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

Similar documents
MAGNETIC CIRCUITS. Magnetic Circuits

Chapter 1 Magnetic Circuits

Lecture Notes ELEC A6

Revision Guide for Chapter 15

Magnetism & Electromagnetism

MAGNETIC CIRCUITS, MOTOR AND GENERATOR ACTION

MCE380: Measurements and Instrumentation Lab. Chapter 5: Electromechanical Transducers

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

Electromagnetism. Topics Covered in Chapter 14:

Lesson 17: Synchronous Machines

An Introduction to Electrical Machines. P. Di Barba, University of Pavia, Italy

ELECTRICALMACHINES-I QUESTUION BANK

The initial magnetization curve shows the magnetic flux density that would result when an increasing magnetic field is applied to an initially

Magnetic Quantities. Magnetic fields are described by drawing flux lines that represent the magnetic field.

Electromagnetic Induction & Inductors

Chapter 7. Chapter 7. Electric Circuits Fundamentals - Floyd. Copyright 2007 Prentice-Hall

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

Revision Guide for Chapter 15

Equal Pitch and Unequal Pitch:

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

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos

Application Of Faraday s Law

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES NQF LEVEL 3. OUTCOME 3 - MAGNETISM and INDUCTION

Electrical Machines and Energy Systems: Operating Principles (Part 2) SYED A Rizvi

Electrics. Electromagnetism

Chapter 15 Magnetic Circuits and Transformers

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

PHYS 1442 Section 004 Lecture #14

Chapter 23 Magnetic Flux and Faraday s Law of Induction

ELECTROMAGNETIC INDUCTION AND FARADAY S LAW

Prof. Krishna Vasudevan, Prof. G. Sridhara Rao, Prof. P. Sasidhara Rao

Dynamic Fields, Maxwell s Equations (Chapter 6)

SYLLABUS(EE-205-F) SECTION-B

Chapter 23 Magnetic Flux and Faraday s Law of Induction

Basic Electrical Engineering SYLLABUS. Total No. of Lecture Hrs. : 50 Exam Marks : 80

LAB REPORT: THREE-PHASE INDUCTION MACHINE

Magnetism is associated with charges in motion (currents):

DO PHYSICS ONLINE MOTORS AND GENERATORS FARADAY S LAW ELECTROMAGNETIC INDUCTION

Sliding Conducting Bar

Chapter 5 Three phase induction machine (1) Shengnan Li

Unit 8: Electromagnetism

Version The diagram below represents lines of magnetic flux within a region of space.

Module 3 Electrical Fundamentals

Automatic Control Systems. -Lecture Note 15-

Review of Basic Electrical and Magnetic Circuit Concepts EE

Physics for Scientists & Engineers 2

Introduction. Energy is needed in different forms: Light bulbs and heaters need electrical energy Fans and rolling miles need mechanical energy

Applied Electronics and Electrical Machines

SECOND ENGINEER REG III/2 MARINE ELECTRO-TECHNOLOGY. 1. Understands the physical construction and characteristics of basic components.

Electric Machines I Three Phase Induction Motor. Dr. Firas Obeidat

IE1206 Embedded Electronics

Part 4: Electromagnetism. 4.1: Induction. A. Faraday's Law. The magnetic flux through a loop of wire is

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.

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

PHYSICS Fall Lecture 15. Electromagnetic Induction and Faraday s Law

Slide 1 / 50. Electromagnetic Induction and Faraday s Law

General Physics II. Electromagnetic Induction and Electromagnetic Waves

IE1206 Embedded Electronics Le2

Chapter 2: Fundamentals of Magnetism. 8/28/2003 Electromechanical Dynamics 1

Demo: Solenoid and Magnet. Topics. Chapter 22 Electromagnetic Induction. EMF Induced in a Moving Conductor

PHYS 202 Notes, Week 6

JRE SCHOOL OF Engineering

FB-DC6 Electric Circuits: Magnetism and Electromagnetism

Lecture 1: Induction Motor

Chapter 30. Inductance

Lecture 24. April 5 th, Magnetic Circuits & Inductance

EC T32 - ELECTRICAL ENGINEERING

ELECTRIC MACHINE TORQUE PRODUCTION 101

David J. Starling Penn State Hazleton PHYS 212

Electromagnetic Induction and Faraday s Law

Chapter 5: Electromagnetic Induction

Chapter 22. Induction

Slide 1 / 50. Slide 2 / 50. Slide 3 / 50. Electromagnetic Induction and Faraday s Law. Electromagnetic Induction and Faraday s Law.

EE 742 Chapter 3: Power System in the Steady State. Y. Baghzouz

Magnetic field and magnetic poles

PHYS 1444 Section 003 Lecture #18

Fachgebiet Leistungselektronik und Elektrische Antriebstechnik. Test Examination: Mechatronics and Electrical Drives

Step Motor Modeling. Step Motor Modeling K. Craig 1

magneticsp17 September 14, of 17

FARADAY S AND LENZ LAW B O O K P G

Michael Faraday. Chapter 31. EMF Produced by a Changing Magnetic Field, 1. Induction. Faraday s Law

Electricity & Optics

CHAPTER 8 DC MACHINERY FUNDAMENTALS

SECTION 3 BASIC AUTOMATIC CONTROLS UNIT 12 BASIC ELECTRICITY AND MAGNETISM

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

Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors

1 (a) Define magnetic flux [1]

13. Faraday s Law. S. G. Rajeev. March 3, 2009

Outside the solenoid, the field lines are spread apart, and at any given distance from the axis, the field is weak.

