Symbolic SPICE TM Circuit Analyzer and Approximator

Size: px
Start display at page:

Download "Symbolic SPICE TM Circuit Analyzer and Approximator"

Transcription

1 ymbolic PICE ymbolic PICE TM Circuit Analyzer and Approximator Application Note AN-001: eries Resonant Circuit by Gregory M. Wierzba Rev 07010

2 A) Introduction The schematic shown below in Fig. 1 is a series RLC circuit. This simple circuit is capable of acting as a low-pass, high-pass, band-pass and band-stop filter [1]. A Ppice input file, rlc.cir, is given in Table 1. The same file is also accepted by ymbolic PICE TM. Table 1. Ppice/ymbolic PICE Input File Figure 1. eries RLC circuit ERIE RLC CIRCUIT V 1 0 AC 1 R L 3 1M C U.AC DEC 500 5K.5MEG.PROBE.END B) Numerical Program Results Running Ppice, we have the following numerical results with the element nodes indicated that create low-pass, high-pass, band-pass and band-stop filters: Figure. Low-pass response

3 Figure 3. High-pass response Figure 4. Band-pass response 3

4 Figure 5. Band-stop response C) Running ymbolic PICE Although a numerical program can show you what a circuit is capable of doing, ymbolic PICE can show you why. ymbolic PICE can also provide design equations. Running [] the same input file shown in Table 1, the following are the prompts. The user responses are shown in bold: ymbolic PICE - Circuit Analyzer and Approximator Demo Version 3.1 (C) Copyright 010 by Willow Electronics, Inc. INPUT FILE NAME [.cir] : rlc OUTPUT FILENAME [rlc.det] : (hit enter) Determinant string sorted according to orders of some variable? (y/n) : n Numerical evaluation of the results? (y/n) : y Discard terms if their magnitude falls below a threshold? (y/n) : n Check and solve for second order filter functions? (y/n) : y FILTER FUNCTION FILE NAME [rlc.fun] : (hit enter) olve for a variable or expression? (y/n) : y Available Unknowns: 4

5 V1 V V3 V5 *Ignore nodes 4 and higher if present. They are used for internal numbering. Valid Operators: +, -, *, /, ( ), { }, [ ] Equation: v3 olve for another variable or expression? (y/n) : y Equation: v(,3) olve for another variable or expression? (y/n) : y Equation: v(1,) olve for another variable or expression? (y/n) : y Equation: v() olve for another variable or expression? (y/n) : n D) ymbolic PICE Determinant Output The output file rlc.det listed in Table is the matrix written by ymbolic PICE and the transfer functions requested. The program formulates this matrix by using admittances [3]. For example, the resistance R is modeled as a conductance G with a value of 1/ É, the capacitance C is modeled as an admittance sc with a value of (0.01:)s and the inductance L is modeled as an admittance 1/(sL ) with a value of 1/[(1m)s] where s is the Laplace operator. All symbols are echoed as uppercase letters except for the Laplace operator. ERIE RLC CIRCUIT Table. ymbolic PICE Output File rlc.det [0 ] [-G G ][V1 ] [0 ][0 -sl sc+1 sl-1 ][V ] [1 ] [ ][V3 ] [0 ] [0 sl+1-1 -sl ][V5 ] *Ignore nodes 4 and higher if present. They are used for internal numbering. Numerator of: v3 s**0 terms: + G * s**0 5

6 Denominator of: v3 s** terms: + sl*sc*g s**1 terms: + sc s**0 terms: + G e-014 * s** + 1e-008 * s** * s**0 Numerator of: v(,3) s** terms: + sl*sc*g e-014 * s** Denominator of: v(,3) s** terms: + sl*sc*g s**1 terms: + sc s**0 terms: + G e-014 * s** + 1e-008 * s** * s**0 6

7 Numerator of: v(1,) s**1 terms: + sc + 1e-008 * s**1 Denominator of: v(1,) s** terms: + sl*sc*g s**1 terms: + sc s**0 terms: + G e-014 * s** + 1e-008 * s** * s**0 Numerator of: v() s** terms: + sl*sc*g s**0 terms: + G e-014 * s** * s**0 7

8 Denominator of: v() s** terms: + sl*sc*g s**1 terms: + sc s**0 terms: + G e-014 * s** + 1e-008 * s** * s**0 ymbolic PICE s format is a collection of strings of symbols sorted by the (default) Laplace operator s. This is usually not how most people view equations, so you may need to do some minor editing. For example, the last transfer function v() is actually V / V V / V 1 V since V 1 1. Thus we have 1 V V sl sc G sc G s L C G sc G s s LG LC s + slscg + G s LCG + G LC s + LC R 1 s + s + L L C Likewise for the numerical results, 1 14 V.1766e s s + 100G V e s + 1e s s + 470k s+ 100G E) ymbolic PICE Filter Function Output ymbolic PICE will examine any transfer function to determine if its denominator is second order in the Laplace operator s. If this is the case then it finds the parameters associated with the different filter functions. ymbolic PICE finds formulas for Q o, T o and H i where some of the various cases of i are listed on the following page: 8

