Prof. David R. Jackson ECE Dept. Fall 2014 Notes 32 ECE 2317 Applied Electricity and Magnetism 1.

Slides:



Advertisements
Similar presentations
CHAPTER 5: TRANSFORMER AND MUTUAL INDUCTANCE
Advertisements

Copyright ©2011, ©2008, ©2005 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electric Circuits, Ninth Edition James.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 9 ECE 2317 Applied Electricity and Magnetism 1.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 18 ECE 2317 Applied Electricity and Magnetism 1.
Lecture 111 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
ECE 201 Circuit Theory I1 Determining Dot Markings.
ECE 201 Circuit Theory 11 Mutual Inductance in Terms of Self - Inductance L1L1 L2L2.
ECE 201 Circuit Theory 11 Energy Calculations for Mutually – Coupled Coils.
ECE 201 Circuit Theory 11 The Concept of Mutual Inductance.
Mutual Inductance Consider two circuits “linked” by a magnetic field (magnetically-coupled coils). ECE 201 Circuit Theory I.
AHBMH DEE2113 : Chapter 5 - Transformer & Mutual Inductance 1 CHAPTER 5: TRANSFORMER AND MUTUAL INDUCTANCE Review of Magnetic Induction Mutual Inductance.
Prof. David R. Jackson Dept. of ECE Fall 2013 Notes 29 ECE 6340 Intermediate EM Waves 1.
Applied Electricity and Magnetism
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 31 ECE 2317 Applied Electricity and Magnetism 1.
Magnetically coupled circuits
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 25 ECE 2317 Applied Electricity and Magnetism 1.
A device that can hold or store a reasonable amount of electric charge It is made of two parallel plates separated by insulator( dielectric) or air It.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 27 ECE 2317 Applied Electricity and Magnetism 1.
Fall 2014 Notes 23 ECE 2317 Applied Electricity and Magnetism Prof. David R. Jackson ECE Dept. 1.
Coupling Element and Coupled circuits Coupled inductor Ideal transformer Controlled sources.
Notes 8 ECE Microwave Engineering Waveguides Part 5:
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 7 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM Group University of Houston 1.
Fall 2013 Notes 2 ECE 6340 Intermediate EM Waves Prof. David R. Jackson Dept. of ECE 1.
ELECTRIC CURRENT 2 Ohm’s law shows the relationship between current, potential, and voltage. We need a few more rules to make predictions about current.
Electric Machinery 王嘉帷 MA
Chapter 13 Magnetically Coupled Circuits
Magnetically Coupled Networks
Prof. Jeffery T. Williams Dept. of Electrical & Computer Engineering University of Houston Fall 2004 Current ECE 2317: Applied Electricity and Magnetism.
MAGNETICALLY COUPLED CIRCUIT
Fundamentals of Electric Circuits Chapter 13 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 15 ECE 2317 Applied Electricity and Magnetism 1.
Prof. D. Wilton ECE Dept. Notes 16 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
Prof. D. Wilton ECE Dept. Notes 27 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
Prof. D. Wilton ECE Dept. Notes 24 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
Prof. D. Wilton ECE Dept. Notes 9 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 3 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM Group University of Houston 1.
Syllabus Resistor Inductor Capacitor Voltage and Current Sources
Engineering Science EAB_S_127 Electricity Chapter 2.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 11 ECE 2317 Applied Electricity and Magnetism 1.
Circuits II EE221 Unit 10 Instructor: Kevin D. Donohue Magnetically Coupled Circuits, Linear Transformers, Transformer Circuits.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 17 ECE 2317 Applied Electricity and Magnetism 1.
16.6 Parallel and Series Circuits. Possible Paths We are now going to look at the different paths that you can set up for electrons Depending on the path.
Circuits Which of the equations is valid for the circuit shown below? 2 – I 1 – 2I 2 = 0 A) 2 – I 1 – 2I 2 = 0 2 – 2I 1 – 2I 2 – 4I 3 = 0 B) 2 – 2I 1 –
MAGNETIC CIRCUITS Electrical current flowing along a wire creates a magnetic field around the wire, as shown in Fig. That magnetic field can be visualized.
LECTURE 23 Pick up lecture notes Pick up lecture notes Reading for next lecture: Start chapter 31: read complete reading & homework assignment.
1 ELECTRICAL TECHNOLOGY EET 103/4 Define and analyze the principle of transformer, its parameters and structure. Describe and analyze Ideal transformer,
1 ELECTRICAL TECHNOLOGY EET 103/4 Define and analyze the principle of transformer, its parameters and structure. Describe and analyze Ideal transformer,
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 10 ECE 3318 Applied Electricity and Magnetism 1.
Prof. David R. Jackson ECE Dept. Spring 2015 Notes 28 ECE 2317 Applied Electricity and Magnetism 1.
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 14 ECE 3318 Applied Electricity and Magnetism 1.
Prof. David R. Jackson ECE Dept. Spring 2015 Notes 33 ECE 2317 Applied Electricity and Magnetism 1.
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 17 ECE 3318 Applied Electricity and Magnetism 1.
Prof. David R. Jackson Dept. of ECE Fall 2015 Notes 29 ECE 6340 Intermediate EM Waves 1.
Chapter 30: Induction and Inductance This chapter covers the following topics: -Faraday’s law of induction -Lenz’s Law -Electric field induced by a changing.
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 33 ECE 3318 Applied Electricity and Magnetism 1.
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 42 ECE 6341 Notes 44 1.
1 ELECTRICAL TECHNOLOGY ERT 105/3 Define and analyze the principle of transformer, its parameters and structure. Describe and analyze Ideal transformer,
Applied Electricity and Magnetism
MAGNETICALLY COUPLED CIRCUIT
Applied Electricity and Magnetism
Applied Electricity and Magnetism
Circuits II EE221 Unit 9 Instructor: Kevin D. Donohue
Circuits II EE221 Unit 9 Instructor: Kevin D. Donohue
MAGNETICALLY COUPLED CIRCUIT
Lecture 09 - Inductors and Capacitors
UNIT 2 Magnetic Circuits
Mutual Inductance Consider two circuits “linked” by a magnetic field (magnetically-coupled coils). ECE 201 Circuit Theory I.
Notes 7 ECE 3318 Applied Electricity and Magnetism Coulomb’s Law I
L-11 ELECTROMAGNETISM ELE 1001: Basic Electrical Technology
MAGNETICALLY COUPLED CIRCUIT
Presentation transcript:

Prof. David R. Jackson ECE Dept. Fall 2014 Notes 32 ECE 2317 Applied Electricity and Magnetism 1

Mutual Inductance I1I1 I2I2 Current reference directions and unit normals are defined on both coils. Two coils are in proximity of each other. (The unit normals are each determined from the corresponding current reference directions, by the right-hand rule.) 2

Mutual Inductance (cont.) In general, if coil 2 has multiple turns: Coil 1 is energized Coil 2 is left open-circuited Define mutual inductance: (calculated when I 2 = 0 )  21 I1I1 Note: For the figure shown,  Hence M 21 < 0. 3

 12 I2I2 In general, if coil 1 has multiple turns, Define mutual inductance: Coil 2 is energized Coil 1 is left open-circuited Mutual Inductance (cont.) 4

A general property (proof omitted) is that both mutual inductance components are always equal: Mutual Inductance (cont.) 5

Circuit Law for Coupled Coils + - v1v1 i1i1 + - v2v2 i2i2 M L1L1 L2L2 Total flux through coil 1: Total flux through coil 2: 6

Example Find M 12, M 21 L s = length For M 12 : 7 R2R2 z R1R1 I2I2 I1I1 Bz2Bz2 R1R1 R2R2 x y

Example (cont.) For M 21 : 8 L s = length R2R2 z R1R1 I2I2 I1I1 Note: B z 1 = 0 for  > R 1. Bz1Bz1 R1R1 R1R1 R2R2 x y

Example (cont.) Summary 9 L s = length R2R2 z R1R1 I2I2 I1I1

Dot Convention 10 This allows us to use mutual inductance without having to visually inspect how the coils are wound. The dots tell us how the voltage on each coil is related to the current on the other coil. Note: We use passive sign convention on both coils. The dots tell us: (1) where the + sign is for the voltage drops (2) which currents to use for the M terms

Dot Convention (cont.) 11 Coil 1 Coil 2 M + - v1(t)v1(t) i2(t)i2(t) i1(t)i1(t) v2(t)v2(t) + - Here is one possible dot arrangement:

Dot Convention (cont.) 12 Here is another possible dot arrangement: Coil 1 Coil 2 M + - v1(t)v1(t) i2(t)i2(t) i1(t)i1(t) v2(t)v2(t) - +