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4
3
2
1
0
30°
60°
90°
120°
150°
180°
F()
Ã
-1
S( )
Ã
-2
Fig. 2.17. Stokes' functions S ( ψ )and F ( ψ )
use ellipsoidal coordinates ϕ, λ . As a spherical approximation, ϑ is the com-
plement of ellipsoidal latitude:
ϑ =90
ϕ.
(2-315)
Hence, we have
= 2 π
λ =0
π/ 2
cos ϕdϕdλ,
(2-316)
ϕ = −π/ 2
σ
so that Stokes' formula now becomes
2 π
π/ 2
R
4 πγ 0
g ( ϕ ) S ( ψ )cos ϕ ,
N ( ϕ, λ )=
(2-317)
λ =0
ϕ = −π/ 2
where ϕ, λ are the ellipsoidal coordinates of the computation point and ϕ
are the coordinates of the variable surface element . The spherical distance
ψ is expressed as a function of these coordinates by
cos ψ =sin ϕ sin ϕ +cos ϕ cos ϕ cos( λ
λ ) .
(2-318)
Stokes' function in terms of spherical harmonics
In Sect. 2.13, Eq. (2-273), we have found
g ( ϑ, λ )= 1
R
( n
1) T n ( ϑ, λ ) .
(2-319)
n =0
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