{[ promptMessage ]}

Bookmark it

{[ promptMessage ]}

jackson 3-9 solution

# jackson 3-9 solution - Physics 505 Homework Assignment#4...

This preview shows pages 1–3. Sign up to view the full content.

Physics 505 Fall 2005 Homework Assignment #4 — Solutions Textbook problems: Ch. 3: 3.4, 3.6, 3.9, 3.10 3.4 The surface of a hollow conducting sphere of inner radius a is divided into an even number of equal segments by a set of planes; their common line of intersection is the z axis and they are distributed uniformly in the angle φ . (The segments are like the skin on wedges of an apple, or the earth’s surface between successive meridians of longitude.) The segments are kept at fixed potentials ± V , alternately. a ) Set up a series representation for the potential inside the sphere for the general case of 2 n segments, and carry the calculation of the coefficients in the series far enough to determine exactly which coefficients are different from zero. For the nonvanishing terms, exhibit the coefficients as an integral over cos θ . The general spherical harmonic expansion for the potential inside a sphere of radius a is Φ( r, θ, φ ) = l,m α lm r a l Y lm ( θ, φ ) where α lm = V ( θ, φ ) Y * lm ( θ, φ ) d Ω In this problem, V ( θ, φ ) = ± V is independent of θ , but depends on the azimuthal angle φ . It can in fact be thought of as a square wave in φ 2 π V V - ϕ n =4 This has a familiar Fourier expansion V ( φ ) = 4 V π k =0 1 2 k + 1 sin[(2 k + 1) ] This is already enough to demonstrate that the m values in the spherical harmonic expansion can only take on the values ± (2 k +1) n . In terms of associated Legendre

This preview has intentionally blurred sections. Sign up to view the full version.

View Full Document
polynomials, the expansion coefficients are α lm = 2 l + 1 4 π ( l - m )! ( l + m )! 2 ± 0 V ( φ ) e - imφ 1 - 1 P m l ( x ) dx = 4 V π 2 l + 1 4 π ( l - m )! ( l + m )! k =0 1 2 k + 1 2 π 0 sin[(2 k + 1) ] e - imφ × 1 - 1 P m l ( x ) dx = - 4 iV 2 l + 1 4 π ( l - m )! ( l + m )! k =0 δ m, (2 k +1) n - δ m, - (2 k +1) n 2 k + 1 1 - 1 P m l ( x ) dx Using P - m l ( x ) = ( - ) m [( l - m )! / ( l + m )!] P m l ( x ), we may write the non-vanishing coefficients as α l, - (2 k +1) n = ( - ) n +1 α l, (2 k +1) n = - 4 iV 2 k + 1 2 l + 1 4 π ( l - (2 k + 1) n )! ( l + (2 k + 1) n )! 1 - 1 P (2 k +1) n l ( x ) dx (1) for k = 0 , 1 , 2 , . . . . Since l (2 k + 1) n , we see that the first non-vanishing term enters at order l = n . Making note of the parity of associated Legendre polyno- mials, P - l m ( - x ) = ( - ) l + m P m l ( x ), we see that the non-vanishing coefficients are given by the sequence α n,n , α n +2 ,n , α n +4 ,n , α n +6 ,n , . . .
This is the end of the preview. Sign up to access the rest of the document.

{[ snackBarMessage ]}

### Page1 / 7

jackson 3-9 solution - Physics 505 Homework Assignment#4...

This preview shows document pages 1 - 3. Sign up to view the full document.

View Full Document
Ask a homework question - tutors are online