Lab 1 Getting Started with EDA Tools
|
|
- Osborne Warren
- 5 years ago
- Views:
Transcription
1 Lab Getting Started with EDA Tools E3-238: Analog LSI Circuits INTRODUCTION The objective of this lab is to familiarize you with the Cadence irtuoso design environment. The irtuoso environment provides a set of tools to perform various operations in custom integrated circuit design, such as, design entry, simulation, extraction, and verification. This lab is focused on the schematic entry and circuit simulation. A subset of tools required for this lab is listed in Table. The problems in this lab are given to serve as a starting point for you to explore the capabilities and limitations of the tools. Table Tools for custom integrated circuit design. Tool Cadence irtuoso (IC67) Library Manager Schematic Editor L Analog Design Environment (ADE) L isualization and Analysis (ia) L Spectre (MMSIM5) Purpose To create and edit design libraries and cells. For graphical entry of circuit topology and parameters. To setup design variables, analyses, and probes. For post simulation data visualization and analysis. For circuit simulation. INSTRUCTIONS. The required device models for this lab are given in Appendix and stored at /Shares/models/lab.scs location at the arslserver. Include this file in ADE- L setup to use the models. 2. Use the inverter cell given in the lab_ref library for Problem 3. To include this library, append the following line in your cds.lib file present in the current working directory (home folder): DEFINE lab_ref /Shares/libraries/lab_ref. Page of 5
2 Problem (DC analysis of linear network) Find out the DC operating point (node voltages) of the circuit shown in Figure by both handcalculation and simulation. R4 5 R probe R2 3 A B C I.5 A I + R 3 2 2I 3 I 2 4 Figure Resistive network with dependent sources. Problem 2 (DC analysis of nonlinear circuit) D/ T Consider the circuit in Figure 2. Assuming the exponential model ( I I e ) for the diode, hand-calculate the exact voltage across the diode (up to four places after the decimal point) using an iterative method. Simulate the DC operating point of the circuit using mydiode model (given in Appendix), and compare the hand-calculated and simulated values. Rk D S D I D mydiode I S 0 fa, Figure 2 Circuit with nonlinear component. Page 2 of 5
3 Problem 3 (DC analysis of circuit with multiple operating points) For the cross-coupled inverter shown in Figure 3, there exists three DC operating points. Obtain both the stable and meta-stable DC operating points by simulation with the inverter circuit given in Figure 4. Without a prior knowledge of the circuit behavior, how would you determine the number of equilibrium states (DC solutions) and check their stability? in 2 out 2 A 2 out, out in2 Stable Solutions in out A out Metastable solution, in out2 Figure 3 Cross-coupled pair of inverting amplifiers and its transfer characteristics. DD 5 mypmos W / L0 m/m in out mynmos W / L0 m/m Figure 4 Circuit description of the inverting amplifier. Page 3 of 5
