LECTURE 6 MUTUAL INDUCTANCE

Size: px
Start display at page:

Download "LECTURE 6 MUTUAL INDUCTANCE"

Transcription

1 ECE 330 POWER CIRCUITS AND ELECTROMECHANICS LECTURE 6 MUTUAL INDUCTANCE Acknowledgment-These handouts and lecture notes given in class are based on material from Prof. Peter Sauer s ECE 330 lecture notes. Some slides are taken from Ali Bazi s presentations Disclaimer- These handouts only provide highlights and should not be used to replace the course textbook. 1/31/018

2 SOURCE ON PRIMARY SIDE When two coils are magnetically coupled there is mutual inductance. Assuming an ac voltage source on one side and an open circuit on the other (i = 0): v N 1 d d 1 N i 1 (t) v 1 (t) 1 l1 N 1 N v (t) 1/31/018

3 SOURCE ON PRIMARY SIDE Let the flux and current be linearly related (no saturation): M i, L i Then, di1 di1 v M 1, and v 1 L1. M 1 is the mutual inductance. L 1 is the self-inductance of coil 1. 1/31/018 3

4 SOURCE ON SECONDARY SIDE Assuming an ac voltage source on one side and an open circuit on the other (i 1 = 0):. l 1 d d N 11, v 1 N 1 Let the flux and current be linearly related (no saturation): M 1 is the mutual inductance and L is the self-inductance of coil. M i, L i. 1 1 di di v L, and v1 M1. N 1 N 1/31/018 4 v 1 (t) 1 l i (t) v (t)

5 SOURCES ON BOTH SIDES Using superposition: Let M 1 = M 1 = M, then: 1 l l N N L i M i N N M i L i L i M i M i L i 1 v 1 (t) i 1 (t) l1 1 N 1 N 1 d1 di1 di v1 L1 M d di di v L M l 1 i (t) v (t) 1/31/018 5

6 COUPLING COEFFICIENT Define the coupling coefficient as: If k = 0, no coupling and M = 0. k If k =1, ideal coupling with zero leakage: M LL 1 k M LL 1 11 l1 1 l 1 Therefore, M is always 0. and 0k 1 0 M L1L. 1/31/018 6

7 What if i is reversed? What if v is reversed? COUPLING COEFFICIENT d1 di1 di ' v1 L1 M d di ' di v L M 1 d1 di1 di ' v1 L1 M d di ' di v ' L M 1 1/31/018 7 i v v i

8 EQUIVALENT CIRCUIT Ni 11 1 l1 1 l l Ni 1/31/018 8

9 DOT MARKINGS Dots relate the flux direction between coils. If two fluxes are in the same direction, they add, otherwise, they subtract. Depending which ends you connect the load to the secondary coil you either get an Output voltage in sync. With the input voltage or in reverse phase. v 1 (t) N 1 N i (t) v (t) 1/31/018 9 i 1 (t) l1 1 l

10 DOT MARKINGS The polarity markings are assigned such that a positively increasing current in the dotted terminal in one winding induces a positive voltage at the dotted terminal of the other winding i 1 (t) i (t) v 1 (t) l1 1 l N 1 N v (t) 1/31/018 10

11 DOT MARKINGS Assume the following configuration. 1) Select one coil and one terminal and place a dot on that terminal. ) Assume a current is flowing and determine the flux direction. 1 i 1 (t) 1 1' 3) Place a test current in the second coil and determine its flux direction. 1/31/ '

12 DOT MARKINGS i 1 (t) 1 1' 1 i (t) ' 1 4) If 1 and add, then place dot on (where test current enters). 5) If they subtract, then place dot on (where test current leaves). 1 1' ' 1/31/018 1

13 DOT MARKINGS Practical determination of dot locations: 1) Build the following circuit. -Turn the switch on => pulse is generated where di/ is not zero on the secondary side. -If the pulse causes the meter (V) to read positive, then the dot on the secondary is on the top terminal. -If (V) reads a negative pulse, then the dot is on the lower side. 1/31/ R + V dc V -

14 EXAMPLES The dots in the circuit below are as shown. i 1 (t) 1 1' i (t) ' 1/31/018 14

15 WRITING EQUATIONS WITH MUTUALLY COUPLED COILS Suppose we have two mutually coupled coils and the dot markings are as shown The self induced voltage due to the self inductance is in the direction of the current and is a voltage drop. The polarity of the mutually induced voltage depends on the dot marking 1/31/018 15

16 WRITING EQUATIONS WITH MUTUALLY COUPLED COILS di v 1 = i1r1 L1 M di 1 Source: jacobs-university.de di v = i R L M di 1 1/31/018 16

17 WRITING EQUATIONS WITH MUTUALLY COUPLED COILS di v 1 = i1r1 L1 M di 1 Source: jacobs-university.de di v = ir L M di 1 1/31/018 17

