Problem 7: Prolate spheroidal coordinates {0 ≤n<∞,0 ≤ 0 ≤ π,0 ≤ 0 < 27} are described by the metric coefficients h1 = h2 = a(sinhn+sin20) }} hg = a sinh nsin20 where a is a constant. Derive Laplace equation and separate it into three ODEs. Don't solve the separated ODES.

Advanced Engineering Mathematics
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Chapter2: Second-order Linear Odes
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Problem 7: Prolate spheroidal coordinates {0 <n<∞0,0<0 < T, 0<¢ < 2n} are described by the
metric coefficients
h1 = h2 = a?(sinh? 7 + sin? 0)
h3 = a? sinh? nsin? 0
where a is a constant. Derive Laplace equation and separate it into three ODESS. Don't solve the separated
ODES.
Transcribed Image Text:Problem 7: Prolate spheroidal coordinates {0 <n<∞0,0<0 < T, 0<¢ < 2n} are described by the metric coefficients h1 = h2 = a?(sinh? 7 + sin? 0) h3 = a? sinh? nsin? 0 where a is a constant. Derive Laplace equation and separate it into three ODESS. Don't solve the separated ODES.
Problem 6: Two spherical conductors of radii a and b (b > a). The sphere of radius r = a is held at a
potential f(0), and the sphere of radius r = b is held at a potential g(0). The problem of the potential
between the two spheres, denoted by u(r, 0), can be described by
2 ди
1 0Pu
cot 0 du
+
0,
a <r < b,
0 < 0 < T,
dr2
r dr
p2 002
r2 d0
u(r, 0) is finite,
u(r, 7) is finite,
u(а, 0) — f(0),
u(b, 0) = g(0).
Solve it.
Transcribed Image Text:Problem 6: Two spherical conductors of radii a and b (b > a). The sphere of radius r = a is held at a potential f(0), and the sphere of radius r = b is held at a potential g(0). The problem of the potential between the two spheres, denoted by u(r, 0), can be described by 2 ди 1 0Pu cot 0 du + 0, a <r < b, 0 < 0 < T, dr2 r dr p2 002 r2 d0 u(r, 0) is finite, u(r, 7) is finite, u(а, 0) — f(0), u(b, 0) = g(0). Solve it.
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