Passive RL and RC Filters

Size: px
Start display at page:

Download "Passive RL and RC Filters"

Transcription

1 NDSU Passive RL and RC Filters ECE 3 Passive RL and RC Filters A filter is a system whose gain changes with frequency. Essentially, all dynamic systems are filters. -Stage Low-Pass Filter For the following -stage RC low-pass filter with R = k, C = uf, Find the transfer function from X to Y Find y(t) assuming x(t) = sin (377t) Check your answer in PartSim V R V = Y X + - C i) Find the transfer function from X to Y: The LaPlace impedance of a capacitor is Z = Cs By voltage division, the gain is then Cs R+ Cs X = RCs+ This is called a low pass filter since Single-Stage RC Low Pass Filter: X RCs+ At low frequencies ( s = jω = j ), the gain is one. The input signal is passed to the output. X At high frequencies ( s large ) the gain goes to zero. The input signal is blocked. ii) Find y(t) assuming x(t) = sin (377t) Since RC =.. JSG July 7, 28

2 NDSU Passive RL and RC Filters ECE 3.s+ X Using superposition, treat this as two separate problems x(t) = 5 x(t) = 2.5 sin (377t) X = 5 X = j2.5 s = jω = j s = j377.s+ 5 s=.s+ ( j2.5) s=j377 Y = 5 Y = ( ) ( j2.5) y(t) = 5 Y = y(t) =.663 cos (377t 78 ) The total input is the sum of the two parts. The total output is the sum of the two outputs y(t) = cos (377t 78 ) The RC filter Passed the DC term ( 5V ), and Attenuated the 6Hz term from 2.5Vp to 66.3mVp iii) Check your answer in PartSim There are two ways to do this: either Check the gain of the filter at DC and 6Hz, or Check the transient response matches our calculations First, input the circuit into PartSim: JSG 2 July 7, 28

3 NDSU Passive RL and RC Filters ECE 3 Run an AC Response from. to Hz (close to Hz and 6Hz) The resulting plot looks like this: Note that At.Hz (almost DC), the gain is. as calculated At 6Hz, the gain is.264 ( vs..265 calculated ). This matches our calculations. A second method to check your answer is to run a transient simulation. A 6Hz signal has a period of 7ms. Running the simulation for 5 cycles (75ms) results in JSG 3 July 7, 28

4 NDSU Passive RL and RC Filters ECE 3 Running a transient simulation to see what the output looks like: Resulting signals at X (black) and Y (blue). Note again that this matches our calculations The output has a DC offset of 5V With a peak-to-peak amplitude of 35mVpp ( vs. 32mVpp computed ) JSG 4 July 7, 28

5 NDSU Passive RL and RC Filters ECE 3 3-Stage RC Low-Pass Filter (take ) A single stage RC low-pass filter helps to remove high-frequency terms, such as the ripple in the above example. On the basis that mode is better, a 3-stage RC low pass filter should be better than a one-stage. Example 2: For the following 3-stage RC low-pass filter with R = k, C = uf, Find the transfer function from X to Y Find y(t) assuming x(t) = sin (377t) Check your answer in PartSim V R R2 R3 V V2 V3 V + - I I2 I3 C C2 C3 3-Stage RC Low Pass Filter i) Find the transfer function from X to Y Due to loading, you can't treat this as three cascaded filters. Instead, use state-space and Matlab to get the transfer function. Assuming zero initial conditions (or that initial conditions don't matter), the voltage node equations are: I = C sv = V V R + V R 2 I 2 = C 2 s = V R 2 + R 3 I 3 = C 3 s = R 3 Solving for the derivatives JSG 5 July 7, 28

6 NDSU Passive RL and RC Filters ECE 3 sv = R C + R 2 C V + R 2 C + R C V s = R 2 C R 2 C 2 V + s = R 3 C 3 + Placing in matrix form: sv s s = Y = = R C + R 2 C R 2 C R 2 C 2 R 2 C 2 + R 3 C 3 V V + R C V Plugging in R = k, C = uf sv s s = 2 2 V + V Using Matlab to find the transfer function to V3: >> A = [-2,, ;,-2, ;,,-] >> B = [;;] >> C = [,,]; >> D = ; >> G = ss(a,b,c,d); >> zpk(g) G(s) = (s+32.47) (s+5.55) (s+.98) JSG 6 July 7, 28

7 NDSU Passive RL and RC Filters ECE 3 Note that You could solve for the transfer function by hand by simplifying 3 equations. Matlab is lots easier. For a single stage RC filter, the poles are at /RC = - For a 3-stage RC filter, the are no longer at s = - due to loading. ii) Find y(t) assuming x(t) = sin (377t) Like before, use superposition and the transfer function we just found: x(t) = 5 x(t) = 2.5 sin (377t) s = s = j377 X = 5 X = j2.5 (s+32.47)(s+5.55)(s+.98) X s= (s+32.47)(s+5.55)(s+.98) X s=j377 Y = () (5) Y = ( ) ( j2.5) Y = 5 Y =.46 7 y(t) = 5 y(t) =.46 cos (377t + 7 ) Putting it all together... y(t) = cos (377t + 7 ) iii) Check your answer in PartSim: Input the circuit into PartSim: Check the gain at DC and 6Hz: JSG 7 July 7, 28

