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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary 4. Introduction to Feedback Amplifiers S. S. Dan and S. R. Zinka Department of Electrical & Electronics Engineering BITS Pilani, Hyderbad Campus March 2, 2016 4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Page 1: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

4. Introduction to Feedback Amplifiers

S. S. Dan and S. R. Zinka

Department of Electrical & Electronics EngineeringBITS Pilani, Hyderbad Campus

March 2, 2016

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 2: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Outline

1 Introduction

2 Properties of Negative Feedback

3 The Four Basic Feedback Topologies

4 Op-Amps – Revisit

5 Summary

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 3: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Outline

1 Introduction

2 Properties of Negative Feedback

3 The Four Basic Feedback Topologies

4 Op-Amps – Revisit

5 Summary

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 4: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Feedback

• The theory of negative feedback has been developed by electronicsengineers

• Harold Black, an electronics engineer with the Western ElectricCompany, invented the feedback amplifier in 1928

• The concept of feedback and its associated theory are currently used inareas other than engineering, such as in the modeling of biologicalsystems

• In this course, we will concentrate mainly on negative feedback

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 5: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Feedback

• The theory of negative feedback has been developed by electronicsengineers

• Harold Black, an electronics engineer with the Western ElectricCompany, invented the feedback amplifier in 1928

• The concept of feedback and its associated theory are currently used inareas other than engineering, such as in the modeling of biologicalsystems

• In this course, we will concentrate mainly on negative feedback

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 6: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Feedback

• The theory of negative feedback has been developed by electronicsengineers

• Harold Black, an electronics engineer with the Western ElectricCompany, invented the feedback amplifier in 1928

• The concept of feedback and its associated theory are currently used inareas other than engineering, such as in the modeling of biologicalsystems

• In this course, we will concentrate mainly on negative feedback

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 7: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Feedback

• The theory of negative feedback has been developed by electronicsengineers

• Harold Black, an electronics engineer with the Western ElectricCompany, invented the feedback amplifier in 1928

• The concept of feedback and its associated theory are currently used inareas other than engineering, such as in the modeling of biologicalsystems

• In this course, we will concentrate mainly on negative feedback

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 8: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Feedback

• The theory of negative feedback has been developed by electronicsengineers

• Harold Black, an electronics engineer with the Western ElectricCompany, invented the feedback amplifier in 1928

• The concept of feedback and its associated theory are currently used inareas other than engineering, such as in the modeling of biologicalsystems

• In this course, we will concentrate mainly on negative feedback

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 9: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 10: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadAxs xo

xo = Axi

xf = βxo

xi = xs − xf

xo

xs=

Axixi + xf

=Axi

xi + βx0=

Axixi + βAxi

=A

1 + Aβ= Af

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 11: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadAxs xo

xo = Axi

xf = βxo

xi = xs − xf

xo

xs=

Axixi + xf

=Axi

xi + βx0=

Axixi + βAxi

=A

1 + Aβ= Af

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 12: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xo

xo = Axi

xf = βxo

xi = xs − xf

xo

xs=

Axixi + xf

=Axi

xi + βx0=

Axixi + βAxi

=A

1 + Aβ= Af

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 13: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

xo = Axi

xf = βxo

xi = xs − xf

xo

xs=

Axixi + xf

=Axi

xi + βx0=

Axixi + βAxi

=A

1 + Aβ= Af

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 14: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

+−

xo = Axi

xf = βxo

xi = xs − xf

xo

xs=

Axixi + xf

=Axi

xi + βx0=

Axixi + βAxi

=A

1 + Aβ= Af

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 15: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

+−

xo = Axi

xf = βxo

xi = xs − xf

xo

xs=

Axixi + xf

=Axi

xi + βx0=

Axixi + βAxi

=A

1 + Aβ= Af

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 16: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

+−

xixs

=1A

xo

xs=

1A

A1 + Aβ

=1

1 + Aβ

xf

xs=

βxo

xs=

1 + Aβ

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 17: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

+−

xixs

=1A

xo

xs=

1A

A1 + Aβ

=1

1 + Aβ

xf

xs=

βxo

xs=

1 + Aβ

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 18: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

+−

xixs

=1A

xo

xs=

1A

A1 + Aβ

=1

1 + Aβ

xf

xs=

βxo

xs=

1 + Aβ

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 19: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

+−

xixs

=1A

xo

xs=

1A

A1 + Aβ

=1

1 + Aβ

xf

xs=

βxo

xs=

1 + Aβ

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 20: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Nomenclature

