This preview has intentionally blurred sections. Sign up to view the full version.View Full Document
Unformatted text preview: Physics 498/MMA Handout 10 Fall 2007 Mathematical Methods in Physics I http://w3.physics.uiuc.edu/ ∼ m-stone5 Prof. M. Stone 2117 ESB University of Illinois 1) Dielectric Sphere : Consider a solid dielectric sphere of radius a and permittivity . The sphere is placed in a electric field which is takes the constant value E = E ˆ z a long distance from the sphere. Recall that Maxwell’s equations require that D ⊥ and E k be continuous across the surface of the sphere. a) Use the expansions Φ in = X l A l r l P l (cos θ ) Φ out = X l ( B l r l + C l r- l- 1 ) P l (cos θ ) and find all non-zero coefficents A l , B l , C l . b) Show that the E field inside the sphere is uniform and of magnitude 3 +2 E . c) Show that the electric field is unchanged if the dielectric is replaced by the polarization- induced surface charge density σ induced = 3- + 2 E cos θ. (Some systems of units may require extra 4 π ’s in this last expression. In SI units D ≡ E = E + P , and the polarization induced charge density is ρ induced =-∇ · P ) 2) Hollow Sphere : The potential on a spherical surface of radius a is Φ( θ, φ ). We want to express the potential inside the sphere as an integral over the surface in a manner analagous to the Poisson kernel in two dimensions. a) By using the generating function for Legendre polynomials, show that 1- r 2 (1 + r 2- 2 r cos θ ) 3 / 2 = ∞ X l =0 (2 l + 1) r l P l (cos θ ) , r < 1 b) Starting from the expansion...
View Full Document
- Fall '07
- Neutron, Magnetic Field, fast breeder reactor, cos cos, Sir Michael Berry