Cylindrical harmonics

In mathematics, the cylindrical harmonics are a set of linearly independent solutions to Laplace's differential equation, ${\displaystyle \nabla ^{2}V=0}$, expressed in cylindrical coordinates, ρ (radial coordinate), φ (polar angle), and z (height). Each function V_n(k) is the product of three terms, each depending on one coordinate alone. The ρ-dependent term is given by Bessel functions (which occasionally are also called cylindrical harmonics).

Definition

Each function ${\displaystyle V_{n}(k)}$ of this basis consists of the product of three functions:

${\displaystyle V_{n}(k;\rho ,\varphi ,z)=P_{n}(k,\rho )\Phi _{n}(\varphi )Z(k,z)\,}$

where ${\displaystyle (\rho ,\varphi ,z)}$ are the cylindrical coordinates, and n and k are constants which distinguish the members of the set from each other. As a result of the superposition principle applied to Laplace's equation, very general solutions to Laplace's equation can be obtained by linear combinations of these functions.

Since all of the surfaces of constant ρ, φ and z  are conicoid, Laplace's equation is separable in cylindrical coordinates. Using the technique of the separation of variables, a separated solution to Laplace's equation may be written:

${\displaystyle V=P(\rho )\,\Phi (\varphi )\,Z(z)}$

and Laplace's equation, divided by V, is written:

${\displaystyle {\frac {\ddot {P}}{P}}+{\frac {1}{\rho }}\,{\frac {\dot {P}}{P}}+{\frac {1}{\rho ^{2}}}\,{\frac {\ddot {\Phi }}{\Phi }}+{\frac {\ddot {Z}}{Z}}=0}$

The Z  part of the equation is a function of z alone, and must therefore be equal to a constant:

${\displaystyle {\frac {\ddot {Z}}{Z}}=k^{2}}$

where k  is, in general, a complex number. For a particular k, the Z(z) function has two linearly independent solutions. If k is real they are:

${\displaystyle Z(k,z)=\cosh(kz)\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,\sinh(kz)\,}$

or by their behavior at infinity:

${\displaystyle Z(k,z)=e^{kz}\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,e^{-kz}\,}$

If k is imaginary:

${\displaystyle Z(k,z)=\cos(|k|z)\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,\sin(|k|z)\,}$

or:

${\displaystyle Z(k,z)=e^{i|k|z}\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,e^{-i|k|z}\,}$

It can be seen that the Z(k,z) functions are the kernels of the Fourier transform or Laplace transform of the Z(z) function and so k may be a discrete variable for periodic boundary conditions, or it may be a continuous variable for non-periodic boundary conditions.

Substituting ${\displaystyle k^{2}}$ for ${\displaystyle {\ddot {Z}}/Z}$ , Laplace's equation may now be written:

${\displaystyle {\frac {\ddot {P}}{P}}+{\frac {1}{\rho }}\,{\frac {\dot {P}}{P}}+{\frac {1}{\rho ^{2}}}{\frac {\ddot {\Phi }}{\Phi }}+k^{2}=0}$

Multiplying by ${\displaystyle \rho ^{2}}$, we may now separate the P  and Φ functions and introduce another constant (n) to obtain:

${\displaystyle {\frac {\ddot {\Phi }}{\Phi }}=-n^{2}}$

${\displaystyle \rho ^{2}{\frac {\ddot {P}}{P}}+\rho {\frac {\dot {P}}{P}}+k^{2}\rho ^{2}=n^{2}}$

Since ${\displaystyle \varphi }$ is periodic, we may take n to be a non-negative integer and accordingly, the ${\displaystyle \Phi (\varphi )}$ the constants are subscripted. Real solutions for ${\displaystyle \Phi (\varphi )}$ are

${\displaystyle \Phi _{n}=\cos(n\varphi )\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,\sin(n\varphi )}$

or, equivalently:

${\displaystyle \Phi _{n}=e^{in\varphi }\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,e^{-in\varphi }}$

The differential equation for ${\displaystyle \rho }$ is a form of Bessel's equation.