Source LoadA

β

xs xi

xf

xo

+−

A : Open-loop gain

β : Feedback factor

Aβ : loop gain

1 + Aβ : Amount of Feedback

Af : gain with feedback or Closed-loop gain

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 21: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Nomenclature

Source LoadA

β

xs xi

xf

xo

+−

A : Open-loop gain

β : Feedback factor

Aβ : loop gain

1 + Aβ : Amount of Feedback

Af : gain with feedback or Closed-loop gain

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 22: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Nomenclature

Source LoadA

β

xs xi

xf

xo

+−

A : Open-loop gain

β : Feedback factor

Aβ : loop gain

1 + Aβ : Amount of Feedback

Af : gain with feedback or Closed-loop gain

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 23: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Nomenclature

Source LoadA

β

xs xi

xf

xo

+−

A : Open-loop gain

β : Feedback factor

Aβ : loop gain

1 + Aβ : Amount of Feedback

Af : gain with feedback or Closed-loop gain

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 24: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Nomenclature

Source LoadA

β

xs xi

xf

xo

+−

A : Open-loop gain

β : Feedback factor

Aβ : loop gain

1 + Aβ : Amount of Feedback

Af : gain with feedback or Closed-loop gain

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 25: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Nomenclature

Source LoadA

β

xs xi

xf

xo

+−

A : Open-loop gain

β : Feedback factor

Aβ : loop gain

1 + Aβ : Amount of Feedback

Af : gain with feedback or Closed-loop gain

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 26: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Nomenclature

Source LoadA

β

xs xi

xf

xo

+−

A : Open-loop gain

β : Feedback factor

Aβ : loop gain

1 + Aβ : Amount of Feedback

Af : gain with feedback or Closed-loop gain

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 27: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Outline

1 Introduction

2 Properties of Negative Feedback

3 The Four Basic Feedback Topologies

4 Op-Amps – Revisit

5 Summary

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 28: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

1. Gain Desensitivity

Source LoadA

β

xs xi

xf

xo

+−

Af =A

1 + Aβ

⇒dAf

dA=

1

(1 + Aβ)2

⇒dAf

Af=

1

(1 + Aβ)2dAAf

=1

(1 + Aβ)

dAA

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 29: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

1. Gain Desensitivity

Source LoadA

β

xs xi

xf

xo

+−

Af =A

1 + Aβ

⇒dAf

dA=

1

(1 + Aβ)2

⇒dAf

Af=

1

(1 + Aβ)2dAAf

=1

(1 + Aβ)

dAA

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 30: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

1. Gain Desensitivity

Source LoadA

β

xs xi

xf

xo

+−

Af =A

1 + Aβ

⇒dAf

dA=

1

(1 + Aβ)2

⇒dAf

Af=

1

(1 + Aβ)2dAAf

=1

(1 + Aβ)

dAA

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 31: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

1. Gain Desensitivity

Source LoadA

β

xs xi

xf

xo

+−

Af =A

1 + Aβ

⇒dAf

dA=

1

(1 + Aβ)2

⇒dAf

Af=

1

(1 + Aβ)2dAAf

=1

(1 + Aβ)

dAA

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 32: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

1. Gain Desensitivity

Source LoadA

β

xs xi

xf

xo

+−

Af =A

1 + Aβ

⇒dAf

dA=

1

(1 + Aβ)2

⇒dAf

Af=

1

(1 + Aβ)2dAAf

=1

(1 + Aβ)

dAA

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 33: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

1. Gain Desensitivity

Source LoadA

β

xs xi

xf

xo

+−

Af =A

1 + Aβ

⇒dAf

dA=

1

(1 + Aβ)2

⇒dAf

Af=

1

(1 + Aβ)2dAAf

=1

(1 + Aβ)

dAA

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 34: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Lowpass Filter)

Consider a lowpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A11

1 + s/ω1,

where A1 denotes the gain at ω = 0 and ω1 is the 3-dB frequency. Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A11+s/ω1

1 + β A11+s/ω1

=A1

1 + s/ω1 + βA1=

A11+A1 β

1 + s/ω1 (1 + A1β).

Thus the feedback lowpass amplifier will have a maximum gain of A11+A1 β and

a 3-dB frequency ω1f given by ω1 (1 + A1β).

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 35: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Lowpass Filter)

Consider a lowpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A11

1 + s/ω1,

where A1 denotes the gain at ω = 0 and ω1 is the 3-dB frequency.

Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A11+s/ω1

1 + β A11+s/ω1

=A1

1 + s/ω1 + βA1=

A11+A1 β

1 + s/ω1 (1 + A1β).

Thus the feedback lowpass amplifier will have a maximum gain of A11+A1 β and

a 3-dB frequency ω1f given by ω1 (1 + A1β).

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 36: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Lowpass Filter)

Consider a lowpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A11

1 + s/ω1,

where A1 denotes the gain at ω = 0 and ω1 is the 3-dB frequency. Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A11+s/ω1

1 + β A11+s/ω1

=A1

1 + s/ω1 + βA1=

A11+A1 β

1 + s/ω1 (1 + A1β).

Thus the feedback lowpass amplifier will have a maximum gain of A11+A1 β and

a 3-dB frequency ω1f given by ω1 (1 + A1β).

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 37: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Lowpass Filter)

Consider a lowpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A11

1 + s/ω1,

where A1 denotes the gain at ω = 0 and ω1 is the 3-dB frequency. Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A11+s/ω1

1 + β A11+s/ω1

=A1

1 + s/ω1 + βA1=

A11+A1 β

1 + s/ω1 (1 + A1β).

Thus the feedback lowpass amplifier will have a maximum gain of A11+A1 β and

a 3-dB frequency ω1f given by ω1 (1 + A1β).

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 38: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Highpass Filter)

Consider a highpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A2s/ω2

1 + s/ω2,

where A2 denotes the gain at ω → ∞ and ω2 is the 3-dB frequency. Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A2s/ω21+s/ω2

1 + β A2s/ω21+s/ω2

=A2

1 + βA2

sω2

(1 + βA2)

1 + sω2

(1 + βA2).

Thus the feedback highpass amplifier will have a maximum gain of A21+A2 β and

a 3-dB frequency ω2f given by ω21+A2 β .

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 39: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Highpass Filter)

Consider a highpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A2s/ω2

1 + s/ω2,

where A2 denotes the gain at ω → ∞ and ω2 is the 3-dB frequency.

Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A2s/ω21+s/ω2

1 + β A2s/ω21+s/ω2

=A2

1 + βA2

sω2

(1 + βA2)

1 + sω2

(1 + βA2).

Thus the feedback highpass amplifier will have a maximum gain of A21+A2 β and

a 3-dB frequency ω2f given by ω21+A2 β .

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

Page 40: 4. Introduction to Feedback Amplifiers - ArraytoolMar 04, 2016  · Feedback The theory of negative feedback has been developed by electronics engineers Harold Black, an electronics

Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Highpass Filter)

Consider a highpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A2s/ω2

1 + s/ω2,

where A2 denotes the gain at ω → ∞ and ω2 is the 3-dB frequency. Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A2s/ω21+s/ω2

1 + β A2s/ω21+s/ω2

=A2

1 + βA2

sω2

(1 + βA2)

1 + sω2

(1 + βA2).

Thus the feedback highpass amplifier will have a maximum gain of A21+A2 β and

a 3-dB frequency ω2f given by ω21+A2 β .

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Highpass Filter)

Consider a highpass amplifier (active filter) whose frequency response is char-acterized by a single pole. Its gain can be expressed as

A (s) = A2s/ω2

1 + s/ω2,

where A2 denotes the gain at ω → ∞ and ω2 is the 3-dB frequency. Applica-tion of negative feedback, with a frequency-independent factor β, around thisamplifier results in

Af =A (s)

1 + βA (s)=

A2s/ω21+s/ω2

1 + β A2s/ω21+s/ω2

=A2

1 + βA2

sω2

(1 + βA2)

1 + sω2

(1 + βA2).

Thus the feedback highpass amplifier will have a maximum gain of A21+A2 β and

a 3-dB frequency ω2f given by ω21+A2 β .

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Bandpass Filter)

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Bandpass Filter)

A

20 log (AM)

-20 dB/decade+20 dB/decade

fL fH f (log scale)

Gain(dB)

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Bandpass Filter)

Af

A

20 log (AM)

-20 dB/decade+20 dB/decade

20 log (AMf)

fLf fL fH fHf f (log scale)

Gain(dB)

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

2. Bandwidth Extension (Bandpass Filter)

Af

A

20 log (AM)

-20 dB/decade+20 dB/decade

20 log (AMf)

fLf fL fH fHf f (log scale)

Gain(dB)

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

3. Noise Reduction

+−

Poweroutputstage(A1)

+

VoRLVS

Vn

SN

=Vs

Vn

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

3. Noise Reduction

+−

Poweroutputstage(A1)