18 WRITING EQUATIONS WITH MUTUALLY COUPLED COILS Source: jacobs-university.de 1/31/018 18

19 WRITING EQUATIONS WITH MUTUALLY COUPLED COILS If the reference current in a coil leaves the dotted (undotted) terminal, then the voltage induced at the dotted (undotted) terminal of the other coil has a negative sign. 1/31/018 19

Fundamentals of Electric Circuits, Second Edition - Alexander/Sadiku

Fundamentals of Electric Circuits, Second Edition - Alexander/Sadiku Chapter 3, Problem 9(8). Find V x in the network shown in Fig. 3.78. Figure 3.78 Chapter 3, Solution 9(8). Consider the circuit below. 2 Ω 2 Ω -j 8 30 o I j 4 j 4 I 2 -j2v For loop, 8 30 = (2 j4)i ji 2

More information

LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1)

LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1) ECE 330 POWER CIRCUITS AND ELECTROMECHANICS LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1) Aknowledgment-These handouts and leture notes given in lass are based on material from Prof. Peter Sauer s ECE

More information

Mutual Inductance: This is the magnetic flux coupling of 2 coils where the current in one coil causes a voltage to be induced in the other coil.

Mutual Inductance: This is the magnetic flux coupling of 2 coils where the current in one coil causes a voltage to be induced in the other coil. agnetically Coupled Circuits utual Inductance: This is the magnetic flux coupling of coils where the current in one coil causes a voltage to be induced in the other coil. st I d like to emphasize that

More information

Chapter 15 Magnetic Circuits and Transformers

Chapter 15 Magnetic Circuits and Transformers Chapter 15 Magnetic Circuits and Transformers Chapter 15 Magnetic Circuits and Transformers 1. Understand magnetic fields and their interactio with moving charges. 2. Use the right-hand rule to determine

More information

Single-phase Transistor Lab Report. Module: EEE 108

Single-phase Transistor Lab Report. Module: EEE 108 Single-phase Transistor Lab Report Author: 1302509 Zhao Ruimin Module: EEE 108 Lecturer: Date: Dr.Gray May/27/2015 Abstract This lab intended to train the experimental skills of the experimenters and help

More information

PHASOR DIAGRAM OF TRANSFORMER. Prepared By ELECTRICALBABA.COM

PHASOR DIAGRAM OF TRANSFORMER. Prepared By ELECTRICALBABA.COM PHASOR DIAGRAM OF TRANSFORMER Prepared By ELECTRICALBABA.COM IMPORTANT POINTS FOR PHASOR OF TRANSFORMER Transformer when excited at no load, only takes excitation current which leads the working Flux by

More information

Electrical Machines-I Prof. D. Kastha Department of Electrical Engineering Indian Institute of Technology, Kharagpur

Electrical Machines-I Prof. D. Kastha Department of Electrical Engineering Indian Institute of Technology, Kharagpur Electrical Machines-I Prof. D. Kastha Department of Electrical Engineering Indian Institute of Technology, Kharagpur Lecture - 20 Potential and Current Transformers (Refer Slide Time: 00:37) So far we

More information

Tutorial Sheet Fig. Q1

Tutorial Sheet Fig. Q1 Tutorial Sheet - 04 1. The magnetic circuit shown in Fig. Q1 has dimensions A c = A g = 9 cm 2, g = 0.050 cm, l c = 30 cm, and N = 500 turns. Assume the value of the relative permeability,µ r = 70,000

More information

LECTURE 8 INTRODUCTION TO MAGNETICS (2)

LECTURE 8 INTRODUCTION TO MAGNETICS (2) ECE 330 POWER CIRCUITS AND ELECTROMECHANICS LECTURE 8 INTRODUCTION TO MAGNETICS (2) Aknowledment-These handouts and leture notes iven in lass are based on material from Prof. Peter Sauer s ECE 330 leture

More information

Texas 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 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 information

Basic Electrical Technology Prof. Dr. L. Umanand Department of Electrical Engineering Indian Institute of Science, Bangalore

Basic Electrical Technology Prof. Dr. L. Umanand Department of Electrical Engineering Indian Institute of Science, Bangalore Basic Electrical Technology Prof. Dr. L. Umanand Department of Electrical Engineering Indian Institute of Science, Bangalore Lecture - 18 Transformer Basics Part - II Hello everybody, in the last session

More information

1 (a) Define magnetic flux [1]

1 (a) Define magnetic flux [1] 1 (a) Define magnetic flux..... [1] (b) Fig. 4.1 shows a generator coil of 5 turns and cross-sectional area 2.5 1 3 m 2 placed in a magnetic field of magnetic flux density.35 T. The plane of the coil is