4 Problem 4 (Transient analysis) For the first-order RC network shown in Figure 5, simulate the behavior of this circuit subject to a 0 to step input having a rise time of no more than 0ns. Plot the voltage waveform across the resistor and capacitor. erify that voltage across the capacitor changes by 63% of its final value in a time of one time constant. Repeat the above experiment with the initial voltage of 0.5 across the capacitor, and observe that initial conditions affect the initial operating point (in transient analysis). Rk 0 in R C C F Figure 5 First order RC network Problem 5 (AC analysis) In AC analysis, the simulator computes the small-signal behavior using phasor analysis of a circuit by first linearizing the circuit about a DC operating point. Compute the frequency response of the series RLC network shown in Figure 6. Plot both the magnitude and phase behavior of the loop current and the voltage across resistor, capacitor and inductor over a frequency range of mhz to MHz. Use 0 points per decade in your plot. Also, observe the following and comment:. The frequency response does not change with the change in initial conditions of the capacitor and inductor which of course affects the DC operating point. Why is it so? 2. At resonant frequency (f 0 = /2π LC), the magnitude of the voltage across capacitor and inductor depends on the value of the resistor and can be greater than the source voltage magnitude. If so, can the circuit be used as a voltage amplifier? If yes, then what about its power gain? Rk C F in R C 0 L LH Figure 6 Series RLC network. Page 4 of 5
5 APPENDIX The content of the lab.scs model file is shown in Table 2. Table 2 Spectre models. model mydiode diode is=0e-5 n= model mynmos mos2 type=n vto = tox = 400e-0 nsub = 8e+5 + xj = 0.5u ld = 0.20u uo = 650 ucrit = 0.62e+5 uexp = vmax = 5.e+4 neff = 4.0 delta =.4 rsh = 36 cgso =.95e-0 + cgdo =.95e-0 cj = 95u cjsw = 500p mj = 0.76 mjsw = pb = 0.8 model mypmos mos2 type=p vto = tox = 400e-0 nsub = 6e+5 + xj = 0.05u ld = 0.20u uo = 255 ucrit = 0.86e+5 uexp = vmax = 3.0e+4 neff = 2.65 delta =.0 rsh = 0 cgso =.90e-0 + cgdo =.90e-0 cj = 250u cjsw = 350p mj = mjsw = pb = 0.8 Page 5 of 5
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 informationThe Devices. Devices
The The MOS Transistor Gate Oxyde Gate Source n+ Polysilicon Drain n+ Field-Oxyde (SiO 2 ) p-substrate p+ stopper Bulk Contact CROSS-SECTION of NMOS Transistor Cross-Section of CMOS Technology MOS transistors
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 6: January 30, 2018 MOS Operating Regions, pt. 2 Lecture Outline! Operating Regions (review) " Subthreshold " Resistive " Saturation! Intro.
More informationProblem info Geometry model Labelled Objects Results Nonlinear dependencies
Problem info Problem type: Transient Magnetics (integration time: 9.99999993922529E-09 s.) Geometry model class: Plane-Parallel Problem database file names: Problem: circuit.pbm Geometry: Circuit.mod Material
More informationQUESTION 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 informationBasic RL and RC Circuits R-L TRANSIENTS: STORAGE CYCLE. Engineering Collage Electrical Engineering Dep. Dr. Ibrahim Aljubouri
st Class Basic RL and RC Circuits The RL circuit with D.C (steady state) The inductor is short time at Calculate the inductor current for circuits shown below. I L E R A I L E R R 3 R R 3 I L I L R 3 R
More informationBasic. Theory. ircuit. Charles A. Desoer. Ernest S. Kuh. and. McGraw-Hill Book Company
Basic C m ш ircuit Theory Charles A. Desoer and Ernest S. Kuh Department of Electrical Engineering and Computer Sciences University of California, Berkeley McGraw-Hill Book Company New York St. Louis San
More information! MOS Capacitances. " Extrinsic. " Intrinsic. ! Lumped Capacitance Model. ! First Order Capacitor Summary. ! Capacitance Implications
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 7: February, 07 MOS SPICE Models, MOS Parasitic Details Lecture Outline! MOS Capacitances " Extrinsic " Intrinsic! Lumped Capacitance Model!