Synchronous Machines

Aircraft Powerplant Electrical Systems AMT 109C

-magnetic dipoles are largely analogous to electric dipole moments -both types of dipoles

Introduction to Synchronous. Machines. Kevin Gaughan

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

Electromagnetic Induction

Chapter 21 Magnetic Induction Lecture 12

Motor-CAD combined electromagnetic and thermal model (January 2015)

College Physics B - PHY2054C

DC motors. 1. Parallel (shunt) excited DC motor

TRANSFORMERS B O O K P G

Transcription:

Definition Application of electrical machines Electromagnetism: review Analogies between electric and magnetic circuits Faraday s Law Electromagnetic Force Motor action Generator action Types and parts of machines 1

1. Definition Electric machines are energy conversion devices that convert electrical energy to mechanical energy and vice versa through the medium of magnetic field. An electric machine is called a generator when it is used to convert mechanical energy to electrical energy. On the contrary, when an electric machine is operated to convert electrical energy to mechanical energy, it is called a motor. 2. Application of Machines Electric motors are used to operate washing machines, elevators, cranes etc while electric generators are used to generate electricity for power generation and alternator for charging car battery. 2

Applications of Machines 3

Applications of Machines 4

Applications of Machines 5

Electromagnetism Magnetic fields are the fundamental mechanism by which energy is conserved from one form to another in motors, generators and transformers. A magnetic field is a condition resulting from electric charges in motion. For convenience in visualization and analysis, magnetic fields are represented on diagrams by close loops. Theses loops, called magnetic flux lines 6

Magnetic Circuit Magnetic circuit showing an arrangement of ferromagnetic materials (core) that forms the path and guide the magnetic flux. The flux always takes the shortest path 7

Megnetomotive force It is the driving force that causes the magnetic filed to appear in a magnetic circuit. Magnetic Field Intensity It is the mmf per unit length of the magnetic circuit and it may vary from point to point throughout the circuit. Flux Density It s a measure of the concentration of lines of flux in a particular section of magnetic circuit 8

Reluctance It s a measure of the opposition the magnetic circuit offers to the flux. The reluctance of a magnetic circuit is related to its length, cross sectional area, and permeability. 9

Relative permeability and magnetization curves Relative permeability is the ratio of the permeability of a material to the permeability of free space. It is very useful for comparing the magnetizability of different magnetic materials whose relative permeabilities are known. 10

The ratio µ=b/h is called magnetic permeability and has different values for different magnetic materials. 11

Analogies between Electric and Magnetic Circuits The relationship between mmf, flux, and reluctance in a magnetic circuit is an analog of the relationship bwteen emf, current and resistance respectively, in an electric circuit. 12

Magnetic Circuit and its Electrical Analog 13

Magnetic Circuit and its Electrical Analog A ferromagnetic core is shown in figure below. The depth of the core is 5 cm. The other dimensions of the core are as shown in the figure. Find the value of the current that will produce a flux of 0.005 Wb. With this current, what is the flux density at the top of the core? What is the flux density at the right side of the core? Assume that the relative permeability of the core is 1000. 14

15

16

Magnetic Hysteresis and hysteresis losses Hysteresis means lagging behind. In magnetic hysteresis, flux density B lags behind the field intensity H Hysteresis loop shows the characteristics of magnetic material. It is obtained by plotting values of flux density B for periodically reversing field intensity 17

Magnetic Field play an important role in electric machines. Magnetic fields are produced when current flows in coils of wire. Magnetic fields have 2 funtions: - produce torque for motor operation - generate voltage for generator operation 18

If a conductor is moved by an external force, D in a magnetic field, an electromagnetic force is produced between the two ends of the conductor. This is the basis for the operation of a generator. According to Faraday s Law, a magnetic field will induce a voltage, e in a coil. This forms the basis for the operation of a generator. The voltage, e is given by, e dnφ dt NdΦ dt N Number of turns of each coil Φ Magnetic flux (Weber) 19

Force F is produced and it acts on the conductor. Force is given by, F = BI (Newtons) Current flows in a conductor and produces a force and a mechanical output i.e. conductor motion. This serves as the basis for motor operation. 20

Michael Faraday showed that passing a current through a conductor freely suspended in a fixed magnetic field creates a force which causes the conductor to move through the field. The force created by the current, now known as the Lorentz force, acts between the current conductor and the magnetic field, or the magnet creating the field.the magnitude of the force acting on the conductor is given by: F = BLI where F is the force on the conductor, L is the length of the conductor and I is the current flowing through the conductor 21

Faraday also showed that the converse is true - moving a conductor through a magnetic field, or moving the magnetic field relative to the conductor, causes a current to flow in the conductor. The magnitude of the EMF generated in this way is given by: E = BLv where E is the generator EMF (or back EMF in a motor) and v is the velocity of the conductor through the field 22

In practice, both the motor and the generator effects take place at the same time. Passing the current through a conductor in the magnetic field causes the conductor to move through the field but once the conductor starts moving it becomes a generator creating a current through the conductor in the opposite direction to the applied current. Thus the motion of the conductor creates a "back EMF " which opposes the applied EMF. Conversely moving the conductor through the field causes a current to flow through the conductor which in turn creates a force on the conductor opposing the applied force. 23

24

25

1. 3 types of rotating machines: - Synchronous AC Machines - Asynchronous Machines or Induction Machines - DC Machines 26

- Shaft is fasten to the rotor so that both rotate at the same angular speed - Connection of the machine to load is through the shaft - 3 main parts for both rotor and stator: - core - winding - insulation 27