More information

CHAPTER 6. Inductance, Capacitance, and Mutual Inductance

CHAPTER 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 information

Notes on Mutual Inductance and Transformers J. McCalley

Notes on Mutual Inductance and Transformers J. McCalley ωωωωωωωω ωωωωωωωω otes on Mutual nductance and Transformers J. McCalley.0 Use of Transformers Transformers are one of the most common electrical devices. Perhaps the most familiar application today is

More information

3rd Semester EE and EEE Network Devices laboratory Manual Under BPUT Odisha Prepared BY: Prof.(Dr.) J.K.Moharana Principal and Professor Department

3rd Semester EE and EEE Network Devices laboratory Manual Under BPUT Odisha Prepared BY: Prof.(Dr.) J.K.Moharana Principal and Professor Department 3rd Semester EE and EEE Network Devices laboratory Manual Under BPUT Odisha Prepared BY: Prof.(Dr.) J.K.Moharana Principal and Professor Department of EE HIT Khurda, Bhubaneswar, Odisha AIM OF THE EXPERIMENT:-Verification

More information

Electricity & Magnetism

Electricity & Magnetism Electricity & Magnetism D.C. Circuits Marline Kurishingal Note : This chapter includes only D.C. In AS syllabus A.C is not included. Recap... Electrical Circuit Symbols : Draw and interpret circuit diagrams

More information

Practical Transformer

Practical Transformer Practical Transformer φ c i P tructure and dot convention ymbol and polarity Dot convention: the primary and secondary currents flowing into the winding terminals marked produce a mutually additive magnetic

More information

INVESTIGATION OF THREE PHASE SYSTEM

INVESTIGATION OF THREE PHASE SYSTEM EXPEIMENT 4 INVESTIGATION OF THEE PHASE SYSTEM. Purpose of the exercise. a) To be familiar with certain methods of the measurements of the average power in the three phases three and four-wire balanced

More information

ROEVER COLLEGE OF ENGINEERING & TECHNOLOGY ELAMBALUR, PERAMBALUR DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING ELECTRICAL MACHINES I

ROEVER COLLEGE OF ENGINEERING & TECHNOLOGY ELAMBALUR, PERAMBALUR DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING ELECTRICAL MACHINES I ROEVER COLLEGE OF ENGINEERING & TECHNOLOGY ELAMBALUR, PERAMBALUR-621220 DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING ELECTRICAL MACHINES I Unit I Introduction 1. What are the three basic types

More information

LECTURES 4 AND 5 THREE-PHASE CONNECTIONS (1)

LECTURES 4 AND 5 THREE-PHASE CONNECTIONS (1) ECE 330 POWER CIRCUITS AND ELECTROMECHANICS LECTURES 4 AND 5 THREEPHASE CONNECTIONS (1) AcknwledgmentThese handuts and lecture ntes given in class are based n material frm Prf. Peter Sauer s ECE 330 lecture

More information

Magnetic Fields from Power Cables 1

Magnetic Fields from Power Cables 1 Power Electronics Notes 30H Magnetic Fields from Power Cables (Case Studies) Marc T. Thompson, Ph.D. Thompson Consulting, Inc. 9 Jacob Gates Road Harvard, MA 01451 Phone: (978) 456-7722 Fax: (240) 414-2655

More information

Lecture 12. Time Varying Electromagnetic Fields

Lecture 12. Time Varying Electromagnetic Fields Lecture. Time Varying Electromagnetic Fields For static electric and magnetic fields: D = ρ () E = 0...( ) D= εe B = 0...( 3) H = J H = B µ...( 4 ) For a conducting medium J =σ E From Faraday s observations,

More information

Induction and Inductance

Induction and Inductance Induction and Inductance Key Contents Faraday s law: induced emf Induction and energy transfer Inductors and inductance RL circuits Magnetic energy density The First Experiment 1. A current appears only

More information

Lecture 17 Push-Pull and Bridge DC-DC converters Push-Pull Converter (Buck Derived) Centre-tapped primary and secondary windings

Lecture 17 Push-Pull and Bridge DC-DC converters Push-Pull Converter (Buck Derived) Centre-tapped primary and secondary windings ecture 17 Push-Pull and Bridge DC-DC converters Push-Pull Converter (Buck Derived) Centre-tapped primary and secondary windings 1 2 D 1 i v 1 v 1s + v C o R v 2 v 2s d 1 2 T 1 T 2 D 2 Figure 17.1 v c (

More information

Electromagnetic Induction

Electromagnetic Induction lectromagnetic Induction Induced MF We already know that moving charge (=current) causes magnetic field It also works the other way around: changing magnetic field (e.g. moving permanent magnet) causes

More information

Self-Inductance. Φ i. Self-induction. = (if flux Φ 1 through 1 loop. Tm Vs A A. Lecture 11-1

Self-Inductance. Φ i. Self-induction. = (if flux Φ 1 through 1 loop. Tm Vs A A. Lecture 11-1 Lecture - Self-Inductance As current i through coil increases, magnetic flux through itself increases. This in turn induces back emf in the coil itself When current i is decreasing, emf is induced again

More information

Tutorial Sheet IV. Fig. IV_2.

