EM & Vector calculus #5 Physical Systems, Tuesday 27 Feb. 2007, EJZ Vector Calculus 1.6: Theory of vector fields Quick homework Q&A thanks to David for.

Slides:



Advertisements
Similar presentations
Differential Calculus (revisited):
Advertisements

VECTOR CALCULUS 1.10 GRADIENT OF A SCALAR 1.11 DIVERGENCE OF A VECTOR
EEE 340Lecture Curl of a vector It is an axial vector whose magnitude is the maximum circulation of per unit area as the area tends to zero and.
Electricity and Magnetism
Hw: All Chapter 3 problems and exercises Reading: Chapter 4.
Mat-F March 14, 2005 Vector Calculus, Åke Nordlund Niels Obers, Sigfus Johnsen Kristoffer Hauskov Andersen Peter Browne Rønne.
Introduction to Physical Systems Dr. E.J. Zita, The Evergreen State College, 30.Sept.02 Lab II Rm 2272, Program syllabus,
Mat-F March 16, 2005 Curvi-linear Coordinates, Åke Nordlund Niels Obers, Sigfus Johnsen Kristoffer Hauskov Andersen Peter Browne Rønne.
Lecture 12: 2nd-order Vector Operators Lecture 11 meaningless Laplace’s Equation is one of the most important in physics.
Chapter 1 Vector analysis
EM & Vector calculus #4 Physical Systems, Tuesday 13 Feb. 2007, EJZ Vector Calculus 1.4: Curvilinear Coordinates Quick review of quiz and homework Review.
1.1 Vector Algebra 1.2 Differential Calculus 1.3 Integral Calculus 1.4 Curvilinear Coordinate 1.5 The Dirac Delta Function 1.6 The Theory of Vector Fields.
EM & Vector calculus #3 Physical Systems, Tuesday 30 Jan 2007, EJZ Vector Calculus 1.3: Integral Calculus Line, surface, volume integrals Fundamental theorems.
Introduction to Physical Systems Dr. E.J. Zita, The Evergreen State College, 30.Sept.02 Lab II Rm 2272, Program syllabus,
EM & Vector calculus #2 Physical Systems, Tuesday 23 Jan 2007, EJZ Vector Calculus 1.2: Differential Calculus Ordinary derivatives Div, Grad, and Curl.
Lecture 18 Today Curl of a vector filed 1.Circulation 2.Definition of Curl operator in Cartesian Coordinate 3.Vector identities involving the curl.
PHY 042: Electricity and Magnetism
Chapter 9 向量分析 (Vector Analysis)
Methods of Math. Physics Dr. E.J. Zita, The Evergreen State College, 6 Jan.2011 Lab II Rm 2272, Winter wk 1 Thursday: Electromagnetism.
Notes 1 ECE 6340 Intermediate EM Waves Fall 2013
Chapter 10 Vector Calculus
PHYSICS-II (PHY C132) ELECTRICITY & MAGNETISM
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.
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.
Electricity and Magnetism (I) 電磁學 (I). WeekDateContentRemark 19/16-17 Chapter 1 The Electromagnetic Model Chapter 2 Vector Analysis 29/23-24 Unit Test.
Wednesday, Feb. 28, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #9 Wednesday, Feb. 28, 2007 Dr. Jae Yu 1.Quantum Electro-dynamics (QED) 2.Local.
§1.2 Differential Calculus
Electrostatic potential and energy fall EM lecture, week 2, 7. Oct
Methods of Math. Physics Dr. E.J. Zita, The Evergreen State College Lab II Rm 2272, Winter wk 3, Thursday 20 Jan Electrostatics.
Copyright © 2011 Pearson Education, Inc. Publishing as Pearson Addison-Wesley Chapter 14 Vector Calculus.
Finish EM Ch. 5: Magnetostatics Methods of Math
Tuesday Sept 21st: Vector Calculus Derivatives of a scalar field: gradient, directional derivative, Laplacian Derivatives of a vector field: divergence,
Chapter 1 Vector Analysis Gradient 梯度, Divergence 散度, Rotation, Helmholtz’s Theory 1. Directional Derivative 方向导数 & Gradient 2. Flux 通量 & Divergence 3.
Do you like math? How about Vector and Calculus?
Finish EM Ch.5: Magnetostatics Methods of Math. Physics, Thus. 10 March 2011, E.J. Zita Lorentz Force Ampere’s Law Maxwell’s equations (d/dt=0) Preview:
Saturday Sept 19th: Vector Calculus Vector derivatives of a scalar field: gradient, directional derivative, Laplacian Vector derivatives of a vector field:
§1.6 Green’s functions; Helmholtz Theorem Christopher Crawford PHY
CALCULUS III CHAPTER 5: Orthogonal curvilinear coordinates
Finding electrostatic potential Griffiths Ch.3: Special Techniques week 3 fall EM lecture, 14.Oct.2002, Zita, TESC Review electrostatics: E, V, boundary.
Spring 2016 Notes 1 ECE 6341 Prof. David R. Jackson ECE Dept. 1.
Vector Fields Def. A vector field is a function F that assigns to every point in the xy-plane a two-dimensional vector F(x,y). F(x,y) = P(x,y)i + Q(x,y)j.
Kankeshwaridevi Institute of Tech. Name of Students:rajput rahulsinh Enrollment no : Subject Code : Name Of Subject : Engineering Electromagnetics.
Del Operator 1. Symbolic notation: the del operator To have a compact notation, wide use is made of the symbolic operator “del” (some call it “nabla”):
Chapter 6 Vector Analysis
ECE 305 Electromagnetic Theory
Integration in Vector Fields
Comparison of Magnetostatics and Electrostatics
Force as gradient of potential energy
Christopher Crawford PHY
1.4 Curvilinear Coordinates Cylindrical coordinates:
Christopher Crawford PHY 416G: Introduction Christopher Crawford
Chapter 5 Magnetostatics
§5.2: Formulations of Magnetostatics
§3.4.1–3 Multipole expansion
Math 265 Created by Educational Technology Network
Find the curl of the vector field. {image}
Chapter 6 Vector Analysis
Electricity and Magnetism
MAXWELL’S EQUATIONS (TIME VARYING FIELDS) ONLINE TEST Q.NO. ANSWER 1 2
Christopher Crawford PHY
Quantum mechanics I Fall 2012
Christopher Crawford PHY
Christopher Crawford PHY 311: Introduction Christopher Crawford
Electricity and Magnetism I
Physics 451/551 Theoretical Mechanics
Review Chapter 1-8 in Jackson
Electricity and Magnetism
Electricity and Magnetism
Notes 24 ECE 6340 Intermediate EM Waves Fall 2016
Presentation transcript:

EM & Vector calculus #5 Physical Systems, Tuesday 27 Feb. 2007, EJZ Vector Calculus 1.6: Theory of vector fields Quick homework Q&A thanks to David for Dirac Delta during jury duty last week Helmholtz Theorem and Potentials E&M Ch.5.3-4: finishing Magnetostatics Quick homework Q&A Review, Div and curl of B Magnetostatic BC Magnetic vector potential Multipole expansion of vector potential?

Vector calculus HW Online solutions at Ch.1.4 (Curvilinear coordinates): VC4.pdf Ch.1.5 (Dirac Delta): VCdd.pdf Lecture notes at

Vector Fields: Helmholtz Theorem For some vector field F, if the divergence = D =   F, and the curl = C =  F, 0 then (a) what do you know about   C ? and (b) Can you find F? (a)   C = 0, because   (  F)  0 (b) Can find F iff we have boundary conditions, and require field to vanish at infinity. Helmholtz: Vector field is uniquely determined by its div and curl (with BC)

Vector Fields: Potentials.1 For some vector field F = -  V, find  F: (hint: look at identities inside front cover)  F = 0  F = -  V Curl-free fields can be written as the gradient of a scalar potential (physically, these are conservative fields, e.g. gravity or electrostatic).

Theorem 1 – examples The second part of each question illustrates Theorem 2, which follows…

Vector Fields: Potentials.2 For some vector field F =  A, find   F :   F = 0  F =  A Divergence-free fields can be written as the curl of a vector potential (physically, these have closed field lines, e.g. magnetic).

Optional – Proof of Thm.2

Practice with vector field theorems

E&M Ch.5b: Magnetostatics Quick homework Q&A Review, Div and curl of B Magnetic vector potential Magnetostatic BC Multipole expansion of vector potential

Magnetostatic BC

Magnetic vector potential

Multipole expansion

Background: vector area

Magnetic Dipole