More informationAC 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 informationPhysics for Scientists & Engineers 2
Electromagnetic Oscillations Physics for Scientists & Engineers Spring Semester 005 Lecture 8! We have been working with circuits that have a constant current a current that increases to a constant current
More informationENGR 2405 Chapter 8. Second Order Circuits
ENGR 2405 Chapter 8 Second Order Circuits Overview The previous chapter introduced the concept of first order circuits. This chapter will expand on that with second order circuits: those that need a second
More informationChapter 3. Steady-State Equivalent Circuit Modeling, Losses, and Efficiency
Chapter 3. Steady-State Equivalent Circuit Modeling, Losses, and Efficiency 3.1. The dc transformer model 3.2. Inclusion of inductor copper loss 3.3. Construction of equivalent circuit model 3.4. How to
More informationAlternating 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 informationUniversity of Pennsylvania Department of Electrical Engineering. ESE 570 Midterm Exam March 14, 2013 FORMULAS AND DATA
University of Pennsylvania Department of Electrical Engineering ESE 570 Midterm Exam March 4, 03 FORMULAS AND DATA. PHYSICAL CONSTANTS: n i = intrinsic concentration undoped) silicon =.45 x 0 0 cm -3 @
More information1 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 informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 7: February 4, 2016 MOS SPICE Models, MOS Parasitic Details Lecture Outline! MOS Capacitances " Extrinsic " Intrinsic! Lumped Capacitance
More informationEDEXCEL NATIONALS UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES. ASSIGNMENT No.2 - CAPACITOR NETWORK
EDEXCEL NATIONALS UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES ASSIGNMENT No.2 - CAPACITOR NETWORK NAME: I agree to the assessment as contained in this assignment. I confirm that the work submitted is
More informationAt point G V = = = = = = RB B B. IN RB f
Common Emitter At point G CE RC 0. 4 12 0. 4 116. I C RC 116. R 1k C 116. ma I IC 116. ma β 100 F 116µ A I R ( 116µ A)( 20kΩ) 2. 3 R + 2. 3 + 0. 7 30. IN R f Gain in Constant Current Region I I I C F
More informationTexas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos
Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Lecture 5: Electrical and Electromagnetic System Components The objective of this
More informationExercise 1: RC Time Constants
Exercise 1: RC EXERCISE OBJECTIVE When you have completed this exercise, you will be able to determine the time constant of an RC circuit by using calculated and measured values. You will verify your results
More informationCircuits. L2: MOS Models-2 (1 st Aug. 2013) B. Mazhari Dept. of EE, IIT Kanpur. B. Mazhari, IITK. G-Number
EE610: CMOS Analog Circuits L: MOS Models- (1 st Aug. 013) B. Mazhari Dept. of EE, IIT Kanpur 3 NMOS Models MOS MODEL Above Threshold Subthreshold ( GS > TN ) ( GS < TN ) Saturation ti Ti Triode ( DS >
More informationNETWORK 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 informationIntegrated Circuit Design: OTA in 0.5µm Technology
Integrated Circuit Design: OTA in 0.5µm Technology Omar X. Avelar, Omar de la Mora & Diego I. Romero INTEGRATED CIRCUITS DESIGN (ESI108A) Instituto Tecnológico y de Estudios Superiores de Occidente (ITESO)
More informationComplete all the identification fields below or 10% of the lab value will be deduced from your final mark for this lab.
Simple circuits 3 hr Identification page Instructions: Print this page and the following ones before your lab session to prepare your lab report. Staple them together with your graphs at the end. If you
More informationAlternating 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 informationEE292: 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 informationInductance, Inductors, RL Circuits & RC Circuits, LC, and RLC Circuits
Inductance, Inductors, RL Circuits & RC Circuits, LC, and RLC Circuits Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the timevarying
More informationESE 570 MOS TRANSISTOR THEORY Part 2
ESE 570 MOS TRANSISTOR THEORY Part 2 GCA (gradual channel approximation) MOS Transistor Model Strong Inversion Operation CMOS = NMOS + PMOS 2 TwoTerminal MOS Capacitor > nmos Transistor VGS
More informationMODULE I. Transient Response:
Transient Response: MODULE I The Transient Response (also known as the Natural Response) is the way the circuit responds to energies stored in storage elements, such as capacitors and inductors. If a capacitor
More informationMarwadi University Draft Syllabus for Bachelor of Technology Electronics and Communication. Subject Code: 03EC0302
Subject Code: 03EC0302 Subject Name: Circuits and Networks B. Tech. Year II (Semester III) Objective: After completion of this course, student will be able to: 1. To introduce electric circuits and its
More informationElectromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3.
Electromagnetic Oscillations and Alternating Current 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3. RLC circuit in AC 1 RL and RC circuits RL RC Charging Discharging I = emf R
More information2005 AP PHYSICS C: ELECTRICITY AND MAGNETISM FREE-RESPONSE QUESTIONS
2005 AP PHYSICS C: ELECTRICITY AND MAGNETISM In the circuit shown above, resistors 1 and 2 of resistance R 1 and R 2, respectively, and an inductor of inductance L are connected to a battery of emf e and
More informationPhysics 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 informationElectrical Circuits Lab Series RC Circuit Phasor Diagram
Electrical Circuits Lab. 0903219 Series RC Circuit Phasor Diagram - Simple steps to draw phasor diagram of a series RC circuit without memorizing: * Start with the quantity (voltage or current) that is
More informationIndustrial Technology: Electronic Technology Crosswalk to AZ Math Standards
Page 1 of 1 August 1998 1M-P1 Compare and contrast the real number system and its various subsystems with regard to their structural characteristics. PO 2 PO 3 2.0 Apply mathematics calculations. 2.1 Apply
More informationLAPLACE TRANSFORMATION AND APPLICATIONS. Laplace transformation It s a transformation method used for solving differential equation.
