An isolated metal sphere of radius R, carrying an electric charge Q, is situated in the medium of relative permitivity, Er. A test charge is placed at a point p, distance r from the surface of the sphere. Let Eo represent the permitivity of free space. The electric potential at p is given by the expression
The electrical potential V at a point P located at a distance r from the surface of an isolated charged metal sphere is given by
V = \(\frac{\text{Q}}{4\pi\varepsilon}\).\(\frac{1}{\text{d}}\)
Where d = R + r is the distance from the center of the sphere to point P
\(\epsilon\) = \(\varepsilon_r\)\(\varepsilon_o\) is the permittivity of the medium, with \(\epsilon_r\) being the relative permittivity and \(\epsilon_o\) the permittivity of free space
\(\therefore\) V = \(\frac{\text{Q}}{4\pi \varepsilon_r \varepsilon_o}.\frac{1}{R + r}\)
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