8 NDSU Passive RL and RC Filters ECE 3 Note that The DC gain is almost (you need to go lower than.hz to see this), and The gain at 6Hz is. 834 ( vs.. 85 computed ) This matches our calculations. -Stage RC Filter (take 2) When building a 3-stage RC low-pass filter, you can't simply tack on three more stages. When analyzing the -stage RC filter we assumed that there was no loading. If you add an identical stage to V, this assumption is violated and the circuit is changed. To avoid loading, one trick is to make the impedance of each stage increase by x relative to the previous stage: R R R V V V2 V3 Y X + - C.C.C 3-Stage RC Low-Pass Filter: Y RCs+ 3 X JSG 8 July 7, 28

9 NDSU Passive RL and RC Filters ECE 3 Now, if R = k C = uf / RC = the dynamics become sv s s = V + V Using Matlab to find the transfer function: >> A = [-,, ;,-, ;,,-] >> B = [;;]; >> C = [,,]; >> D = ; >> G = ss(a,b,c,d); >> zpk(g) G(s) = (s+5.25) (s+.5) (s+6.24) This is closer to having three poles at -, but it's still a little off. JSG 9 July 7, 28

Superposition (take 3)

Superposition (take 3) Superposition (take 3) Previously, we looked at how to analyze an AC to DC converter and a Buck converter. To solve these circuits, we changed the problem so that the input contained A DC signal, and An

More information

Finding Transfer Functions of Circuits Using State-Space

Finding Transfer Functions of Circuits Using State-Space Objective: Finding Transfer Functions of Circuits Using State-Space Write the state-space model for a circuit Find the transfer function for a system in state-space form Discussion Assume either The input

More information

Operational Amplifiers

Operational Amplifiers NDSU Operational Amplifiers ECE 06 JSG Operational Amplifiers An operational amplifier is a input device with V o k(v V ) where k is a large number. For short, the following symbol is used for an differential

More information

Fourier Transform. Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function

Fourier Transform. Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function Objectives: Be able to Fourier Transform Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function Filters with a Single Sinusoidal Input: Suppose

More information

Sophomore Physics Laboratory (PH005/105)

Sophomore Physics Laboratory (PH005/105) CALIFORNIA INSTITUTE OF TECHNOLOGY PHYSICS MATHEMATICS AND ASTRONOMY DIVISION Sophomore Physics Laboratory (PH5/15) Analog Electronics Active Filters Copyright c Virgínio de Oliveira Sannibale, 23 (Revision

More information

Dynamic circuits: Frequency domain analysis

Dynamic circuits: Frequency domain analysis Electronic Circuits 1 Dynamic circuits: Contents Free oscillation and natural frequency Transfer functions Frequency response Bode plots 1 System behaviour: overview 2 System behaviour : review solution

More information

Input and Output Impedances with Feedback

Input and Output Impedances with Feedback EE 3 Lecture Basic Feedback Configurations Generalized Feedback Schemes Integrators Differentiators First-order active filters Second-order active filters Review from Last Time Input and Output Impedances

More information

Chapter 10: Sinusoids and Phasors

Chapter 10: Sinusoids and Phasors Chapter 10: Sinusoids and Phasors 1. Motivation 2. Sinusoid Features 3. Phasors 4. Phasor Relationships for Circuit Elements 5. Impedance and Admittance 6. Kirchhoff s Laws in the Frequency Domain 7. Impedance

More information

Poles, Zeros, and Frequency Response

Poles, Zeros, and Frequency Response Complex Poles Poles, Zeros, and Frequency esponse With only resistors and capacitors, you're stuck with real poles. If you want complex poles, you need either an op-amp or an inductor as well. Complex

More information

Rotational Systems, Gears, and DC Servo Motors

Rotational Systems, Gears, and DC Servo Motors Rotational Systems Rotational Systems, Gears, and DC Servo Motors Rotational systems behave exactly like translational systems, except that The state (angle) is denoted with rather than x (position) Inertia

More information

Chapter 6: The Laplace Transform. Chih-Wei Liu

Chapter 6: The Laplace Transform. Chih-Wei Liu Chapter 6: The Laplace Transform Chih-Wei Liu Outline Introduction The Laplace Transform The Unilateral Laplace Transform Properties of the Unilateral Laplace Transform Inversion of the Unilateral Laplace

More information

Control Systems Engineering (Chapter 2. Modeling in the Frequency Domain) Prof. Kwang-Chun Ho Tel: Fax:

Control Systems Engineering (Chapter 2. Modeling in the Frequency Domain) Prof. Kwang-Chun Ho Tel: Fax: Control Systems Engineering (Chapter 2. Modeling in the Frequency Domain) Prof. Kwang-Chun Ho kwangho@hansung.ac.kr Tel: 02-760-4253 Fax:02-760-4435 Overview Review on Laplace transform Learn about transfer

More information

Meeting Design Specs using Root Locus

Meeting Design Specs using Root Locus Meeting Design Specs using Root Locus So far, we have Lead compensators which cancel a pole and move it left, speeding up the root locus. PID compensators which add a zero at s=0 and add zero, one, or

More information

Poles, Zeros, and Frequency Response

Poles, Zeros, and Frequency Response Poles, Zeros, and Frequency Response With the previous circuits, you can build filters with Real poles Complex Poles, and Zeros at s = 0 Filter design uses this to places poles and zeros to give a desired