Tutorial Sheet IV. Fig. IV_2. Tutorial Sheet IV 1. Two identical inductors 1 H each are connected in series as shown. Deduce the combined inductance. If a third and then a fourth are similarly connected in series with this combined

More information

9-3 Inductance. * We likewise can have self inductance, were a timevarying current in a circuit induces an emf voltage within that same circuit!

9-3 Inductance. * We likewise can have self inductance, were a timevarying current in a circuit induces an emf voltage within that same circuit! /3/004 section 9_3 Inductance / 9-3 Inductance Reading Assignment: pp. 90-86 * A transformer is an example of mutual inductance, where a time-varying current in one circuit (i.e., the primary) induces

More information

ASSOCIATE DEGREE IN ENGINEERING RESIT EXAMINATIONS SEMESTER 1. "Electrical Eng Science"

ASSOCIATE 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 information

LECTURE 31: Basics of Magnetically Coupled Circuits Part 1

LECTURE 31: Basics of Magnetically Coupled Circuits Part 1 LECTURE 31: Basics of Magnetically Coupled Circuits Part 1 1 Question 1: What is a magnetically coupled circuit? Answer: voltages and currents of two nearby inductors affect each other when excited by

More information

Induction_P1. 1. [1 mark]

Induction_P1. 1. [1 mark] Induction_P1 1. [1 mark] Two identical circular coils are placed one below the other so that their planes are both horizontal. The top coil is connected to a cell and a switch. The switch is closed and

More information

Recap (1) Maxwell s Equations describe the electric field E and magnetic field B generated by stationary charge density ρ and current density J:

Recap (1) Maxwell s Equations describe the electric field E and magnetic field B generated by stationary charge density ρ and current density J: Class 13 : Induction Phenomenon of induction and Faraday s Law How does a generator and transformer work? Self- and mutual inductance Energy stored in B-field Recap (1) Maxwell s Equations describe the

More information

Lesson 17: Synchronous Machines

Lesson 17: Synchronous Machines Lesson 17: Synchronous Machines ET 332b Ac Motors, Generators and Power Systems Lesson 17_et332b.pptx 1 Learning Objectives After this presentation you will be able to: Explain how synchronous machines

More information

Texas 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 Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Lecture 6: Modeling of Electromechanical Systems Principles of Motor Operation

More information

DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION

DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION English Michael Faraday (1791 1867) who experimented with electric and magnetic phenomena discovered that a changing magnetic

More information

Pretest ELEA1831 Module 11 Units 1& 2 Inductance & Capacitance

Pretest ELEA1831 Module 11 Units 1& 2 Inductance & Capacitance Pretest ELEA1831 Module 11 Units 1& 2 Inductance & Capacitance 1. What is Faraday s Law? Magnitude of voltage induced in a turn of wire is proportional to the rate of change of flux passing through that

More information

Force and Displacement Measurement

Force and Displacement Measurement Force and Displacement Measurement Prof. R.G. Longoria Updated Fall 20 Simple ways to measure a force http://scienceblogs.com/dotphysics/200/02/diy_force_probe.php Example: Key Force/Deflection measure

More information

Switched Mode Power Conversion Prof. L. Umanand Department of Electronics System Engineering Indian Institute of Science, Bangalore

Switched Mode Power Conversion Prof. L. Umanand Department of Electronics System Engineering Indian Institute of Science, Bangalore Switched Mode Power Conversion Prof. L. Umanand Department of Electronics System Engineering Indian Institute of Science, Bangalore Lecture - 39 Magnetic Design Good day to all of you. Today, we shall

More information

Basics of Network Theory (Part-I)

Basics 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

1 Fig. 3.1 shows the variation of the magnetic flux linkage with time t for a small generator. magnetic. flux linkage / Wb-turns 1.

1 Fig. 3.1 shows the variation of the magnetic flux linkage with time t for a small generator. magnetic. flux linkage / Wb-turns 1. 1 Fig. 3.1 shows the variation of the magnetic flux linkage with time t for a small generator. 2 magnetic 1 flux linkage / 0 10 2 Wb-turns 1 2 5 10 15 t / 10 3 s Fig. 3.1 The generator has a flat coil

More information

NEPTUNE -code: KAUVG11ONC Prerequisites:... Knowledge description:

NEPTUNE -code: KAUVG11ONC Prerequisites:... Knowledge description: Subject name: Electrical Machines Credits: 9 Requirement : Course director: Dr. Vajda István Position: Assessment and verification procedures: NEPTUNE -code: KAUVG11ONC Prerequisites:... Number of hours:

