Frequency Effects Chapter 16.

Slides:



Advertisements
Similar presentations
Lecture 4 Operational Amplifiers—Non-ideal behavior
Advertisements

CHAPTER 3: SPECIAL PURPOSE OP-AMP CIRCUITS
EC 2208 – Electronic Circuits Lab 1
Electronic Devices Ninth Edition Floyd Chapter 10.
Chapter 9: BJT and FET Frequency Response
Basic Electronics Ninth Edition Basic Electronics Ninth Edition ©2002 The McGraw-Hill Companies Grob Schultz.
Chapter 18 Operational Amplifiers. The typical op amp has a differential input and a single-ended output. Class B push-pull emitter follower Diff amp.
Principles & Applications Operational Amplifiers
Amplifier Frequency Response
Amplifier Frequency Response Chapter 10. Effect of Capacitors Capacitor have capacitive reactance (Xc) – Coupling capacitors (C1 and C3) – Bypass capacitors.
The maximum current flows when |X C |
Applications of Logarithms Decibels – Power Gain Decibels – Voltage Gain Frequency and Gain Bode Plot Bode Plot - 2.
1 FET FREQUENCY RESPONSE LOW FREQUENCY. 2 LOW FREQUENCY – COMMON SOURCE.
Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.
 The output from a single amplifier is generally insufficient to drive an output device. In other words, the gain of a single amplifier is inadequate.
ANALOGUE ELECTRONICS II
BJT FREQUENCY RESPONSE
Robert Boylestad Digital Electronics Copyright ©2002 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Chapter 11: BJT.
1 Frequency response I As the frequency of the processed signals increases, the effects of parasitic capacitance in (BJT/MOS) transistors start to manifest.
Frequency Analysis of BJT and MOSFET Amplifiers
Active Filters. This is not in the lab manual While the circuit that will be used is very similar to the one described in the lab manual, the steps in.
Filters and the Bode Plot
Chapter 6 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Electronic Troubleshooting
McGraw-Hill © 2008 The McGraw-Hill Companies Inc. All rights reserved. Electronics Principles & Applications Seventh Edition Chapter 7 More About Small-Signal.
Chapter Seven Frequency Response. Figure 7.1 Amplifier gain versus frequency.
RLC Band-pass Filters. Band-pass Filters and Resonant Circuits Resonant frequency Quality factor.
9-1 McGraw-Hill © 2013 The McGraw-Hill Companies, Inc. All rights reserved. Electronics Principles & Applications Eighth Edition Chapter 9 Operational.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 9-1 Electronics Principles & Applications Eighth Edition Chapter 9 Operational.
Electronics Principles & Applications Fifth Edition Chapter 9 Operational Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 6-1 Electronics Principles & Applications Eighth Edition Chapter 6 Introduction.
Electronics Principles & Applications Fifth Edition Chapter 6 Introduction to Small-Signal Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 6-1 Electronics Principles & Applications Eighth Edition Chapter 6 Introduction.
1 The Operational Amplifier continued The voltage follower provides unity gain, however, the output impedance is changed according to the o/p impedance.
1 Op-Amp Imperfections in The Linear Range of Operations Gain and Bandwidth Limitations  Ideal op amps have infinite open-loop gain magnitude (A oL is.
Minute Paper If you know the input and the output, but you don’t know the circuitry, using the transfer function can you figure out the circuitry without.
Logarithmic scale Linear scale A logarithmic scale compresses large values and allows a large range to be covered without losing.
MALVINO Electronic PRINCIPLES SIXTH EDITION.
Electronics Technology Fundamentals Chapter 15 Frequency Response and Passive Filters.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Frequency response of an amplifier Decibel power gain Decibel.
The Working Theory of an RC Coupled Amplifier in Electronics.
BJT and JFET Frequency Response
Electronic Devices Ninth Edition Floyd Chapter 14.
(4) Filters.
Common Base and Common Collector Amplifiers
Frequency response I As the frequency of the processed signals increases, the effects of parasitic capacitance in (BJT/MOS) transistors start to manifest.
Transistor and Operational Amplifiers
Maj Jeffrey Falkinburg Room 2E46E
The open loop gain of this op-amp is 105 and the bandwidth is 10 Hz
Filters and the Bode Plot
Subject Name: LINEAR IC’s AND APPLICATIONS Subject Code:10EC46 Prepared By: Aparna.P / MP Priyadarshini Department: Electronics and Communication Date:
Principles & Applications Operational Amplifiers
FREQUENCY RESPONSE BJT AMPLIFIER.
SMALL SIGNAL ANALYSIS OF CE AMPLIFIER
Principles & Applications Small-Signal Amplifiers
Lecture V Low Frequency Response of BJT Amplifiers
MALVINO Electronic PRINCIPLES SIXTH EDITION.
Principles & Applications
Common-Base Amplifier
Principles & Applications Small-Signal Amplifiers
ELECTRONIC CIRCUIT ANALYSIS
Electronic PRINCIPLES
Electronic PRINCIPLES
C H A P T E R 17 A.C. Filter Networks.
ENT 162 ANALOG ELECTRONICS
10k 20k Vin Vout H3 What is the gain?
MALVINO Electronic PRINCIPLES SIXTH EDITION.
6.0 Frequency Response 6.1 Introduction 6.2 Basic Concept
MALVINO Electronic PRINCIPLES SIXTH EDITION.
Frequency response I As the frequency of the processed signals increases, the effects of parasitic capacitance in (BJT/MOS) transistors start to manifest.
Presentation transcript:

