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l 0 R sin /2)
P
P'
(
R
Ã
Fig. 1.9. Spatial distance between two points on a sphere
l 0 =2 R sin ψ
2 ,
(1-141)
and the function M takes the simple form
1
4 R 2 sin 3 2
= 2 R
l 0
M ( R, ψ )=
.
(1-142)
For ψ
, and we cannot use the original formula
(1-135) at the surface of the sphere r = R . In the transformed equation
(1-139), however, we have V
0wehave M ( R, ψ )
→∞
V P
0for ψ
0, and the singularity of
M for ψ
0 will be neutralized (provided V is differentiable twice at P ).
Thus, we obtain the gradient formula
2 π
π
R V P + R 2
∂V
∂r
1
V
V P
sin ϑ .
=
(1-143)
l 0
2 π
λ =0
ϑ =0
This equation expresses ∂V/∂r on the sphere r = R in terms of V on this
sphere; thus, we now have
V = V ( R, ϑ ) .
V P
= V ( R, ϑ, λ ) ,
(1-144)
Solution in terms of spherical harmonics
We may express V P
as
R
r
n +1
=
V P
Y n ( ϑ, λ ) .
(1-145)
n =0
Differentiation yields
( n +1) R n +1
r n +2
∂V
∂r
=
Y n ( ϑ, λ ) .
(1-146)
n =0
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