| 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 
 then the Helmholtz Differential Equation becomes|  | (1) | 
 Now divide by|  | (2) | 
 , 
 so the equation has been separated.  Since the solution must be periodic in|  | (3) | 
 from the definition of the circularcylindrical coordinate system, the solution to the second part of (3) must have a Negative separation constant 
 which has a solution|  | (4) | 
 Plugging (5) back into (3) gives|  | (5) | 
 |  | (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 
 and the solution is|  | (8) | 
 Plugging (9) back into (7) and multiplying through by|  | (9) | 
 yields 
 |  | (10) | 
 |  | (11) | 
 This is the Bessel Differential Equation, which has a solution|  | (12) | 
 where|  | (13) | 
 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 
 See also Cylindrical Coordinates, Helmholtz Differential Equation|  | (15) | 
References
 Morse, P. M. and Feshbach, H.  Methods of Theoretical Physics, Part I.  New York:  McGraw-Hill, pp. 514 and 656-657, 1953. |