More information

EE221 Circuits II. Chapter 14 Frequency Response

EE221 Circuits II. Chapter 14 Frequency Response EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active

More information

EE221 Circuits II. Chapter 14 Frequency Response

EE221 Circuits II. Chapter 14 Frequency Response EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active

More information

ECE-342 Test 3: Nov 30, :00-8:00, Closed Book. Name : Solution

ECE-342 Test 3: Nov 30, :00-8:00, Closed Book. Name : Solution ECE-342 Test 3: Nov 30, 2010 6:00-8:00, Closed Book Name : Solution All solutions must provide units as appropriate. Unless otherwise stated, assume T = 300 K. 1. (25 pts) Consider the amplifier shown

More information

To find the step response of an RC circuit

To find the step response of an RC circuit To find the step response of an RC circuit v( t) v( ) [ v( t) v( )] e tt The time constant = RC The final capacitor voltage v() The initial capacitor voltage v(t ) To find the step response of an RL circuit

More information

Sinusoidal Response of RLC Circuits

Sinusoidal Response of RLC Circuits Sinusoidal Response of RLC Circuits Series RL circuit Series RC circuit Series RLC circuit Parallel RL circuit Parallel RC circuit R-L Series Circuit R-L Series Circuit R-L Series Circuit Instantaneous

More information

QUESTION BANK SUBJECT: NETWORK ANALYSIS (10ES34)

QUESTION BANK SUBJECT: NETWORK ANALYSIS (10ES34) QUESTION BANK SUBJECT: NETWORK ANALYSIS (10ES34) NOTE: FOR NUMERICAL PROBLEMS FOR ALL UNITS EXCEPT UNIT 5 REFER THE E-BOOK ENGINEERING CIRCUIT ANALYSIS, 7 th EDITION HAYT AND KIMMERLY. PAGE NUMBERS OF

More information

ECE 201 Fall 2009 Final Exam

ECE 201 Fall 2009 Final Exam ECE 01 Fall 009 Final Exam December 16, 009 Division 0101: Tan (11:30am) Division 001: Clark (7:30 am) Division 0301: Elliott (1:30 pm) Instructions 1. DO NOT START UNTIL TOLD TO DO SO.. Write your Name,

More information

Lecture 16 FREQUENCY RESPONSE OF SIMPLE CIRCUITS

Lecture 16 FREQUENCY RESPONSE OF SIMPLE CIRCUITS Lecture 6 FREQUENCY RESPONSE OF SIMPLE CIRCUITS Ray DeCarlo School of ECE Purdue University West Lafayette, IN 47907-285 decarlo@ecn.purdue.edu EE-202, Frequency Response p 2 R. A. DeCarlo I. WHAT IS FREQUENCY

More information

Some of the different forms of a signal, obtained by transformations, are shown in the figure. jwt e z. jwt z e

Some of the different forms of a signal, obtained by transformations, are shown in the figure. jwt e z. jwt z e Transform methods Some of the different forms of a signal, obtained by transformations, are shown in the figure. X(s) X(t) L - L F - F jw s s jw X(jw) X*(t) F - F X*(jw) jwt e z jwt z e X(nT) Z - Z X(z)

More information

EE/ME/AE324: Dynamical Systems. Chapter 7: Transform Solutions of Linear Models

EE/ME/AE324: Dynamical Systems. Chapter 7: Transform Solutions of Linear Models EE/ME/AE324: Dynamical Systems Chapter 7: Transform Solutions of Linear Models The Laplace Transform Converts systems or signals from the real time domain, e.g., functions of the real variable t, to the

More information

ECE 202 Fall 2013 Final Exam

ECE 202 Fall 2013 Final Exam ECE 202 Fall 2013 Final Exam December 12, 2013 Circle your division: Division 0101: Furgason (8:30 am) Division 0201: Bermel (9:30 am) Name (Last, First) Purdue ID # There are 18 multiple choice problems

More information

ECE3050 Assignment 7

ECE3050 Assignment 7 ECE3050 Assignment 7. Sketch and label the Bode magnitude and phase plots for the transfer functions given. Use loglog scales for the magnitude plots and linear-log scales for the phase plots. On the magnitude

More information

OPERATIONAL AMPLIFIER APPLICATIONS

OPERATIONAL AMPLIFIER APPLICATIONS OPERATIONAL AMPLIFIER APPLICATIONS 2.1 The Ideal Op Amp (Chapter 2.1) Amplifier Applications 2.2 The Inverting Configuration (Chapter 2.2) 2.3 The Non-inverting Configuration (Chapter 2.3) 2.4 Difference

More information

Filters and Tuned Amplifiers

Filters and Tuned Amplifiers Filters and Tuned Amplifiers Essential building block in many systems, particularly in communication and instrumentation systems Typically implemented in one of three technologies: passive LC filters,

More information

Basic Electronics. Introductory Lecture Course for. Technology and Instrumentation in Particle Physics Chicago, Illinois June 9-14, 2011

Basic Electronics. Introductory Lecture Course for. Technology and Instrumentation in Particle Physics Chicago, Illinois June 9-14, 2011 Basic Electronics Introductory Lecture Course for Technology and Instrumentation in Particle Physics 2011 Chicago, Illinois June 9-14, 2011 Presented By Gary Drake Argonne National Laboratory Session 2

More information

Schedule. ECEN 301 Discussion #20 Exam 2 Review 1. Lab Due date. Title Chapters HW Due date. Date Day Class No. 10 Nov Mon 20 Exam Review.

