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In spherical polar coordinates (r, 0, ¢), the general solution of Laplaces equation which has cylindrical symmetry about the
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differential is, quntions The n(n+) R=0, (r >o) ye dR dr dr Solution the that assume Let us of the is - (n+) (noo,e.) R(v) =equatim is, 8 ht) (m=0,2,) Kn (r)= A where An, B, Constants, 8. the solution of Rün) From Ca), Substitudting P Cese) u(r,e)=-(n+1) Pin Ccose). Applaing B.C yain, -(n+1) ula,0) = s B, Gr a ఒG6) 2+ Cose, Let Coso = x, Pm Cc) and, intguting Multiplying-(m+) (2+x) Pm (2) dz %3D (2mt) But mtk-1 C. 2 5 x k-o Pm (x)= above equation, Sabettating in to - (m+1) mtkt 2. (2mt1) ktilk+1 mtk1 C. kti k+2 k+2 (2mt1) 2 B = 2. 2. k-o kt 2 (-t) + (-6) k+2 The Solution - (n+)) P, Ccase) ulr,0) = 5 BY B is ex pres

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