Hysteresis When we increased the current we observed, saturation. What would happen if I decrease the current after saturation? The flux for a given H.

Slides:



Advertisements
Similar presentations
Electrical Machines LSEGG216A 9080V.
Advertisements

By: Cody Balogh POE 2A. An AC motor can consist of a varying assortment of pieces all of which can include; a positive(N) and a negative(S) magnet, copper(or.
MAGNETISM. The Earth Magnetic Poles North and South Geographic Poles North and South Earth is a giant magnet.
Chapter 22 Electromagnetic Induction Induced Emf and Induced Current There are a number of ways a magnetic field can be used to generate an electric.
Magnetic Circuits and Transformers
12: Electromagnetic Induction 12.2 Alternating Current.
Engr. Abbas Abbasi Behavior of Ferromagnetic Materials Saturation and Hysteresis.
DC Motors KL3073.
Chapter 17 Electromagnetic Induction. The prime link between electricity and magnetism is… MOTION.
Summary of the last lecture
Magnetic Field Basic Concepts: A current carrying wire produces a magnetic field in the area around it. A time changing magnetic field induces a voltage.
By Stephen, Victor, Thomas and Tim. What Is a Transformer? A device designed to transfer energy from one electrical circuit to another.
Lecture No. 15 By. Sajid Hussain Qazi.  Physical explanation of Hysteresis loss ▪ The magnetic core of transformer is made of ′ Cold Rolled Grain Oriented.
DC motors.
Magnetic and Electromagnetic Fields
Day 4: Transformers Definition of a Transformer Transformer Windings Transformer Operation using Faraday’s Law Step-up & Step-down Transformers Turns Ratio.
DC GENERATOR CHAPTER-9.
MUZAIDI BIN MARZUKI Chapter 4: Electromagnetic.
Chapter 16 DC Generators.
When a ferromagnetic material is magnetized in one direction, it will not relax back to zero magnetization when the imposed magnetizing field is removed.
Elec467 Power Machines & Transformers
Chapter 1 MAGNETIC CIRCUIT.
Electromagnetic Induction
Producing Electric Current
ELECTRICAL BASICS (Chapter 8) Electrical terms Electricity & magnetism Electricity Circuits Magnetism Electrical units Electric potential or eletromotive.
Fundamentals of Electromagnetics and Electromechanics
Lecture 14 Magnetic Domains Induced EMF Faraday’s Law Induction Motional EMF.
Chapter 22 Electromagnetic Induction. When a coil of wire is in a magnetic field, the magnetic flux Ф is the strength of the field B multiplied by the.
Transformers Transformers are some of the most efficient machines that can be built, with efficiencies exceeding 99%. Only simple machines (levers, inclined.
DC Generators.
AC Machines Fundamentals. Introduction Synchronous machines: Motors and generators whose magnetic field is supplied by a separate dc power supply. Induction.
BASIC ELECTRICAL TECHNOLOGY Chapter 6: Single Phase Transformer
Tuesday April 19, PHYS , Dr. Andrew Brandt PHYS 1444 – Section 02 Lecture #18 Tuesday April 19, 2011 Dr. Andrew Brandt Chapter 29 Lenz Law.
Electromagnetic Induction. Electric Fields Electric fields are created bycharges A charge in an electric field always has a force on it + force.
3/17/2014 PHYS , Dr. Andrew Brandt 1 PHYS 1442 – Section 004 Lecture #15 Monday March 17, 2014 Dr. Andrew Brandt Chapter 21 Generator Transformer.
Magnets and Electromagnetism Chapter Outline 1.Magnets, magnetic poles, and magnetic force. 2.Magnetic effects of electric current. 3.Magnetic effects.
Lecture 18 Chapter 32 Outline Gauss Law for Mag Field Maxwell extension of Ampere’s Law Displacement Current Spin/ Orbital Mag Dipole Moment Magnetic Properties.
Lecture 02Electro Mechanical System1 Assignment 1 Page 46, Problem 2.4, 2.5, 2.7 & 2.8 Due Date: Tuesday 1 st Feb, 2011.
Transformer The working principle of a transformer
Wednesday, April 11, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #18 Wednesday, April Dr. Andrew Brandt.
ELECTRICAL MACHINE DET 204/3 JIMIRAFIZI BIN JAMIL Transformer CHAPTER 1.
DC Generators (ii) Lecture No 4. Armature Resistance (Ra) The resistance offered by the armature circuit is known as armature resistance (Ra) and includes:
Magnets and Electromagnetism Chapter Outline 1.Magnets, magnetic poles, and magnetic force. 2.Magnetic effects of electric current. 3.Magnetic effects.
POWER CIRCUIT & ELECTROMAGNETICS EET 221 Transformer.
Practice Problems A horizontal wire is moving vertically upwards in a horizontal magnetic field of strength tesla which is perpendicular to the.
1 Figure 17.1 A Rotating Electric Machine. 2 Configurations of the three types of electric machines Table 17.1.
L-8 MAGNETIC CIRCUITS ELE 1001: Basic Electrical Technology
OPERATING CHARACTERISTICS OF DC GENERATOR
AQA Physics Magnetic Fields Section 7 Transformers.
Magnetic Circuits and Magnetic Materials
True-False Questions. A magnetic core material may exhibit hysteresis or saturation but not both.
TERMINAL CHARCATERISTIC of a SHUNT DC MOTOR
DC Machine 1. 直流發電機原理 磁場 法拉第定理與感應電壓 2. 交直流發電機與結構 3. 反電動式的電壓 4. 繞組方式 5. 電樞反應與解決方法 6. 電壓調整率.
DCMT PRESENTATION DEVANSH KHARE ( )
Warm-up Why do loops of wire in a motor rotate?
True-False Questions.
& 13 transformers.
DC Generators.
Hansaba College of Engineering & Technology
Power Magnetic Devices: A Multi-Objective Design Approach
Electromagnetic Induction
DC Machines Fundamentals
© 2011 Cengage Learning Engineering. All Rights Reserved.
Principles & Applications
PHYS 1444 – Section 003 Lecture #18
Chapter 1 Introduction to Machinery Principles
Electromagnetic Induction
Transformers Elliott.
Electrical Machines (EELE 3351)
Unit-1 Transformer.
Presentation transcript:

Hysteresis When we increased the current we observed, saturation. What would happen if I decrease the current after saturation? The flux for a given H is higher when decreasing

Hysteresis Losses Figure shows the effect within ferromagnetic materials known as hysteresis. ferromagnetic We start with an unmagnetized sample at the origin (P1) where both field strength and flux density are zero. The field strength is increased in the positive direction and the flux begins to grow along the dotted path until we reach P2. This is called the initial magnetization curve.field strengthflux densityinitial magnetization curve.

Hysteresis Losses….contd If the field strength is now relaxed then some curious behavior occurs. Instead of retracing the initial magnetization curve the flux falls more slowly. In fact, even when the applied field is returned to zero there will still be a remaining (remnant or remanent) flux density at P3. It is this phenomenon which makes permanent magnets possible.remnant or remanent

Can we explain the hysteresis phenomena? All materials consist of small magnetic domains. When they are in a magnetic field the domains are intended to be in line with the field.

The domains before applying magnetic field The domains after applying magnetic field When the magnetic field is removed, not all domains are randomized again

Hysteresis loss Hysteresis is not a serious problem when we have DC excitation (the examples considered so far). It causes some loss when we have AC excitation, called hysteresis loss. If we have AC excitation, e.g. the current i is sinusoid, the hysteresis happens at each cycle. The hysteresis loss is proportional to the frequency and also depends on the area of the hysteresis loop.

Other losses - Copper loss: - Eddy Current loss: - Core losses:

Eddy Current Eddy current: As we saw, a flux induces a voltage on a coil. Q: Why not inducing a voltage on the core itself? A: It actually does. The result is eddy current. That is why the transformers core are laminated.

Eddy current losses

How do we reduce Eddy current losses LAMINATED SOLID

Eddy current losses

Eddy current losses in windings Can be a problem with thick wires - Low voltage machines - High speed machines