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 R. W. Erickson Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder Part III. Magnetics 13 Basic Magnetics Theory 14 Inductor Design 15 Transformer Design 1 Chapter

More information

Transformer Fundamentals

Transformer Fundamentals Transformer Fundamentals 1 Introduction The physical basis of the transformer is mutual induction between two circuits linked by a common magnetic field. Transformer is required to pass electrical energy

More information

SECTION 7: FAULT ANALYSIS. ESE 470 Energy Distribution Systems

SECTION 7: FAULT ANALYSIS. ESE 470 Energy Distribution Systems SECTION 7: FAULT ANALYSIS ESE 470 Energy Distribution Systems 2 Introduction Power System Faults 3 Faults in three-phase power systems are short circuits Line-to-ground Line-to-line Result in the flow

More information

Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance

Electromagnetic 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 information

Chapter 21 Magnetic Induction Lecture 12

Chapter 21 Magnetic Induction Lecture 12 Chapter 21 Magnetic Induction Lecture 12 21.1 Why is it called Electromagnetism? 21.2 Magnetic Flux and Faraday s Law 21.3 Lenz s Law and Work-Energy Principles 21.4 Inductance 21.5 RL Circuits 21.6 Energy

More information

The self-inductance depends on the geometric shape of the coil. An inductor is a coil of wire used in a circuit to provide inductance is an inductor.

The self-inductance depends on the geometric shape of the coil. An inductor is a coil of wire used in a circuit to provide inductance is an inductor. Self Inductance and Mutual Inductance Script Self-Inductance Consider a coil carrying a current i. The current in the coil produces a magnetic field B that varies from point to point in the coil. The magnetic

More information

Handout 10: Inductance. Self-Inductance and inductors

Handout 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 information

Step Motor Modeling. Step Motor Modeling K. Craig 1

Step Motor Modeling. Step Motor Modeling K. Craig 1 Step Motor Modeling Step Motor Modeling K. Craig 1 Stepper Motor Models Under steady operation at low speeds, we usually do not need to differentiate between VR motors and PM motors (a hybrid motor is

More information

Circuit Theorems Overview Linearity Superposition Source Transformation Thévenin and Norton Equivalents Maximum Power Transfer

Circuit Theorems Overview Linearity Superposition Source Transformation Thévenin and Norton Equivalents Maximum Power Transfer Circuit Theorems Overview Linearity Superposition Source Transformation Thévenin and Norton Equivalents Maximum Power Transfer J. McNames Portland State University ECE 221 Circuit Theorems Ver. 1.36 1

More information

JRE SCHOOL OF Engineering

JRE SCHOOL OF Engineering JRE SCHOOL OF Engineering Class Test-1 Examinations September 2014 Subject Name Electromechanical Energy Conversion-II Subject Code EEE -501 Roll No. of Student Max Marks 30 Marks Max Duration 1 hour Date

More information

TRANSFORMERS B O O K P G

TRANSFORMERS B O O K P G TRANSFORMERS B O O K P G. 4 4 4-449 REVIEW The RMS equivalent current is defined as the dc that will provide the same power in the resistor as the ac does on average P average = I 2 RMS R = 1 2 I 0 2 R=

More information

Physics 102: Lecture 11 Generators and Transformers

Physics 102: Lecture 11 Generators and Transformers Physics 102: Lecture 11 Generators and Transormers Physics 102: Lecture 11, Slide 1 Reiew: Magnetic Flux & Induction B Flux: Induced oltage: = B A cos() is angle between normal and B ε = Φ Δt = Φ Φ i t

More information

Reactor Characteristic Evaluation and Analysis Technologies of JFE Steel

Reactor Characteristic Evaluation and Analysis Technologies of JFE Steel JFE TECHNICAL REPORT No. 21 (Mar. 2016) Reactor Characteristic Evaluation and Analysis Technologies of HIRATANI Tatsuhiko *1 NAMIKAWA Misao *2 NISHINA Yoshiaki *3 Abstract: Reactor characteristic evaluation

More information

EC T32 - ELECTRICAL ENGINEERING

EC T32 - ELECTRICAL ENGINEERING EC T32 - ELECTRICAL ENGINEERING UNIT-I - TRANSFORMER 1. What is a transformer? 2. Briefly explain the principle of operation of transformers. 3. What are the parts of a transformer? 4. What are the types

More information

Tactics: Evaluating line integrals

Tactics: Evaluating line integrals Tactics: Evaluating line integrals Ampère s law Whenever total current I through passes through an area bounded by a closed curve, the line integral of the magnetic field around the curve is given by Ampère

More information

Book Page cgrahamphysics.com Transformers

Book Page cgrahamphysics.com Transformers Book Page 444-449 Transformers Review The RMS equivalent current is defined as the dc that will provide the same power in the resistor as the ac does on average P average = I 2 RMS R = 1 2 I 0 2 R= V RMS

More information

EN Power Electronics and Machines

EN Power Electronics and Machines 1/19 - Power Electronics and Machines Transformers Suryanarayana Doolla Department of Energy Science and Engineering Indian Institute of Technology, Bombay suryad@iitb.ac.in Lecture Organization - Modules

More information

Power Transformers 1. Download/read notes on transformers from website. 2. Download HW4 on website; I will give due-date next week. 3.

