Linear Circuits. Concept Map 9/10/ Resistive Background Circuits. 5 Power. 3 4 Reactive Circuits. Frequency Analysis
|
|
- Felicia Wiggins
- 5 years ago
- Views:
Transcription
1 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 and Computer Engineering Concept Map 1 2 Resistive Background Circuits 5 Power 3 4 Reactive Circuits Frequency Analysis 2 1
2 Resistive vs Reactive Circuit Voltage Time 3 Concept Map Background Resistive Circuits Current, voltage, sources, resistance Reactive Circuits Capacitors RC Circuits Inductors RL Circuits Differential Reactive 2-order Diff Eqn Equations Circuits RLC Circuits Applications Methods to obtain circuit equations (KCL, KVL, mesh, node, Thévenin) Frequency Analysis Power 4 2
3 Capacitance Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Describe the behavior of capacitors by calculating: the charge stored on the capacitor plates the current flowing through the capacitor the voltage across the capacitor the capacitance of the capacitor School of Electrical and Computer Engineering Lesson Objectives Describe the construction of a capacitor Find charge stored on a capacitor Find the current through a capacitor Find the voltage across a capacitor Calculate the capacitance of a capacitor Explain how current flows through a capacitor 5 1
4 Capacitors 6 Capacitors and Charge 7 2
5 Current and Voltage 8 Calculating Capacitance 9 3
6 Permittivity of Common Materials Material Approximate ε r (or k) Air 1 Teflon 2.1 Paper 3.9 Glass 4.7 Rubber 7.0 Silicon 11.7 Water 78.5 (varies by T) 10 Current Through A Capacitor 11 4
7 Summary Identified how capacitors work Calculated charge stored on a capacitor Identified the relationship between current and voltage on a capacitor Calculated capacitance Explained how current flows through a capacitor 12 5
8 Capacitors Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Present how capacitors work in a system Identify behavior in DC circuits Graphically represent the relationships between current, voltage, power, and energy School of Electrical and Computer Engineering Lesson Objectives Analyzing capacitors in series/parallel Analyze DC circuits with capacitors Calculate energy in a capacitor Sketch current/voltage/power/energy curves 5 1
9 Capacitors in Parallel 6 Capacitors in Series 7 2
10 Behavior in DC Circuits 8 Stored Energy 9 3
11 Graphs 10 Summary Calculated capacitance for capacitors in parallel/series configurations Identified how capacitors in DC circuits behave like open circuits Derived an equation for the energy stored by a capacitor as an electric field Showed graphically the relationships between voltage/current/power/energy in capacitors 11 4
12 Inductance Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Introduce inductors and describe how they work Calculate current and voltage for inductors School of Electrical and Computer Engineering Lesson Objectives Describe the construction and behavior of an inductor Find current through an inductor Find voltage across an inductor Explain how a voltage is created across an inductor 5 1
13 Inductors 6 Current and Voltage 7 2
14 Ampère s Law 8 How Inductors Work 9 3
15 Voltages Across a Wire 10 Summary Presented the equations for current and voltage in inductors Introduced Ampère s Law and showed how inductors work in context of this law Showed how a voltage is created across an inductor as currents change in a system 11 4
16 Inductors Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Present how inductors work in a system Identify behavior in DC circuits Graphically represent the relationships between current, voltage, power, and energy School of Electrical and Computer Engineering Learning Objectives Analyze inductors in series/parallel Analyze DC circuits with inductors Calculate the energy in an inductor Sketch current/voltage/power/energy curves 5 1
17 Inductors in Series 6 Inductors in Parallel 7 2
18 Behavior in DC Circuits 8 Stored Energy 9 3
19 Graphs 10 Summary Calculated inductance for inductors in parallel/series configurations Identified how inductors in DC circuits behave like short circuits Derived an equation for the energy stored by an inductor as a magnetic field Showed graphically the relationships between voltage/current/power/energy in inductors 11 4
20 Dr. Bonnie H. Ferri Professor and Associate Chair School of Electrical and Computer Engineering First-Order Differential Equations Solve and graph solutions to first-order differential equations School of Electrical and Computer Engineering Lesson Objectives Examine first-order differential equations with a constant input Write the solution Sketch the solution 5 1
