
Cylindrical coordinates are a generalization of two-dimensional polar coordinates to three dimensions by superposing a height
( ) axis. Unfortunately, there are a number
of different notations used for the other two coordinates. Either or is used to refer
to the radial coordinate and either or to the azimuthal
coordinates. Arfken (1985), for instance, uses , while
Beyer (1987) uses . In
this work, the notation is used.
The following table summarizes notational conventions used by a number of authors.
| (radial, azimuthal, vertical) | reference |  | this work, Beyer (1987, p. 212) | | (Rr,
Ttheta, Zz) | SetCoordinates[Cylindrical] in the Mathematica add-on package Calculus`VectorAnalysis`
(which can be loaded with the command <<Calculus`) |  | Arfken
(1985, p. 95) |  | Moon and Spencer (1988, p. 12) |  | Korn and
Korn (1968, p. 60) |  | Morse and Feshbach (1953) |
In terms of the Cartesian coordinates ,
where , ,
, and the inverse tangent must be suitably defined to take the correct
quadrant of into account.
In terms of , , and
Note that Morse and Feshbach (1953) define the cylindrical coordinates by
where and .
The metric elements of the cylindrical
coordinates are
so the scale factors are
The line element is
 |
(16)
|
and the volume element is
 |
(17)
|
The Jacobian is
 |
(18)
|
A Cartesian vector is given in cylindrical coordinates by
![r==[rcostheta; rsintheta; z].](CylindricalCoordinates_files/equation4.gif) |
(19)
|
To find the unit vectors,
Derivatives of unit vectors with
respect to the coordinates are
The gradient of a vector field in cylindrical coordinates is given by
 |
(32)
|
so the gradient components become
The Christoffel symbols of the second kind in the definition of Misner et al. (1973, p.
209) are given by
The Christoffel
symbols of the second kind in the definition of Arfken (1985) are given by
(Walton 1967; Arfken 1985, p. 164, Ex. 3.8.10; Moon and Spencer 1988, p. 12a).
The covariant derivatives
are then given by
 |
(48)
|
are
Cross products of the coordinate
axes are
The commutation coefficients
are given by
![c_(alphabeta)^mue^->_mu==[e^->_alpha,e^->_beta]==del _alphae^->_beta-del _betae^->_alpha,](CylindricalCoordinates_files/equation7.gif) |
(61)
|
But
![[r^^,r^^]==[theta^^,theta^^]==[phi^^,phi^^]==0,](CylindricalCoordinates_files/equation8.gif) |
(62)
|
so ,
where . Also
![[r^^,theta^^]==-[theta^^,r^^]==del _rtheta^^-del _thetar^^==0-1/rtheta^^==-1/rtheta^^,](CylindricalCoordinates_files/equation9.gif) |
(63)
|
so ,
. Finally,
![[r^^,phi^^]==[theta^^,phi^^]==0.](CylindricalCoordinates_files/equation10.gif) |
(64)
|
Summarizing,
Time derivatives of the vector are
Speed is given by
 |
(72)
|
Time derivatives of the unit vectors
are
The convective derivative
is
 |
(76)
|
To rewrite this, use the identity
 |
(77)
|
and set , to obtain
 |
(78)
|
so
 |
(79)
|
Then
 |
(80)
|
The curl in the above expression gives
 |
(81)
|
so
 |
(82)
|
We expect the gradient term to vanish since speed does not depend on position. Check this using the identity ,
 |
(83)
|
Examining this term by term,
so, as expected,
 |
(89)
|
We have already computed , so combining
all three pieces gives
The divergence is
or, in vector notation
 |
(96)
|
The curl is
The scalar Laplacian is
The vector Laplacian is
![del ^2v==[(partial^2v_r)/(partialr^2)+1/(r^2)(partial^2v_r)/(partialtheta^2)+(partial^2v_r)/(partialz^2)+1/r(partialv_r)/(partialr)-2/(r^2)(partialv_theta)/(partialtheta)-(v_r)/(r^2); (partial^2v_theta)/(partialr^2)+1/(r^2)(partial^2v_theta)/(partialtheta^2)+(partial^2v_theta)/(partialz^2)+1/r(partialv_theta)/(partialr)+2/(r^2)(partialv_r)/(partialtheta)-(v_theta)/(r^2); (partial^2v_z)/(partialr^2)+1/(r^2)(partial^2v_z)/(partialtheta^2)+(partial^2v_z)/(partialz^2)+1/r(partialv_z)/(partialr)].](CylindricalCoordinates_files/equation22.gif) |
(100)
|
The Helmholtz differential equation is separable in cylindrical coordinates and has Stäckel determinant (for , , ) or
(for Morse and Feshbach's , , and ).
Arfken, G. "Circular Cylindrical Coordinates." §2.4 in Mathematical Methods for Physicists, 3rd ed. Orlando, FL:
Academic Press, pp. 95-101, 1985.
Beyer, W. H. CRC Standard Mathematical Tables, 28th ed. Boca Raton,
FL: CRC Press, 1987.
Korn, G. A. and Korn, T. M. Mathematical Handbook for Scientists and Engineers. New
York: McGraw-Hill, 1968.
Misner, C. W.; Thorne, K. S.; and Wheeler, J. A. Gravitation. San Francisco: W. H. Freeman, 1973.
Moon, P. and Spencer, D. E. "Circular-Cylinder Coordinates ."
Table 1.02 in Field Theory Handbook, Including Coordinate Systems, Differential
Equations, and Their Solutions, 2nd ed. New York: Springer-Verlag, pp. 12-17,
1988.
Morse, P. M. and Feshbach, H. Methods of Theoretical Physics, Part I. New York: McGraw-Hill,
p. 657, 1953.
Walton, J. J. "Tensor Calculations on Computer: Appendix." Comm. ACM 10,
183-186, 1967.
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