Schedule. ECEN 301 Discussion #20 Exam 2 Review 1. Lab Due date. Title Chapters HW Due date. Date Day Class No. 10 Nov Mon 20 Exam Review. Schedule Date Day lass No. 0 Nov Mon 0 Exam Review Nov Tue Title hapters HW Due date Nov Wed Boolean Algebra 3. 3.3 ab Due date AB 7 Exam EXAM 3 Nov Thu 4 Nov Fri Recitation 5 Nov Sat 6 Nov Sun 7 Nov Mon

More information

EE292: Fundamentals of ECE

EE292: Fundamentals of ECE EE292: Fundamentals of ECE Fall 2012 TTh 10:00-11:15 SEB 1242 Lecture 14 121011 http://www.ee.unlv.edu/~b1morris/ee292/ 2 Outline Review Steady-State Analysis RC Circuits RL Circuits 3 DC Steady-State

More information

Lecture 37: Frequency response. Context

Lecture 37: Frequency response. Context EECS 05 Spring 004, Lecture 37 Lecture 37: Frequency response Prof J. S. Smith EECS 05 Spring 004, Lecture 37 Context We will figure out more of the design parameters for the amplifier we looked at in

More information

Frequency Response Prof. Ali M. Niknejad Prof. Rikky Muller

Frequency Response Prof. Ali M. Niknejad Prof. Rikky Muller EECS 105 Spring 2017, Module 4 Frequency Response Prof. Ali M. Niknejad Department of EECS Announcements l HW9 due on Friday 2 Review: CD with Current Mirror 3 Review: CD with Current Mirror 4 Review:

More information

EE40 Lecture 11 Josh Hug 7/19/2010

EE40 Lecture 11 Josh Hug 7/19/2010 EE40 Lecture Josh 7/9/200 Logistical Things Lab 4 tomorrow Lab 5 (active filter lab) on Wednesday Prototype for future lab for EE40 Prelab is very short, sorry. Please give us our feedback Google docs

More information

Source-Free RC Circuit

Source-Free RC Circuit First Order Circuits Source-Free RC Circuit Initial charge on capacitor q = Cv(0) so that voltage at time 0 is v(0). What is v(t)? Prof Carruthers (ECE @ BU) EK307 Notes Summer 2018 150 / 264 First Order

More information

Exact Analysis of a Common-Source MOSFET Amplifier

Exact Analysis of a Common-Source MOSFET Amplifier Exact Analysis of a Common-Source MOSFET Amplifier Consider the common-source MOSFET amplifier driven from signal source v s with Thévenin equivalent resistance R S and a load consisting of a parallel

More information

Taking the Laplace transform of the both sides and assuming that all initial conditions are zero,

Taking the Laplace transform of the both sides and assuming that all initial conditions are zero, The transfer function Let s begin with a general nth-order, linear, time-invariant differential equation, d n a n dt nc(t)... a d dt c(t) a 0c(t) d m = b m dt mr(t)... a d dt r(t) b 0r(t) () where c(t)

More information

Possible

Possible Department of Electrical Engineering and Computer Science ENGR 21. Introduction to Circuits and Instruments (4) ENGR 21 SPRING 24 FINAL EXAMINATION given 5/4/3 Possible 1. 1 2. 1 3. 1 4. 1 5. 1 6. 1 7.

More information

Linear Circuit Experiment (MAE171a) Prof: Raymond de Callafon

Linear Circuit Experiment (MAE171a) Prof: Raymond de Callafon Linear Circuit Experiment (MAE171a) Prof: Raymond de Callafon email: callafon@ucsd.edu TA: Younghee Han tel. (858) 8221763/8223457, email: y3han@ucsd.edu class information and lab handouts will be available

More information

Homework Assignment 11

Homework Assignment 11 Homework Assignment Question State and then explain in 2 3 sentences, the advantage of switched capacitor filters compared to continuous-time active filters. (3 points) Continuous time filters use resistors

More information

Lab Experiment 2: Performance of First order and second order systems

Lab Experiment 2: Performance of First order and second order systems Lab Experiment 2: Performance of First order and second order systems Objective: The objective of this exercise will be to study the performance characteristics of first and second order systems using

More information

Prepare for this experiment!

Prepare for this experiment! Notes on Experiment #8 Theorems of Linear Networks Prepare for this experiment! If you prepare, you can finish in 90 minutes. If you do not prepare, you will not finish even half of this experiment. So,

More information

Time Response Analysis (Part II)

Time Response Analysis (Part II) Time Response Analysis (Part II). A critically damped, continuous-time, second order system, when sampled, will have (in Z domain) (a) A simple pole (b) Double pole on real axis (c) Double pole on imaginary

More information

EE105 Fall 2015 Microelectronic Devices and Circuits Frequency Response. Prof. Ming C. Wu 511 Sutardja Dai Hall (SDH)

EE105 Fall 2015 Microelectronic Devices and Circuits Frequency Response. Prof. Ming C. Wu 511 Sutardja Dai Hall (SDH) EE05 Fall 205 Microelectronic Devices and Circuits Frequency Response Prof. Ming C. Wu wu@eecs.berkeley.edu 5 Sutardja Dai Hall (SDH) Amplifier Frequency Response: Lower and Upper Cutoff Frequency Midband