9 Low-pass filter T lp s Hlp ωo ω o + s + ω Q o o High-pass filter T hp s Hhp s ω s Q + o + ωo o Band-pass filter T bp s H ωο s Qo ω bp o + s + ω o Q o Band-stop filter T bs z Hbs ( s + ω ) ω s s Q + o + ωo o The output file rlc.fun listed in Table 3 contains the filter parameters solved for by ymbolic PICE. Table 3. ymbolic PICE Output File rlc.fun ERIE RLC CIRCUIT ECOND ORDER FILTER PARAMETER: Qo is: ( + G)*QRT{ + L} QRT{ + C} Wo** is: ( + 1) ( + L*C) 9

10 fo 5039.Hz **************************************** There exists a LOW PA filter for : v3 LOW PA GAIN (Hlp) is: ( + 1) **************************************** There exists a HIGH PA filter for : v(,3) HIGH PA GAIN (Hhp) is: ( + 1) **************************************** There exists a BAND PA filter for : v(1,) BAND PA GAIN (Hbp) is: ( + 1) **************************************** There exists a BAND TOP filter for : v() BAND TOP GAIN (Hbs) is: ( + 1) BAND TOP FREQUENCY (Wz**) is: ( + 1) ( + L*C) fz 5039.Hz **************************************** 10

11 F) Comparison of Results From Fig. 5, we can read the numerical value of f o f z 50.31k Hz. The exact value of f o is 50.39k Hz. This is a difference of 0.195% which is approximately the default accuracy of Ppice. Likewise we can calculate the numerical value of Q o from the data [1] in Fig. 5 where Q o f o /(-3dB bandwidth) 50.31k / (100.75k k) The exact value is This is a difference of 0.40%. Besides the numerical results, we now have the formulas for f o f z ( π ) 1 LC and L 1 L Qo G C R C To turn these formulas into a design procedure[1]: Pick L tandard inductor value then C 1 ( o) π f L and R 1 L Q C o G) Conclusion ymbolic PICE can be used to analyze passive filters. ymbolic PICE can recognize second order transfer functions in the Laplace operator s. It can also determine the filter type such as low-pass, high-pass, band-pass and band-stop and then solve for the filter parameters T o, Q o and H i. 11

12 H) References [1] G. M. Wierzba, ECE 0: Electric Circuits and ystems II - Class Notes, Ch.1, pp. 6-4.This e-book is available at [] G. M. Wierzba, ymbolic PICE User Manual, p. 6. This e-book is available at [3] G. M. Wierzba, ymbolic PICE User Manual, p

Symbolic SPICE TM Circuit Analyzer and Approximator

Symbolic SPICE TM Circuit Analyzer and Approximator Symbolic SPICE Symbolic SPICE TM Circuit Analyzer and Approximator Application Note AN-006: Magnetic Microphone Amplifier by Gregory M. Wierzba Rev 072010 A) Introduction The schematic shown below in Fig.

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

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

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

AC Circuits Homework Set

AC Circuits Homework Set Problem 1. In an oscillating LC circuit in which C=4.0 μf, the maximum potential difference across the capacitor during the oscillations is 1.50 V and the maximum current through the inductor is 50.0 ma.

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

AC Circuit Analysis and Measurement Lab Assignment 8

AC Circuit Analysis and Measurement Lab Assignment 8 Electric Circuit Lab Assignments elcirc_lab87.fm - 1 AC Circuit Analysis and Measurement Lab Assignment 8 Introduction When analyzing an electric circuit that contains reactive components, inductors and

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

Berkeley. Matching Networks. Prof. Ali M. Niknejad. U.C. Berkeley Copyright c 2016 by Ali M. Niknejad

Berkeley. Matching Networks. Prof. Ali M. Niknejad. U.C. Berkeley Copyright c 2016 by Ali M. Niknejad Berkeley Matching Networks Prof. Ali M. Niknejad U.C. Berkeley Copyright c 2016 by Ali M. Niknejad February 9, 2016 1 / 33 Impedance Matching R S i i i o Z in + v i Matching Network + v o Z out RF design

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

A DIFFERENT POINT OF VIEW

A DIFFERENT POINT OF VIEW A Different Point of View about Gravity Eelectronics Resonance from John R. Majka / Tommy's Holiday Camp Remote Online Systems +1 604 598-4259 / Title : Gravity Paper Keywords: GRAVITY ELECTRONICS RESONANCE

More information

LECTURE 25 and MORE: Basic Ingredients of Butterworth Filtering. Objective: Design a second order low pass filter whose 3dB down point is f c,min

