Classical Electrodynamics

Similar documents
CHAPTER 2: Boundary-Value Problems in Electrostatics: I. Applications of Green s theorem

Eigenfunction Expansion. For a given function on the internal a x b the eigenfunction expansion of f(x):

Schrödinger Equation Via Laplace-Beltrami Operator

Using Quantum Mechanics in Simple Systems Chapter 15

Lecture 38 (Trapped Particles) Physics Spring 2018 Douglas Fields

PhysicsAndMathsTutor.com

MA6351-TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS SUBJECT NOTES. Department of Mathematics FATIMA MICHAEL COLLEGE OF ENGINEERING & TECHNOLOGY

Name of the Student:

Chem 253A. Crystal Structure. Chem 253B. Electronic Structure

is completely general whenever you have waves from two sources interfering. 2

Chem 253B. Crystal Structure. Chem 253C. Electronic Structure

Remarks: (a) The Dirac delta is the function zero on the domain R {0}.

3.1 Laplace s Equation 3.2 The Method of Images 3.3 Separation of Variables

A GENERAL METHOD FOR SOLVING ORDINARY DIFFERENTIAL EQUATIONS: THE FROBENIUS (OR SERIES) METHOD

Indices and Logarithms

SOLUTION OF DIFFERENTIAL EQUATION FOR THE EULER-BERNOULLI BEAM

The Reimann Integral is a formal limit definition of a definite integral

Assessment Center Elementary Algebra Study Guide for the ACCUPLACER (CPT)

CITY UNIVERSITY LONDON

[Q. Booklet Number]

Notes 17 Sturm-Liouville Theory

Topic 4 Fourier Series. Today

[5 points] (c) Find the charge enclosed by the cylindrical surface of radius ρ 0 = 9 mm and length L = 1 m. [2

Physics 241 Exam 1 February 19, 2004

ALGEBRA. Set of Equations. have no solution 1 b1. Dependent system has infinitely many solutions

Interpolation. 1. What is interpolation?

Chapter 10 Partial Differential Equations and Fourier Series

The evaluation of P, and T from these formulae indeed requires that the energy E be expressed as a function of the quantities N, V and S.

Particle in a Box. and the state function is. In this case, the Hermitian operator. The b.c. restrict us to 0 x a. x A sin for 0 x a, and 0 otherwise

0 otherwise. sin( nx)sin( kx) 0 otherwise. cos( nx) sin( kx) dx 0 for all integers n, k.

( ) dx ; f ( x ) is height and Δx is

Westchester Community College Elementary Algebra Study Guide for the ACCUPLACER

Numerical Solutions of Fredholm Integral Equations Using Bernstein Polynomials

Exercises and Problems

Add Maths Formulae List: Form 4 (Update 18/9/08)

PhysicsAndMathsTutor.com

sin m a d F m d F m h F dy a dy a D h m h m, D a D a c1cosh c3cos 0

PhysicsAndMathsTutor.com

Theorem 5.3 (Continued) The Fundamental Theorem of Calculus, Part 2: ab,, then. f x dx F x F b F a. a a. f x dx= f x x

Presentation for use with the textbook, Algorithm Design and Applications, by M. T. Goodrich and R. Tamassia, Wiley, Divide-and-Conquer

Frequency-domain Characteristics of Discrete-time LTI Systems

Postulates of quantum mechanics

Auto-correlation. Window Selection: Hamming. Hamming Filtered Power Spectrum. White Noise Auto-Covariance vs. Hamming Filtered Noise

Strauss PDEs 2e: Section Exercise 4 Page 1 of 5. u tt = c 2 u xx ru t for 0 < x < l u = 0 at both ends u(x, 0) = φ(x) u t (x, 0) = ψ(x),

Linear Programming. Preliminaries

Capacitance Computation of a Charge Conducting Plate using Method of Moments

Crushed Notes on MATH132: Calculus

Matsubara-Green s Functions

Second Mean Value Theorem for Integrals By Ng Tze Beng. The Second Mean Value Theorem for Integrals (SMVT) Statement of the Theorem

(1) Functions A relationship between two variables that assigns to each element in the domain exactly one element in the range.

Digital Signal Processing, Fall 2006

8.1 Arc Length. What is the length of a curve? How can we approximate it? We could do it following the pattern we ve used before

Handout #2. Introduction to Matrix: Matrix operations & Geometric meaning

( ) 2 3 ( ) I. Order of operations II. Scientific Notation. Simplify. Write answers in scientific notation. III.