More information

School of Engineering Faculty of Built Environment, Engineering, Technology & Design

School of Engineering Faculty of Built Environment, Engineering, Technology & Design Module Name and Code : ENG60803 Real Time Instrumentation Semester and Year : Semester 5/6, Year 3 Lecture Number/ Week : Lecture 3, Week 3 Learning Outcome (s) : LO5 Module Co-ordinator/Tutor : Dr. Phang

More information

GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING FINAL EXAM. COURSE: ECE 3084A (Prof. Michaels)

GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING FINAL EXAM. COURSE: ECE 3084A (Prof. Michaels) GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING FINAL EXAM DATE: 30-Apr-14 COURSE: ECE 3084A (Prof. Michaels) NAME: STUDENT #: LAST, FIRST Write your name on the front page

More information

Review of Linear Time-Invariant Network Analysis

Review of Linear Time-Invariant Network Analysis D1 APPENDIX D Review of Linear Time-Invariant Network Analysis Consider a network with input x(t) and output y(t) as shown in Figure D-1. If an input x 1 (t) produces an output y 1 (t), and an input x

More information

Prepare for this experiment!

Prepare for this experiment! Notes on Experiment #8 Theorems of Linear Networks Prepare for this experiment! If you prepare, you can finish in 90 minutes. If you do not prepare, you will not finish even half of this experiment. So,

More information

8 sin 3 V. For the circuit given, determine the voltage v for all time t. Assume that no energy is stored in the circuit before t = 0.

8 sin 3 V. For the circuit given, determine the voltage v for all time t. Assume that no energy is stored in the circuit before t = 0. For the circuit given, determine the voltage v for all time t. Assume that no energy is stored in the circuit before t = 0. Spring 2015, Exam #5, Problem #1 4t Answer: e tut 8 sin 3 V 1 For the circuit

More information

LECTURE 8 RC AND RL FIRST-ORDER CIRCUITS (PART 1)

LECTURE 8 RC AND RL FIRST-ORDER CIRCUITS (PART 1) CIRCUITS by Ulaby & Maharbiz LECTURE 8 RC AND RL FIRST-ORDER CIRCUITS (PART 1) 07/18/2013 ECE225 CIRCUIT ANALYSIS All rights reserved. Do not copy or distribute. 2013 National Technology and Science Press

More information

Lecture 46 Bode Plots of Transfer Functions:II A. Low Q Approximation for Two Poles w o

Lecture 46 Bode Plots of Transfer Functions:II A. Low Q Approximation for Two Poles w o Lecture 46 Bode Plots of Transfer Functions:II A. Low Q Approximation for Two Poles w o ----------- ----------- w L =Q - w o πf o w h =Qw o w L ~ RC w h w L f(l) w h f(c) B. Construction from T(s) Asymptotes

More information

Advanced Analog Building Blocks. Prof. Dr. Peter Fischer, Dr. Wei Shen, Dr. Albert Comerma, Dr. Johannes Schemmel, etc

Advanced Analog Building Blocks. Prof. Dr. Peter Fischer, Dr. Wei Shen, Dr. Albert Comerma, Dr. Johannes Schemmel, etc Advanced Analog Building Blocks Prof. Dr. Peter Fischer, Dr. Wei Shen, Dr. Albert Comerma, Dr. Johannes Schemmel, etc 1 Topics 1. S domain and Laplace Transform Zeros and Poles 2. Basic and Advanced current

More information

Chapter 8: Converter Transfer Functions

Chapter 8: Converter Transfer Functions Chapter 8. Converter Transfer Functions 8.1. Review of Bode plots 8.1.1. Single pole response 8.1.2. Single zero response 8.1.3. Right half-plane zero 8.1.4. Frequency inversion 8.1.5. Combinations 8.1.6.

More information

Circuit Analysis Using Fourier and Laplace Transforms

Circuit Analysis Using Fourier and Laplace Transforms EE2015: Electrical Circuits and Networks Nagendra Krishnapura https://wwweeiitmacin/ nagendra/ Department of Electrical Engineering Indian Institute of Technology, Madras Chennai, 600036, India July-November

More information

K.K. Gan L3: R-L-C AC Circuits. amplitude. Volts. period. -Vo

K.K. Gan L3: R-L-C AC Circuits. amplitude. Volts. period. -Vo Lecture 3: R-L-C AC Circuits AC (Alternative Current): Most of the time, we are interested in the voltage at a point in the circuit will concentrate on voltages here rather than currents. We encounter

More information

Lecture 15: Sinusoidal Steady State (SSS) Analysis or Phasors without a Phasor more or less

Lecture 15: Sinusoidal Steady State (SSS) Analysis or Phasors without a Phasor more or less Spring 18 page 1 Lecture 15: Sinusoidal Steady State (SSS) Analysis or Phasors without a Phasor more or less 1. Definition. A signal f (t) is periodic with period T > 0 if f (t) = f (t + T ) ; the smallest

More information

ECE Networks & Systems

ECE Networks & Systems ECE 342 1. Networks & Systems Jose E. Schutt Aine Electrical & Computer Engineering University of Illinois jschutt@emlab.uiuc.edu 1 What is Capacitance? 1 2 3 Voltage=0 No Charge No Current Voltage build

More information

R-L-C Circuits and Resonant Circuits

R-L-C Circuits and Resonant Circuits P517/617 Lec4, P1 R-L-C Circuits and Resonant Circuits Consider the following RLC series circuit What's R? Simplest way to solve for is to use voltage divider equation in complex notation. X L X C in 0

More information

NETWORK ANALYSIS WITH APPLICATIONS

NETWORK ANALYSIS WITH APPLICATIONS NETWORK ANALYSIS WITH APPLICATIONS Third Edition William D. Stanley Old Dominion University Prentice Hall Upper Saddle River, New Jersey I Columbus, Ohio CONTENTS 1 BASIC CIRCUIT LAWS 1 1-1 General Plan

More information

Solved Problems. Electric Circuits & Components. 1-1 Write the KVL equation for the circuit shown.