LECTURE 25 and MORE: Basic Ingredients of Butterworth Filtering. Objective: Design a second order low pass filter whose 3dB down point is f c,min LECTURE 25 and MORE: Basic Ingredients of Butterworth Filtering INTRODUCTION: A SIMPLISTIC DESIGN OVERVIEW Objective: Design a second order low pass filter whose 3dB down point is f c,min 500 Hz or ω c,min

More information

Bfh Ti Control F Ws 2008/2009 Lab Matlab-1

Bfh Ti Control F Ws 2008/2009 Lab Matlab-1 Bfh Ti Control F Ws 2008/2009 Lab Matlab-1 Theme: The very first steps with Matlab. Goals: After this laboratory you should be able to solve simple numerical engineering problems with Matlab. Furthermore,

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-202 Exam III April 10, 2008

EE-202 Exam III April 10, 2008 EE-202 Exam III April 10, 2008 Name: (Please print clearly) Student ID: CIRCLE YOUR DIVISION Morning 8:30 MWF Afternoon 12:30 MWF INSTRUCTIONS There are 13 multiple choice worth 5 points each and there

More information

MODULE-4 RESONANCE CIRCUITS

MODULE-4 RESONANCE CIRCUITS Introduction: MODULE-4 RESONANCE CIRCUITS Resonance is a condition in an RLC circuit in which the capacitive and inductive Reactance s are equal in magnitude, there by resulting in purely resistive impedance.

More information

RLC Series Circuit. We can define effective resistances for capacitors and inductors: 1 = Capacitive reactance:

RLC Series Circuit. We can define effective resistances for capacitors and inductors: 1 = Capacitive reactance: RLC Series Circuit In this exercise you will investigate the effects of changing inductance, capacitance, resistance, and frequency on an RLC series AC circuit. We can define effective resistances for

More information

LECTURE 21: Butterworh & Chebeyshev BP Filters. Part 1: Series and Parallel RLC Circuits On NOT Again

LECTURE 21: Butterworh & Chebeyshev BP Filters. Part 1: Series and Parallel RLC Circuits On NOT Again LECTURE : Butterworh & Chebeyshev BP Filters Part : Series and Parallel RLC Circuits On NOT Again. RLC Admittance/Impedance Transfer Functions EXAMPLE : Series RLC. H(s) I out (s) V in (s) Y in (s) R Ls

More information

8. Active Filters - 2. Electronic Circuits. Prof. Dr. Qiuting Huang Integrated Systems Laboratory

8. Active Filters - 2. Electronic Circuits. Prof. Dr. Qiuting Huang Integrated Systems Laboratory 8. Active Filters - 2 Electronic Circuits Prof. Dr. Qiuting Huang Integrated Systems Laboratory Blast From The Past: Algebra of Polynomials * PP xx is a polynomial of the variable xx: PP xx = aa 0 + aa

More information

Second-order filters. EE 230 second-order filters 1

Second-order filters. EE 230 second-order filters 1 Second-order filters Second order filters: Have second order polynomials in the denominator of the transfer function, and can have zeroth-, first-, or second-order polynomials in the numerator. Use two

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

Alternating Current Circuits. Home Work Solutions

Alternating Current Circuits. Home Work Solutions Chapter 21 Alternating Current Circuits. Home Work s 21.1 Problem 21.11 What is the time constant of the circuit in Figure (21.19). 10 Ω 10 Ω 5.0 Ω 2.0µF 2.0µF 2.0µF 3.0µF Figure 21.19: Given: The circuit

More information

Frequency Response part 2 (I&N Chap 12)

Frequency Response part 2 (I&N Chap 12) Frequency Response part 2 (I&N Chap 12) Introduction & TFs Decibel Scale & Bode Plots Resonance Scaling Filter Networks Applications/Design Frequency response; based on slides by J. Yan Slide 3.1 Example

More information

0-2 Operations with Complex Numbers

0-2 Operations with Complex Numbers Simplify. 1. i 10 2. i 2 + i 8 3. i 3 + i 20 4. i 100 5. i 77 esolutions Manual - Powered by Cognero Page 1 6. i 4 + i 12 7. i 5 + i 9 8. i 18 Simplify. 9. (3 + 2i) + ( 4 + 6i) 10. (7 4i) + (2 3i) 11.

More information

0-2 Operations with Complex Numbers

0-2 Operations with Complex Numbers Simplify. 1. i 10 1 2. i 2 + i 8 0 3. i 3 + i 20 1 i esolutions Manual - Powered by Cognero Page 1 4. i 100 1 5. i 77 i 6. i 4 + i 12 2 7. i 5 + i 9 2i esolutions Manual - Powered by Cognero Page 2 8.