21 Ordinary Differential Equations ODE: Include functions of variables and their derivatives. dy dt + 2y= 4 dy dt d 2 y dy dv dt y= f (t) dt 2y = 4sin(ωt) dt + 2v= i(t) 6 Models of Physical Systems Inputs, f(t) System Model Outputs, y(t) dy dt + ay= f (t) Heat source Thermal System Temp Production Biological System Population Voltage or current source Linear Circuit Voltage or current 7 2
22 Solution to First-Order Differential Equation dy dt + ay= K, y(0) Has solution: y(t) = K a (1 e at )+ y(0)e at, t 0 If a 0, e at 0 y(t) K a = steady-state 8 Graph of Response y(t) = K a (1 e at )+ y(0)e at, t 0 K a y(0) K e at, t 0 a 9 3
23 Time Constant y(t) Time (sec) y(t) Time (sec) time,τ, for exponential transient to decay to e of its initial value (or 63% to its final value) 10 Sample Problems Pause 11 4
24 Summary Discussed how various physical phenomena are modeled by differential equations Showed the solution to a generic first-order differential equation with a constant input and initial condition Introduced the transient and steady-state responses Showed how to sketch the response and plot the time constant 12 5
25 RC Circuits Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Generate a differential equation that describes the behavior of a circuit with resistors and capacitors Solve the differential equation for step inputs (or switching constant inputs) Graph the behavior School of Electrical and Computer Engineering Lesson Objectives Generate a differential equation from a circuit Identify initial and final conditions Solve the differential equation Graph the result 5 1
26 Behavior of RC circuits 6 Example 1: Initial and Final Conditions 7 2
27 Example 1: Differential Equation 8 Example 1: Graph 9 3
28 Example 2: Initial and Final Conditions 10 Example 2: Differential Equation 11 4
29 Example 2: Graph 12 Summary Got some intuition about how RC circuits behave Identified initial and final conditions Found differential equations for the circuit and solved them Graphed the results 13 5
30 Dr. Bonnie Ferri Professor and Associate Chair School of Electrical and Computer Engineering Module 3 Lab Demo: RC Circuits Summary of Reactive Circuits Module School of Electrical and Computer Engineering RC Circuit + - v - + R + C v c - ~ C v c v s R
31 RC Circuit + - v - + R + C v c - ~ C v c v s R RC Circuit + - v - + R + C v c - ~ C v c v s R
32 RC Circuit + - v - + R + C v c - ~ C v c v s R RC Circuit + - v - + R + C v c - ~ C v c v s R
33 Lab Demo: RC Circuits 8 Summary An oscilloscope is used to measure and record voltage signals versus time. A function generator allows you to input voltage signals into a circuit Inputting a square wave into a circuit allows you to capture RC circuit transient behavior and to measure the time constant 9 4
34 RL Circuits Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Use differential equations to show the behavior of an RL circuit as the system changes. School of Electrical and Computer Engineering Lesson Objectives Generate a differential equation from a circuit Identify initial and final conditions Solve the differential equation Graph the result 5 1
35 Behavior of RL circuits 6 Example 1: Initial and Final Conditions 7 2
36 Example 1: Differential Equation 8 Example 1: Graph v L 5V 1.84V (63.2%) 0.68V (86.5%) t 9 3
37 Example 2: Initial and Final Conditions 10 Example 2: Differential Equation 11 4
38 Example 2: Graph i L 4mA 1.16mA (63.2%) 0.11mA (86.5%) 1 2 ma t 12 Summary Got some intuition about how RL circuits behave Identified initial and final conditions Found differential equations for the circuit and solved them Graphed the results 13 5
39 Second-Order Differential Equations Dr. Bonnie H. Ferri Professor and Associate Chair School of Electrical and Computer Engineering Recognize types of second-order responses School of Electrical and Computer Engineering Lesson Objectives Examine second-order differential equations with a constant input: Determine the steady-state solution Determine the type of transient response Recognize the characteristics of the plot of the solution 5 1
40 Ordinary Differential Equations ODE: Include functions of variables and their derivatives d 2 y dy dt y= f (t) dt 6 Models of Physical Systems Inputs, f(t) System Model Outputs, y(t) d 2 y dy dt y= f (t) dt Force Vibratory System Position Voltage or current source RLC Circuit Voltage or current 7 2
41 Solutions to Second-Order Differential Equation d 2 y dt 2+ a dy 1 dt + a 2y=K, y(0)and dy dt t=0 Solution: y(t) = steady-state + transient y( t) K a 2 Three possible forms depending on roots of (s 2 +a 1 s+a 2 )=0. 8 Transient Response (s 2 +a 1 s+a 2 )=0. ((real and distinct roots, r 1 and r 2 ) r t r t K e 1 K e ((real and equal roots, r and r) rt K1 e + K2 ((complex roots, a±jb) Ke at te rt sin( bt+ ϕ) 9 3
