Laplace equation in cylindrical coordinates

1 Laplace Equation in Cylindrical Coordinates

Solutions to the Laplace equation in cylindrical coordinates have wide applicability from fluid mechanics to electrostatics. Applying the method of separation of variables to Laplace’s partial differential equation and then enumerating the various forms of solutions will lay down a foundation for solving problems in this coordinate system. Finally, the use of Bessel functions in the solution reminds us why they are synonymous with the cylindrical domain.

1.1 Separation of Variables

Beginning with the Laplacian in Cylindrical Coordinates, apply the operator to a potential function and set it equal to zero to get the Laplace equation

( ) 2 1-∂Φ- ∂-Φ -1 ∂2Φ- ∂2Φ- ∇ Φ = r ∂r r ∂r + r2 ∂𝜃2 + ∂z2 = 0.

(1)

First expand out the terms

2 2 2 ∇2 Φ = 1-∂Φ-+ ∂-Φ-+ 1-∂-Φ- + ∂-Φ- = 0. r ∂r ∂r2 r2∂ 𝜃2 ∂z2

(2)

Then apply the method of separation of variables by assuming the solution is in the form

Φ (r,𝜃,z) = R (r)P (ϕ )Z(z).

Plug this into (2) and note how we can bring out the functions that are not affected by the derivatives

P (ϕ)Z (z)∂R (r) ∂2R (r) R (r)Z (z )∂2P (ϕ) ∂2Z(z) ---------------- + P (ϕ )Z(z)-----2- + -----2--------2---+ R (r)P(ϕ) ----2--= 0. r ∂r ∂r r ∂𝜃 ∂z

Divide by R(r)P(ϕ)Z(z) and use short hand notation to get

1 ∂R 1 ∂2R 1 ∂2P 1∂2Z -------+ ----2-+ ---2---2 + -----2 = 0. Rr ∂r R ∂r P r ∂ 𝜃 Z dz

“Separating” the z term to the other side gives

1 dR 1 d2R 1 d2P 1d2Z --- ---+ -----2 + ---2---2 = − -----2 . Rr dr R dr P r d 𝜃 Z dz

This equation can only be satisfied for all values if both sides are equal to a constant, λ, such that

-1 d2Z- − Z dz2 = λ

(3)

1 dR 1d2R 1 d2P ------ + -----2 + ---2 --2-= λ. Rr dr R dr P r d𝜃

(4)

Before we can focus on solutions, we need to further separate (4), so multiply (4) by r²

rdR r2d2R 1 d2P ----- + -----2 + -----2 = λr2. R dr R dr P d𝜃

Separate the terms

r dR r2d2R 1d2P -- ---+ -----2 − λr2 = − -----2 . R dr R dr P d𝜃

As before, set both sides to a constant, κ

1 d2P − -- --2-= κ P d𝜃

(5)

r-dR- r2 d2R- 2 R dr + R dr2 − λr = κ.

(6)

Now there are three differential equations and we know the form of these solutions. The differential equations of (3) and (5) are ordinary differential equations, while (6) is a little more complicated and we must turn to Bessel functions.

1.2 Axial Solutions (z)

Following the guidelines setup in [Etgen] for linear homogeneous differential equations, the first step in solving

d2Z --2-+ Zλ = 0 dz

is to find the roots of the characteristic polynomial

C(r) = r2 + λ = 0

√ ---- r = ± − λ.

Although, one can go forward using the square root, here we will introduce another constant, γ to imply the following cases. So if we want real roots, then we want to ensure a negative constant

2 λ = − γ

and if we want complex roots, then we want to ensure a positive constant

λ = γ2,

Case 1: λ ≤ 0 and real roots (λ = −γ²).

For every real root, there will be an exponential in the general solution. The real roots are

r1 = γ

r2 = − γ

r3 = 0.

Therefore, the solutions for these roots are

h1(z) = C1e γz

h (z) = C e−γz 2 2

h (z) = C ze0 = C z. 3 3 3

Combining these using the principle of superposition, gives the general solution,

γz −γz Zγ(z) = C1e + C2e + C3z + C4.

(7)

Case 2: λ > 0 and complex roots (λ = γ²).

