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Christopher Crawford PHY

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1 Christopher Crawford PHY 417 2014-02-27
§7.2 Maxwell Equations Christopher Crawford PHY 417

2 Outline Review – TWO separate derivative chains (in space only)
ES and MS formulations: potentials and Poisson’s equation THREE observations: a) Coulomb, b) Ampere, c) Faraday the third ties the derivative chains of the other two together TWO+1 cracks in the foundation – patching up space and time Scalar potential, Maxwell’s displacement current Example: potential momentum associated with a B-field Example: the displacement current through a capacitor Materials: THREE+1 charges and SIX currents Maxwell Equations – unified symmetry in space and time Differential & integral fields, potentials, boundary cond’s Space-time symmetry – ONE complete derivative chain Duality rotations – magnetic monopoles revisited

3 Two separate formulations
ELECTROSTATICS Coulomb’s law MAGNETOSTATICS Ampère’s law

4 Two separate formulations
ELECTROSTATICS MAGNETOSTATICS Faraday’s law stitches the two formulations together in space and time

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

6 TWO cracks in the foundation
Faraday’s law appears to violate conservation of energy? Unified gauge transformation for V and A Continuity equation vs. Ampère’s law

7 Example: current through a capacitor
Which surface should one use for Ampère’s law? Maxwell’s displacement current Fluid mechanical model Elasticity of medium –> EM waves On Faraday's Lines of Force (1855) On Physical Lines of Force (1961) The Dynamical Theory of the Electromagnetic Field (1865)

8 Example 7.8: potential momentum
Charges moving in magnetic field Charges in abruptly changing magnetic field Magnetic field energy acts as “electromagnetic inertia”

9 Maxwell’s equations Integral & differential Potentials & wave eq.
Boundary conditions Constitution equations Continuity equation Lorentz Force Field energy

10 Electrical properties of materials
Same old THREE charges (plus one magnetic) Now: SIX currents, including displacement!

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

12 Unification of D and H Summary

13 Duality Rotation (ε,1/μ) tensor behaves like i : converts between flux and flow Compare (E,B) to (x,y) in the complex plane

14 Conservation of Energy
Similar to other fluxes x flows


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