42 Sample Problems Overdamped 2 d y dy y= 1, 2 dt dt y(0) = 0, dy dt t= 0 = y(t) Time (sec) Sample Problems Underdamped 2 d y dy y= 1, 2 dt dt y(0) = 0, dy dt t= 0 = y(t) Time (sec) 11 4
43 Summary Examined generic 2 nd order differential equation Vibratory systems, RLC circuits Showed steady-state solution Showed generic transient solutions to underdamped and overdamped responses Showed characteristic plots of under damped and overdamped responses to a constant input applied at t=0 12 5
44 RLC Circuits Part 1 Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Use differential equations to show the behavior of an RLC circuit as the system changes. School of Electrical and Computer Engineering Lesson Objectives Generate a second-order differential equation from a RLC circuit Identify initial and final conditions Solve the differential equation Recognize if a system is underdamped/overdamped 5 1
45 Example 1: Initial and Final Conditions 6 Example 1: Differential Equation 7 2
46 Example 1: Transient Characteristic Equation: 8 Example 1: Steady State 9 3
47 Example 1: Solving for Constants 10 Example 1: Final Solution 11 4
48 Summary Looked at an overdamped case Identified initial and final conditions Found and solved representative differential equation Plotted the results 12 5
49 RLC Circuits Part 2 Nathan V. Parrish PhD Candidate & Graduate Research Assistant School of Electrical and Computer Engineering Use differential equations to show the behavior of an RLC circuit as the system changes. School of Electrical and Computer Engineering Lesson Objectives Generate a second-order differential equation from an underdamped RLC circuit Identify initial and final conditions Solve the differential equation Recognize if a system is underdamped/overdamped Identify the effect of damping on a second-order system 5 1
50 Example 2: Initial and Final Conditions 6 Example 2: Differential Equation 7 2
51 Example 2: Final Solution 8 Damping Ratio 9 3
52 Summary Got some intuition about how RLC circuits behave and contrasted overdamped and underdamped cases Identified initial and final conditions Found and solved representative differential equations Plotted the results Animated response as the resistance changes to show the effect of damping on the system 10 4
53 Lab Demo: RLC Circuit Dr. Bonnie Ferri Professor and Associate Chair School of Electrical and Computer Engineering Transient response of an RLC circuit School of Electrical and Computer Engineering RLC Circuit Measurements + +15v Buffer (Op Amp) - -15v + 3.3mH v s 20kΩ 0.01µf v c - 4 1
54 Lab Demo: RLC Circuits 5 Summary An underdamped RLC circuit has a small R value and results in large peaks An overdamped RLC circuit has a large R value 6 2
55 Lab Demo: Applications of Capacitance Dr. Bonnie H. Ferri Professor and Associate Chair School of Electrical and Computer Engineering Show common applications of capacitance School of Electrical and Computer Engineering Applications of Capacitance C = εwl d 1
56 Lab Demo: Applications of Capacitance 5 Summary Showed capacitive sensors such as touch pads and capacitive microphone, and antenna tuner 6 2
57 Credits Thanks to Allen Robinson, James Steinberg, Kevin Pham, and Al Ferri for help with demonstration ideas. Thanks to Marion Crowder for videotaping the demonstration. Capacitance drawings done by Nathan Parrish. 7 3
58 Dr. Bonnie H. Ferri Professor and Associate Chair School of Electrical and Computer Engineering Lab Demo: Applications of Inductance Show common applications of inductance School of Electrical and Computer Engineering Lab Demo: Applications of Inductance 4 1
59 Summary Discussed energy exchange in inductors mechanical to electrical and vice versa Moving conductor in magnetic field induces current Changing current in coiled wire causes a magnetic field Showed inductance applications Passive Sensing (guitar pick-up) Active Sensing (metal detector) Actuation (solenoid, speaker) 5 Credits Thanks to Allen Robinson, James Steinberg, Kevin Pham, and Al Ferri for help with demonstration ideas. Thanks to Ken Connor and Don Millard for the guitar string experiment. Thanks to Marion Crowder for videotaping the demonstration. Inductance drawings done by Nathan Parrish. 6 2
