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Without loss of generality, let us choose the direction of the dipole moment as the z-axis. The external uniform electric field is thus also aligned along the z-axis.
Consider a sphere of radius R with its center at the origin. From Problem 3.39 we know that the potential at any point on this sphere in the absence of the electric field is given by,
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In other words the potential difference between any two points (x1,y1,z1) and (x2,y2,z2) in the absence of the external electric field is given by,
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Since the external electric field is aligned with the electric dipole moment, it is along the z-axis. The additional potential difference induced due to the electric field between points is given by E(z1-z2). The net potential difference between at any two points on this sphere are thus given by,
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On an equipotential surface the potential difference between any two points is zero. Hence, for this spherical surface to be equipotential,
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