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

Deliyannis, Theodore L. et al "Two Integrator Loop OTA-C Filters" Continuous-Time Active Filter Design Boca Raton: CRC Press LLC,1999

Deliyannis, Theodore L. et al Two Integrator Loop OTA-C Filters Continuous-Time Active Filter Design Boca Raton: CRC Press LLC,1999 Deliyannis, Theodore L. et al "Two Integrator Loop OTA-C Filters" Continuous-Time Active Filter Design Boca Raton: CRC Press LLC,1999 Chapter 9 Two Integrator Loop OTA-C Filters 9.1 Introduction As discussed

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

Chapter 33. Alternating Current Circuits

Chapter 33. Alternating Current Circuits Chapter 33 Alternating Current Circuits 1 Capacitor Resistor + Q = C V = I R R I + + Inductance d I Vab = L dt AC power source The AC power source provides an alternative voltage, Notation - Lower case

More information

Active Filters an Introduction

Active Filters an Introduction Active Filter an Introduction + Vin() - Filter circuit G() + Vout() - Active Filter. Continuou-time or Sampled-data. Employ active element (e.g. tranitor, amplifier, op-amp) a. inductor-le (continuou-time)

More information

FEEDBACK, STABILITY and OSCILLATORS

FEEDBACK, STABILITY and OSCILLATORS FEEDBACK, STABILITY and OSCILLATORS à FEEDBACK, STABILITY and OSCILLATORS - STABILITY OF FEEDBACK SYSTEMS - Example : ANALYSIS and DESIGN OF PHASE-SHIFT-OSCILLATORS - Example 2: ANALYSIS and DESIGN OF

More information

Open Baffle w/ 2 Drivers - Acoustic Response 12/27/12. Copyright 2012 by Martin J. King. All Rights Reserved.

Open Baffle w/ 2 Drivers - Acoustic Response 12/27/12. Copyright 2012 by Martin J. King. All Rights Reserved. Open Baffle w/ 2 Drivers - Acoustic Response 12/27/12 Software : by Martin J. King e-mail MJKing57@aol.com Copyright 212 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/

More information

Solutions to Problems in Chapter 6

Solutions to Problems in Chapter 6 Appendix F Solutions to Problems in Chapter 6 F.1 Problem 6.1 Short-circuited transmission lines Section 6.2.1 (book page 193) describes the method to determine the overall length of the transmission line

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

Electronic Circuits EE359A

Electronic Circuits EE359A Electronic Circuits EE359A Bruce McNair B26 bmcnair@stevens.edu 21-216-5549 Lecture 22 569 Second order section Ts () = s as + as+ a 2 2 1 ω + s+ ω Q 2 2 ω 1 p, p = ± 1 Q 4 Q 1 2 2 57 Second order section

More information

Modelling Non-Ideal Inductors in SPICE

Modelling Non-Ideal Inductors in SPICE Modelling Non-Ideal Inductors in SPICE Martin O'Hara Technical Manager, Newport Components, Milton Keynes November 1994 Abstract The non-ideal inductor exhibits both self resonance and non-linear current

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

Expressions for f r (T ) and Q i (T ) from Mattis-Bardeen theory

Expressions for f r (T ) and Q i (T ) from Mattis-Bardeen theory 8 Appendix A Expressions for f r (T ) and Q i (T ) from Mattis-Bardeen theory The Mattis-Bardeen theory of the anomalous skin effect in superconductors [0] may be used to derive the behavior of the resonance

More information

Electricity and Light Pre Lab Questions

Electricity and Light Pre Lab Questions Electricity and Light Pre Lab Questions The pre lab questions can be answered by reading the theory and procedure for the related lab. You are strongly encouraged to answers these questions on your own.

More information

Case Study: Parallel Coupled- Line Combline Filter

Case Study: Parallel Coupled- Line Combline Filter MICROWAVE AND RF DESIGN MICROWAVE AND RF DESIGN Case Study: Parallel Coupled- Line Combline Filter Presented by Michael Steer Reading: 6. 6.4 Index: CS_PCL_Filter Based on material in Microwave and RF

More information

Op-Amp Circuits: Part 3

Op-Amp Circuits: Part 3 Op-Amp Circuits: Part 3 M. B. Patil mbpatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Department of Electrical Engineering Indian Institute of Technology Bombay Introduction to filters Consider v(t) = v

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

Physics 4B Chapter 31: Electromagnetic Oscillations and Alternating Current

Physics 4B Chapter 31: Electromagnetic Oscillations and Alternating Current Physics 4B Chapter 31: Electromagnetic Oscillations and Alternating Current People of mediocre ability sometimes achieve outstanding success because they don't know when to quit. Most men succeed because

More information

Handout 11: AC circuit. AC generator

Handout 11: AC circuit. AC generator Handout : AC circuit AC generator Figure compares the voltage across the directcurrent (DC) generator and that across the alternatingcurrent (AC) generator For DC generator, the voltage is constant For