60 Dr. Bonnie Ferri Professor and Associate Chair School of Electrical and Computer Engineering Module 3 Reactive Circuit Wrap Up Summary of Reactive Circuits Module School of Electrical and Computer Engineering Concept Map Background Resistive Circuits Current, voltage, sources, resistance Reactive Circuits Capacitors RC Circuits Inductors RL Circuits Differential Reactive 2-order Diff Eqn Equations Circuits RLC Circuits Applications Methods to obtain circuit equations (KCL, KVL, mesh, node, Thévenin) Frequency Analysis Power 3 1
61 Important Concepts and Skills Understand the basic structure of a capacitor and its fundamental physical behavior Be able to use the i-v relationship to calculate current from voltage or vice versa Be able to reduce capacitor connections using using parallel and series connections Be able to calculate energy in a capacitor Be able to sketch current/voltage/power/energy curves 4 Important Concepts and Skills Be able to describe the construction and behavior of an inductor Be able to use the i-v relationship to find current through an inductor from the voltage across it, and vice versa Be able to explain how a voltage is created across an inductor Be able to analyze inductors in series/parallel Be able to calculate the energy in an inductor Be able to sketch current/voltage/power/energy curves 5 2
62 Important Concepts and Skills Given a constant input, be able to determine the steady-state value, time constant, and sketch the response Be able to write a differential equation governing the behavior of the circuit Be able to calculate the time constant, steadystate value, and sketch the response 6 Important Concepts and Skills Be able to identify the steady-state value Be able to predict the type of response from the roots (underdamped, critically damped, overdamped) Be able to write the differential equation that governs the behavior Be able to predict the type of response (underdamped, overdamped, critically damped) Be able to compute the damping factor and the resonant frequency Know that the smaller the damping factor, the larger the oscillations 7 3
63 Important Concepts and Skills Know the purposes of an oscilloscope and a function generator Know several applications of inductors and capacitors when they are used with non-electrical components 8 Concept Map 1 2 Resistive Background Circuits 5 Power 3 4 Reactive Circuits Frequency Analysis 9 4
64 Reminder Do all homework for this module Study for the quiz Continue to visit the forum 10 5
ENGR 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 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 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 informationECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance
ECE2262 Electric Circuits Chapter 6: Capacitance and Inductance Capacitors Inductors Capacitor and Inductor Combinations Op-Amp Integrator and Op-Amp Differentiator 1 CAPACITANCE AND INDUCTANCE Introduces
More informationTo 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 informationECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance
ECE2262 Electric Circuits Chapter 6: Capacitance and Inductance Capacitors Inductors Capacitor and Inductor Combinations 1 CAPACITANCE AND INDUCTANCE Introduces two passive, energy storing devices: Capacitors
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 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 informationResponse of Second-Order Systems
Unit 3 Response of SecondOrder Systems In this unit, we consider the natural and step responses of simple series and parallel circuits containing inductors, capacitors and resistors. The equations which
More informationIntroduction to AC Circuits (Capacitors and Inductors)
Introduction to AC Circuits (Capacitors and Inductors) Amin Electronics and Electrical Communications Engineering Department (EECE) Cairo University elc.n102.eng@gmail.com http://scholar.cu.edu.eg/refky/
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 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 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 information8 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 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 informationThe RLC circuits have a wide range of applications, including oscillators and frequency filters
9. The RL ircuit The RL circuits have a wide range of applications, including oscillators and frequency filters This chapter considers the responses of RL circuits The result is a second-order differential
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 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 informationElectric Circuits Fall 2015 Solution #5
RULES: Please try to work on your own. Discussion is permissible, but identical submissions are unacceptable! Please show all intermeate steps: a correct solution without an explanation will get zero cret.