Power Transformers 1. Download/read notes on transformers from website. 2. Download HW4 on website; I will give due-date next week. 3. Power Transformers. Download/read notes on transformers from website.. Download HW4 on website; I will give due-date next week.. Read Chapters 5 and 6 in Kirtley s text Power Industry Uses of Transformers

More information

Chapter 23: Magnetic Flux and Faraday s Law of Induction

Chapter 23: Magnetic Flux and Faraday s Law of Induction Chapter 3: Magnetic Flux and Faraday s Law of Induction Answers Conceptual Questions 6. Nothing. In this case, the break prevents a current from circulating around the ring. This, in turn, prevents the

More information

Errors in Electrical Measurements

Errors in Electrical Measurements 1 Errors in Electrical Measurements Systematic error every times you measure e.g. loading or insertion of the measurement instrument Meter error scaling (inaccurate marking), pointer bending, friction,

More information

ElectroMagnetic Induction

ElectroMagnetic Induction ElectroMagnetic Induction Physics 1 What is E/M Induction? Electromagnetic Induction is the process of using magnetic fields to produce voltage, and in a complete circuit, a current. Michael Faraday first

More information

Modelling, Simulation and Temperature Effect Analysis of Mutual Induction based High Temperature Level Sensor using COMSOL Multiphysics

Modelling, Simulation and Temperature Effect Analysis of Mutual Induction based High Temperature Level Sensor using COMSOL Multiphysics Modelling, Simulation and Temperature Effect Analysis of Mutual Induction based High Temperature Level Sensor using COMSOL Multiphysics Rajalakshmi R. Subhasis Dutta Bhabha Atomic Research Center, Mumbai

More information

Basics of Network Theory (Part-I)

Basics of Network Theory (Part-I) Basics of Network Theory (Part-I) 1. One coulomb charge is equal to the charge on (a) 6.24 x 10 18 electrons (b) 6.24 x 10 24 electrons (c) 6.24 x 10 18 atoms (d) none of the above 2. The correct relation

More information

MAY/JUNE 2006 Question & Model Answer IN BASIC ELECTRICITY 194

MAY/JUNE 2006 Question & Model Answer IN BASIC ELECTRICITY 194 MAY/JUNE 2006 Question & Model Answer IN BASIC ELECTRICITY 194 Question 1 (a) List three sources of heat in soldering (b) state the functions of flux in soldering (c) briefly describe with aid of diagram

More information

Mutual Inductance. The field lines flow from a + charge to a - change

Mutual Inductance. The field lines flow from a + charge to a - change Capacitors Mutual Inductance Since electrical charges do exist, electric field lines have a starting point and an ending point. For example, if you have a + and a - change, the field lines would look something

More information

PRACTICE EXAM 1 for Midterm 2

PRACTICE EXAM 1 for Midterm 2 PRACTICE EXAM 1 for Midterm 2 Multiple Choice Questions 1) The figure shows three identical lightbulbs connected to a battery having a constant voltage across its terminals. What happens to the brightness

More information

Transformer. Transformer comprises two or more windings coupled by a common magnetic circuit (M.C.).

Transformer. Transformer comprises two or more windings coupled by a common magnetic circuit (M.C.). . Transformers Transformer Transformer comprises two or more windings coupled by a common magnetic circuit (M.C.). f the primary side is connected to an AC voltage source v (t), an AC flux (t) will be

More information

Chapter 30. Inductance. PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow

Chapter 30. Inductance. PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow Chapter 30 Inductance PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow Learning Goals for Chapter 30 Looking forward at how a time-varying

More information

coil of the circuit. [8+8]

coil of the circuit. [8+8] Code No: R05310202 Set No. 1 III B.Tech I Semester Regular Examinations, November 2008 ELECTRICAL MEASUREMENTS (Electrical & Electronic Engineering) Time: 3 hours Max Marks: 80 Answer any FIVE Questions

More information

ENGG4420 LECTURE 7. CHAPTER 1 BY RADU MURESAN Page 1. September :29 PM

ENGG4420 LECTURE 7. CHAPTER 1 BY RADU MURESAN Page 1. September :29 PM CHAPTER 1 BY RADU MURESAN Page 1 ENGG4420 LECTURE 7 September 21 10 2:29 PM MODELS OF ELECTRIC CIRCUITS Electric circuits contain sources of electric voltage and current and other electronic elements such

