Let, R be the radius of the shell and Q be the charge uniformly distributed on the surface.
i) For a point outside the shell :
By Gauss's law, "E.4\u03c0r ^\n2\n =\n\u200b\t\n \nQ _{\nen}\/\\epsilon_0\n\n\u200b"
here r be the distance from centre of shell (r>R) and charge enclosed by surface "Qeq\n\n\u200b=Q."
So, the electic field outside the shell is "E\n =\n\u200b\t\n \nQ _{\nen}\/(4\u03c0r^2\\epsilon_0)" , the electric potential outside the shell is "V(r)=-\\int_{\\infin}^r \\frac{Q_{en}}{4\\pi r_1^2 \\epsilon_0}d r_1=\\frac{Q_{en}}{4\\pi r\\epsilon_0}."
Comments
Dear Awesh, thank you for correcting us.
Totally wrong... According to question find 'Electric Potential' ("V")... But in the solution the expert has found 'Electric Field' ("E").
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