More informationProblem Set 5 Solutions
University of California, Berkeley Spring 01 EE /0 Prof. A. Niknejad Problem Set 5 Solutions Please note that these are merely suggested solutions. Many of these problems can be approached in different
More informationECE 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 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 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 informationChapter 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 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 informationELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT
Chapter 31: ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT 1 A charged capacitor and an inductor are connected in series At time t = 0 the current is zero, but the capacitor is charged If T is the
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 informationEIT Review. Electrical Circuits DC Circuits. Lecturer: Russ Tatro. Presented by Tau Beta Pi The Engineering Honor Society 10/3/2006 1
EIT Review Electrical Circuits DC Circuits Lecturer: Russ Tatro Presented by Tau Beta Pi The Engineering Honor Society 10/3/2006 1 Session Outline Basic Concepts Basic Laws Methods of Analysis Circuit
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 informationAP Physics C. Magnetism - Term 4
AP Physics C Magnetism - Term 4 Interest Packet Term Introduction: AP Physics has been specifically designed to build on physics knowledge previously acquired for a more in depth understanding of the world
More informationFirst Order RC and RL Transient Circuits
First Order R and RL Transient ircuits Objectives To introduce the transients phenomena. To analyze step and natural responses of first order R circuits. To analyze step and natural responses of first
More informationFigure Circuit for Question 1. Figure Circuit for Question 2
Exercises 10.7 Exercises Multiple Choice 1. For the circuit of Figure 10.44 the time constant is A. 0.5 ms 71.43 µs 2, 000 s D. 0.2 ms 4 Ω 2 Ω 12 Ω 1 mh 12u 0 () t V Figure 10.44. Circuit for Question
More informationa + b Time Domain i(τ)dτ.
R, C, and L Elements and their v and i relationships We deal with three essential elements in circuit analysis: Resistance R Capacitance C Inductance L Their v and i relationships are summarized below.
More informationApplications of Second-Order Differential Equations
Applications of Second-Order Differential Equations ymy/013 Building Intuition Even though there are an infinite number of differential equations, they all share common characteristics that allow intuition
More informationChapter 30 INDUCTANCE. Copyright 2012 Pearson Education Inc.
Chapter 30 INDUCTANCE Goals for Chapter 30 To learn how current in one coil can induce an emf in another unconnected coil To relate the induced emf to the rate of change of the current To calculate the
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 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 informationELECTRONICS E # 1 FUNDAMENTALS 2/2/2011
FE Review 1 ELECTRONICS E # 1 FUNDAMENTALS Electric Charge 2 In an electric circuit it there is a conservation of charge. The net electric charge is constant. There are positive and negative charges. Like
More informationMidterm Exam 2. Prof. Miloš Popović
Midterm Exam 2 Prof. Miloš Popović 100 min timed, closed book test. Write your name at top of every page (or initials on later pages) Aids: single page (single side) of notes, handheld calculator Work
More informationChapter 32. Inductance
Chapter 32 Inductance Inductance Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying current. Basis of the electrical circuit
More informationELECTROMAGNETIC INDUCTION AND FARADAY S LAW