More information

magneticsp17 September 14, of 17

magneticsp17 September 14, of 17 EXPERIMENT Magnetics Faraday s Law in Coils with Permanent Magnet, DC and AC Excitation OBJECTIVE The knowledge and understanding of the behavior of magnetic materials is of prime importance for the design

More information

LR Circuits. . The voltage drop through both resistors will equal. Hence 10 1 A

LR Circuits. . The voltage drop through both resistors will equal. Hence 10 1 A The diagram shows a classic R circuit, containing both resistors and inductors. The switch shown is initially connected to neither terminal, and is then thrown to position a at time t = 0. R Circuits E

More information

RC Circuits (32.9) Neil Alberding (SFU Physics) Physics 121: Optics, Electricity & Magnetism Spring / 1

RC Circuits (32.9) Neil Alberding (SFU Physics) Physics 121: Optics, Electricity & Magnetism Spring / 1 (32.9) We have only been discussing DC circuits so far. However, using a capacitor we can create an RC circuit. In this example, a capacitor is charged but the switch is open, meaning no current flows.

More information

Symmetrical Components

Symmetrical Components Prof. Dr.-Ing. Ralph Kennel (ralph.kennel@tum.de) Technische Universität München Lehrstuhl für Elektrische Antriebssysteme und Leistungselektronik München, 06. März 2018 1 symmetrical 3phase system U 1

More information

Chapter 23 Magnetic Flux and Faraday s Law of Induction

Chapter 23 Magnetic Flux and Faraday s Law of Induction Chapter 23 Magnetic Flux and Faraday s Law of Induction 1 Overview of Chapter 23 Induced Electromotive Force Magnetic Flux Faraday s Law of Induction Lenz s Law Mechanical Work and Electrical Energy Generators

More information

MODELING AND MODIFICATION FOR DISTRIBUTION TRANSFORMER (250 KVA, 11/0.416 KV) TO REDUCE THE TOTAL LOSSES

MODELING AND MODIFICATION FOR DISTRIBUTION TRANSFORMER (250 KVA, 11/0.416 KV) TO REDUCE THE TOTAL LOSSES MODELING AND MODIFICATION FOR DISTRIBUTION TRANSFORMER (250 KVA, 11/0.416 KV) TO REDUCE THE TOTAL LOSSES Assist. Prof. Ibtisam A. Hasan Dr. Sahar R. Fafraj Eng. Azhar K. Azeez Electromechanical Eng. Dept.

More information

Electromagnetic Induction

Electromagnetic Induction Faraday s Discovery Faraday found that there is a current in a coil of wire if and only if the magnetic field passing through the coil is changing. This is an informal statement of Faraday s law. Electromagnetic

More information

Switched Mode Power Conversion

Switched Mode Power Conversion Inductors Devices for Efficient Power Conversion Switches Inductors Transformers Capacitors Inductors Inductors Store Energy Inductors Store Energy in a Magnetic Field In Power Converters Energy Storage

More information

Doubly salient reluctance machine or, as it is also called, switched reluctance machine. [Pyrhönen et al 2008]

Doubly salient reluctance machine or, as it is also called, switched reluctance machine. [Pyrhönen et al 2008] Doubly salient reluctance machine or, as it is also called, switched reluctance machine [Pyrhönen et al 2008] Pros and contras of a switched reluctance machine Advantages Simple robust rotor with a small

More information

Chapter 4 Circuit Theorems: Linearity & Superposition

Chapter 4 Circuit Theorems: Linearity & Superposition Chapter 4 Circuit Theorems: Linearity & Superposition Dr. Waleed Al-Hanafy waleed alhanafy@yahoo.com Faculty of Electronic Engineering, Menoufia Univ., Egypt MSA Summer Course: Electric Circuit Analysis

More information

e453.eps 1 Change (or the absolute value) in the measured physical variable 2 Change in the sensor property is translated into low-power-level

e453.eps 1 Change (or the absolute value) in the measured physical variable 2 Change in the sensor property is translated into low-power-level 3 Basic Phenomenon in Effect in Sensor Operation Sensors Prof. Dr. M. Zahurul Haq zahurul@me.buet.ac.bd http://teacher.buet.ac.bd/zahurul/ Department of Mechanical Engineering Bangladesh University of

More information

Chapter 6. Induction Motors. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

Chapter 6. Induction Motors. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Chapter 6 Induction Motors 1 The Development of Induced Torque in an Induction Motor Figure 6-6 The development of induced torque in an induction motor. (a) The rotating stator field B S induces a voltage

More information

ELECTRICITY AND MAGNETISM, A. C. THEORY AND ELECTRONICS, ATOMIC AND NUCLEAR PHYSICS

ELECTRICITY AND MAGNETISM, A. C. THEORY AND ELECTRONICS, ATOMIC AND NUCLEAR PHYSICS UNIT 2: ELECTRICITY AND MAGNETISM, A. C. THEORY AND ELECTRONICS, ATOMIC AND NUCLEAR PHYSICS MODULE 1: ELECTRICITY AND MAGNETISM GENERAL OBJECTIVES On completion of this Module, students should: 1. understand

