Prof. D. Wilton ECE Dept. Notes 27 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.

Slides:



Advertisements
Similar presentations
Two questions: (1) How to find the force, F on the electric charge, Q excreted by the field E and/or B? (2) How fields E and/or B can be created?
Advertisements

Prof. D. Wilton ECE Dept. Notes 22 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston. (used by Dr. Jackson,
Magnetic Domains – Randomly Oriented ~ atoms in each domain.
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.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 18 ECE 2317 Applied Electricity and Magnetism 1.
ECE 201 Circuit Theory I1 Magnetic Field Permanent magnet –Electrons spinning about their own axis in a particular alignment Charges in motion –Electric.
ECE 201 Circuit Theory I1 Determining Dot Markings.
ECE 201 Circuit Theory 11 Mutual Inductance in Terms of Self - Inductance L1L1 L2L2.
The Electric and Magnetic fields Maxwell’s equations in free space References: Feynman, Lectures on Physics II Davis & Snyder, Vector Analysis.
ECE 201 Circuit Theory 11 The Concept of Mutual Inductance.
ECE 201 Circuit Theory I1 Physical Characteristics of Inductors.
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.
Electricity and Magnetism: Electromagnets Mr D. Patterson.
Applied Electricity and Magnetism
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 31 ECE 2317 Applied Electricity and Magnetism 1.
ConcepTest 29.1a Magnetic Field of a Wire I P If the currents in these wires have the same magnitude, but opposite directions, what is the direction.
Electromagnetic Induction Faraday’s Law. Induced Emf A magnet entering a wire causes current to move with in the wires I = Emf / R The induced current.
Electromagnetic Force
Chapter 5 Overview. Electric vs Magnetic Comparison.
Prof. D. Wilton ECE Dept. Notes 12 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM Group, University of Houston.
Fall 2014 Notes 23 ECE 2317 Applied Electricity and Magnetism Prof. David R. Jackson ECE Dept. 1.
Prof. D. Wilton ECE Dept. Notes 25 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
Physics of Magnetism PA STEM monthly meeting Lincoln HS, Philadelphia January 13, 2015.
Prof. D. Wilton ECE Dept. Notes 15 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
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.
Physics Magnetism 20.1 Magnets and magnetic fields 20.2 Electric currents produce magnetism 20.3 Force on current in magnetic field 20.4 Force.
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.
Notes 13 ECE 2317 Applied Electricity and Magnetism Prof. D. Wilton
Notes 11 ECE 2317 Applied Electricity and Magnetism Prof. D. Wilton
Magnetic Fields and Induced EMFs. Electromagnetic Induction  Just as a magnetic field can be formed by a current in a circuit, a current can be produced.
Quick Practice In what direction is the magnetic force on the wire?
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.
Chapter 20 Electromagnetic Induction. Electricity and magnetism Generators, motors, and transformers.
MAGNETICALLY COUPLED CIRCUIT
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 32 ECE 2317 Applied Electricity and Magnetism 1.
Chapter 28 Inductance; Magnetic Energy Storage. Self inductance 2 Magnetic flux Φ B ∝ current I Electric currentmagnetic fieldEMF (changing) Phenomenon.
Maxwell’s Equations Faraday Induction (Serway)
Prof. D. Wilton ECE Dept. Notes 16 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
Physics Sources of the Magnetic Field 30.1 Biot-Savart Law 30.2 Force between two parallel wires 30.3 Ampere’s Law 30.4 Magnetic Field (B) of.
Direction of Magnetic Field
Prof. D. Wilton ECE Dept. Notes 5 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.
Notes 2 ECE 2317 Applied Electricity and Magnetism Prof. D. Wilton
Circuits II EE221 Unit 10 Instructor: Kevin D. Donohue Magnetically Coupled Circuits, Linear Transformers, Transformer Circuits.
Prof. Jeffery T. Williams Dept. of Electrical & Computer Engineering University of Houston Fall 2004 Coulomb’s Law ECE 2317: Applied Electricity and Magnetism.
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.
5. Magnetostatics Applied EM by Ulaby, Michielssen and Ravaioli.
Prof. David R. Jackson ECE Dept. Spring 2015 Notes 33 ECE 2317 Applied Electricity and Magnetism 1.
MAGNETISM! Who doesn’t think magnets are cool?. MAGNETIC FIELD Understand the concept of a magnetic field – Is it like an electric field? – What produces.
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.
PHY 2049: Physics II Tutoring Center is open in room NPB 1215, M-F 12:00AM -4:00PM. It is free.
Applied Electricity and Magnetism
Induction and Inductance
Magnets and Electromagnetic Induction
Electromagnetism.
Circuits II EE221 Unit 9 Instructor: Kevin D. Donohue
Overview of Electrical Engineering
Electric Currents from Magnetism
6. Maxwell’s Equations In Time-Varying Fields
6. Maxwell’s Equations In Time-Varying Fields
Magnetic Field Permanent magnet Charges in motion
6. Maxwell’s Equations In Time-Varying Fields
Notes 7 ECE 3318 Applied Electricity and Magnetism Coulomb’s Law I
Magnetic Field Permanent magnet Charges in motion
Electric Currents from Magnetism
6. Maxwell’s Equations In Time-Varying Fields
5. Magnetostatics 7e Applied EM by Ulaby and Ravaioli.
Chapter 30 Induction and Inductance
Presentation transcript:

Prof. D. Wilton ECE Dept. Notes 27 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.

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

Mutual Inductance (cont.)  21 I1I1 In general, if coil 2 has multiple turns Coil 1 is energized. Coil 2 is left open-circuited Define mutual inductance:

 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.)

Property: Mutual Inductance (cont.)

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

Example Bz2Bz2 R1R1 Find M 12, M 21 L s = length R2R2 z R1R1 I2I2 I1I1

Example (cont.) Bz1Bz1 R1R1 R2R2 z R1R1 I2I2 I1I1

R2R2 z R1R1 I2I2 I1I1

Force on Wire charge: wire: q B v F B I dl F The contour C is in the direction of the reference direction for the current.

Example I2I2 I1I1 1 2 z h z = 0 z = L x Note: there is no self-force on wire 2 due to the magnetic field produced by the current on wire 2.

Example (cont.) F F