More information

EE-202 Exam III April 13, 2015

EE-202 Exam III April 13, 2015 EE-202 Exam III April 3, 205 Name: (Please print clearly.) Student ID: CIRCLE YOUR DIVISION DeCarlo-7:30-8:30 Furgason 3:30-4:30 DeCarlo-:30-2:30 202 2022 2023 INSTRUCTIONS There are 2 multiple choice

More information

Introduction. HFSS 3D EM Analysis S-parameter. Q3D R/L/C/G Extraction Model. magnitude [db] Frequency [GHz] S11 S21 -30

Introduction. HFSS 3D EM Analysis S-parameter. Q3D R/L/C/G Extraction Model. magnitude [db] Frequency [GHz] S11 S21 -30 ANSOFT Q3D TRANING Introduction HFSS 3D EM Analysis S-parameter Q3D R/L/C/G Extraction Model 0-5 -10 magnitude [db] -15-20 -25-30 S11 S21-35 0 1 2 3 4 5 6 7 8 9 10 Frequency [GHz] Quasi-static or full-wave

More information

( s) N( s) ( ) The transfer function will take the form. = s = 2. giving ωo = sqrt(1/lc) = 1E7 [rad/s] ω 01 := R 1. α 1 2 L 1.

( s) N( s) ( ) The transfer function will take the form. = s = 2. giving ωo = sqrt(1/lc) = 1E7 [rad/s] ω 01 := R 1. α 1 2 L 1. Problem ) RLC Parallel Circuit R L C E-4 E-0 V a. What is the resonant frequency of the circuit? The transfer function will take the form N ( ) ( s) N( s) H s R s + α s + ω s + s + o L LC giving ωo sqrt(/lc)

More information

Decibel measurements

Decibel measurements Decibel measurements This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,

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

Contents The Real Number System

Contents The Real Number System Contents 1. The Real Number System 2 1.1 Some Sets and Basic Laws of Real Numbers................ 2 Example 1.15................................ 2 Example 1.16................................ 3 1.2 Basic

More information

Kirchhoff's Laws and Circuit Analysis (EC 2)

Kirchhoff's Laws and Circuit Analysis (EC 2) Kirchhoff's Laws and Circuit Analysis (EC ) Circuit analysis: solving for I and V at each element Linear circuits: involve resistors, capacitors, inductors Initial analysis uses only resistors Power sources,

More information

Copyright 2014 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass Driver Mounted on an Open Baffle

Copyright 2014 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass Driver Mounted on an Open Baffle Open Baffle w/ 3 Drivers - Acoustic Response 12/3/1 Software : by Martin J. King e-mail MJKing57@aol.com Copyright 21 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass

More information

Open Baffle w/ 2 Drivers - Acoustic Response 12/30/14. Copyright 2014 by Martin J. King. All Rights Reserved.

Open Baffle w/ 2 Drivers - Acoustic Response 12/30/14. Copyright 2014 by Martin J. King. All Rights Reserved. Open Baffle w/ 2 Drivers - Acoustic Response 12/3/14 Software : by Martin J. King e-mail MJKing57@aol.com Copyright 214 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/

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

Alternating Current Circuits

Alternating Current Circuits Alternating Current Circuits AC Circuit An AC circuit consists of a combination of circuit elements and an AC generator or source. The output of an AC generator is sinusoidal and varies with time according

More information

EE40 Midterm Review Prof. Nathan Cheung

EE40 Midterm Review Prof. Nathan Cheung EE40 Midterm Review Prof. Nathan Cheung 10/29/2009 Slide 1 I feel I know the topics but I cannot solve the problems Now what? Slide 2 R L C Properties Slide 3 Ideal Voltage Source *Current depends d on

More information

SUGGESTED LESSON PLANS FOR PHY 097 SEMESTER NOV10 Text Book : PHYSICS FOR SCIENTISTS & ENGINEERS WITH MODERN PHYSICS BY GIANCOLI, FOURTH EDITION

SUGGESTED LESSON PLANS FOR PHY 097 SEMESTER NOV10 Text Book : PHYSICS FOR SCIENTISTS & ENGINEERS WITH MODERN PHYSICS BY GIANCOLI, FOURTH EDITION SUGGESTED LESSON PLANS FOR PHY 097 SEMESTER NOV0 Text Book : PHYSICS FOR SCIENTISTS & ENGINEERS WITH MODERN PHYSICS BY GIANCOLI, FOURTH EDITION Week Topics Section Page Hrs Sub-Topics WAVES AND OPTICS,.0

More information

LAB MANUAL EXPERIMENT NO. 7

LAB MANUAL EXPERIMENT NO. 7 LAB MANUAL EXPERIMENT NO. 7 Aim of the Experiment: Concept of Generalized N-port scattering parameters, and formulation of these parameters into 2-port reflection and transmission coefficients. Requirement:

More information

Start with the transfer function for a second-order high-pass. s 2. ω o. Q P s + ω2 o. = G o V i

Start with the transfer function for a second-order high-pass. s 2. ω o. Q P s + ω2 o. = G o V i 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

More information

Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies

Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies Induced emf - Faraday s Experiment When a magnet moves toward a loop of wire, the ammeter shows the presence of a current When

More information

Electronics II. Final Examination

Electronics II. Final Examination The University of Toledo f17fs_elct27.fm 1 Electronics II Final Examination Problems Points 1. 11 2. 14 3. 15 Total 40 Was the exam fair? yes no The University of Toledo f17fs_elct27.fm 2 Problem 1 11

More information

EE-202 Exam III April 15, 2010

EE-202 Exam III April 15, 2010 EE-0 Exam III April 5, 00 Name: SOLUTION (No period) (Please print clearly) Student ID: CIRCLE YOUR DIVISION Morning 8:30 MWF Afternoon 3:30 MWF INSTRUCTIONS There are 9 multiple choice worth 5 points

More information

Laplace Transform Analysis of Signals and Systems

Laplace Transform Analysis of Signals and Systems Laplace Transform Analysis of Signals and Systems Transfer Functions Transfer functions of CT systems can be found from analysis of Differential Equations Block Diagrams Circuit Diagrams 5/10/04 M. J.

More information

Lecture 6: Impedance (frequency dependent. resistance in the s- world), Admittance (frequency. dependent conductance in the s- world), and

Lecture 6: Impedance (frequency dependent. resistance in the s- world), Admittance (frequency. dependent conductance in the s- world), and Lecture 6: Impedance (frequency dependent resistance in the s- world), Admittance (frequency dependent conductance in the s- world), and Consequences Thereof. Professor Ray, what s an impedance? Answers:

More information

IMPERIAL COLLEGE OF SCIENCE, TECHNOLOGY AND MEDICINE UNIVERSITY OF LONDON DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2010

IMPERIAL COLLEGE OF SCIENCE, TECHNOLOGY AND MEDICINE UNIVERSITY OF LONDON DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2010 Paper Number(s): E1.1 IMPERIAL COLLEGE OF SCIENCE, TECHNOLOGY AND MEDICINE UNIVERSITY OF LONDON DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2010 EEE/ISE PART I: MEng, BEng and ACGI

More information

1 Phasors and Alternating Currents

1 Phasors and Alternating Currents Physics 4 Chapter : Alternating Current 0/5 Phasors and Alternating Currents alternating current: current that varies sinusoidally with time ac source: any device that supplies a sinusoidally varying potential

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

EE -213 BASIC CIRCUIT ANALYSIS LAB MANUAL

EE -213 BASIC CIRCUIT ANALYSIS LAB MANUAL EE -213 BASIC CIRCUIT ANALYSIS LAB MANUAL EE 213 Fall 2009 LABORATORY #1 INTRODUCTION TO MATLAB INTRODUCTION The purpose of this laboratory is to introduce you to Matlab and to illustrate some of its circuit

More information

D is the voltage difference = (V + - V - ).

D is the voltage difference = (V + - V - ). 1 Operational amplifier is one of the most common electronic building blocks used by engineers. It has two input terminals: V + and V -, and one output terminal Y. It provides a gain A, which is usually

More information

Signal Processing. Lecture 10: FIR Filter Design. Ahmet Taha Koru, Ph. D. Yildiz Technical University Fall

Signal Processing. Lecture 10: FIR Filter Design. Ahmet Taha Koru, Ph. D. Yildiz Technical University Fall Signal Processing Lecture 10: FIR Filter Design Ahmet Taha Koru, Ph. D. Yildiz Technical University 2017-2018 Fall ATK (YTU) Signal Processing 2017-2018 Fall 1 / 47 Introduction Introduction ATK (YTU)

More information

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. Solutions to Assignment 3 February 2005.

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. Solutions to Assignment 3 February 2005. SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuit II Solution to Aignment 3 February 2005. Initial Condition Source 0 V battery witch flip at t 0 find i 3 (t) Component value:

More information

CHAPTER 5 ANALYSIS OF EXTRAPOLATION VOLTAGES

CHAPTER 5 ANALYSIS OF EXTRAPOLATION VOLTAGES CHAPTER 5 ANALYSIS OF EXTRAPOLATION VOLTAGES In the previous chapters, the emphasis was on understanding the acoustical nonlinearities that would corrupt the ideal voltage based linear extrapolation. However,

More information

Algebraic substitution for electric circuits

Algebraic substitution for electric circuits Algebraic substitution for electric circuits This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,

