DHANALAKSHMI COLLEGE OF ENGINEERING DEPARTMENT OF EEE PART A. 1. Define mutual inductance and self inductance. (A/M-15)

Similar documents
Lecture 35. PHYC 161 Fall 2016

Lecture 33. PHYC 161 Fall 2016

COLLEGE PHYSICS Chapter 23 ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES

MAGNETIC CIRCUITS. Magnetic Circuits

UNIT I ELECTROSTATIC FIELDS

we can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron.

ELECTROMAGNETIC FIELD

UNIT-III Maxwell's equations (Time varying fields)

Slide 1 / 24. Electromagnetic Induction 2011 by Bryan Pflueger

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING QUESTION BANK

UNIT-I INTRODUCTION TO COORDINATE SYSTEMS AND VECTOR ALGEBRA

Chapter 21 Magnetic Induction Lecture 12

Induction. Chapter 29. PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman. Lectures by James Pazun

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

Motional Electromotive Force

ELECTRO MAGNETIC FIELDS

FB-DC6 Electric Circuits: Magnetism and Electromagnetism

Electromagnetic Induction

MAGNETIC CIRCUITS, MOTOR AND GENERATOR ACTION

Electromagnetic Field Theory (EMT) Lecture # 25

DHANALAKSHMI SRINIVASAN INSTITUTE OF RESEARCH AND TECHNOLOGY

Chapter 27, 28 & 29: Magnetism & Electromagnetic Induction. Magnetic flux Faraday s and Lenz s law Electromagnetic Induction Ampere s law

Chapter 23 Magnetic Flux and Faraday s Law of Induction

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.

General Physics II. Electromagnetic Induction and Electromagnetic Waves

Electromagnetic Induction & Inductors

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.

CHAPTER 7 ELECTRODYNAMICS

Electromagnetic Field Theory Chapter 9: Time-varying EM Fields

Chapter 29 Electromagnetic Induction

Chapter 30 Inductance and Electromagnetic Oscillations

PHYSICS. Chapter 30 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

Electromagnetic Induction

Module 3 Electrical Fundamentals

While the Gauss law forms for the static electric and steady magnetic field equations

E or B? It Depends on Your Perspective

Physics 54 Lecture March 1, Micro-quiz problems (magnetic fields and forces) Magnetic dipoles and their interaction with magnetic fields

Tactics: Evaluating line integrals

Section 11: Magnetic Fields and Induction (Faraday's Discovery)

2426 Required Topics (May 4, 2012 draft) Halliday, FUNDAMENTALS OF PHYSICS, 9e Required topics are in bold text. Optional topics are in normal text.

Describe the forces and torques exerted on an electric dipole in a field.

Magnetic Induction Faraday, Lenz, Mutual & Self Inductance Maxwell s Eqns, E-M waves. Reading Journals for Tuesday from table(s)

PHYS 202 Notes, Week 6

Section 11: Magnetic Fields and Induction (Faraday's Discovery)

Chapter 1 Magnetic Circuits

Transmission Lines and E. M. Waves Prof. R. K. Shevgaonkar Department of Electrical Engineering Indian Institute of Technology, Bombay

DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION

r r 1 r r 1 2 = q 1 p = qd and it points from the negative charge to the positive charge.

PHYSICS Fall Lecture 15. Electromagnetic Induction and Faraday s Law

October 23. Physics 272. Fall Prof. Philip von Doetinchem

ELECTRICITY AND MAGNETISM

r where the electric constant

Chapter 2 Basics of Electricity and Magnetism

Unit-1 Electrostatics-1

Agenda for Today. Elements of Physics II. Forces on currents

Electromagnetic Induction. Bo Zhou Faculty of Science, Hokudai

Faraday s Law. Lecture 17. Chapter 33. Physics II. Course website:

AP Physics C Electricity and Magnetism

Faraday s Law. Lecture 17. Chapter 33. Physics II. Course website:

AP Physics C - E & M

Electromagnetic Induction

CHAPTER 5 ELECTROMAGNETIC INDUCTION

Maxwell Equations: Electromagnetic Waves

Magnetic inductance & Solenoids. P.Ravindran, PHY041: Electricity & Magnetism 22 February 2013: Magnetic inductance, and Solenoid

Induction_P1. 1. [1 mark]

Here are some internet links to instructional and necessary background materials:

FARADAY S AND LENZ LAW B O O K P G

Chapter Three: Propagation of light waves

Calculus Relationships in AP Physics C: Electricity and Magnetism

Magnetic flux. where θ is the angle between the magnetic field and the area vector. The unit of magnetic flux is the weber. 1 Wb = 1 T m 2.