The roots are

r4 = iγ

r5 = − iγ

and the corresponding solutions

h4(z) = C5e0 cos(γz) = C5 cos(γz)

h (z) = C e0sin (γz) = C sin(γz ). 5 6 6

Combining these into a general solution yields

Z (z) = C cos(γz ) + C sin(γz) + C . γ 5 6 7

1.3 Azimuthal Solutions (𝜃)

Azimuthal solutions for

2 d-P-+ κP = 0 d𝜃2

are in the most general sense obtained similarly to the axial solutions with the characteristic polynomial

2 C (r) = r + κ = 0

√ ---- r = ± − κ.

Using another constant, ν to ensure positive or negative constants, we get two cases.

Case 1: κ ≤ 0 and real roots (κ = −ν²).

The solutions for these roots are then

h1(z) = C1e ν𝜃

−ν𝜃 h2(z) = C2e

0 h3(z) = C3 𝜃e = C3𝜃.

Combining these for the general solution,

Pν(𝜃) = C1e ν𝜃 + C2e −ν𝜃 + C3𝜃 + C4.

(8)

Case 2: κ > 0 and complex roots (κ = ν²).

The roots are

r = iν 4

r = − iν 5

and the corresponding solutions

0 h4(𝜃) = C5e cos(ν𝜃) = C5 cos(ν𝜃)

h (𝜃) = C e0sin (ν𝜃) = C sin(ν 𝜃). 5 6 6

Combining these into a general solution

P ν(𝜃) = C5cos(ν 𝜃) + C6 sin(ν𝜃) + C7.

For the first glimpse at simplification, we will note a restriction on κ that is used when it is required that the solution be periodic to ensure P is single valued

P (𝜃) = P(𝜃 + 2nπ ).

Then we are left with either the periodic solutions that occur with complex roots or the zero case. So not only

(κ = ν2)

but also ν must be an integer, i.e.

P (𝜃) = C cos(ν 𝜃) + C sin(ν𝜃) + C ν = 0,1,2,... ν 5 6 7

(9)

Note, that ν = 0, is still a solution, but to be periodic we can only have a constant

P (𝜃) = C4.

1.4 Radial Solutions (r)

The radial solutions are the more difficult ones to understand for this problem and are solved using a power series. The two types of solutions generated based on the choices of constants from the 𝜃 and z solutions (excluding non-periodic solutions for P) leads to the Bessel functions and the modified Bessel functions. The first step for both these cases is to transform (6) into the Bessel differential equation.

Case 1: λ < 0 (λ = −γ²), κ > 0 (κ = ν²).

Substitute γ and ν into the radial equation (6) to get

2 2 r-dR- r- d-R- 2 2 2 R dr + R dr2 + γ r − ν = 0.

(10)

Next, use the substitution

x = γr

x- r = γ.

Therefore, the derivatives are

dx = γdr

dx- dr = γ

and make a special note that

d2 d d --2-= ------ dx dx dx

2 2 2 dx = dx ∗ dx = γ dr

2 dx2 dr = γ2-.

Substituting these relationships into (10) gives us

x γ dR x2γ2 d2R -------+ -2-----2-+ x2 − ν2 = 0. γR dx γ R dx

Finally, multiply by R∕x² to get the Bessel differential equation

2 ( 2) d-R- + 1-dR-+ 1 − ν-- R = 0. dx2 x dx x2

(11)

Delving into all the nuances of solving Bessel’s differential equation is beyond the scope of this article, however, the curious are directed to Watson’s in depth treatise [Watson]. Here, we will just present the results as we did for the previous differential equations. The general solution is a linear combination of the Bessel function of the first kind J_ν(r) and the Bessel function of the second kind Y _ν(r). Remebering that ν is a positive integer or zero.

R ν(r) = C1J ν(γr) + C2Yν(γr ) + C3

(12)

Bessel function of the first kind:

∑∞ m −1- ν+2m Jν(x) = (−-1)-(-2-x)-----. m=0 m!(m + ν)!