ELECTROMAGNETIC INDUCTION AND FARADAY S LAW Magnetic Flux The emf is actually induced by a change in the quantity called the magnetic flux rather than simply py by a change in the magnetic field Magnetic
More informationfiziks 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 informationChapter 30 Inductance
Chapter 30 Inductance In this chapter we investigate the properties of an inductor in a circuit. There are two kinds of inductance mutual inductance and self-inductance. An inductor is formed by taken
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 informationRLC Circuit (3) We can then write the differential equation for charge on the capacitor. The solution of this differential equation is
RLC Circuit (3) We can then write the differential equation for charge on the capacitor The solution of this differential equation is (damped harmonic oscillation!), where 25 RLC Circuit (4) If we charge
More informationSlide 1 / 26. Inductance by Bryan Pflueger
Slide 1 / 26 Inductance 2011 by Bryan Pflueger Slide 2 / 26 Mutual Inductance If two coils of wire are placed near each other and have a current passing through them, they will each induce an emf on one
More informationPhysics 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 information8. 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 informationChapter 32. Inductance
Chapter 32 Inductance Joseph Henry 1797 1878 American physicist First director of the Smithsonian Improved design of electromagnet Constructed one of the first motors Discovered self-inductance Unit of
More informationUnit-2.0 Circuit Element Theory
Unit2.0 Circuit Element Theory Dr. Anurag Srivastava Associate Professor ABVIIITM, Gwalior Circuit Theory Overview Of Circuit Theory; Lumped Circuit Elements; Topology Of Circuits; Resistors; KCL and KVL;
More informationGraduate Diploma in Engineering Circuits and waves
9210-112 Graduate Diploma in Engineering Circuits and waves You should have the following for this examination one answer book non-programmable calculator pen, pencil, ruler No additional data is attached
More informationSinusoidal Steady-State Analysis
Chapter 4 Sinusoidal Steady-State Analysis In this unit, we consider circuits in which the sources are sinusoidal in nature. The review section of this unit covers most of section 9.1 9.9 of the text.
More informationHOMEWORK 4: MATH 265: SOLUTIONS. y p = cos(ω 0t) 9 ω 2 0
HOMEWORK 4: MATH 265: SOLUTIONS. Find the solution to the initial value problems y + 9y = cos(ωt) with y(0) = 0, y (0) = 0 (account for all ω > 0). Draw a plot of the solution when ω = and when ω = 3.
More informationChapter 10 Sinusoidal Steady State Analysis Chapter Objectives:
Chapter 10 Sinusoidal Steady State Analysis Chapter Objectives: Apply previously learn circuit techniques to sinusoidal steady-state analysis. Learn how to apply nodal and mesh analysis in the frequency
More informationEECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits
EECE25 Circuit Analysis I Set 4: Capacitors, Inductors, and First-Order Linear Circuits Shahriar Mirabbasi Department of Electrical and Computer Engineering University of British Columbia shahriar@ece.ubc.ca
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 informationCHAPTER 6. Inductance, Capacitance, and Mutual Inductance
CHAPTER 6 Inductance, Capacitance, and Mutual Inductance 6.1 The Inductor Inductance is symbolized by the letter L, is measured in henrys (H), and is represented graphically as a coiled wire. The inductor
More informationSelf-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying current.
Inductance Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying current. Basis of the electrical circuit element called an
More informationWhat happens when things change. Transient current and voltage relationships in a simple resistive circuit.