Solved Problems. Electric Circuits & Components. 1-1 Write the KVL equation for the circuit shown. Solved Problems Electric Circuits & Components 1-1 Write the KVL equation for the circuit shown. 1-2 Write the KCL equation for the principal node shown. 1-2A In the DC circuit given in Fig. 1, find (i)

More information

Total No. of Questions :09] [Total No. of Pages : 03

Total No. of Questions :09] [Total No. of Pages : 03 EE 4 (RR) Total No. of Questions :09] [Total No. of Pages : 03 II/IV B.Tech. DEGREE EXAMINATIONS, APRIL/MAY- 016 Second Semester ELECTRICAL & ELECTRONICS NETWORK ANALYSIS Time: Three Hours Answer Question

More information

GATE EE Topic wise Questions SIGNALS & SYSTEMS

GATE EE Topic wise Questions SIGNALS & SYSTEMS www.gatehelp.com GATE EE Topic wise Questions YEAR 010 ONE MARK Question. 1 For the system /( s + 1), the approximate time taken for a step response to reach 98% of the final value is (A) 1 s (B) s (C)

More information

Lecture 6, ATIK. Switched-capacitor circuits 2 S/H, Some nonideal effects Continuous-time filters

Lecture 6, ATIK. Switched-capacitor circuits 2 S/H, Some nonideal effects Continuous-time filters Lecture 6, ATIK Switched-capacitor circuits 2 S/H, Some nonideal effects Continuous-time filters What did we do last time? Switched capacitor circuits The basics Charge-redistribution analysis Nonidealties

More information

Single-Time-Constant (STC) Circuits This lecture is given as a background that will be needed to determine the frequency response of the amplifiers.

Single-Time-Constant (STC) Circuits This lecture is given as a background that will be needed to determine the frequency response of the amplifiers. Single-Time-Constant (STC) Circuits This lecture is given as a background that will be needed to determine the frequency response of the amplifiers. Objectives To analyze and understand STC circuits with

More information

ECE 304: Design Issues for Voltage Follower as Output Stage S&S Chapter 14, pp

ECE 304: Design Issues for Voltage Follower as Output Stage S&S Chapter 14, pp ECE 34: Design Issues for oltage Follower as Output Stage S&S Chapter 14, pp. 131133 Introduction The voltage follower provides a good buffer between a differential amplifier and a load in two ways: 1.

More information

4/27 Friday. I have all the old homework if you need to collect them.

4/27 Friday. I have all the old homework if you need to collect them. 4/27 Friday Last HW: do not need to turn it. Solution will be posted on the web. I have all the old homework if you need to collect them. Final exam: 7-9pm, Monday, 4/30 at Lambert Fieldhouse F101 Calculator

More information

Series RC and RL Time Domain Solutions

Series RC and RL Time Domain Solutions ECE2205: Circuits and Systems I 6 1 Series RC and RL Time Domain Solutions In the last chapter, we saw that capacitors and inductors had element relations that are differential equations: i c (t) = C d

More information

ECE315 / ECE515 Lecture 11 Date:

ECE315 / ECE515 Lecture 11 Date: ecture 11 Date: 15.09.016 MOS Differential Pair Quantitative Analysis differential input Small Signal Analysis MOS Differential Pair ECE315 / ECE515 M 1 and M are perfectly matched (at least in theory!)

More information

ECE 255, Frequency Response

ECE 255, Frequency Response ECE 255, Frequency Response 19 April 2018 1 Introduction In this lecture, we address the frequency response of amplifiers. This was touched upon briefly in our previous lecture in Section 7.5 of the textbook.

More information

Chapter 10 AC Analysis Using Phasors

Chapter 10 AC Analysis Using Phasors Chapter 10 AC Analysis Using Phasors 10.1 Introduction We would like to use our linear circuit theorems (Nodal analysis, Mesh analysis, Thevenin and Norton equivalent circuits, Superposition, etc.) to

More information

Fall 2011 ME 2305 Network Analysis. Sinusoidal Steady State Analysis of RLC Circuits

Fall 2011 ME 2305 Network Analysis. Sinusoidal Steady State Analysis of RLC Circuits Fall 2011 ME 2305 Network Analysis Chapter 4 Sinusoidal Steady State Analysis of RLC Circuits Engr. Humera Rafique Assistant Professor humera.rafique@szabist.edu.pk Faculty of Engineering (Mechatronics)

More information

Section 5 Dynamics and Control of DC-DC Converters

Section 5 Dynamics and Control of DC-DC Converters Section 5 Dynamics and ontrol of D-D onverters 5.2. Recap on State-Space Theory x Ax Bu () (2) yxdu u v d ; y v x2 sx () s Ax() s Bu() s ignoring x (0) (3) ( si A) X( s) Bu( s) (4) X s si A BU s () ( )

