CH6 Static Magnetic Field

Slides:



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

Electromagnetic Induction Inductors. Problem A metal rod of length L and mass m is free to slide, without friction, on two parallel metal tracks. The.
Chapter 30 Sources of the magnetic field
Induction and Inductance Induction Faraday’s Law of Induction Lenz’s Law Energy Transfer Induced Electric Fields Inductance and Self Inductance RL Circuits.
Magnetic Circuits and Transformers
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.
Magnetostatics Magnetostatics is the branch of electromagnetics dealing with the effects of electric charges in steady motion (i.e, steady current or DC).
EEE340Lecture : Magnetic Circuits Analysis of magnetic circuits is based on Or where V m =NI is called a magnetomotive force (mmf) Also Or (6.83)
Sources of Magnetic Field Chapter 28 Study the magnetic field generated by a moving charge Consider magnetic field of a current-carrying conductor Examine.
Copyright © 2009 Pearson Education, Inc. Lecture 9 – Electromagnetic Induction.
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 14.1 Inductance and Magnetic Fields  Introduction  Electromagnetism  Reluctance.
AP Physics C Chapter 28.  s1/MovingCharge/MovingCharge.html s1/MovingCharge/MovingCharge.html.
Sources of Magnetic Field
UNIVERSITI MALAYSIA PERLIS
Physics 121: Electricity & Magnetism – Lecture 11 Induction I Dale E. Gary Wenda Cao NJIT Physics Department.
1 EEE 498/598 Overview of Electrical Engineering Lecture 8: Magnetostatics: Mutual And Self-inductance; Magnetic Fields In Material Media; Magnetostatic.
MAGNETOSTATIC FIELD (STEADY MAGNETIC)
Lecture 9 Vector Magnetic Potential Biot Savart Law
Chapter 7 Electrodynamics
Sources of the Magnetic Field
Chapter 20 The Production and Properties of Magnetic Fields.
Nov PHYS , Dr. Andrew Brandt PHYS 1444 – Section 003 Lecture #20, Review Part 2 Tues. November Dr. Andrew Brandt HW28 solution.
Chapter 2 Electromagnetism Dr. Mohd Junaidi Abdul Aziz
Introduction to Electromechanical Energy Conversion
Magnetism 1. 2 Magnetic fields can be caused in three different ways 1. A moving electrical charge such as a wire with current flowing in it 2. By electrons.
Chapter 5 Overview. Electric vs Magnetic Comparison.
Chung-Ang University Field & Wave Electromagnetics CH 6. Static Magnetic Fields.
5. Magnetostatics Applied EM by Ulaby, Michielssen and Ravaioli.
Fundamentals of Electromagnetics and Electromechanics
ELECTROMAGNETIC THEORY EKT 241/4: ELECTROMAGNETIC THEORY PREPARED BY: NORDIANA MOHAMAD SAAID CHAPTER 4 – MAGNETOSTATICS.
Lecture 8 MAGNETOSTATICS Magnetic Fields Fundamental Postulates of Magnetostatics in Free Space Prof. Viviana Vladutescu.
MAGNETOSTATIK Ampere’s Law Of Force; Magnetic Flux Density; Lorentz Force; Biot-savart Law; Applications Of Ampere’s Law In Integral Form; Vector Magnetic.
ENE 325 Electromagnetic Fields and Waves
Fundamental Physics II PETROVIETNAM UNIVERSITY FACULTY OF FUNDAMENTAL SCIENCES Vungtau, 2013 Pham Hong Quang
Electricity and magnetism
ELECTRICAL ENGINEERING: PRINCIPLES AND APPLICATIONS, Fourth Edition, by Allan R. Hambley, ©2008 Pearson Education, Inc. Lecture 21 Magnetic Circuits, Materials.
EKT241 - Electromagnetic Theory
CHAPTER 2 MAGNETIC MATERIALS AND CIRCUITS
EKT241 - Electromagnetic Theory Chapter 3 - Electrostatics.
22.7 Source of magnetic field due to current
1 MAGNETOSTATIC FIELD (MAGNETIC FORCE, MAGNETIC MATERIAL AND INDUCTANCE) CHAPTER FORCE ON A MOVING POINT CHARGE 8.2 FORCE ON A FILAMENTARY CURRENT.
Chapter 26 Sources of Magnetic Field. Biot-Savart Law (P 614 ) 2 Magnetic equivalent to C’s law by Biot & Savart . P. P Magnetic field due to an infinitesimal.
1 Engineering Electromagnetics Essentials Chapter 4 Basic concepts of static magnetic fields.
Magnetic Fields. Magnetic Fields and Forces a single magnetic pole has never been isolated magnetic poles are always found in pairs Earth itself is a.
Lecture 28: Currents and Magnetic Field: I
Biot-Savart Law Biot-Savart law: The constant  o is called the permeability of free space  o = 4  x T. m / A.
UNIVERSITI MALAYSIA PERLIS
5. Magnetostatics Applied EM by Ulaby, Michielssen and Ravaioli.
1 ENE 325 Electromagnetic Fields and Waves Lecture 9 Magnetic Boundary Conditions, Inductance and Mutual Inductance.
BASIC ELECTRICAL TECHNOLOGY Chapter 4 – Magnetic Circuits
ENE 325 Electromagnetic Fields and Waves
EMLAB 1 Chapter 9. Magnetic forces, materials, and inductance.
Magnetics.
ELECTRICAL MACHINES Electrical Machines.
UPB / ETTI O.DROSU Electrical Engineering 2
BASIC ELECTRICAL TECHNOLOGY Chapter 4 – Magnetic Circuits
Fundamentals of Applied Electromagnetics
EET 423 POWER ELECTRONICS -2
UNIVERSITI MALAYSIA PERLIS
Chapter 3 Magnetostatics
Overview of Electrical Engineering
Electromagnetic Theory
Magnetic Circuits.
ENE 325 Electromagnetic Fields and Waves
Magnetostatics.
UNIT 2 Magnetic Circuits
EET141 Electric Circuit II MAGNETIC CIRCUIT -Part 2-
E&M I Griffiths Chapter 7.
ENE/EIE 325 Electromagnetic Fields and Waves
5. Magnetostatics 7e Applied EM by Ulaby and Ravaioli.
Presentation transcript:

CH6 Static Magnetic Field

Electric force Magnetic force Elecmagnetic fore (N) ~ Lorentz’s force equation

Free space Static Electric Field Static Magnetic Field Steady current Permeability of free space

No magnetic flow sources Magnetic flux lines always close Low of conservation of magnetic flux Each magnets has a north south Magnetic poles cannot be isolated pole

Ampere’s circuital law summary

EX 6-1 Inside conductor Outside conductor C2 outside conductor encloses I

If b 空心圓柱(柱座標)

EX 6-2 (Toroidal Coil) A circular contour C with radius r (b - a) < r < (b + a) (b - a) < r < (b + a) (No source)

EX 6-3 (Solenoid Coil) (a) Direct application of Ampere Law (b) Special case of torid Ex 6-2,

6-3 Vector Magnetic Potential : magnetic potential [Vector] c.f : electric potential [Scalar] 取 Vector Poisson’s equation Coulomb gauge

In Cartesian coordinates, Vector

Magnetic Flux through a given area S which is bounded by contour C

6-4 Biot-Savart Law and applications Vector source Magnetic: 3-dim Volume current density 2-dim Surface current density 1-dim current 0-dim Current distribution Current element

Biot-Savart Law:[Valid in steady current] c.f. 因次分析

Biot-Sarvart Law: Action at a distance: field

Gauss thm. 特殊式 Biot-Sarvart Law Poission Eqe. Stoke Thm. Ampere’s Law

PF: =0 =0 N 封閉磁迴路 S C.F 孤立電單極

From 其中

From Steady current Static magnetic field 其中: Coulomb Gauge Steady state Coulomb Gauge

其中: Ampere’ Law Poission Equ.