LAPLACE TRANSFORMATION AND APPLICATIONS Laplace transformation It s a transformation method used for solving differential equation. Advantages The solution of differential equation using LT, progresses
More informationChapter 10: Sinusoidal Steady-State Analysis
Chapter 10: Sinusoidal Steady-State Analysis 10.1 10.2 10.3 10.4 10.5 10.6 10.9 Basic Approach Nodal Analysis Mesh Analysis Superposition Theorem Source Transformation Thevenin & Norton Equivalent Circuits
More informationPRESIDENCY UNIVERSITY DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING EE 310: VLSI System Laboratory. Contents
PRESIDENCY UNIVERSITY DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING EE 310: VLSI System Laboratory Contents Experiment No Name of The Experiments. Page Experiment-1 INTRODUCTION TO CIRCUIT SIMULATION
More informationRC, RL, and LCR Circuits
RC, RL, and LCR Circuits EK307 Lab Note: This is a two week lab. Most students complete part A in week one and part B in week two. Introduction: Inductors and capacitors are energy storage devices. They
More informationUnit 2: Modeling in the Frequency Domain. Unit 2, Part 4: Modeling Electrical Systems. First Example: Via DE. Resistors, Inductors, and Capacitors
Unit 2: Modeling in the Frequency Domain Part 4: Modeling Electrical Systems Engineering 582: Control Systems I Faculty of Engineering & Applied Science Memorial University of Newfoundland January 20,
More informationIE1206 Embedded Electronics
IE1206 Embedded Electronics Le1 Le3 Le4 Le2 Ex1 Ex2 PIC-block Documentation, Seriecom Pulse sensors I, U, R, P, series and parallel KC1 LAB1 Pulse sensors, Menu program Start of programing task Kirchhoffs
More informationECE Spring 2015 Final Exam
ECE 20100 Spring 2015 Final Exam May 7, 2015 Section (circle below) Jung (1:30) 0001 Qi (12:30) 0002 Peleato (9:30) 0004 Allen (10:30) 0005 Zhu (4:30) 0006 Name PUID Instructions 1. DO NOT START UNTIL
More informationEXPERIMENT 07 TO STUDY DC RC CIRCUIT AND TRANSIENT PHENOMENA
EXPERIMENT 07 TO STUDY DC RC CIRCUIT AND TRANSIENT PHENOMENA DISCUSSION The capacitor is a element which stores electric energy by charging the charge on it. Bear in mind that the charge on a capacitor
More informationTopic 4. The CMOS Inverter
Topic 4 The CMOS Inverter Peter Cheung Department of Electrical & Electronic Engineering Imperial College London URL: www.ee.ic.ac.uk/pcheung/ E-mail: p.cheung@ic.ac.uk Topic 4-1 Noise in Digital Integrated
More informationEE115C Digital Electronic Circuits Homework #4
EE115 Digital Electronic ircuits Homework #4 Problem 1 Power Dissipation Solution Vdd =1.0V onsider the source follower circuit used to drive a load L =20fF shown above. M1 and M2 are both NMOS transistors
More informationSinusoidal 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 informationEE 242 EXPERIMENT 8: CHARACTERISTIC OF PARALLEL RLC CIRCUIT BY USING PULSE EXCITATION 1
EE 242 EXPERIMENT 8: CHARACTERISTIC OF PARALLEL RLC CIRCUIT BY USING PULSE EXCITATION 1 PURPOSE: To experimentally study the behavior of a parallel RLC circuit by using pulse excitation and to verify that
More information15EE103L ELECTRIC CIRCUITS LAB RECORD