Module 4 AC Theory What happens when things change. What you'll learn in Module 4. 4.1 Resistors in DC Circuits Transient events in DC circuits. The difference between Ideal and Practical circuits Transient
More information4/27 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 informationActive Figure 32.3 (SLIDESHOW MODE ONLY)
RL Circuit, Analysis An RL circuit contains an inductor and a resistor When the switch is closed (at time t = 0), the current begins to increase At the same time, a back emf is induced in the inductor
More informationAssessment Schedule 2015 Physics: Demonstrate understanding of electrical systems (91526)
NCEA Level 3 Physics (91526) 2015 page 1 of 6 Assessment Schedule 2015 Physics: Demonstrate understanding of electrical systems (91526) Evidence Q Evidence Achievement Achievement with Merit Achievement
More informationElectrical 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 informationE40M Review - Part 1
E40M Review Part 1 Topics in Part 1 (Today): KCL, KVL, Power Devices: V and I sources, R Nodal Analysis. Superposition Devices: Diodes, C, L Time Domain Diode, C, L Circuits Topics in Part 2 (Wed): MOSFETs,
More informationENGR 2405 Chapter 6. Capacitors And Inductors
ENGR 2405 Chapter 6 Capacitors And Inductors Overview This chapter will introduce two new linear circuit elements: The capacitor The inductor Unlike resistors, these elements do not dissipate energy They
More informationIntroduction to Electric Circuit Analysis
EE110300 Practice of Electrical and Computer Engineering Lecture 2 and Lecture 4.1 Introduction to Electric Circuit Analysis Prof. Klaus Yung-Jane Hsu 2003/2/20 What Is An Electric Circuit? Electrical
More informationAP Physics C. Electricity - Term 3
AP Physics C Electricity - Term 3 Interest Packet Term Introduction: AP Physics has been specifically designed to build on physics knowledge previously acquired for a more in depth understanding of the
More informationAlternating Currents. The power is transmitted from a power house on high voltage ac because (a) Electric current travels faster at higher volts (b) It is more economical due to less power wastage (c)
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 informationLecture 39. PHYC 161 Fall 2016
Lecture 39 PHYC 161 Fall 016 Announcements DO THE ONLINE COURSE EVALUATIONS - response so far is < 8 % Magnetic field energy A resistor is a device in which energy is irrecoverably dissipated. By contrast,
More informationPHYS 241 EXAM #2 November 9, 2006
1. ( 5 points) A resistance R and a 3.9 H inductance are in series across a 60 Hz AC voltage. The voltage across the resistor is 23 V and the voltage across the inductor is 35 V. Assume that all voltages
More informationEE1305/EE1105 Intro to Electrical and Computer Engineering Lecture Week 6
EE1305/EE1105 Intro to Electrical and Computer Engineering Lecture Week 6 Homework Passive Components Capacitors RC Filters fc Calculations Bode Plots Module III Homework- due 2/20 (Najera), due 2/23 (Quinones)
More informationa. Clockwise. b. Counterclockwise. c. Out of the board. d. Into the board. e. There will be no current induced in the wire
Physics 1B Winter 2012: Final Exam For Practice Version A 1 Closed book. No work needs to be shown for multiple-choice questions. The first 10 questions are the makeup Quiz. The remaining questions are
More informationLectures 16 & 17 Sinusoidal Signals, Complex Numbers, Phasors, Impedance & AC Circuits. Nov. 7 & 9, 2011
Lectures 16 & 17 Sinusoidal Signals, Complex Numbers, Phasors, Impedance & AC Circuits Nov. 7 & 9, 2011 Material from Textbook by Alexander & Sadiku and Electrical Engineering: Principles & Applications,
More informationECE 212H1F Circuit Analysis October 30, :10-19: Reza Iravani 02 Reza Iravani 03 Piero Triverio. (Non-programmable Calculators Allowed)
Please Print Clearly Last Name: First Name: Student Number: Your Tutorial Section (CIRCLE ONE): 01 Thu. 9-11 RS211 02 Thu. 9-11 GB119 03 Tue. 10-12 SF2202 04 Tue. 10-12 SF3201 05 Tue. 13-15 GB304 06 Tue.
More informationA capacitor is a device that stores electric charge (memory devices). A capacitor is a device that stores energy E = Q2 2C = CV 2
Capacitance: Lecture 2: Resistors and Capacitors Capacitance (C) is defined as the ratio of charge (Q) to voltage (V) on an object: C = Q/V = Coulombs/Volt = Farad Capacitance of an object depends on geometry
More informationPhysics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS:
Physics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Closed book. No work needs to be shown for multiple-choice questions. 1. A charge of +4.0 C is placed at the origin. A charge of 3.0 C
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 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 informationElectrical Engineering Fundamentals for Non-Electrical Engineers
Electrical Engineering Fundamentals for Non-Electrical Engineers by Brad Meyer, PE Contents Introduction... 3 Definitions... 3 Power Sources... 4 Series vs. Parallel... 9 Current Behavior at a Node...
