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Helmholtz Differential Equation--Spherical Surface


On the surface of a sphere, attempt separation of variables in spherical coordinates by writing

 F(theta,phi)=Theta(theta)Phi(phi),
(1)

then the Helmholtz differential equation becomes

 1/(sin^2phi)(d^2Theta)/(dtheta^2)Phi+(cosphi)/(sinphi)(dPhi)/(dphi)Theta+(d^2Phi)/(dphi^2)Theta+k^2ThetaPhi=0.
(2)

Dividing both sides by PhiTheta,

 ((cosphisinphi)/Phi(dPhi)/(dphi)+(sin^2phi)/Phi(d^2Phi)/(dphi^2))+(1/Theta(d^2Theta)/(dtheta^2)+k^2)=0,
(3)

which can now be separated by writing

 (d^2Theta)/(dtheta^2)1/Theta=-(k^2+m^2).
(4)

The solution to this equation must be periodic, so m must be an integer. The solution may then be defined either as a complex function

 Theta(theta)=A_me^(isqrt(k^2+m^2)theta)+B_me^(-isqrt(k^2+m^2)theta)
(5)

for m=-infty, ..., infty, or as a sum of real sine and cosine functions

 Theta(theta)=S_msin(sqrt(k^2+m^2)theta)+C_mcos(sqrt(k^2+m^2)theta)
(6)

for m=0, ..., infty. Plugging (4) into (3) gives

 (cosphisinphi)/Phi(dPhi)/(dphi)+(sin^2phi)/Phi(d^2Phi)/(dphi^2)+m^2=0
(7)
 Phi^('')+(cosphi)/(sinphi)Phi^'+(m^2)/(sin^2phi)Phi=0,
(8)

which is the Legendre differential equation for x=cosphi with

 m^2=l(l+1),
(9)

giving

 l^2+l-m^2=0
(10)
 l=1/2(-1+/-sqrt(1+4m^2)).
(11)

Solutions are therefore Legendre polynomials with a complex index. The general complex solution is then

 F(theta,phi)=sum_(m=-infty)^inftyP_l(cosphi)(A_me^(imtheta)+B_me^(-imtheta)),
(12)

and the general real solution is

 F(theta,phi)=sum_(m=0)^inftyP_l(cosphi)[S_msin(mtheta)+C_mcos(mtheta)].
(13)

Note that these solutions depend on only a single variable m. However, on the surface of a sphere, it is usual to express solutions in terms of the spherical harmonics derived for the three-dimensional spherical case, which depend on the two variables l and m.


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Cite this as:

Weisstein, Eric W. "Helmholtz Differential Equation--Spherical Surface." From MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/HelmholtzDifferentialEquationSphericalSurface.html

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