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§7.2 Maxwell Equations the wave equation

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1 §7.2 Maxwell Equations the wave equation
Christopher Crawford PHY 311

2 Final Exam Based on 5 formulations of electromagnetism
Derivative chain – gauge, potentials, fields, sources Structure of and relations between different formulations Field calculation methods organized around formulations Cumulative – uniform weighting through whole semester Will be 50% longer than midterm exams Similar problems as midterms Essay question – structure of EM fields / media Proof – relation between formulations Integration – Coulomb / Biot-Savart / Potential Integral – Gauss / Ampère [or modified versions] Boundary value problem – see examples Components – capacitor, resistor, inductor

3 Outline Review – electromagnetic potential & displacement current propagate electromagnetic waves Capacitive ‘tension’ vs. inductive ‘inertia’ Unification of E and B – filling in the cracks Derivative chain – different representations of fields Wave equation and solution – Green’s fn. and eigenfn’s

4 Electromagnetic Waves
Sloshing back and forth between electric and magnetic energy Interplay: Faraday’s EMF  Maxwell’s displacement current Displacement current (like a spring) – converts E into B EMF induction (like a mass) – converts B into E Two material constants  two wave properties

5 Review: Two separate formulations
ELECTROSTATICS Coulomb’s law MAGNETOSTATICS Ampère’s law E+B: Faraday’s law; b) rho + J: conservation of charge; c) space + time

6 Review: One unified formulation
ELECTROMAGNETISM Faraday’s law stitches the two formulations together in space and time Previous hint: continuity equation

7 Unification of E and B Projections of electromagnetic field in space and time That is the reason for the twisted symmetry in field equations

8 Unification of D and H Summary

9 Wave equation: potentials

10 Wave equation: gauge

11 Wave equation: fields

12 Wave equation: summary
d’Alembert operator (4-d version of Laplacian)

13 Homogenous solution Separate time variable to obtain Helmholtz equation General solution for wave Boundary Value Problems

14 Particular solution Green’s function of d’Alembertian
Wikipedia: Green’s functions


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