature, variations in transistor parameters and frequency. Hence, the gain of the amplifier is extremely stable.
  • 17. Distortion: A power amplifier will have non-linear distortion because of large signal variations. The negative feedback reduces the nonlinear distortion. It can be proved mathematically that: Df = D/(1+Aβ) Where D = distortion in amplifier without feedback Df = distortion in amplifier with negative feedback It is clear that by applying negative feedback, the distortion is reduced by a factor (1+Aβ)
  • 18. Noise : There are numbers of sources of noise in an amplifier. The noise N can be reduced by the factor of (1+Aβ), in a similar manner to non-linear distortion, so that the noise with feedback is given by However, if it is necessary to increase the gain to its original level by the addition of another stage, it is quite possible that the overall system will be noisier that it was at the start. If the increase in gain can be accomplished by the adjustment of circuit parameters, a definite reduction in noise will result from the use of negative feedback. Nf = N/(1+Aβ)
  • 19. Input / Output Impedance : The input and output impedances will also improve by a factor of (1+Aβ), based on feedback connection type.
  • 20. Bandwidth and Gain-bandwidth Product: Bandwidth and Gain-bandwidth Product Each of higher and lower cut-off frequencies will improve by a factor of (1+Aβ). However, gain-bandwidth product remains constant. fhf= fh (1+Aβ) flf= fl /(1+Aβ)
  • 21. An important piece of information that can be obtained from a frequency response curve is the bandwidth of the amplifier. This refers to the ‘band’ of frequencies for which the amplifier has a useful gain. Outside this useful band, the gain of the amplifier is considered to be insufficient compared with the gain at the centre of the bandwidth. The bandwidth specified for the voltage amplifiers is the range of frequencies for which the amplifiers gain is greater than 0.707 of the maximum gain Alternatively, decibels are used to indicate gain, the ratio of output to input voltage. The useful bandwidth would be described as extending to those frequencies at which the gain is -3db down compared to the gain at the mid-band frequency.
  • 22. Diagram of an emitter follower Feedback in Emitter Follower Amplifier:
  • 23. Operation: For the emitter follower, the input voltage is applied at base and the resulting a.c. emitter current produces an output voltage (IeRE) across the emitter resistance. This voltage opposes the input voltage, thus providing negative feedback (Voltage series). It is called emitter follower because the output voltage follows the input voltage. The major characteristics of the emitter follower are: The voltage gain of an emitter follower is close to 1. Relatively high current gain and power gain. High input impedance and low output impedance. Input and output ac voltages are in phase.
  • 24. Classification of Basic Amplifiers: Amplifiers can be classified broadly as, • Voltage amplifiers. • Current amplifiers. • Transconductance amplifiers. • Transresistance amplifiers.
  • 25. Voltage Amplifier: Equivalent circuit of voltage amplifier. Ri >> Rs and Ro << RL
  • 26. Current Amplifier: Ri << Rs and Ro >> RL Equivalent circuit for current amplifier
  • 27. Transconductance Amplifier: Equivalent circuit for transconductance amplifier Ri >> Rs and Ro >> RL
  • 28. Transresistance Amplifier: Ri << Rs and Ro << RL Equivalent circuit for transresistance amplifier
  • 29. Sl. No. Type Input Output Ri Ro 1 Voltage Amplifier Voltage Voltage High Low 2 Current Amplifier Current Current Low High 3 Transconductance Amplifier Voltage Current High High 4 Transresistance Amplifier Current Voltage Low Low Summary:
  • 30. Classification of Feedback Amplifiers: There are four types of feedback, • Voltage series feedback. • Voltage shunt feedback. • Current shunt feedback. • Current series feedback
  • 31. Voltage series feedback. Voltage shunt Feedback Rif = Ri (1+Aβ) Rof = Ro / (1+Aβ) Rif = Ri / (1+Aβ) Rof = Ro / (1+Aβ)
  • 32. Current Shunt Feedback Current Series Feedback Rif = Ri / (1+Aβ) Rof = Ro (1+Aβ) Rif = Ri (1+Aβ) Rof = Ro (1+Aβ)
  • 33. Effect of feedback on Input Resistance: Voltage shunt Feedback Current Shunt Feedback Voltage series feedback. Current series Feedback Rif = Ri / (1+Aβ) Rif = Ri / (1+Aβ) Rif = Ri (1+Aβ) Rif = Ri (1+Aβ)
  • 34. Effect of feedback on Output Resistance: Voltage shunt Feedback Current Shunt Feedback Voltage series feedback. Current series Feedback Rof = Ro / (1+Aβ) Rof = Ro / (1+Aβ) Rof = Ro (1+Aβ) Rof = Ro (1+Aβ)
  • 35. Sl. No. Type Rif Rof 1 Voltage Shunt Feedback Amplifier 2 Current Shunt Feedback Amplifier 3 Voltage Series Feedback Amplifier 4 Current Series Feedback Amplifier Summary: Rif = Ri / (1+Aβ) Rif = Ri / (1+Aβ) Rif = Ri (1+Aβ) Rif = Ri (1+Aβ) Rof = Ro / (1+Aβ) Rof = Ro / (1+Aβ) Rof = Ro (1+Aβ) Rof = Ro (1+Aβ)
  • 37. Current Series Feedback Voltage Shunt Feedback
  • 38. GATE Questions and Solutions
  • 75. 14. Match the following 1. 2. 3. 4.
  • 76. Sol: Trick to remember The first term shows how the feedback is taken Voltage is measured in parallel (by voltmeter) - Hence 1st term voltage means, the parallel connection at the output Current is measured in series - Hence 1st term current means series connection at the output. Series connection increases resistance. Parallel connection decreases resistance . Answer: 1