More information

Algebraic substitution for electric circuits

Algebraic substitution for electric circuits Algebraic substitution for electric circuits This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,

More information

LCR Series Circuits. AC Theory. Introduction to LCR Series Circuits. Module. What you'll learn in Module 9. Module 9 Introduction

LCR Series Circuits. AC Theory. Introduction to LCR Series Circuits. Module. What you'll learn in Module 9. Module 9 Introduction Module 9 AC Theory LCR Series Circuits Introduction to LCR Series Circuits What you'll learn in Module 9. Module 9 Introduction Introduction to LCR Series Circuits. Section 9.1 LCR Series Circuits. Amazing

More information

First and Second Order Circuits. Claudio Talarico, Gonzaga University Spring 2015

First and Second Order Circuits. Claudio Talarico, Gonzaga University Spring 2015 First and Second Order Circuits Claudio Talarico, Gonzaga University Spring 2015 Capacitors and Inductors intuition: bucket of charge q = Cv i = C dv dt Resist change of voltage DC open circuit Store voltage

More information

Sinusoidal Steady State Analysis (AC Analysis) Part I

Sinusoidal Steady State Analysis (AC Analysis) Part I Sinusoidal Steady State Analysis (AC Analysis) Part I Amin Electronics and Electrical Communications Engineering Department (EECE) Cairo University elc.n102.eng@gmail.com http://scholar.cu.edu.eg/refky/

More information

Prefix Prefix Scaling Example EXP Name

Prefix Prefix Scaling Example EXP Name MATHEMATICS PRIMER Introduction This part of the course of study toward the Radio Communications Examination (RCE) is primarily concerned with ensuring that students can cope with the mathematics required.

More information

Q. 1 Q. 25 carry one mark each.

Q. 1 Q. 25 carry one mark each. GATE 5 SET- ELECTRONICS AND COMMUNICATION ENGINEERING - EC Q. Q. 5 carry one mark each. Q. The bilateral Laplace transform of a function is if a t b f() t = otherwise (A) a b s (B) s e ( a b) s (C) e as

More information

Proofs, Strings, and Finite Automata. CS154 Chris Pollett Feb 5, 2007.

Proofs, Strings, and Finite Automata. CS154 Chris Pollett Feb 5, 2007. Proofs, Strings, and Finite Automata CS154 Chris Pollett Feb 5, 2007. Outline Proofs and Proof Strategies Strings Finding proofs Example: For every graph G, the sum of the degrees of all the nodes in G

More information

BME/ISE 3511 Bioelectronics - Test Five Review Notes Fall 2015

BME/ISE 3511 Bioelectronics - Test Five Review Notes Fall 2015 BME/ISE 35 Bioelectronics - Test Five Review Notes Fall 205 Test Five Topics: RMS Resistive Power oss (I 2 R) A Reactance, Impedance, Power Factor R ircuit Analysis alculate Series R Impedance alculate

More information

Electronic Circuits EE359A

Electronic Circuits EE359A Electronic Circuits EE359A Bruce McNair B26 bmcnair@stevens.edu 21-216-5549 Lecture 22 578 Second order LCR resonator-poles V o I 1 1 = = Y 1 1 + sc + sl R s = C 2 s 1 s + + CR LC s = C 2 sω 2 s + + ω

More information

The process of analysing a circuit using the Laplace technique can be broken down into a series of straightforward steps:

The process of analysing a circuit using the Laplace technique can be broken down into a series of straightforward steps: Analysis of a series RLC circuit using Laplace Transforms Part. How to do it. The process of analysing a circuit using the Laplace technique can be broken down into a series of straightforward steps:.

More information

Analysis and Design of Differential LNAs with On-Chip Transformers in 65-nm CMOS Technology

Analysis and Design of Differential LNAs with On-Chip Transformers in 65-nm CMOS Technology Analysis and Design of Differential LNAs with On-Chip Transformers in 65-nm CMOS Technology Takao Kihara, Shigesato Matsuda, Tsutomu Yoshimura Osaka Institute of Technology, Japan June 27, 2016 2 / 16

More information

Electronic Circuits Summary

Electronic Circuits Summary Electronic Circuits Summary Andreas Biri, D-ITET 6.06.4 Constants (@300K) ε 0 = 8.854 0 F m m 0 = 9. 0 3 kg k =.38 0 3 J K = 8.67 0 5 ev/k kt q = 0.059 V, q kt = 38.6, kt = 5.9 mev V Small Signal Equivalent

More information

(amperes) = (coulombs) (3.1) (seconds) Time varying current. (volts) =

(amperes) = (coulombs) (3.1) (seconds) Time varying current. (volts) = 3 Electrical Circuits 3. Basic Concepts Electric charge coulomb of negative change contains 624 0 8 electrons. Current ampere is a steady flow of coulomb of change pass a given point in a conductor in