15EE103L ELECTRIC CIRCUITS LAB RECORD REGISTER NO: NAME OF THE STUDENT: SEMESTER: DEPARTMENT: INDEX SHEET S.No. Date of Experiment Name of the Experiment Date of submission Marks Staff Sign 1 Verification
More informationEE 330 Homework 5 Fall 2018 (This assignment is due Wednesday Sept 19 at 12:00 noon)
EE 330 Homework 5 Fall 2018 (This assignment is due Wednesday Sept 19 at 12:00 noon) Assume the CMOS process is characterized by model parameters VTH=1V and µcox=100µa/v 2. If any other model parameters
More informationSource-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 informationOld Dominion University Physics 112N/227N/232N Lab Manual, 13 th Edition
RC Circuits Experiment PH06_Todd OBJECTIVE To investigate how the voltage across a capacitor varies as it charges. To find the capacitive time constant. EQUIPMENT NEEDED Computer: Personal Computer with
More informationEE 330 Homework 5 Spring 2017 (This assignment will not be collected or graded)
EE 330 Homework 5 Spring 2017 (This assignment will not be collected or graded) Assume the CMOS process is characterized by model parameters V TH =1V and µc OX =100µA/V 2. If any other model parameters
More informationPrerequisites: Successful completion of PHYS 2222 General Physics (Calculus) with a grade of C or better.
Prepared by: P. Blake Reviewed by: M. Mayfield Date prepared: March 13, 2017 C&GE approved: April 17, 2017 Board approved: May 10, 2017 Semester effective: Spring 2018 Engineering (ENGR) 2000 Circuit Analysis
More informationIE1206 Embedded Electronics Le2
Le1 Le3 Le4 Le6 Le8 IE1206 Embedded Electronics Le2 Ex1 Ex2 Ex4 Ex5 PIC-block Documentation, Seriecom Pulse sensors I, U, R, P, serial and parallel KC1 LAB1 Pulse sensors, Menu program Kirchhoffs laws
More informationHandout 10: Inductance. Self-Inductance and inductors
1 Handout 10: Inductance Self-Inductance and inductors In Fig. 1, electric current is present in an isolate circuit, setting up magnetic field that causes a magnetic flux through the circuit itself. This
More informationCS 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 informationOutline. Week 5: Circuits. Course Notes: 3.5. Goals: Use linear algebra to determine voltage drops and branch currents.
Outline Week 5: Circuits Course Notes: 3.5 Goals: Use linear algebra to determine voltage drops and branch currents. Components in Resistor Networks voltage source current source resistor Components in
More informationChapter 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 informationExercise 1: Capacitors
Capacitance AC 1 Fundamentals Exercise 1: Capacitors EXERCISE OBJECTIVE When you have completed this exercise, you will be able to describe the effect a capacitor has on dc and ac circuits by using measured
More informationnum1a ** num_1a.sp **SAM *circuit description * bias conditions vds vgs * Mosfet circuit M nch L=.5u w=8u R page 1
** num_1a.sp **SAM *circuit description vds 1 0 10 vgs 3 0 5 * Mosfet circuit M1 2 3 0 0 nch L=.5u w=8u R1 1 2 0 ~, Mosfet model.model nch nmos LEVEL = 1 TONS LST NODE POST.DC vds 0 10 100m vgs 0 1.PRNT
More informationElectricity 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 informationRLC 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 informationPHASOR DIAGRAMS HANDS-ON RELAY SCHOOL WSU PULLMAN, WA.