More information

ECE-202 FINAL April 30, 2018 CIRCLE YOUR DIVISION

ECE-202 FINAL April 30, 2018 CIRCLE YOUR DIVISION ECE 202 Final, Spring 8 ECE-202 FINAL April 30, 208 Name: (Please print clearly.) Student Email: CIRCLE YOUR DIVISION DeCarlo- 7:30-8:30 DeCarlo-:30-2:45 2025 202 INSTRUCTIONS There are 34 multiple choice

More information

Electric Circuits II Sinusoidal Steady State Analysis. Dr. Firas Obeidat

Electric Circuits II Sinusoidal Steady State Analysis. Dr. Firas Obeidat Electric Circuits II Sinusoidal Steady State Analysis Dr. Firas Obeidat 1 Table of Contents 1 2 3 4 5 Nodal Analysis Mesh Analysis Superposition Theorem Source Transformation Thevenin and Norton Equivalent

More information

Speaker: Arthur Williams Chief Scientist Telebyte Inc. Thursday November 20 th 2008 INTRODUCTION TO ACTIVE AND PASSIVE ANALOG

Speaker: Arthur Williams Chief Scientist Telebyte Inc. Thursday November 20 th 2008 INTRODUCTION TO ACTIVE AND PASSIVE ANALOG INTRODUCTION TO ACTIVE AND PASSIVE ANALOG FILTER DESIGN INCLUDING SOME INTERESTING AND UNIQUE CONFIGURATIONS Speaker: Arthur Williams Chief Scientist Telebyte Inc. Thursday November 20 th 2008 TOPICS Introduction

More information

Problem Set 3: Solution Due on Mon. 7 th Oct. in class. Fall 2013

Problem Set 3: Solution Due on Mon. 7 th Oct. in class. Fall 2013 EE 56: Digital Control Systems Problem Set 3: Solution Due on Mon 7 th Oct in class Fall 23 Problem For the causal LTI system described by the difference equation y k + 2 y k = x k, () (a) By first finding

More information

PROBLEMS OF CHAPTER 4: INTRODUCTION TO PASSIVE FILTERS.

PROBLEMS OF CHAPTER 4: INTRODUCTION TO PASSIVE FILTERS. PROBEMS OF CHAPTER 4: INTRODUCTION TO PASSIVE FITERS. April 4, 27 Problem 4. For the circuit shown in (a) we want to design a filter with the zero-pole diagram shown in (b). C X j jω e g (t) v(t) - σ (a)

More information

8. Introduction and Chapter Objectives

8. Introduction and Chapter Objectives Real Analog - Circuits Chapter 8: Second Order Circuits 8. Introduction and Chapter Objectives Second order systems are, by definition, systems whose input-output relationship is a second order differential

More information

Georgia Institute of Technology School of Electrical and Computer Engineering. Midterm-1 Exam (Solution)

Georgia Institute of Technology School of Electrical and Computer Engineering. Midterm-1 Exam (Solution) Georgia Institute of Technology School of Electrical and Computer Engineering Midterm-1 Exam (Solution) ECE-6414 Spring 2012 Friday, Feb. 17, 2012 Duration: 50min First name Solutions Last name Solutions

More information

Chapter 9 Objectives

Chapter 9 Objectives Chapter 9 Engr8 Circuit Analysis Dr Curtis Nelson Chapter 9 Objectives Understand the concept of a phasor; Be able to transform a circuit with a sinusoidal source into the frequency domain using phasor

More information

Chapter 4 Transients. Chapter 4 Transients

Chapter 4 Transients. Chapter 4 Transients Chapter 4 Transients Chapter 4 Transients 1. Solve first-order RC or RL circuits. 2. Understand the concepts of transient response and steady-state response. 1 3. Relate the transient response of first-order

More information

EE102 Homework 2, 3, and 4 Solutions

EE102 Homework 2, 3, and 4 Solutions EE12 Prof. S. Boyd EE12 Homework 2, 3, and 4 Solutions 7. Some convolution systems. Consider a convolution system, y(t) = + u(t τ)h(τ) dτ, where h is a function called the kernel or impulse response of

More information

Linear Systems Theory

Linear Systems Theory ME 3253 Linear Systems Theory Review Class Overview and Introduction 1. How to build dynamic system model for physical system? 2. How to analyze the dynamic system? -- Time domain -- Frequency domain (Laplace

More information

The general form for the transform function of a second order filter is that of a biquadratic (or biquad to the cool kids).

