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Prof. David R. Jackson ECE Dept.

ECE 6341 . Spring 2014. Prof. David R. Jackson ECE Dept. Notes 8. Cylindrical Wave Functions. Helmholtz equation:. Separation of variables:. let. Substitute into previous equation and divide by  . Cylindrical Wave Functions (cont.). Divide by . let.

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Prof. David R. Jackson ECE Dept.

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  1. ECE 6341 Spring 2014 Prof. David R. Jackson ECE Dept. Notes 8

  2. Cylindrical Wave Functions Helmholtz equation: Separation of variables: let Substitute into previous equation and divide by .

  3. Cylindrical Wave Functions (cont.) Divide by  let

  4. Cylindrical Wave Functions (cont.) (1) or Hence, f(z) =constant = - kz2

  5. Cylindrical Wave Functions (cont.) Hence Next, to isolate the  -dependent term, multiply Eq. (1) by 2:

  6. Cylindrical Wave Functions (cont.) Hence (2) Hence, so

  7. Cylindrical Wave Functions (cont.) From Eq. (2) we now have The next goal is to solve this equation for R(). First, multiply by R and collect terms:

  8. Cylindrical Wave Functions (cont.) Define Then, Next, define Note that and

  9. Cylindrical Wave Functions (cont.) Then we have Bessel equation of order  Two independent solutions: Hence Therefore

  10. Cylindrical Wave Functions (cont.) Summary

  11. References for Bessel Functions • M. R. Spiegel, Schaum’s Outline Mathematical Handbook, McGraw-Hill, 1968. • M. Abramowitz and I. E. Stegun, Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, National Bureau of Standards, Government Printing Office, Tenth Printing, 1972. • N. N. Lebedev, Special Functions & Their Applications, Dover Publications, New York, 1972.

  12. Properties of Bessel Functions n =0 n =1 n =2 Jn (x) x

  13. Bessel Functions (cont.) n =0 n =1 n =2 Yn (x) x

  14. Bessel Functions (cont.) Small-Argument Properties (x0): The order is arbitrary here, as long as it is not a negative integer. For order zero, the Bessel function of the second kind behaves as ln rather than algebraically.

  15. Bessel Functions (cont.) Non-Integer Order: Two linearly independent solutions Bessel equation is unchanged by Note: is a always a valid solution These are linearly independent when is not an integer.

  16. Bessel Functions (cont.) (This definition gives a “nice” asymptotic behavior as x .)

  17. Bessel Functions (cont.)  = n Integer Order: Symmetry property (They are no longer linearly independent.) In this case,

  18. Bessel Functions (cont.) Frobenius solution†:   - 1, -2, …   …- 2, -1, 0, 1, 2 … †Ferdinand Georg Frobenius (October 26, 1849 – August 3, 1917) was a German mathematician, best known for his contributions to the theory of differential equations and to group theory (Wikipedia).

  19. Bessel Functions (cont.) From the limiting definition, we have, as  n: (Schaum’s Outline Mathematical Handbook, Eq. (24.9)) where

  20. Bessel Functions (cont.) From the Frobenius solution and the symmetry property, we have that

  21. Bessel Functions (cont.) (To derive this, see the eqs. on slides 18 and 20.)

  22. Bessel Functions (cont.) Asymptotic Formulas

  23. Hankel Functions Incoming wave Outgoing wave These are valid for arbitrary order .

  24. Fields In Cylindrical Coordinates We expand the curls in cylindrical coordinates to get the following results.

  25. TMzFields TMz:

  26. TEzFields TEz:

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