+

VoRLVS

Vn

SN

=Vs

Vn

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

3. Noise Reduction

+−

Poweroutputstage(A1)

+

VoRLVS

Vn

SN

=Vs

Vn

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

3. Noise Reduction ... Cont’d

+−

Feedbacknetwork

(β)

+

+−VfVoRLVS

Vn

Poweroutputstage(A1)

Preamplifier

(A2)

Vo = VsA1A2

1 + A1A2β︸ ︷︷ ︸+VnA1

1 + A1A2β︸ ︷︷ ︸SN

=Vs

VnA2

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

3. Noise Reduction ... Cont’d

+−

Feedbacknetwork

(β)

+

+−VfVoRLVS

Vn

Poweroutputstage(A1)

Preamplifier

(A2)

Vo = VsA1A2

1 + A1A2β︸ ︷︷ ︸+VnA1

1 + A1A2β︸ ︷︷ ︸SN

=Vs

VnA2

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

3. Noise Reduction ... Cont’d

+−

Feedbacknetwork

(β)

+

+−VfVoRLVS

Vn

Poweroutputstage(A1)

Preamplifier

(A2)

Vo = VsA1A2

1 + A1A2β︸ ︷︷ ︸+VnA1

1 + A1A2β︸ ︷︷ ︸

SN

=Vs

VnA2

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

3. Noise Reduction ... Cont’d

+−

Feedbacknetwork

(β)

+

+−VfVoRLVS

Vn

Poweroutputstage(A1)

Preamplifier

(A2)

Vo = VsA1A2

1 + A1A2β︸ ︷︷ ︸+VnA1

1 + A1A2β︸ ︷︷ ︸SN

=Vs

VnA2

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

4. Reduction in Nonlinear Distortion

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

4. Reduction in Nonlinear Distortion

(a)

vO (V)

vI, vS (V)

1

2

3

4

-1

-2

-3

-4

0.02 0.04 0.06 0.08-0.02-0.04-0.06-0.08

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

4. Reduction in Nonlinear Distortion

(a) (b)

vO (V)

vI, vS (V)

1

2

3

4

-1

-2

-3

-4

0.02 0.04 0.06 0.08-0.02-0.04-0.06-0.08

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Outline

1 Introduction

2 Properties of Negative Feedback

3 The Four Basic Feedback Topologies

4 Op-Amps – Revisit

5 Summary

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Voltage Amplifiers

+−

Basicvoltage

amplifier

Feedbacknetwork

+

+−VfVoRL

RS

VS

Voltagesampling

Voltagemixing

Why are we using series-shunt (i.e., voltage sampling-voltage mixing)configuration for voltage amplifiers?

Because, series-shunt configuration increases the input impedance anddecreases the output impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Voltage Amplifiers

+−

Basicvoltage

amplifier

Feedbacknetwork

+

+−VfVoRL

RS

VS

Voltagesampling

Voltagemixing

Why are we using series-shunt (i.e., voltage sampling-voltage mixing)configuration for voltage amplifiers?

Because, series-shunt configuration increases the input impedance anddecreases the output impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Voltage Amplifiers

+−

Basicvoltage

amplifier

Feedbacknetwork

+

+−VfVoRL

RS

VS

Voltagesampling

Voltagemixing

Why are we using series-shunt (i.e., voltage sampling-voltage mixing)configuration for voltage amplifiers?

Because, series-shunt configuration increases the input impedance anddecreases the output impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Voltage Amplifiers

+−

Basicvoltage

amplifier

Feedbacknetwork

+

+−VfVoRL

RS

VS

Voltagesampling

Voltagemixing

Why are we using series-shunt (i.e., voltage sampling-voltage mixing)configuration for voltage amplifiers?

Because, series-shunt configuration increases the input impedance anddecreases the output impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Current Amplifiers

Io

Io

If If

RL

2

Is Rs

1

Basiccurrent

amplifier

Feedbacknetwork

Shunt-series configuration decreases the input impedance and increases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Current Amplifiers

Io

Io

If If

RL

2

Is Rs

1

Basiccurrent

amplifier

Feedbacknetwork

Shunt-series configuration decreases the input impedance and increases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Current Amplifiers

Io

Io

If If

RL

2

Is Rs

1

Basiccurrent

amplifier

Feedbacknetwork

Shunt-series configuration decreases the input impedance and increases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Transconductance Amplifiers

Vf

RL

Rs

2

Vs

1

Basictransconductance

amplifier

Feedbacknetwork

Io

Io

Series-series configuration increases the input impedance and increases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Transconductance Amplifiers