Supplemental Handout #1. Orthogonal Functions & Expansions

National Quali cations SPECIMEN ONLY

Sharjah Institute of Technology

Important Facts You Need To Know/Review:

Discrete Mathematics I Tutorial 12

Convergence rates of approximate sums of Riemann integrals

Student Success Center Elementary Algebra Study Guide for the ACCUPLACER (CPT)

Simpson s 1/3 rd Rule of Integration

lecture 24: Gaussian quadrature rules: fundamentals

Accuplacer Elementary Algebra Study Guide

Mathematical Notation Math Calculus & Analytic Geometry I

FOURIER SERIES PART I: DEFINITIONS AND EXAMPLES. To a 2π-periodic function f(x) we will associate a trigonometric series. a n cos(nx) + b n sin(nx),

Trapezoidal Rule of Integration

ENGINEERING PROBABILITY AND STATISTICS

t=a z=t z=a INTEGRAL EQUATIONS t=z z=x dz D.C. Sharma z=a z=a z t=z z=x t=a M.C. Goyal z=a

Mathematics Last Minutes Review

Fourier Series. Topic 4 Fourier Series. sin. sin. Fourier Series. Fourier Series. Fourier Series. sin. b n. a n. sin

Lecture 2: Matrix Algebra

Synopsis Grade 12 Math Part II

General properties of definite integrals

Lecture 4 Recursive Algorithm Analysis. Merge Sort Solving Recurrences The Master Theorem

An Analytic Potential Solution for Incompressible 2D Channel Inviscid Flow with Wall Injection

Homework Assignment 3 Solution Set

Lecture 2. Rational Exponents and Radicals. 36 y. b can be expressed using the. Rational Exponent, thus b. b can be expressed using the

Fig. 1. I a. V ag I c. I n. V cg. Z n Z Y. I b. V bg

MTH213 Calculus. Trigonometry: Unit Circle ( ) ( ) ( )

Taylor Polynomials. The Tangent Line. (a, f (a)) and has the same slope as the curve y = f (x) at that point. It is the best

Elementary Linear Algebra

Inner Product Spaces (Chapter 5)

Problem 1. Solution: a) The coordinate of a point on the disc is given by r r cos,sin,0. The potential at P is then given by. r z 2 rcos 2 rsin 2

BRAIN TEASURES INDEFINITE INTEGRATION+DEFINITE INTEGRATION EXERCISE I

Things I Should Know In Calculus Class

2.1.1 Definition The Z-transform of a sequence x [n] is simply defined as (2.1) X re x k re x k r

Chapter 10: The Z-Transform Adapted from: Lecture notes from MIT, Binghamton University Dr. Hamid R. Rabiee Fall 2013

An application of a subset S of C onto another S' defines a function [f(z)] of the complex variable z.

Mathacle. PSet Stats, Concepts In Statistics Level Number Name: Date:

Quantum Mechanics I. 21 April, x=0. , α = A + B = C. ik 1 A ik 1 B = αc.

Surface profiles with zero and finite adhesion force and adhesion instabilities

Vectors. Vectors in Plane ( 2

Qn Suggested Solution Marking Scheme 1 y. G1 Shape with at least 2 [2]


National Quali cations AHEXEMPLAR PAPER ONLY

ON THE EIGENFUNCTION EXPANSION METHOD FOR THE CALCULATION OF GREEN S FUNCTIONS

Mth 95 Notes Module 1 Spring Section 4.1- Solving Systems of Linear Equations in Two Variables by Graphing, Substitution, and Elimination

ON THE EIGENFUNCTION EXPANSION METHOD FOR THE CALCULATION OF GREEN S FUNCTIONS

Trapezoidal Rule of Integration

Transcription:

A First Look t Qutum Phsics Clssicl Electrodmics Chpter Boudr-Vlue Prolems i Electrosttics: I 11 Clssicl Electrodmics Prof. Y. F. Che

Cotets A First Look t Qutum Phsics.1 Poit Chrge i the Presece of Grouded Coductig Sphere Imge Chrge Method. Poit Chrge i the Presece of Chrged, Isulted, Coductig Sphere.3 Solve Poisso Equtio with Sphericl Boudr.4 Gree Fuctio of Two-Dimesiol (D) Rectgulr Sstem 11 Clssicl Electrodmics Prof. Y. F. Che

.1 Poit Chrge i the Presece of Grouded Coductig Sphere Imge Chrge Method ˆ p q ˆ q q : imge chrge : imge positio 1 q q 4 1 q q cos 4 cos 1 q q 4 cos cos q q 1 11 Clssicl Electrodmics Prof. Y. F. Che

.1 Poit Chrge i the Presece of Grouded Coductig Sphere Imge Chrge Method (1) Potetil t 1 q 4 cos q cos () iduced chrge desit o the surfce of the sphere cos q cos 3 3 4 cos cos q 4 cos 3 11 Clssicl Electrodmics Prof. Y. F. Che

