释义 |
Helmholtz Differential Equation--Circular Cylindrical CoordinatesIn Cylindrical Coordinates, the Scale Factors are , , and the separation functions are , , , so the Stäckel Determinant is 1. Attempt Separation of Variables by writing
 | (1) |
then the Helmholtz Differential Equation becomes
 | (2) |
Now divide by ,
 | (3) |
so the equation has been separated. Since the solution must be periodic in from the definition of the circularcylindrical coordinate system, the solution to the second part of (3) must have a Negative separation constant
 | (4) |
which has a solution
 | (5) |
Plugging (5) back into (3) gives
 | (6) |
 | (7) |
The solution to the second part of (7) must not be sinusoidal at for a physical solution, so thedifferential equation has a Positive separation constant
 | (8) |
and the solution is
 | (9) |
Plugging (9) back into (7) and multiplying through by yields
 | (10) |
 | (11) |
 | (12) |
This is the Bessel Differential Equation, which has a solution
 | (13) |
where and are Bessel Functions of the First andSecond Kinds, respectively. The general solution is therefore | |  | (14) |
Actually, the Helmholtz Differential Equation is separable for general of the form
 | (15) |
See also Cylindrical Coordinates, Helmholtz Differential Equation References
Morse, P. M. and Feshbach, H. Methods of Theoretical Physics, Part I. New York: McGraw-Hill, pp. 514 and 656-657, 1953. |