PHASOR DIAGRAMS HANDS-ON RELAY SCHOOL WSU PULLMAN, WA. RON ALEXANDER - BPA What are phasors??? In normal practice, the phasor represents the rms maximum value of the positive half cycle of the sinusoid
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 10 6/12/2007 Electricity and Magnetism Induced voltages and induction Self-Inductance RL Circuits Energy in magnetic fields AC circuits and EM waves Resistors, capacitors
More informationBesides resistors, capacitors are one of the most common electronic components that you will encounter. Sometimes capacitors are components that one
1 Besides resistors, capacitors are one of the most common electronic components that you will encounter. Sometimes capacitors are components that one would deliberately add to a circuit. Other times,
More informationStudy of MOSFET circuit
ECE 570 Computer Aided Engineering for Integrated Circuits IC 752 - E Simulation Assignment No. 3 - Due: Oct. 30 (Th.), 2003 Study of MOSFET circuit Simulate the basic circuit of CMOS shift register shown
More informationECE 342 Electronic Circuits. 3. MOS Transistors
ECE 342 Electronic Circuits 3. MOS Transistors Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jschutt@emlab.uiuc.edu 1 NMOS Transistor Typically L = 0.1 to 3 m, W = 0.2 to
More informationLab #10: Design of Finite State Machines
Lab #10: Design of Finite State Machines ECE/COE 0501 Date of Experiment: 3/1/2017 Report Written: 3/4/2017 Submission Date: 3/15/2017 Nicholas Haver nicholas.haver@pitt.edu 1 H a v e r PURPOSE The purpose
More informationAppendix A Installing QUCS
Appendix A Installing QUCS In this appendix, we will discuss how to install QUCS [1]. Note that QUCS has a lot of components, many of which we will not use. Nevertheless, we will install all components
More informationBasics of Network Theory (Part-I)
Basics of Network Theory (PartI). A square waveform as shown in figure is applied across mh ideal inductor. The current through the inductor is a. wave of peak amplitude. V 0 0.5 t (m sec) [Gate 987: Marks]
More informationLECTURE 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 informationInductors. 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 informationPHASOR DIAGRAMS HANDS-ON RELAY SCHOOL WSU PULLMAN, WA. RON ALEXANDER - BPA
PHASOR DIAGRAMS HANDS-ON RELAY SCHOOL WSU PULLMAN, WA. RON ALEXANDER - BPA I m VECTOR. Cause I m committing crimes with magnitude and direction at the same time!" What are phasors??? In normal practice,
More informationChapter 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 informationElectric Circuits I FINAL EXAMINATION
EECS:300, Electric Circuits I s6fs_elci7.fm - Electric Circuits I FINAL EXAMINATION Problems Points.. 3. 0 Total 34 Was the exam fair? yes no 5//6 EECS:300, Electric Circuits I s6fs_elci7.fm - Problem
More informationPage 1 of (2 pts) What is the purpose of the keeper transistor in a dynamic logic gate?
Page 1 of 6 EE 434 Exam 2 Fall 2004 Name Instructions: nswer the following questions and solve the following problems. In problems relating to timing or delay calculations, assume you are working in a
More informationMODULE-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 informationChapter 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 informationASSOCIATE DEGREE IN ENGINEERING RESIT EXAMINATIONS SEMESTER 1. "Electrical Eng Science"
ASSOCIATE DEGREE IN ENGINEERING RESIT EXAMINATIONS SEMESTER 1 COURSE NAME: "Electrical Eng Science" CODE: GROUP: "[ADET 2]" DATE: December 2010 TIME: DURATION: 9:00 am "Two hours" INSTRUCTIONS: 1. This
More informationElectric Circuits. Overview. Hani Mehrpouyan,
Electric Circuits Hani Mehrpouyan, Department of Electrical and Computer Engineering, Lecture 15 (First Order Circuits) Nov 16 th, 2015 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 2015 1 1 Overview
More informationPURPOSE: See suggested breadboard configuration on following page!