.1 Poit Chrge i the Presece of Grouded Coductig Sphere Imge Chrge Method (3) totl iduced chrge tot q d d S 3 4 cos Assume q is o the z-is, u q 1 d sidd S 3 4 cos cos q 1 q 1 1 d dud 3 S 1 4 u u u1 u1 q q 11 Clssicl Electrodmics Prof. Y. F. Che

(4) totl force ctig o the surfce q cos 3 cos F cosd d 3 Assume q is o the z-is, q cos 3 cos F si d d 3 q u 3 u F dud 3 q u du 3 16 u u1 q u 1 1 1 du 16 4 u 4 u u1 q 4 4 16 4 8 q 1 q 4 1 1 1 1 1 1 11 Clssicl Electrodmics Prof. Y. F. Che

q q p ˆ ˆ Q q Use the cocept of lier superpositio 1 4 q q Q q 1 4 q Q q q () Electric force ctig o the chrge is 1 4 ˆ q Q q q F q (1) Potetil t 11 Clssicl Electrodmics Prof. Y. F. Che. Poit Chrge i the Presece of Chrged, Isulted, Coductig Sphere

.3 Solve Poisso Equtio with Sphericl Boudr ˆ p ˆ mes of Gree fuctio (1) How to oti Gree fuctio? GD,, S, 4 o S G D with Aove Equtios re equivlet, i.e. G D,,, q 4 Hece, we c oti Gree fuctio from eq. (1) G D q o S 1 1 cos cos 11 Clssicl Electrodmics Prof. Y. F. Che with

() Geerl solutio of the potetil i terms of Gree fuctio,, P ˆ ˆ P ẑ P P ŷ 1 4 S G D, ˆ d cos GD, GD, 1 cos 1 cos cos 3 3 cos 3 1,, d 3 4 S cos cos coscos sisicos 11 Clssicl Electrodmics Prof. Y. F. Che

.4 Gree Fuctio of Two-Dimesiol (D) Rectgulr Sstem Oe Dimesiol Helmholtz Equtio d d k with Geerl solutio: AsikBcos k B k Asi fuctios d 1 re orthoorml fuctios which c e used to epd ritrr f C Epsio of Delt fuctio: C A C si si 11 Clssicl Electrodmics Prof. Y. F. Che

(1) Gree fuctio: Eigefuctio epsio method m m,, si si km, m,, m km,, G, ;, 4 D m GD, ;, Fm, m,, Fm, si si m, m, let m m m,, m,, si si si si m, m, G, ;, GD, ;, m 4 Fm, m,, m D Fm, m,, 4 m,, m,, m, m, 16 1 m m GD, ;, si si si si m m 11 Clssicl Electrodmics Prof. Y. F. Che

() Solutio of Lplce Equtio i D Rectgulr Sstem Lplce Equtio:, V, let X Y 1 d 1 d, X d Y d Geerl solutio V V V V m X si, m 1, m Y Am sih, Am si sih m1 m m 11 Clssicl Electrodmics Prof. Y. F. Che

Appl oudr coditio for, m m, V Am si sih m1 Multipl si i oth side d itegrte m m m V si d A si si sih d A sih m m m m1 1 V m Am V si d 1 1 m m m sih sih Fill, we oti 4V 1 1 m m, si sih modd m m sih Specil cses if the sih e e 4V 1 1 m, si e m modd m e m 11 Clssicl Electrodmics Prof. Y. F. Che

(3) Gree Fuctio: Divisio of regio method V V, V t : ΙΙ Ι V, ;, 4 G D regio Ι : regio ΙΙ : G, ;, G, ;, Ι Accordig to the geerl solutio i the previous ΙΙ 3 m m m GΙ, ;, Am si si sih m m m m GΙΙ, ;, Bm si si sih m m m Amsih Bmsih We c oti the geerl solutio m m m m G, ;, Fm si si sih sih m Sustitute eq. (4) ito eq. (3) d itegrte m d m m Fm sih sih 8 m d 4 5 11 Clssicl Electrodmics Prof. Y. F. Che

Upper limit: d m m m m m Fm sih sih Fm sih cosh d lower limit: d m m m m m Fm sih sih Fm cosh sih d 6 7 Sustitute eq. (6) d eq. (7) ito eq. (5) m m m m m 8 Fm sih cosh cosh sih F m 8 m msih Fill, we oti 8 m m m m G, ;, si si sih sih m m msih mi, where m, 8 11 Clssicl Electrodmics Prof. Y. F. Che

(4) Gree fuctio i eq. () d eq. (8) re equivlet 16 1 m m G, ;, si si si si m m eq. (): D 8 m m m m m msih eq. (8): G, ;, si si sih sih m m m si si sih sih m m m sih 11 Clssicl Electrodmics Prof. Y. F. Che