§5.2: Formulations of Magnetostatics

Slides:



Advertisements
Similar presentations
Magnetic Fields Due To Currents
Advertisements

Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Dr. Charles Patterson 2.48 Lloyd Building
PH0101 UNIT 2 LECTURE 2 Biot Savart law Ampere’s circuital law
MAXWELL’S EQUATIONS 1. 2 Maxwell’s Equations in differential form.
1 Electromagnetism We want to apply the reaction theory developed in the first few lectures to electronuclear interactions. It is worthwhile reviewing.
MAGNETOSTATICS ONLINE TEST Q.NO.ANSWER Q.NO.ANSWER Q.NO.ANSWER
Example: What is the magnetic field at the center of a circular arc of wire? 1 This will work for any current carrying arc, where  (in radians) is the.
Phy 213: General Physics III Chapter 29: Magnetic Fields to Currents Lecture Notes.
§5.2: Biot-Savart Law Christopher Crawford PHY
EM & Vector calculus #3 Physical Systems, Tuesday 30 Jan 2007, EJZ Vector Calculus 1.3: Integral Calculus Line, surface, volume integrals Fundamental theorems.
MAGNETOSTATIC FIELD (STEADY MAGNETIC)
Lecture 9 Vector Magnetic Potential Biot Savart Law
Christopher Crawford PHY
Chapter 5 Overview. Electric vs Magnetic Comparison.
Operators. 2 The Curl Operator This operator acts on a vector field to produce another vector field. Let be a vector field. Then the expression for the.
EEL 3472 Magnetostatics 1. If charges are moving with constant velocity, a static magnetic (or magnetostatic) field is produced. Thus, magnetostatic fields.
ENE 325 Electromagnetic Fields and Waves
Physics 202, Lecture 13 Today’s Topics Magnetic Forces: Hall Effect (Ch. 27.8) Sources of the Magnetic Field (Ch. 28) B field of infinite wire Force between.
Chapter 5 Magnetostatics 5.1 The Lorentz Force Law 5.2 The Biot-Savart Law 5.3 The Divergence and Curl of 5.4 Magnetic Vector Potential.
CHECKPOINT: What is the current direction in this loop
Physics 2102 Magnetic fields produced by currents Physics 2102 Gabriela González.
5.3 Divergence and Curl of B Ampere’s law differential form.
* Turn the compass needle so it is approximately parallel to the wire. * Close the switch to send the current through the wire for about 5-10 seconds.
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.
Christopher Crawford PHY 417G: Introduction Christopher Crawford
5. Magnetostatics Applied EM by Ulaby, Michielssen and Ravaioli.
§1.6 Green’s functions; Helmholtz Theorem Christopher Crawford PHY
SILVER OAK COLLEGE OF ENGG&TECH NAME:-KURALKAR PRATIK S. EN.NO: SUBJECT:- EEM GUIDED BY:- Ms. REENA PANCHAL THE STEADY STATE OF MAGNETIC.
Darryl Michael/GE CRD Fields and Waves Lesson 4.2 MAGNETOSTATICS.
Lecture 20 Dielectric-Conductor boundary Lecture 20 Conductor-Conductor boundary.
Magnetic Field Due To A Current Loop.
(i) Divergence Divergence, Curl and Gradient Operations
Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Comparison of Magnetostatics and Electrostatics
Magnetic Fields Due to Currents
§7.2 Maxwell Equations the wave equation
Magnetic Fields Due To A Moving Charged Particle.
Christopher Crawford PHY
Christopher Crawford PHY
Magnetic Fields due to Currents
Lecture 9 Magnetic Fields due to Currents Ch. 30
§1.5 Delta Function; Function Spaces
Christopher Crawford PHY
Christopher Crawford PHY 416G: Introduction Christopher Crawford
static magnetic fields
CHECKPOINT: What is the current direction in this loop
Exam 2 covers Ch , Lecture, Discussion, HW, Lab
Chapter 5 Magnetostatics
Lecture 19 Maxwell equations E: electric field intensity
Christopher Crawford PHY
Christopher Crawford PHY
Biot and savart law A small presentation.
The Steady State Magnetic Field
Christopher Crawford PHY
Christopher Crawford PHY
Christopher Crawford PHY
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 12:
Christopher Crawford PHY 311: Introduction Christopher Crawford
Magnetic Fields Due to Currents
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 11:
Magnetic Fields Due to Currents
Sources of Magnetic Fields
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 11:
5. Magnetostatics 7e Applied EM by Ulaby and Ravaioli.
The Steady State Magnetic Field
Stationary Magnetic field
Presentation transcript:

§5.2: Formulations of Magnetostatics Christopher Crawford PHY 417 2014-01-23

Outline Ampère’s law Pseudo-derivation / application – straight wire Example – current sheet septum Example – infinite solenoid 5 formulations of Magnetostatics Review – electrostatics FLUX FLOW Vector potential A Divergence and curl of B Integrals – flux and flow

Ampère’s law on a straight wire Andre Marie Ampère shows that parallel currents attract and antiparallel currents repel Integral field equation – Ampère’s law Differential field equation – also Ampère’s law

Example 5.8: current septum Similar to Ch. 2: plane charge

Example 5.9: infinite solenoid

5 Formulations of Magnetostatics Electrostatics Magnetostatics

Magnetic vector potential A Derivation A from Biot-Savart law Divergence of A

Div. and curl of B Divergence – Gauss-like law Curl – vector Poisson equation –> Ampère’s law