More informationOAKTON COMMUNITY COLLEGE COURSE SYLLABUS. I. Course Course Course Prefix Number Name Credit: Lecture Lab. PHY 132 College Physics II 4 3 2
OAKTON COMMUNITY COLLEGE COURSE SYLLABUS I. Course Course Course Prefix Number Name Credit: Lecture Lab PHY 132 College Physics II 4 3 2 II. Prerequisites: PHY 131 III. Course (catalog) Description: Course
More informationPart 4: Electromagnetism. 4.1: Induction. A. Faraday's Law. The magnetic flux through a loop of wire is
1 Part 4: Electromagnetism 4.1: Induction A. Faraday's Law The magnetic flux through a loop of wire is Φ = BA cos θ B A B = magnetic field penetrating loop [T] A = area of loop [m 2 ] = angle between field
More informationCapacitors. Chapter How capacitors work Inside a capacitor
Chapter 6 Capacitors In every device we have studied so far sources, resistors, diodes and transistors the relationship between voltage and current depends only on the present, independent of the past.
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 informationCircuit Analysis. by John M. Santiago, Jr., PhD FOR. Professor of Electrical and Systems Engineering, Colonel (Ret) USAF. A Wiley Brand FOR-
Circuit Analysis FOR A Wiley Brand by John M. Santiago, Jr., PhD Professor of Electrical and Systems Engineering, Colonel (Ret) USAF FOR- A Wiley Brand Table of Contents. ' : '" '! " ' ' '... ',. 1 Introduction
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 informationModule 25: Outline Resonance & Resonance Driven & LRC Circuits Circuits 2
Module 25: Driven RLC Circuits 1 Module 25: Outline Resonance & Driven LRC Circuits 2 Driven Oscillations: Resonance 3 Mass on a Spring: Simple Harmonic Motion A Second Look 4 Mass on a Spring (1) (2)
More informationPhysics 420 Fall 2004 Quiz 1 Wednesday This quiz is worth 6 points. Be sure to show your work and label your final answers.
Quiz 1 Wednesday This quiz is worth 6 points. Be sure to show your work and label your final answers. 1. A charge q 1 = +5.0 nc is located on the y-axis, 15 µm above the origin, while another charge q
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 informationCoupled Electrical Oscillators Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 5/24/2018
Coupled Electrical Oscillators Physics 3600 - Advanced Physics Lab - Summer 08 Don Heiman, Northeastern University, 5/4/08 I. INTRODUCTION The objectives of this experiment are: () explore the properties
More informationBasic 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 drake@anl.gov
More informationUNIVERSITY OF TECHNOLOGY, JAMAICA Faculty of Engineering and Computing School of Engineering
UNIVERSITY OF TECHNOLOGY, JAMAICA Faculty of Engineering and Computing School of Engineering SYLLABUS OUTLINE FACULTY: SCHOOL/DEPT: COURSE OF STUDY: Engineering and Computing Engineering Diploma in Electrical
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 informationReal Analog Chapter 7: First Order Circuits. 7 Introduction and Chapter Objectives
1300 Henley Court Pullman, WA 99163 509.334.6306 www.store. digilent.com 7 Introduction and Chapter Objectives First order systems are, by definition, systems whose inputoutput relationship is a first
More informationTransient Analysis of First-Order Circuits: Approaches and Recommendations
Transient Analysis of First-Order Circuits: Approaches and Recommendations Khalid Al-Olimat Heath LeBlanc ECCS Department ECCS Department Ohio Northern University Ohio Northern University Ada, OH 45810
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 informationEECE 2510 Circuits and Signals, Biomedical Applications Final Exam Section 3. Name:
EECE 2510 Circuits and Signals, Biomedical Applications Final Exam Section 3 Instructions: Closed book, closed notes; Computers and cell phones are not allowed Scientific calculators are allowed Complete
More informationBasics of Electric Circuits
António Dente Célia de Jesus February 2014 1 Alternating Current Circuits 1.1 Using Phasors There are practical and economic reasons justifying that electrical generators produce emf with alternating and
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 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 information