Gauss Thm.

Example 6-4 (a)

Example 6-5 From 6-4

Example 6-6 is canceled due to cylindrical sym.

6-5 Magnetic Dipole 20 pole = 0 2’ pole = 0

c.f.

c.f.

Scalar Magnetic Potential (not physical) : Non conservative (path dependent)

6-6 Magnetization and Equivalent Current Density free electron Conductor polarized ion Non-conductor source Components 磁性物質 定義

c.f.

EX : 6-8

靜磁學 (包含導體與磁性材料) C.F.

Static Magnetic Source : Conductor : Magnetic material : (permeativity) Conductor : Magnetic material : Copy 電學 數學上等效,無物理

Ex 6-9 電場 與(Dipole 類似)

6-7 Ampere’s circuital law ; relative permeability

6-8 Magnetic Circuits Electric circuit : Voltage / Current source ; V, I, … Magnetic circuit : Transformer / Generator / Motor … ; closed path c to enclose N turns of I (m.m.f) magnetomotive force [Amp]

Ex 6-10 Sol : is identical in different material ; f : ferromagnetic g : gap Ampere law

Magnetic Flux ; S : cross-section : length of ferromagnetic core. :ferromagnetic core :air gap : Reluctance Analog to : [Electric circuit]

Magnetic circuit Electric circuit mmf mag. flux reluctance Permeability emf electric current , resistance , conductivity ,

An exact analysis of magnetic circuits is difficult ◎Leakage Fluxes ◎Fringing effect ◎ 2 conditions must be satisfied Similar to Kirchhoff’s voltage Law Kirchhoff’s current Law

EX.6-11 K.V.L. (Time Independent) Loop1: Loop2:

6-9 Behavior of Magnetic Materials ◎Diamagetic: ◎Paramagnetic: ◎Ferromagnetic:

6-10 Boundary Conditions for Magnetostatic Field

Ex 6-12 Bn component component or Similar to E-field Magnitude of In ferromagnetic parallel interface Originates in a ferromangeitc , Flux perpendicular to interface

Ex 6-13 Surface current Example 6-8 [p246] Center End at interface quantity

6-11 Inductances & Inductors Mutual flux : mutual inductance between loops C1 and C2 If loop C2 has N2 turns , Generalizes to

Some of produced by I1 links only with C1 loop itself, not with C2 Self inductance of C1 loop Procedure for Finding Inductance 1. Appropriate coordinate system 4. 2. Find 5. 3.

EX 6-14 flux linkage total current

EX 6-15 Long solenoid From(Ex6-3) p231 Inductance per unit length

EX 6-16 Current in annular ring a) Inside inner conductor. b) Between inner & outer conductors

EX 6-17 Internal total 2 wires : external :

Neumann Formula

EX:6-18 Outer coil has N2 turns,

EX:6-19 Find B2 is caused by long wire I2.

6-12 Magnetic Energy Loop 1 Similary Total work at C2 Loop 2 : C1 & C2 Generalizing I1, I2, I3, … IN,

Consider Kth loop of N coupled loops Magnetic energy Total magnetic energy

6-12.1 Wm in terms of Field Quantities 其中 All space Vector identity

Magnetic energy density Wm or c.f.

Ex 6-20 (Ref. Ex 6-16) Wm in inner conductor Wm between inner & outer Hence,

6-13 Magnetic forces & Torques electron move toward to x-dir. Creating a transverse -field. Steady state, net force is Zero.

S.W.(OFF) S.W.(ON) system s.w.

Two coils

Home Work #6 P6-2, P6-4, P6-5, P6-6, P6-10,P6-11,P6-12 David Cheng: Chapter6 P6-2, P6-4, P6-5, P6-6, P6-10,P6-11,P6-12 P6-13,P6-15,P6-18,P6-19,P6-22,P6-26, P6-27,P6-29,P6-32,P6-37,P6-38,P6-39, P6-40,P6-41,P6-42,P6-43,P6-44,P6-46, P6-50,P6-53 Due: 2 weeks