Frequency Effects Chapter 16

The cutoff frequencies Also called the half-power frequencies The frequency response curve of an ac amplifier A Amid 0.707 Amid f f1 10f1 0.1f2 f2 The cutoff frequencies The midband The gain is maximum in the midband. Also called the half-power frequencies

Review of logarithms A logarithm is an exponent If x = 10y, then y = log10x y = log 10 = 1 y = log 100 = 2 y = log 1000 = 3 y = log 0.1 = -1 y = log 0.01 = -2 y = log 0.001 = -3

Definition of GdB G = pout/pin GdB = 10 log G Memorize: if G = 2, GdB = +3 if G = 0.5, GdB = -3 if G = 10, GdB = +10 if G = 0.1, GdB = -10

Definition of AdB A = vout/vin Adb = 20 log A Memorize: if A = 2, AdB = +6 if A = 0.5, AdB = -6 if A = 10, AdB = +20 if A = 0.1, AdB = -20 Cascade: A = A1A2, AdB = A1dB + A2dB

More on the decibel GdB = AdB only if impedance matched G = antilog GdB/10 A = antilog AdB/20 PdBm = 10 log P/1 mW P = antilog PdBm/10 VdBV = 20 log V V = antilog VdBV/20

A logarithmic scale compresses large values 1 2 3 4 5 6 7 8 9 10 Linear scale 1 2 3 4 5 6 7 8 9 10 Logarithmic scale A logarithmic scale compresses large values and allows a large range to be covered without losing resolution for the smaller values.

Bode plots Use semilogarithmic graph paper (the horizontal axis is logarithmic; the vertical is linear) Plot dB voltage gain on the vertical axis Plot frequency on the horizontal axis An octave refers to a ratio of 2 A decade refers to a ratio of 10

Cutoff (-3dB) frequencies* Ideal Bode plot of an ac amplifier Cutoff (-3dB) frequencies* 50 dB Midband gain 40 dB 30 dB 20 dB/decade rolloff 20 dB 10 dB 0 dB 10 Hz 100 Hz 1 kHz 10 kHz 100 kHz 1 MHz 10 MHz Unity gain frequency *also called corner or break frequencies

( ) Amplitude response of RC lag circuit R 1 f2 = C 2pRC 1 A = f 1+ f2 ( ) 2 1+ 1 A = f2 10f2 100f2 1000f2 0 dB -20 dB -40 dB -60 dB

Angular response of RC lag circuit f = -arctan 0.1f2 f2 10f2 0o -45o -90o

Ideal Bode plot of a dc amplifier with two break frequencies. 50 dB 40 dB 20 dB/decade 30 dB 20 dB 40 dB/decade 10 dB 0 dB 10 Hz 100 Hz 1 kHz 10 kHz 100 kHz fb1 fb2

C Inverting amplifier A vin vout Inverting amplifier with feedback capacitor Inverting amplifier A vin Cin Cout vout Miller equivalent circuit Cout = C A+1 A Cin = C(A+1)

Frequency compensation Most op amps are internally compensated to prevent oscillations One dominant internal compensation capacitor rolls off the gain at 20 dB/decade IC capacitors are limited to the pF range The Miller effect makes the internal compensation capacitor equivalent to a much larger capacitor

Square-wave response of a circuit with limited bandwidth V C V 0.9V TR = 2.2RC fcutoff = 0.35 TR 0.1V TR

Cutoff frequency of input coupling capacitor zin(stage) = R1 R2 bre’ +VCC A f1 = 2p(RG + zin(stage))C 1 f RC f1 R1 RG RL C vG R2 RE

Cutoff frequency of output coupling capacitor +VCC A 1 f1 = f RC f1 2p(RC + RL)C R1 RG C RL vG R2 RE

( ) Cutoff frequency of emitter bypass capacitor re’ + R1 R2 RG b zout = RE +VCC A f f1 = 2p zoutC 1 RC f1 R1 RG RL vG R2 RE C

Combined frequency effects The input coupling, output coupling, and emitter bypass capacitors each produce a cutoff frequency. One is usually dominant (the highest frequency) and produces a rolloff of 20 dB/decade as frequency decreases. When the next cutoff is reached, the gain rolloff increases to 40 dB/decade. When the third is reached, it becomes 60 dB/decade.

Base and collector bypass circuits C’c A f f2 C’e CMiller Cstray CMiller C’e

Bypass circuits The base bypass circuit contains the internal base-emitter capacitance (C’e) and the Miller capacitance due to the internal collector-base feedback capacitance (C’c) The collector bypass circuit contains the Miller capacitance and the stray (wiring) capacitance.