Physics Notes for Class 12 chapter 6 ELECTROMAGNETIC I NDUCTION

Application Of Faraday s Law

ELECTROMAGNETISM. Second Edition. I. S. Grant W. R. Phillips. John Wiley & Sons. Department of Physics University of Manchester

Magnetism. and its applications

CHAPTER 2. COULOMB S LAW AND ELECTRONIC FIELD INTENSITY. 2.3 Field Due to a Continuous Volume Charge Distribution

Definition Application of electrical machines Electromagnetism: review Analogies between electric and magnetic circuits Faraday s Law Electromagnetic

Faraday s Law of Electromagnetic Induction

Lecture Notes ELEC A6

r where the electric constant

Chapter 15 Magnetic Circuits and Transformers

CHAPTER 29: ELECTROMAGNETIC INDUCTION

Last Homework. Reading: Chap. 33 and Chap. 33. Suggested exercises: 33.1, 33.3, 33.5, 33.7, 33.9, 33.11, 33.13, 33.15,

Physics 1308 Exam 2 Summer 2015

Lecture 24. April 5 th, Magnetic Circuits & Inductance

AQA Physics A-level Section 7: Fields and Their Consequences

Electromagnetic Induction

UNIT-I INTRODUCTION. 1. State the principle of electromechanical energy conversion.

Chapter 12. Magnetism and Electromagnetism

PHYS 241 EXAM #2 November 9, 2006

1 (a) Define magnetic flux [1]

EELE 3332 Electromagnetic II Chapter 9. Maxwell s Equations. Islamic University of Gaza Electrical Engineering Department Dr.

Dynamic Fields, Maxwell s Equations (Chapter 6)

cancel each other out. Thus, we only need to consider magnetic field produced by wire carrying current 2.

Sliding Conducting Bar

Magnetostatic fields! steady magnetic fields produced by steady (DC) currents or stationary magnetic materials.

Chapter 23 Magnetic Flux and Faraday s Law of Induction

Mansfield Independent School District AP Physics C: Electricity and Magnetism Year at a Glance

PhysicsAndMathsTutor.com

University Of Pennsylvania Department of Physics PHYS 141/151 Engineering Physics II (Course Outline)

Engineering Electromagnetics

Transcription:

DHANALAKSHMI COLLEGE OF ENGINEERING DEPARTMENT OF EEE EE6302-ELECTROMAGNETIC THEORY UNIT 4 PART A 1. Define mutual inductance and self inductance. (A/M-15) Self inductance is the ration between the induced Electro Motive Force (EMF) across a coil to the rate of change of current through this coil. Self inductance is related term to self induction phenomenon. Mutual Inductance is the ratio between induced Electro Motive Force across a coil to the rate of change of current of another adjacent coil in such a way that two coils are in possibility of flux linkage. 2. Distinguish between transformer emf and motional emf. (A/M-15) ``Induced emf'' is the more general term. By Faraday's Law, you get an induced emf whenever there's a changing magnetic flux through a loop.... But if the changing magnetic flux were due to, say, an increasing current in a wire, you wouldn't call it a ``motional'' emf. 3. State Faraday s law of Electromagnetic induction. (M/J 16) Faraday's law of induction is a basic law of electromagnetism predicting how a magnetic field will interact with an electric circuit to produce an electromotive force (EMF) a phenomenon called electromagnetic induction. 4. What is meant by displacement current? (M/J 16)

In electromagnetism, displacement current is a quantity appearing in Maxwell's equations that is defined in terms of the rate of change of electric displacement field. Displacement current has the units of electric current density, and it has an associated magnetic field just as actual currents do. 5. State Ohm s law for magnetic circuits. (N/D-14) ohm's law for magnetic circuits. Φ=mmf/R where Φ is the magnetic Flux, mmf is the magnetomotive force, and R is the Reluctance. 6. State Faraday s Law. (N/D-16) Faraday's law of induction is a basic law of electromagnetism predicting how a magnetic field will interact with an electric circuit to produce an electromotive force (EMF) a phenomenon called electromagnetic induction. 7) Differentiate transformer and motional emf. (A/M-17) ``Induced emf'' is the more general term. By Faraday's Law, you get an induced emf whenever there's a changing magnetic flux through a loop.... But if the changing magnetic flux were due to, say, an increasing current in a wire, you wouldn't call it a ``motional'' emf. 8) State: Poynting Theorem. (M/J-14) This theorem states that the cross product of electric field vector, E and magnetic field vector, H at any point is a measure of the rate of flow of electromagnetic energy per unit area at that point, that is P = E x H

Here P Poynting vector and it is named after its discoverer, J.H. Poynting. The direction of P is perpendicular to E and H and in the direction of vector E x H PART B 1. Derive the Maxwell s equations both in integral and point forms. (A/M-17).(M/J-11),(N/D-11), (M/J-12),( N/D-12),( M/J-13),( M/J-14)( N/D- 14),( A/M-16)

2. Explain the relation between field theory and circuit theory in detail. (A/M-17)

3. State Faraday s Law of Electromagnetic induction. (M/J-15) Faraday's law of induction is a basic law of electromagnetism predicting how a magnetic field will interact with an electric circuit to produce an electromotive force (EMF) a phenomenon called electromagnetic induction.

4. Compare and explain conduction and displacement currents. Conduction current is the electric current that flows through a conductor because of an applied potential difference. Displacement current I D is the current that is included to explain the magnetic field inside the capacitor due to mounting up of charges on its plates. Mathematically displacement current I D is expressed as the following: Displacement current appears as a theoretical necessity in situations where non steady current is encountered. Example: If we keep a magnetic needle between the plates of a charging capacitor (incompletely charged) consisting of parallel plates shows a deflection indicating that there exists a magnetic field between plates.