This preview shows pages 1–2. Sign up to view the full content.
This preview has intentionally blurred sections. Sign up to view the full version.View Full Document
Unformatted text preview: Electromagnetic Theory I Problem Set 6 Due: 3 October 2011 21.a) Use the power series definition of the Bessel function J m ( x ) X k =0 (- ) k k !( k + 1 + m ) x 2 2 k + m (1) to derive the recursion formulas for Bessel functions: J m- 1 ( x ) + J m +1 ( x ) = 2 m x J m ( x ) , J m- 1 ( x )- J m +1 ( x ) = 2 dJ m ( x ) dx (2) b) Explain why these same recursion formulas are valid for N m , H (1) m , H (2) m . c) Using the definitions I m ( x ) = i- m J m ( ix ) , K m ( x ) = i m +1 2 H (1) m ( ix ) (3) obtain the analogous recursion formulas for I m , K m . d)Use the power series defintion of J m , and the fact that ( z ) when z a nonpositive integer, to prove that J- m ( x ) = (- ) m J m ( x ) when m is an integer. 22. In class, we obtained the empty space Green function in cylindrical coordiantes in the form 1 4 | x- x | = 1 4 X m =- Z dkJ | m | ( k ) J | m | ( k ) e im ( - ) e- k | z- z | (4) a) By adjusting the z dependent factors in this formula obtain the Dirichlet Green function...
View Full Document
This note was uploaded on 09/25/2011 for the course PHY 6346 taught by Professor Staff during the Spring '08 term at University of Florida.
- Spring '08