Bessel function of the second kind (using Hankel’s formula):

( ( x) ) (x )− ν ν∑−1 (ν − m − 1)!( x)2m Y ν(x) = 2Jν(x) η + ln -- − -- ------------- -- 2 2 m=0 m! 2

∞ m x ν+2m { } ∑ (−-1)-(-2)---- 1- 1- 1- 1- 1- ---1-- − m!(ν + m )! 1 + 2 + ...+ m + 1 + 2 + ...+ ν + m . m=0

For the unfortunate person who has to evaluate this function, note that when m = 0, the singularity is taken care of by replacing the series in brackets by

{ } 1- 1- 1- 1 + 2 + ...+ ν .

Some solace can be found since most physical problems need to be analytic at x = 0 and therefore Y _ν(x) breaks down at ln(0). This leads to the choice of constant C₂ to be zero.

Case 2: λ > 0 (λ = γ²), κ > 0 (κ = ν²).

Using the previous method of substitution, we just get the change of sign

2 ( 2) d-R- + 1-dR-− 1 + ν-- R = 0. dx2 x dx x2

(13)

This leads to the modified Bessel functions as a solution, which are also known as the pure imaginary Bessel functions. The general solution is denoted

R ν(r) = C1Iν(γr ) + C2K ν(γr ) + C3

(14)

where I_ν is the modified Bessel function of the first kind and K_ν is the modified Bessel function of the second kind

−ν Iν(γr) = i Jν(iγr)

π-ν+1 K ν(γr) = 2i (Jν(iγr) + iYν(iγr)).

1.5 Combined Solution

Keeping track of all the different cases and choosing the right terms for boundary conditions is a daunting task when one attempts to solve Laplace’s equation. The short hand notation used in [Kusse] and [Arfken] will be presented here to help organize the choices as a reference. It is important to remember that these solutions are only for the single valued azimuth cases (κ = ν²).

Once the separate solutions are obtained, the rest is simple since our solution is separable

Φ (r,𝜃,z ) = R (r)P (𝜃)Z(z).

so we just combine the individual solutions to get the general solutions to the Laplace equation in cylindrical coordinates.

Case 1: λ < 0 (λ = −γ²), κ > 0 (κ = ν²).

∑ ∑ { γz { { Φ (r,𝜃,z) = e−γz cos(ν𝜃 ) Jν(γr) ν γ e sin(ν𝜃) Yν(γr)

(15)

Case 2: λ > 0 (λ = γ²), κ > 0 (κ = ν²).

{ { { ∑ ∑ cos(γz) cos(ν 𝜃) Iν(γr ) Φ (r,𝜃,z) = sin(γz) sin(ν 𝜃) K ν(γr) ν γ

(16)

Interpreting the short hand notation is as simple as expanding terms and not forgetting the linear solutions, i.e. (γ = 0) . As an example, case 1, expanded out while ignoring the linear terms would give

( ) || A νγeγz cos(ν𝜃)Jν(γr) || ||| +B νγeγz cos(ν𝜃 )Y ν(γr) ||| ||| γz ||| ∑ ∑ ||{ +C νγeγzsin(ν𝜃)J ν(γr ) ||} Φ (r,𝜃,z) = +D νγe sin(ν𝜃 )Y ν(γr) . ν γ || +E νγe− γz cos(ν𝜃)Jν(γr )|| |||| +F νγe− γz cos(ν𝜃)Yν(γr) |||| ||| +G νγe−γz sin(ν𝜃)Jν(γr) ||| |( −γz |) +H νγe sin(ν𝜃)Yν(γr )

(17)

References

[1] Arfken, George, Weber, Hans, Mathematical Physics. Academic Press, San Diego, 2001.

[2] Etgen, G., Calculus. John Wiley & Sons, New York, 1999.

[3] Guterman, M., Nitecki, Z., Differential Equations, 3rd Edition. Saunders College Publishing, Fort Worth, 1992.

[4] Jackson, J.D., Classical Electrodynamics, 2nd Edition. John Wiley & Sons, New York, 1975.

[5] Kusse, Bruce, Westwig, Erik, Mathematical Physics. John Wiley & Sons, New York, 1998.

[6] Lebedev, N., Special Functions & Their Applications. Dover Publications, New York, 1995.

[7] Watson, G.N., A Treatise on the Theory of Bessel Functions. Cambridge University Press, New York, 1995.

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