The general form for the transform function of a second order filter is that of a biquadratic (or biquad to the cool kids). nd-order filters The general form for the transform function of a second order filter is that of a biquadratic (or biquad to the cool kids). T (s) A p s a s a 0 s b s b 0 As before, the poles of the transfer

More information

H(s) = 2(s+10)(s+100) (s+1)(s+1000)

H(s) = 2(s+10)(s+100) (s+1)(s+1000) Problem 1 Consider the following transfer function H(s) = 2(s10)(s100) (s1)(s1000) (a) Draw the asymptotic magnitude Bode plot for H(s). Solution: The transfer function is not in standard form to sketch

More information

Inductors. Hydraulic analogy Duality with capacitor Charging and discharging. Lecture 12: Inductors

Inductors. Hydraulic analogy Duality with capacitor Charging and discharging. Lecture 12: Inductors Lecture 12: nductors nductors Hydraulic analogy Duality with capacitor Charging and discharging Robert R. McLeod, University of Colorado http://hilaroad.com/camp/projects/magnet.html 99 Lecture 12: nductors

More information

GATE : , Copyright reserved. Web:www.thegateacademy.com

GATE : , Copyright reserved. Web:www.thegateacademy.com GATE-2016 Index 1. Question Paper Analysis 2. Question Paper & Answer keys : 080-617 66 222, info@thegateacademy.com Copyright reserved. Web:www.thegateacademy.com ANALYSIS OF GATE 2016 Electrical Engineering

More information

EE292: Fundamentals of ECE

EE292: Fundamentals of ECE EE292: Fundamentals of ECE Fall 2012 TTh 10:00-11:15 SEB 1242 Lecture 20 121101 http://www.ee.unlv.edu/~b1morris/ee292/ 2 Outline Chapters 1-3 Circuit Analysis Techniques Chapter 10 Diodes Ideal Model

More information

ECE Circuit Theory. Final Examination. December 5, 2008

ECE Circuit Theory. Final Examination. December 5, 2008 ECE 212 H1F Pg 1 of 12 ECE 212 - Circuit Theory Final Examination December 5, 2008 1. Policy: closed book, calculators allowed. Show all work. 2. Work in the provided space. 3. The exam has 3 problems

More information

Sinusoids and Phasors

Sinusoids and Phasors CHAPTER 9 Sinusoids and Phasors We now begins the analysis of circuits in which the voltage or current sources are time-varying. In this chapter, we are particularly interested in sinusoidally time-varying

More information

DOING PHYSICS WITH MATLAB FINITE DIFFERENCE METHOD: NUMERICAL ANAYSIS OF RC CIRCUITS

DOING PHYSICS WITH MATLAB FINITE DIFFERENCE METHOD: NUMERICAL ANAYSIS OF RC CIRCUITS DOING PHYSICS WITH MATLAB FINITE DIFFERENCE METHOD: NUMERICAL ANAYSIS OF RC CIRCUITS Matlab download directory Matlab script CN03.m Modelling RC circuits using the finite difference method to approximate

More information

Analogue Filters Design and Simulation by Carsten Kristiansen Napier University. November 2004

Analogue Filters Design and Simulation by Carsten Kristiansen Napier University. November 2004 Analogue Filters Design and Simulation by Carsten Kristiansen Napier University November 2004 Title page Author: Carsten Kristiansen. Napier No: 04007712. Assignment title: Analogue Filters Design and

More information

Homework Assignment 09

Homework Assignment 09 Homework Assignment 09 Question 1 (Short Takes) Two points each unless otherwise indicated. 1. What is the 3-dB bandwidth of the amplifier shown below if r π = 2.5K, r o = 100K, g m = 40 ms, and C L =

More information

Today. 1/25/11 Physics 262 Lecture 2 Filters. Active Components and Filters. Homework. Lab 2 this week

Today. 1/25/11 Physics 262 Lecture 2 Filters. Active Components and Filters. Homework. Lab 2 this week /5/ Physics 6 Lecture Filters Today Basics: Analog versus Digital; Passive versus Active Basic concepts and types of filters Passband, Stopband, Cut-off, Slope, Knee, Decibels, and Bode plots Active Components

More information

Fourier Series Representation of

Fourier Series Representation of Fourier Series Representation of Periodic Signals Rui Wang, Assistant professor Dept. of Information and Communication Tongji University it Email: ruiwang@tongji.edu.cn Outline The response of LIT system

More information

Lecture 7, ATIK. Continuous-time filters 2 Discrete-time filters

Lecture 7, ATIK. Continuous-time filters 2 Discrete-time filters Lecture 7, ATIK Continuous-time filters 2 Discrete-time filters What did we do last time? Switched capacitor circuits with nonideal effects in mind What should we look out for? What is the impact on system

More information

EE 330 Lecture 22. Small Signal Modelling Operating Points for Amplifier Applications Amplification with Transistor Circuits

EE 330 Lecture 22. Small Signal Modelling Operating Points for Amplifier Applications Amplification with Transistor Circuits EE 330 Lecture 22 Small Signal Modelling Operating Points for Amplifier Applications Amplification with Transistor Circuits Exam 2 Friday March 9 Exam 3 Friday April 13 Review Session for Exam 2: 6:00

More information

Physics 116A Notes Fall 2004

Physics 116A Notes Fall 2004 Physics 116A Notes Fall 2004 David E. Pellett Draft v.0.9 Notes Copyright 2004 David E. Pellett unless stated otherwise. References: Text for course: Fundamentals of Electrical Engineering, second edition,

More information

ECE 546 Lecture 11 MOS Amplifiers

ECE 546 Lecture 11 MOS Amplifiers ECE 546 Lecture MOS Amplifiers Spring 208 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 546 Jose Schutt Aine Amplifiers Definitions Used to increase

More information

Electrical Circuits (2)

Electrical Circuits (2) Electrical Circuits (2) Lecture 7 Transient Analysis Dr.Eng. Basem ElHalawany Extra Reference for this Lecture Chapter 16 Schaum's Outline Of Theory And Problems Of Electric Circuits https://archive.org/details/theoryandproblemsofelectriccircuits

More information