ECE4902 Lab 1 C2011 PURPOSE: Determining Capacitance with Risetime Measurement Reverse Biased Diode Junction Capacitance MOSFET Gate Capacitance Simulation: SPICE Parameter Extraction, Transient Analysis
More informationLecture 1. EE70 Fall 2007
Lecture 1 EE70 Fall 2007 Instructor Joel Kubby (that would be me) Office: BE-249 Office Hours: M,W,F 2-3 PM or by appointment Phone: (831) 459-1073 E-mail: jkubby@soe.ucsc.edu Teaching Assistant Drew Lohn
More informationEXP. NO. 3 Power on (resistive inductive & capacitive) load Series connection
OBJECT: To examine the power distribution on (R, L, C) series circuit. APPARATUS 1-signal function generator 2- Oscilloscope, A.V.O meter 3- Resisters & inductor &capacitor THEORY the following form for
More informationEE292: 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 informationElectric Circuit Theory
Electric Circuit Theory Nam Ki Min nkmin@korea.ac.kr 010-9419-2320 Chapter 8 Natural and Step Responses of RLC Circuits Nam Ki Min nkmin@korea.ac.kr 010-9419-2320 8.1 Introduction to the Natural Response
More informationE40M Capacitors. M. Horowitz, J. Plummer, R. Howe
E40M Capacitors 1 Reading Reader: Chapter 6 Capacitance A & L: 9.1.1, 9.2.1 2 Why Are Capacitors Useful/Important? How do we design circuits that respond to certain frequencies? What determines how fast
More informationR. 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 2.4 Cuk converter example L 1 C 1 L 2 Cuk converter, with ideal switch i 1 i v 1 2 1 2 C 2 v 2 Cuk
More informationControl 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 informationECE2262 Electric Circuit
ECE2262 Electric Circuit Chapter 7: FIRST AND SECOND-ORDER RL AND RC CIRCUITS Response to First-Order RL and RC Circuits Response to Second-Order RL and RC Circuits 1 2 7.1. Introduction 3 4 In dc steady
More informationExperiment 8: Capacitance and the Oscilloscope
Experiment 8: Capacitance and the Oscilloscope Nate Saffold nas2173@columbia.edu Office Hour: Mondays, 5:30PM-6:30PM @ Pupin 1216 INTRO TO EXPERIMENTAL PHYS-LAB 1493/1494/2699 Outline Capacitance: Capacitor
More informationAchieving Accurate Results With a Circuit Simulator. Ken Kundert and Ian Clifford Cadence Design Systems Analog Division San Jose, Calif 95134
Achieving Accurate Results With a Circuit Simulator Ken Kundert and Ian Clifford Cadence Design Systems Analog Division San Jose, Calif 95134 1 Outline Solving Nonlinear Systems of Equations Convergence
More informationInductance, RL and RLC Circuits
Inductance, RL and RLC Circuits Inductance Temporarily storage of energy by the magnetic field When the switch is closed, the current does not immediately reach its maximum value. Faraday s law of electromagnetic
More informationLinear Circuits. Concept Map 9/10/ Resistive Background Circuits. 5 Power. 3 4 Reactive Circuits. Frequency Analysis
Linear Circuits Dr. Bonnie Ferri Professor School of Electrical and Computer Engineering An introduction to linear electric components and a study of circuits containing such devices. School of Electrical
More informationElectromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance
Lesson 7 Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance Oscillations in an LC Circuit The RLC Circuit Alternating Current Electromagnetic
More informationMathematical Modelling Using SimScape (Electrical Systems)
Experiment Three Mathematical Modelling Using SimScape (Electrical Systems) Control Systems Laboratory Dr. Zaer Abo Hammour Dr. Zaer Abo Hammour Control Systems Laboratory 1. Model and simulate MultiDomain
More informationName: Lab Partner: Section:
Chapter 6 Capacitors and RC Circuits Name: Lab Partner: Section: 6.1 Purpose The purpose of this experiment is to investigate the physics of capacitors in circuits. The charging and discharging of a capacitor
More informationNote 11: Alternating Current (AC) Circuits
Note 11: Alternating Current (AC) Circuits V R No phase difference between the voltage difference and the current and max For alternating voltage Vmax sin t, the resistor current is ir sin t. the instantaneous
More informationES205 Analysis and Design of Engineering Systems: Lab 1: An Introductory Tutorial: Getting Started with SIMULINK
ES205 Analysis and Design of Engineering Systems: Lab 1: An Introductory Tutorial: Getting Started with SIMULINK What is SIMULINK? SIMULINK is a software package for modeling, simulating, and analyzing
More informationThe 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 informationExperiment Guide for RC Circuits
Guide-P1 Experiment Guide for RC Circuits I. Introduction 1. Capacitors A capacitor is a passive electronic component that stores energy in the form of an electrostatic field. The unit of capacitance is
More information