If k is zero, but n is not, the solutions are:

${\displaystyle P_{n}(0,\rho )=\rho ^{n}\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,\rho ^{-n}\,}$

If both k and n are zero, the solutions are:

${\displaystyle P_{0}(0,\rho )=\ln \rho \,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,1\,}$

If k is a real number we may write a real solution as:

${\displaystyle P_{n}(k,\rho )=J_{n}(k\rho )\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,Y_{n}(k\rho )\,}$

where ${\displaystyle J_{n}(z)}$ and ${\displaystyle Y_{n}(z)}$ are ordinary Bessel functions.

If k  is an imaginary number, we may write a real solution as:

${\displaystyle P_{n}(k,\rho )=I_{n}(|k|\rho )\,\,\,\,\,\,\mathrm {or} \,\,\,\,\,\,K_{n}(|k|\rho )\,}$

where ${\displaystyle I_{n}(z)}$ and ${\displaystyle K_{n}(z)}$ are modified Bessel functions.

The cylindrical harmonics for (k,n) are now the product of these solutions and the general solution to Laplace's equation is given by a linear combination of these solutions:

${\displaystyle V(\rho ,\varphi ,z)=\sum _{n}\int dk\,\,A_{n}(k)P_{n}(k,\rho )\Phi _{n}(\varphi )Z(k,z)\,}$

where the ${\displaystyle A_{n}(k)}$ are constants with respect to the cylindrical coordinates and the limits of the summation and integration are determined by the boundary conditions of the problem. Note that the integral may be replaced by a sum for appropriate boundary conditions. The orthogonality of the ${\displaystyle J_{n}(x)}$ is often very useful when finding a solution to a particular problem. The ${\displaystyle \Phi _{n}(\varphi )}$ and ${\displaystyle Z(k,z)}$ functions are essentially Fourier or Laplace expansions, and form a set of orthogonal functions. When ${\displaystyle P_{n}(k\rho )}$ is simply ${\displaystyle J_{n}(k\rho )}$ , the orthogonality of ${\displaystyle J_{n}}$, along with the orthogonality relationships of ${\displaystyle \Phi _{n}(\varphi )}$ and ${\displaystyle Z(k,z)}$ allow the constants to be determined.[1]

If ${\displaystyle (x)_{k}}$ is the sequence of the positive zeros of ${\displaystyle J_{n}}$ then:

${\displaystyle \int _{0}^{1}J_{n}(x_{k}\rho )J_{n}(x_{k}'\rho )\rho \,d\rho ={\frac {1}{2}}J_{n+1}(x_{k})^{2}\delta _{kk'}}$[2]

In solving problems, the space may be divided into any number of pieces, as long as the values of the potential and its derivative match across a boundary which contains no sources.

Example: Point source inside a conducting cylindrical tube

As an example, consider the problem of determining the potential of a unit source located at ${\displaystyle (\rho _{0},\varphi _{0},z_{0})}$ inside a conducting cylindrical tube (e.g. an empty tin can) which is bounded above and below by the planes ${\displaystyle z=-L}$ and ${\displaystyle z=L}$ and on the sides by the cylinder ${\displaystyle \rho =a}$.[3] (In MKS units, we will assume ${\displaystyle q/4\pi \epsilon _{0}=1}$). Since the potential is bounded by the planes on the z axis, the Z(k,z) function can be taken to be periodic. Since the potential must be zero at the origin, we take the ${\displaystyle P_{n}(k\rho )}$ function to be the ordinary Bessel function ${\displaystyle J_{n}(k\rho )}$, and it must be chosen so that one of its zeroes lands on the bounding cylinder. For the measurement point below the source point on the z axis, the potential will be:

${\displaystyle V(\rho ,\varphi ,z)=\sum _{n=0}^{\infty }\sum _{r=0}^{\infty }\,A_{nr}J_{n}(k_{nr}\rho )\cos(n(\varphi -\varphi _{0}))\sinh(k_{nr}(L+z))\,\,\,\,\,z\leq z_{0}}$

where ${\displaystyle k_{nr}a}$ is the r-th zero of ${\displaystyle J_{n}(z)}$ and, from the orthogonality relationships for each of the functions:

${\displaystyle A_{nr}={\frac {4(2-\delta _{n0})}{a^{2}}}\,\,{\frac {\sinh k_{nr}(L-z_{0})}{\sinh 2k_{nr}L}}\,\,{\frac {J_{n}(k_{nr}\rho _{0})}{k_{nr}[J_{n+1}(k_{nr}a)]^{2}}}\,}$

Above the source point:

${\displaystyle V(\rho ,\varphi ,z)=\sum _{n=0}^{\infty }\sum _{r=0}^{\infty }\,A_{nr}J_{n}(k_{nr}\rho )\cos(n(\varphi -\varphi _{0}))\sinh(k_{nr}(L-z))\,\,\,\,\,z\geq z_{0}}$

${\displaystyle A_{nr}={\frac {4(2-\delta _{n0})}{a^{2}}}\,\,{\frac {\sinh k_{nr}(L+z_{0})}{\sinh 2k_{nr}L}}\,\,{\frac {J_{n}(k_{nr}\rho _{0})}{k_{nr}[J_{n+1}(k_{nr}a)]^{2}}}.\,}$

It is clear that when ${\displaystyle \rho =a}$ or ${\displaystyle |z|=L}$, the above function is zero. It can also be easily shown that the two functions match in value and in the value of their first derivatives at ${\displaystyle z=z_{0}}$.

Point source inside cylinder

Removing the plane ends (i.e. taking the limit as L approaches infinity) gives the field of the point source inside a conducting cylinder:

${\displaystyle V(\rho ,\varphi ,z)=\sum _{n=0}^{\infty }\sum _{r=0}^{\infty }\,A_{nr}J_{n}(k_{nr}\rho )\cos(n(\varphi -\varphi _{0}))e^{-k_{nr}|z-z_{0}|}}$

${\displaystyle A_{nr}={\frac {2(2-\delta _{n0})}{a^{2}}}\,\,{\frac {J_{n}(k_{nr}\rho _{0})}{k_{nr}[J_{n+1}(k_{nr}a)]^{2}}}.\,}$

Point source in open space

As the radius of the cylinder (a) approaches infinity, the sum over the zeroes of J_n(z) becomes an integral, and we have the field of a point source in infinite space:

${\displaystyle V(\rho ,\varphi ,z)={\frac {1}{R}}=\sum _{n=0}^{\infty }\int _{0}^{\infty }dk\,A_{n}(k)J_{n}(k\rho )\cos(n(\varphi -\varphi _{0}))e^{-k|z-z_{0}|}}$

${\displaystyle A_{n}(k)=(2-\delta _{n0})J_{n}(k\rho _{0})\,}$

and R is the distance from the point source to the measurement point:

${\displaystyle R={\sqrt {(z-z_{0})^{2}+\rho ^{2}+\rho _{0}^{2}-2\rho \rho _{0}\cos(\varphi -\varphi _{0})}}.\,}$

Point source in open space at origin

Finally, when the point source is at the origin, ${\displaystyle \rho _{0}=z_{0}=0}$

${\displaystyle V(\rho ,\varphi ,z)={\frac {1}{\sqrt {\rho ^{2}+z^{2}}}}=\int _{0}^{\infty }J_{0}(k\rho )e^{-k|z|}\,dk.}$

See also

• Spherical harmonics

Notes

1. Smythe 1968, p. 185.
2. Guillopé 2010.
3. Configuration and variables as in Smythe 1968

References

• Smythe, William R. (1968). Static and Dynamic Electricity (3rd ed.). McGraw-Hill.CS1 maint: ref=harv (link)
• Guillopé, Laurent (2010). "Espaces de Hilbert et fonctions spéciales" (PDF) (in French).CS1 maint: ref=harv (link)