More information

Slide 1 / 26. Inductance by Bryan Pflueger

Slide 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 information

ECE2210 Final given: Fall 13

ECE2210 Final given: Fall 13 ECE22 Final given: Fall 3. (23 pts) a) Draw the asymptotic Bode plot (the straight-line approximation) of the transfer function below. Accurately draw it on the graph provided. You must show the steps

More information

Behaviour of synchronous machine during a short-circuit (a simple example of electromagnetic transients)

Behaviour of synchronous machine during a short-circuit (a simple example of electromagnetic transients) ELEC0047 - Power system dynamics, control and stability (a simple example of electromagnetic transients) Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct October 2018 1 / 25 Objectives

More information

8. (6) Consider the circuit here with resistors R A, R B and R C. Rank the

8. (6) Consider the circuit here with resistors R A, R B and R C. Rank the General Physics II Exam 2 - Chs. 18B 21 - Circuits, Magnetism, EM Induction - Oct. 3, 2013 Name Rec. Instr. Rec. Time For full credit, make your work clear. Show formulas used, essential steps, and results

More information

Chapter 30 Inductance

Chapter 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 information

1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields.

1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields. 1. An isolated stationary point charge produces around it. a) An electric field only. b) A magnetic field only. c) Electric as well magnetic fields. 2. An isolated moving point charge produces around it.

More information

Chapter 30. Induction and Inductance

Chapter 30. Induction and Inductance Chapter 30 Induction and Inductance 30.2: First Experiment: 1. A current appears only if there is relative motion between the loop and the magnet (one must move relative to the other); the current disappears

More information

Exam 2 Solutions. PHY2054 Spring Prof. Paul Avery Prof. Pradeep Kumar Mar. 18, 2014

Exam 2 Solutions. PHY2054 Spring Prof. Paul Avery Prof. Pradeep Kumar Mar. 18, 2014 Exam 2 Solutions Prof. Paul Avery Prof. Pradeep Kumar Mar. 18, 2014 1. A series circuit consists of an open switch, a 6.0 Ω resistor, an uncharged 4.0 µf capacitor and a battery with emf 15.0 V and internal

More information

Introduction to Synchronous. Machines. Kevin Gaughan

Introduction to Synchronous. Machines. Kevin Gaughan Introduction to Synchronous Machines Kevin Gaughan The Synchronous Machine An AC machine (generator or motor) with a stator winding (usually 3 phase) generating a rotating magnetic field and a rotor carrying

More information

Chapter 30 INDUCTANCE. Copyright 2012 Pearson Education Inc.

Chapter 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 information

Can a Magnetic Field Produce a Current?

Can a Magnetic Field Produce a Current? Can a Magnetic Field Produce a Current? In our study of magnetism we learned that an electric current through a wire, or moving electrically charged objects, produces a magnetic field. Could the reverse

More information

CHAPTER 8 DC MACHINERY FUNDAMENTALS

CHAPTER 8 DC MACHINERY FUNDAMENTALS CHAPTER 8 DC MACHINERY FUNDAMENTALS Summary: 1. A Simple Rotating Loop between Curved Pole Faces - The Voltage Induced in a Rotating Loop - Getting DC voltage out of the Rotating Loop - The Induced Torque

More information

Sliding Conducting Bar

Sliding Conducting Bar Motional emf, final For equilibrium, qe = qvb or E = vb A potential difference is maintained between the ends of the conductor as long as the conductor continues to move through the uniform magnetic field

More information

Chapter 21. Derivations for the Design Equations

Chapter 21. Derivations for the Design Equations Chapter 21 Derivations for the Design Equations The author would like to thank Richard Ozenbaugh of Linear Magnetics for his help with the derivations. Table of Contents 1. Output Power, P 0, Versus Apparent

More information

DcMotor_ Model Help File

DcMotor_ Model Help File Name of Model: DcMotor_021708 Author: Vladimir L. Chervyakov Date: 2002-10-26 Executable file name DcMotor_021708.vtm Version number: 1.0 Description This model represents a Nonlinear model of a permanent

More information

Physics - Grade 12. Revision Sheet for the Final Exam / Second Term. Academic Year: 2018/2019. Student s Name:.. Date: /3/2018

Physics - Grade 12. Revision Sheet for the Final Exam / Second Term. Academic Year: 2018/2019. Student s Name:.. Date: /3/2018 Physics - Grade 12 Revision Sheet for the Final Exam / Second Term Academic Year: 2018/2019 Student s Name:.. Date: /3/2018 Required Material: Chapter 18: Sections 1,2 & 3 (Textbook Pages: 628-661) Chapter

More information