Electromagnetism Lecture#9 Instructor: Engr. Muhammad Mateen Yaqoob.

Slides:



Advertisements
Similar presentations
Faradays Law of Induction A changing magnetic field induces an electric field. The induced electric field causes a current to flow in a conductor.
Advertisements

Topic 12.1 Induced electromotive force (emf) 3 hours.
Magnetic Flux Let us consider a loop of current I shown in Figure(a). The flux  1 that passes through the area S 1 bounded by the loop is Suppose we pass.
Biot-Savart Law The Field Produced by a Straight Wire.
Self Inductance. Solenoid Flux  Coils of wire carrying current generate a magnetic field. Strong field inside solenoidStrong field inside solenoid 
Copyright © 2009 Pearson Education, Inc. Lecture 9 – Electromagnetic Induction.
Physics 121: Electricity & Magnetism – Lecture 11 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
G L Pollack and D R Stump Electromagnetism Electromagnetic Induction Faraday’s law If a magnetic field changes in time there is an induced electric.
ECE 201 Circuit Theory I1 Physical Characteristics of Inductors.
Current carrying wires 1820 Hans Christian Oersted Hans Christian Ørsted.
Department of Electrical & Electronics Engineering ELE 1001: Basic Electrical Technology Lecture 5 Inductor.
Biot-Savart Law The Field Produced by a Straight Wire.
Electromagnetic Induction. Currents Create Magnetic Fields 1820 Hans Christian Oersted found that magnetism was produced by current-carrying wires.
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 14.1 Inductance and Magnetic Fields  Introduction  Electromagnetism  Reluctance.
Inductors Chap 11.
Chapter 29 Electromagnetic Induction and Faraday’s Law HW#9: Chapter 28: Pb.18, Pb. 31, Pb.40 Chapter 29:Pb.3, Pb 30, Pb. 48 Due Wednesday 22.
22/12/2014.
Electromagnetic Induction
Electromagnetic Induction
Unit 5: Day 8 – Mutual & Self Inductance
AP Physics C Montwood High School R. Casao
Chapter 30 Inductance. Self Inductance When a time dependent current passes through a coil, a changing magnetic flux is produced inside the coil and this.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits.
Unit 14 Magnetic Induction. Objectives: Discuss magnetic induction. List factors that determine the amount and polarity of an induced voltage. Discuss.
Electromagnetism Lecture#06 MUHAMMAD MATEEN YAQOOB THE UNIVERSITY OF LAHORE SARGODHA CAMPUS.
Field Lines.
Chapter 22: Electromagnetic Induction Essential Concepts and Summary.
B due to a moving point charge where  0 = 4  x10 -7 T.m/A Biot-Savart law: B due to a current element B on the axis of a current loop B inside a solenoid.
AP Physics C III.E – Electromagnetism. Motional EMF. Consider a conducting wire moving through a magnetic field.
Motional EMF This is the emf induced in a conductor moving through a magnetic field. Examples on sheet 10 To change the magnetic flux we can change: 1.the.
Lecture # 11 Magnetism and Inductance. Magnetism Magnetism is a phenomenon which includes forces exerted by magnets on other magnets It has its origin.
Electromagnetism Lecture#8 Instructor: Engr. Muhammad Mateen Yaqoob.
EENG 2610: Circuit Analysis Class 10: Capacitors and Inductors
Electromagnetic Induction
305221, Computer Electrical Circuit Analysis การวิเคราะห์วงจรไฟฟ้าทาง คอมพิวเตอร์ 3(2-3-6) ณรงค์ชัย มุ่งแฝงกลาง คมกริช มาเที่ยง สัปดาห์ที่ 9 Reactive.
Copyright © 2009 Pearson Education, Inc. Chapter 32: Inductance, Electromagnetic Oscillations, and AC Circuits.
Electromagnetism Lecture#16-17 Instructor: Muhammad Mateen Yaqoob.
 In 1820 Danish science Hans Christian Oersted accidentally discovered that electric current produces a magnetic field.  He set up compasses around.
My Chapter 20 Lecture Outline.
Electro- magnetic Induction Lecture 3 AP Physics.
Chapter 20 Electromagnetic Induction. Electricity and magnetism Generators, motors, and transformers.
Electromagnetic Induction. Current can be created in a wire by a magnetic field British scientist Michael Faraday and American scientist Joseph Henry.
Chapter 28 Inductance; Magnetic Energy Storage. Self inductance 2 Magnetic flux Φ B ∝ current I Electric currentmagnetic fieldEMF (changing) Phenomenon.
Electromagnetism. Current-Carrying Wire As you know from last year… Whenever a current flows, it creates a magnetic field.
Ch 21 1 Chapter 21 Electromagnetic Induction Faraday’s Law AC Circuits © 2006, B.J. Lieb Some figures electronically reproduced by permission of Pearson.
Electromagnetism Lecture#8-11 Instructor: Engr. Muhammad Mateen Yaqoob.
1 ECE 3144 Lecture 26 Dr. Rose Q. Hu Electrical and Computer Engineering Department Mississippi State University.
Inductors ? circuit diagram symbol.
Electromagnetism Lecture#12-13 Instructor: Engr. Muhammad Mateen Yaqoob.
Electromagnetic Induction and Faraday’s Law.. Induced Current.
1 ENE 325 Electromagnetic Fields and Waves Lecture 9 Magnetic Boundary Conditions, Inductance and Mutual Inductance.
Electromagnetism.  A moving charge creates a magnetic field  Electric current (I) is moving electrons, so a current-carrying wire creates a magnetic.
Problem 4 A metal wire of mass m can slide without friction on two parallel, horizontal, conducting rails. The rails are connected by a generator which.
ENE 325 Electromagnetic Fields and Waves
Inductance Inductor A coil of wire wrapped around a supporting core (magnetic or non-magnetic) The time-varying current in the wire produces a time-varying.
Chapter 21: Electromagnetic Induction
14.1 Introduction Earlier we noted that capacitors store energy by producing an electric field within a piece of dielectric material Inductors also store.
Energy in Electrical Systems
Magnetism & Electricity.
Lecture 3-6 Self Inductance and Mutual Inductance
Electromagnetism.
Electricity and Magnetism
Electromagnetic Induction
Current flowing out Current flowing in 14-1
Last lecture Motional EMF
UNIT 2 Magnetic Circuits
Electromagnetic Induction and Faraday’s Law.
Inductance Inductor A coil of wire wrapped around a supporting core (magnetic or non-magnetic) The time-varying current in the wire produces a time-varying.
ElectroMagnetic Induction
Chapter 32 Problems 6,7,9,16,29,30,31,37.
Presentation transcript:

Electromagnetism Lecture#9 Instructor: Engr. Muhammad Mateen Yaqoob

Lenz’s Law The direction of the induced current is determined by Lenz’s law To illustrate how Lenz’s law works, let’s consider a conducting loop placed in a magnetic field. We follow the procedure below: MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Example#1: Field inside and outside a Current-carrying wire Consider a long straight wire of radius R carrying a current I of uniform current density, as shown in Figure. Find the magnetic field everywhere. MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Solution MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Inductor An inductor is a passive element designed to store energy in its magnetic field. Inductors find numerous applications in electronic and power systems. They are used in power supplies, transformers, radios, TVs, radars and electric motors. Any conductor of electric current has inductive properties and may be regarded as an inductor. But in order to enhance the inductive effect, a practical inductor is usually formed into a cylindrical coil with many turns of conducting wire. MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Inductor An inductor is made of a coil of conducting wire Inductors are formed with wire tightly wrapped around a solid central core MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Inductance Inductance (or electric inductance) is a measure of the amount of magnetic flux produced for a given electric current. The inductance has the following relationship: L= Φ/i where ◦L is the inductance in henrys, ◦i is the current in amperes, ◦Φ is the magnetic flux in webers MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

If current is allowed to pass through an inductor, it is found that the voltage across the inductor is directly proportional to the time rate of change of the current. Using the passive sign convention, where L is the constant of proportionality called the inductance of the inductor. The unit of inductance is the henry (H), named in honor of the American inventor Joseph Henry (1797–1878). MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

Flux in Inductors The relation between the flux in inductor and the current through the inductor is given below. i φ Linear Nonlinear MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

+ - v L where i(t 0 ) is the total current for −∞ < t < t 0 and i(−∞) = 0. The idea of making i(−∞) = 0 is practical and reasonable, because there must be a time in the past when there was no current in the inductor. MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE

The inductor is designed to store energy in its magnetic field The energy stored in an inductor + - v L MATEEN YAQOOB DEPARTMENT OF COMPUTER SCIENCE