Stokes Equation - Solution in Spherical Polar Coordinates
Stokes Equation - Solution in Spherical Polar Coordinates
Stokes Equation - Solution in Spherical Polar Coordinates
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d ⎡ 2 dΦ<br />
⎤<br />
( 1 η ) n( n 1)<br />
0<br />
dη<br />
⎢ − + + Φ=<br />
dη<br />
⎥<br />
(5)<br />
⎣ ⎦<br />
Many important properties of the Legendre Polynomials can be found <strong>in</strong><br />
MacRobert (1967) and <strong>in</strong> Abramowitz and Stegun (1965).<br />
Some useful relationships <strong>in</strong>volv<strong>in</strong>g the Gegenbauer Polynomials are given<br />
below.<br />
( η) − P ( η)<br />
P<br />
2n<br />
−1<br />
η<br />
−1/2<br />
C<br />
n ( η ) = − ∫ P<br />
1 ( )<br />
1<br />
n−<br />
s ds<br />
(7)<br />
−<br />
−1/2<br />
n−2<br />
n<br />
C<br />
n ( η ) =<br />
(6)<br />
The first few Gegenbauer and Legendre Polynomials are<br />
C<br />
C<br />
C<br />
P<br />
P<br />
P<br />
−<br />
( ) 1 C ( )<br />
η = η = η<br />
−1/2 1/2<br />
0 1<br />
1 1<br />
2 2<br />
1 1<br />
8 5 1<br />
−<br />
( η) = ( 1− η ) C ( η) = η ( 1−η<br />
)<br />
−1/2 2 1/2 2<br />
2 3<br />
( η) = ( −η )( η − )<br />
−1/2 2 2<br />
4<br />
( ) 1<br />
P ( )<br />
0 1<br />
2 2<br />
( η) = ( 3η − 1) P ( η) = η( 5η<br />
−3)<br />
2 3<br />
4<br />
η = η = η<br />
1 1<br />
2 2<br />
1 35<br />
8 30 3<br />
4 2<br />
( η) = ( η − η + )<br />
The Gegenbauer Polynomials satisfy the orthogonality property<br />
for values of mn≥ , 2.<br />
−1/2 −1/2<br />
+ 1<br />
m ( η) n ( η)<br />
2<br />
∫ C C dη<br />
=<br />
δ<br />
1<br />
2<br />
mn<br />
(8)<br />
−<br />
1−η<br />
n( n−1)( 2n−1)<br />
2