§3.4. 1–3 Multipole expansion Christopher Crawford PHY 311 2014-02-28.

Slides:



Advertisements
Similar presentations
VEKTORANALYS Kursvecka 6 övningar. PROBLEM 1 SOLUTION A dipole is formed by two point sources with charge +c and -c Calculate the flux of the dipole.
Advertisements

EE3321 ELECTROMAGENTIC FIELD THEORY
EE3321 ELECTROMAGENTIC FIELD THEORY
Fundamentals of Applied Electromagnetics
Transitions. 2 Some questions... Rotational transitions  Are there any?  How intense are they?  What are the selection rules? Vibrational transitions.
Lecture 2eee3401 Chapter 2 Coordinate Systems 1)Cartesian (rectangular) 2)Circular cylindrical 3)Spherical 4)Others (elliptic cylindrical, conical,…) A.
3-6. Conductors in Static Electric Field
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.
1 Model 6:Electric potentials We will determine the distribution of electrical potential (V) in a structure. x y z x y V=0 V=To be specified Insulation.
PHY 042: Electricity and Magnetism Multipole expansion Prof. Hugo Beauchemin 1.
EM & Vector calculus #3 Physical Systems, Tuesday 30 Jan 2007, EJZ Vector Calculus 1.3: Integral Calculus Line, surface, volume integrals Fundamental theorems.
02/03/2014PHY 712 Spring Lecture 81 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 8: Start reading Chapter 4 Multipole moment.
Lecture 4: Boundary Value Problems
UNIVERSITI MALAYSIA PERLIS
Boundary-Value Problems in Other Coordinates CHAPTER 14.
§ Separation of spherical variables: zonal harmonics Christopher Crawford PHY
3. 3 Separation of Variables We seek a solution of the form Cartesian coordinatesCylindrical coordinates Spherical coordinates Not always possible! Usually.
Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration.
Intermolecular Forces:Electrostatics “Dielectrics Different classical electrostatic interactions.
Outline Magnetic dipole moment Magnetization Magnetic induction
EMLAB Chapter 4. Potential and energy 1. EMLAB 2 Solving procedure for EM problems Known charge distribution Coulomb’s law Known boundary condition Gauss’
§4.1–2 Polarization Christopher Crawford PHY
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility 1 Lecture 5  Magnetic Multipoles Magnetic Multipoles,
Electrostatic potential and energy fall EM lecture, week 2, 7. Oct
PHY 417G: Review Christopher Crawford
Methods of excitation: nuclear reactions
Finish EM Ch. 5: Magnetostatics Methods of Math
§ Separation of Cartesian variables: Orthogonal functions Christopher Crawford PHY
Wave Dispersion EM radiation Maxwell’s Equations 1.
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:
3.3 Separation of Variables 3.4 Multipole Expansion
Dielectric Ellipsoid Section 8. Dielectric sphere in a uniform external electric field Put the origin at the center of the sphere. Field that would exist.
Fourier resolution of electrostatic field LL2 section 51.
§1.4 Curvilinear coordinates Christopher Crawford PHY
Wave Equations: EM Waves. Electromagnetic waves for E field for B field.
§6.1–2 Magnetization Christopher Crawford PHY
Multipole Moments Section 41. Expand potential  in powers of 1/R 0.
Maxwell’s Equations are Lorentz Invariant
§1.6 Green’s functions; Helmholtz Theorem Christopher Crawford PHY
CALCULUS III CHAPTER 5: Orthogonal curvilinear coordinates
§4.1–2 Polarization Christopher Crawford PHY
§ Separation of spherical variables: zonal harmonics Christopher Crawford PHY
Christopher Crawford PHY
System of charges in an external field
4. Multipoles and Dielectrics 4A. Multipole Expansion Revisited
Christopher Crawford PHY
Dielectric Ellipsoid Section 8.
Christopher Crawford PHY
CSE245: Computer-Aided Circuit Simulation and Verification
Electromagnetics II.
Christopher Crawford PHY 416G: Introduction Christopher Crawford
ENE/EIE 325 Electromagnetic Fields and Waves
§5.3: Magnetic Multipole Expansion
Christopher Crawford PHY
§3.3.1 Separation of Cartesian variables: Orthogonal functions
Christopher Crawford PHY
§3.4.1–3 Multipole expansion
課程大綱 OUTLINE Double Integrals(二重積分) Triple Integrals(三重積分)
§7.2 Maxwell Equations the wave equation
Christopher Crawford PHY
Related OSE's.
Christopher Crawford PHY 311: Introduction Christopher Crawford
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 8:
Multipole Magnets from Maxwell’s Equations
Magnetic Multipoles, Magnet Design
15. Legendre Functions Legendre Polynomials Orthogonality
15. Legendre Functions Legendre Polynomials Orthogonality
Fundamentals of Applied Electromagnetics
Lecture 16 Gradient in Cartesian Coordinates
§3.3.1 Sturm-Liouville theorem: orthogonal eigenfunctions
Presentation transcript:

§3.4. 1–3 Multipole expansion Christopher Crawford PHY

Outline Review of boundary value problem General solution to Laplace equation Internal and external boundary conditions Orthogonal functions – extracting A n from f(x) Multipole expansion Binomial series – expansion of functions 2-pole expansion – dipole field (first term) General multipole expansion Calculation of multipoles Example: pure dipole spherical distribution of charge Lowest order multipoles Monopole – point charge (l=0, scalar) Dipole – two points (l=1, vector) Quadrupole – four points(l=2, tensor [matrix]) Octupole – eight points(l=3, tensor [cubic matrix]) 2

Review: separation of variables k 2 = curvature of wave –> 0 [Laplacian] 3

Polar waves – Legendre functions 4

General solutions to Laplace eq’n Cartesian coordinates – no general boundary conditions! Cylindrical coordinates – azimuthal continuity Spherical coordinates – azimuthal and polar continuity Boundary conditions – Internal: 2 conditions across boundary – External: 1 condition (flux or potential) on boundary Orthogonality – to extract components 5

Expansion of functions Closely related to functions as vectors (basis functions) 6

Expansion of 2-pole potential Electric dipole moment 7

General multipole expansion Brute force method – see HW 6 for simpler approach 8

Example: integration of multipole Pure spherical dipole distribution – will use in Chapter 4, 6 9

Monopole Point-charge equivalent of total charge in the distribution 10

Dipole “center of charge” of distribution – Significant when total charge is zero 11

Quadrupole 12