ECE 3336 Introduction to Circuits & Electronics

Slides:



Advertisements
Similar presentations
Electrostatics, Circuits, and Magnetism 4/29/2008
Advertisements

Faradays Law of Induction A changing magnetic field induces an electric field. The induced electric field causes a current to flow in a conductor.
Chapter 11 Inductors.
CHAPTER 5: TRANSFORMER AND MUTUAL INDUCTANCE
Induction and Inductance Induction Faraday’s Law of Induction Lenz’s Law Energy Transfer Induced Electric Fields Inductance and Self Inductance RL Circuits.
Electricity and Magnetism Electromagnetic Induction Mr D. Patterson.
Electromagnetism Physics 100 Chapt 15 Michael Faraday.
Current carrying wires 1820 Hans Christian Oersted Hans Christian Ørsted.
AHBMH DEE2113 : Chapter 5 - Transformer & Mutual Inductance 1 CHAPTER 5: TRANSFORMER AND MUTUAL INDUCTANCE Review of Magnetic Induction Mutual Inductance.
1 Electronics Inductance Copyright © Texas Education Agency, All rights reserved.
Biot-Savart Law The Field Produced by a Straight Wire.
Basics in Magnetism Electromagnetism Force on a Current-Carrying Wire EM Induction Transformer Generators Electric Motors ELECTROMAGNETISM.
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 14.1 Inductance and Magnetic Fields  Introduction  Electromagnetism  Reluctance.
Inductors. Inductance Electrons in motion create electromagnetic fields – Recall from previous section that electrons in motion also create an electrostatic.
1 DC ELECTRICAL CIRCUITS INDUCTANCE. 2 DC ELECTRICAL CIRCUITS When current travels down a conductor it creates a magnetic field around the conductor,
Electromagnetic Induction
AP Physics C Montwood High School R. Casao
Magnetic Flux and Faraday’s Law of Induction. Questions 1.What is the name of the disturbance caused by electricity moving through matter? 2.How does.
1 ECE 3336 Introduction to Circuits & Electronics Lecture Set #7 Inductors and Capacitors Fall 2012, TUE&TH 5:30-7:00pm Dr. Wanda Wosik Notes developed.
Induction Consider a conductor moving in a magnetic field…. X X X X X.
Electromagnetic Induction
Chapter 20 Induced Voltages and Inductance. Faraday’s Experiment A primary coil is connected to a battery and a secondary coil is connected to an ammeter.
1. ____The polarity of an electromagnet can be determined using the second right-hand rule. 2. ____Current passing through a conductor is increased from.
Chapter 21 Electromagnetic Induction and Faraday’s Law.
1 ECE 3336 Introduction to Circuits & Electronics Note Set #7a Capacitors Fall 2012, TUE&TH 4:00-5:30pm Dr. Wanda Wosik.
ARRDEKTA INSTITUTE OF TECHNOLOGY GUIDED BY. GUIDED BY. Prof.Y.B.Vaghela. Prof.Y.B.Vaghela. Asst.prof in electrical Asst.prof in electrical Department Department.
Chapter 31 Faraday’s Law.
ELECTROMAGNETISM. ELECTROMAGNETISM ????? ELECTROMAGNETISM THE BRANCH OF PHYSICS THAT DEALS WITH THE RELATIONSHIP BETWEEN ELECTRICITY & MAGNETISM.
Chapter 20 Induced Voltages and Inductance. Faraday’s Experiment – Set Up A current can be produced by a changing magnetic field First shown in an experiment.
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.
1 Electromagnetic Induction We introduced motional emf and Faraday’s Law through these two examples: Today we will the discussion about Faraday’s Law of.
Induced Voltage and Inductance
Faraday’s Law and Induction
Electromagnetic Induction Any current or moving charge is surrounded by a magnetic field. Likewise any moving magnet or changing magnetic field creates.
Magnetic Flux and Faraday’s Law of Induction
Electromagnetic Induction AP Physics Chapter 21. Electromagnetic Induction 21.1 Induced EMF.
INDUCTANCE. When the current in a loop if wire changes with time, an emf is induced in the loop according to Faraday’s law. The self- induced emf is Ɛ.
Today Course overview and information 09/16/2010 © 2010 NTUST.
My Chapter 20 Lecture Outline.
Faraday’s Law and Inductance. Faraday’s Law A moving magnet can exert a force on a stationary charge. Faraday’s Law of Induction Induced emf is directly.
Electro- magnetic Induction Lecture 3 AP Physics.
Chapter 20 Electromagnetic Induction. Electricity and magnetism Generators, motors, and transformers.
Unit 5: Electromagnetism. Day 1: Faraday’s Law of Induction Objectives: Induced EMF Electromagnetic Induction Magnetic Flux Faraday’s law of Induction.
Electromagnetic Induction
Magnetic Induction. Key Points about Induction  If the current in the primary circuit is constant, then the current in the secondary circuit is zero.
Faraday’s Law.
©F.M. Rietti Electro Dynamics Fundamentals. ©F.M. Rietti LM-18 Computer Science SSI Embedded Systems I 2 Electro Dynamics (cont) Ohm Law (DC) –Ohm's law.
Chapter 21 Electromagnetic Induction and Faraday’s Law.
Electromagnetic Induction and Faraday’s Law. Induced EMF Almost 200 years ago, Faraday looked for evidence that a magnetic field would induce an electric.
L 29 Electricity and Magnetism [6]
Inductors ? circuit diagram symbol.
Magnets and Electromagnetism Chapter Outline 1.Magnets, magnetic poles, and magnetic force. 2.Magnetic effects of electric current. 3.Magnetic effects.
Chapter 21.  Electromagnetic induction is the process of generating a current by moving an electrical conductor relative to a magnetic field.  This.
Magnetism and Electromagnetic Induction PHYSICS 1-2 MR. CHUMBLEY CHAPTER 19: MAGNETISM CHAPTER 20: ELECTROMAGNETIC INDUCTION.
Electromagnetism.  A moving charge creates a magnetic field  Electric current (I) is moving electrons, so a current-carrying wire creates a magnetic.
 Electromagnetic Induction – The production of an emf (the energy per unit charge supplied by a source of electric current) in a conducting circuit by.
AP Physics C III.E – Electromagnetism. Motional EMF. Consider a conducting wire moving through a magnetic field.
Electromagnetic Induction and Faraday’s Law Chapter 21.
Chapter 21 Magnetic Induction and Chapter 22.9: Transformers.
14.1 Introduction Earlier we noted that capacitors store energy by producing an electric field within a piece of dielectric material Inductors also store.
Electromagnetism.
Section 2: Magnetic Induction
Moving conductor – eddy currents
Last lecture Motional EMF
Electric Currents from Magnetism
UNIT 2 Magnetic Circuits
Lecture 2 Electrical and Electronics Circuits. After you study, and apply ideas in this Lecture, you will: Understand differences among resistance, capacitance,
Presentation transcript:

ECE 3336 Introduction to Circuits & Electronics Note Set #7b Inductors Fall 2012, TUE&TH 4:00-5:30pm Dr. Wanda Wosik

Current Can Generate Magnetic Field From Amper law Hans Christian Oersted (1777-1851) r

Magnetic Field Generated by Current Loop Superposition of the magnetic fields from the loops creates a uniform B field in the coil = solenoid N S Solenoid http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/magfie.html#c1

Lorentz Force Law Moving Charges Rotate I towards B Wires carrying currents will experience forces http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/magfor.html#c2

Moving Charges and Magnetic Forces Wires w/ current placed in the magnet feel force moves Faraday’s Law of Induction + - Wire w/o current moved () in the magnet  Charges forced to move=current Voltage generate + -  http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/magint.html#c1

1. 2. 3. 4. http://hyperphysics.phy-astr.gsu.edu/hbase/electric/farlaw.html#c1

Faraday’s Law  Lenz’s Law Electromagnetic induction produces current in a conductor, which is being moved in the magnetic field. That creates a magnetic field in a coil opposing any change of original magnetic field  VOLTAGE Lenz’s Law Directions of Voltages N S N S S N S N http://hyperphysics.phy-astr.gsu.edu/hbase/electric/farlaw.html#c2

Inductors in Circuits  Emf applied Define INDUCTANCE L  So the Emf gives us voltage of an opposite sign than the applied voltage V(t) http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/indcur.html#c2 EXAMPLE http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/coilbulb.html#c1

Inductors Inductance is present in wires whenever ac currents flow and ac magnetic fields are produced. The ac current produces a voltage, which counteracts the changes of this current Fast changes of currents i.e. high frequency signals result in high opposing voltages; that leads to very low currents making the inductor to appear as an open circuit. The energy stored In magnetic fields has effects on voltage and current. We use the inductor component to model these effects. Chokes – used for high inductance i.e. it will block high frequency signals.

Transients in Inductors http://hyperphysics.phy-astr.gsu.edu/hbase/electric/indtra.html#c1

Polarities of Inductors  None Unlike reference polarities of current sources and voltages sources, there is no polarity to an inductor. Just like in resistors: there was no polarities, either. And as for resistor, the voltage and current directions follow the passive (or active) sign convention. Passive Sign Convention Active Sign Convention

Voltage vL≠0 only if iL=f(t) Ideal inductor does not have resistance Finding Currents in Inductors  Voltage vL≠0 only if iL=f(t) Ideal inductor does not have resistance s is dummy variable Initial conditions They do not produce voltage vL But the energy is stored

Current Change is Limited so is the Voltage  The current through an inductor cannot be changed instantaneously. This would make the voltage infinite - but large voltages can be produced. and

Energy in Inductors We can find the energy stored in the magnetic field associated with the inductor. Start with power  find energy. Integration limits: when the current is zero  no magnetic field  no energy stored So lower limit=0; The upper limits set by the value of current, iL. 

Series Inductors Equivalent Circuits Series inductors, L1 and L2… and Ln, can be replaced with an equivalent circuit with a single inductor LEQ iLEQ From KVL:  (∑Li is as for resistors)

Parallel Inductors Equivalent Circuits Parallel inductors, L1 and L2 …Ln, can be replaced with an equivalent circuit inductor LEQ + vL(t) - iL1\2(t) iLn(t) iL1(t) iLEQ(t)  LEQ Use KCL As for resistors ∑(1/Ri) 

Rules for Inductors Passive sign convention

Some Applications: Electric Motors AC operation DC operation http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/motdc.html#c1

Mutual Inductance (M) “M” describes how current in one coil induces the current/voltage in the second coil. This concept will be used in Transformers

Mutual Inductance and Transformers

Transformers Number of turns in primary and secondary coils important More on Transformers in Note Set #16