More information

MARK SCHEME for the October/November 2012 series 9702 PHYSICS

MARK SCHEME for the October/November 2012 series 9702 PHYSICS CAMBRIDGE INTERNATIONAL EXAMINATIONS GCE Advanced Subsidiary Level and GCE Advanced Level MARK SCHEME for the October/November 2012 series 9702 PHYSICS 9702/42 Paper 4 (A2 Structured Questions), maximum

More information

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. R 4 := 100 kohm

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. R 4 := 100 kohm SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuit II Solution to Aignment 3 February 2003. Cacaded Op Amp [DC&L, problem 4.29] An ideal op amp ha an output impedance of zero,

More information

Name: (Please print clearly) Student ID: CIRCLE YOUR DIVISION INSTRUCTIONS

Name: (Please print clearly) Student ID: CIRCLE YOUR DIVISION INSTRUCTIONS EE 202 Exam III April 13 2011 Name: (Please print clearly) Student ID: CIRCLE YOUR DIVISION Morning 7:30 MWF Furgason INSTRUCTIONS Afternoon 3:30 MWF DeCarlo There are 10 multiple choice worth 5 points

More information

fiziks Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES

fiziks Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES Content-ELECTRICITY AND MAGNETISM 1. Electrostatics (1-58) 1.1 Coulomb s Law and Superposition Principle 1.1.1 Electric field 1.2 Gauss s law 1.2.1 Field lines and Electric flux 1.2.2 Applications 1.3

More information

ESE319 Introduction to Microelectronics Bode Plot Review High Frequency BJT Model

ESE319 Introduction to Microelectronics Bode Plot Review High Frequency BJT Model Bode Plot Review High Frequency BJT Model 1 Logarithmic Frequency Response Plots (Bode Plots) Generic form of frequency response rational polynomial, where we substitute jω for s: H s=k sm a m 1 s m 1

More information

6.1 Introduction

6.1 Introduction 6. Introduction A.C Circuits made up of resistors, inductors and capacitors are said to be resonant circuits when the current drawn from the supply is in phase with the impressed sinusoidal voltage. Then.

More information

y(d) = j

y(d) = j Problem 2.66 A 0-Ω transmission line is to be matched to a computer terminal with Z L = ( j25) Ω by inserting an appropriate reactance in parallel with the line. If f = 800 MHz and ε r = 4, determine the

More information

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder . W. Erickson Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder 8.1.7. The low-q approximation Given a second-order denominator polynomial, of the form G(s)= 1

More information

(3), where V is the peak value of the tank voltage in the LC circuit. 2 The inductor energy is: E.l= LI 2

(3), where V is the peak value of the tank voltage in the LC circuit. 2 The inductor energy is: E.l= LI 2 Frequency compensated LC networks for oscillators with the wide tuning range. Theoretical discussion section. by Vladimir Novichkov 02/2/202 rev 0.42. Properties of passive, capacitively tuned LC resonator

More information

Plumber s LCR Analogy

Plumber s LCR Analogy Plumber s LCR Analogy Valve V 1 V 2 P 1 P 2 The plumber s analogy of an LC circuit is a rubber diaphragm that has been stretched by pressure on the top (P 1 ) side. When the valve starts the flow, the

More information

Lecture 14 Date:

Lecture 14 Date: Lecture 14 Date: 18.09.2014 L Type Matching Network Examples Nodal Quality Factor T- and Pi- Matching Networks Microstrip Matching Networks Series- and Shunt-stub Matching L Type Matching Network (contd.)

More information

CS 436 HCI Technology Basic Electricity/Electronics Review

CS 436 HCI Technology Basic Electricity/Electronics Review CS 436 HCI Technology Basic Electricity/Electronics Review *Copyright 1997-2008, Perry R. Cook, Princeton University August 27, 2008 1 Basic Quantities and Units 1.1 Charge Number of electrons or units

More information

Exercise s = 1. cos 60 ± j sin 60 = 0.5 ± j 3/2. = s 2 + s + 1. (s + 1)(s 2 + s + 1) T(jω) = (1 + ω2 )(1 ω 2 ) 2 + ω 2 (1 + ω 2 )

Exercise s = 1. cos 60 ± j sin 60 = 0.5 ± j 3/2. = s 2 + s + 1. (s + 1)(s 2 + s + 1) T(jω) = (1 + ω2 )(1 ω 2 ) 2 + ω 2 (1 + ω 2 ) Exercise 7 Ex: 7. A 0 log T [db] T 0.99 0.9 0.8 0.7 0.5 0. 0 A 0 0. 3 6 0 Ex: 7. A max 0 log.05 0 log 0.95 0.9 db [ ] A min 0 log 40 db 0.0 Ex: 7.3 s + js j Ts k s + 3 + j s + 3 j s + 4 k s + s + 4 + 3

More information