Vf

RL

Rs

2

Vs

1

Basictransconductance

amplifier

Feedbacknetwork

Io

Io

Series-series configuration increases the input impedance and increases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Transconductance Amplifiers

Vf

RL

Rs

2

Vs

1

Basictransconductance

amplifier

Feedbacknetwork

Io

Io

Series-series configuration increases the input impedance and increases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Transresistance Amplifiers

RL

2

Is

1

Basictransresistance

amplifier

Feedbacknetwork

Io

Rs

If If

Vo

Shunt-shunt configuration decreases the input impedance and decreases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Transresistance Amplifiers

RL

2

Is

1

Basictransresistance

amplifier

Feedbacknetwork

Io

Rs

If If

Vo

Shunt-shunt configuration decreases the input impedance and decreases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Transresistance Amplifiers

RL

2

Is

1

Basictransresistance

amplifier

Feedbacknetwork

Io

Rs

If If

Vo

Shunt-shunt configuration decreases the input impedance and decreases theoutput impedance.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Outline

1 Introduction

2 Properties of Negative Feedback

3 The Four Basic Feedback Topologies

4 Op-Amps – Revisit

5 Summary

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Non-Inverting Op-amp Configuration

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Non-Inverting Op-amp Configuration

_

+

_+vI

R1

+vO

R2

vf = voR1

R1 + R2︸ ︷︷ ︸β

Therefore, close-loop gain Af is given as

Af = limA→∞

A1 + Aβ

=1β=

R1 + R2R1

= 1 +R2R1

.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Non-Inverting Op-amp Configuration

_

+

_+vI

R1

+vO

R2

vf = voR1

R1 + R2︸ ︷︷ ︸β

Therefore, close-loop gain Af is given as

Af = limA→∞

A1 + Aβ

=1β=

R1 + R2R1

= 1 +R2R1

.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Non-Inverting Op-amp Configuration

_

+

_+vI

R1

+vO

R2

vf = voR1

R1 + R2︸ ︷︷ ︸β

Therefore, close-loop gain Af is given as

Af = limA→∞

A1 + Aβ

=1β=

R1 + R2R1

= 1 +R2R1

.

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

A Few other Op-amp Circuits with Feedback

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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A Few other Op-amp Circuits with Feedback

++−

+

+−

R1 R2

RL

vs

RL

rR2R1

vs

+

+

R2

RL

is

is

RL

rR2

(a) (b)

(c) (d)

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Outline

1 Introduction

2 Properties of Negative Feedback

3 The Four Basic Feedback Topologies

4 Op-Amps – Revisit

5 Summary

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

The General Feedback Structure (Signal Flow Graph)

Source LoadA

β

xs xi

xf

xo

+−

xo = Axi

xf = βxo

xi = xs − xf

xo

xs=

Axixi + xf

=Axi

xi + βx0=

Axixi + βAxi

=A

1 + Aβ= Af

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Filters

Low-pass:

H (jω) = A× 11 + jωτ

= A× 11 + jω/ω0

High-pass:

H (jω) = A× jωτ

1 + jωτ= A× jω/ω0

1 + jω/ω0

Cut-off Frequency:

f0 =1

2πτ

τ =

{RC for RC networksL/R for RL networks

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Properties of Negative Feedback

Gain Desensitivity:

dAf

Af=

1(1 + Aβ)

dAA

Bandwidth Extension:

Lowpass Filter : A1f =A1

1+A1 β ; ω1f = ω1 (1 + A1β)

Highpass Filter : A2f =A2

1+A1 β ; ω2f =ω2

1+A1 β

Noise Reduction:

SN

=Vs

VnA2

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Sampling & Mixing

• Series sampling or series mixing always increases the (output/input)Impedances.

• Shunt sampling or shunt mixing always decreases the (output/input)Impedances.

• Best Feedback Topologies for Various Amplifiers:

• Voltage Amplifiers : Series-Shunt

• Current Amplifiers : Shunt-Series

• Transconductance Amplifiers : Series-Series

• Transresistance Amplifiers : Shunt-Shunt

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus

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Introduction Properties of Negative Feedback The Four Basic Feedback Topologies Op-Amps – Revisit Summary

Bye Bye Basics ...

Now, you got almost all the tools that you need to understand therest of the course !

4. Introduction to Feedback Amplifiers ECE/EEE/INSTR F244, Dept. of EEE, BITS Pilani Hyderabad Campus