An equipotential surface is a surface on which the electric potential is constant at all points.
1. For a point charge:
The electric potential is given by:
\[ V = \frac{kQ}{r} \]
where:
Since this potential depends only on the distance from the charge, the equipotential surfaces for a point charge are spherical. These surfaces are concentric spheres with the point charge at the center.
2. For a dipole:
The electric potential at a point is a function of both distance and angle from the dipole. At large distances, the equipotential surfaces are approximately spherical. However, at small distances, the equipotential surfaces take a more complicated shape and are not purely spherical.
Therefore, the correct answer is that the equipotential surface is spherical for a point charge.
Thus, the correct answer is:
\[ \boxed{\text{D) Spherical for a point charge}} \]
The y-intercept of the graph between the terminal voltage \(V\) with load resistance \(R\) along \(y\) and \(x\) – axis, respectively, of a cell with internal resistance \(r\), as shown, is:

If $ | \vec{a} | = 3 $, $ | \vec{b} | = 2 $, then find $ (3\vec{a} - 2\vec{b}) \cdot (3\vec{a} + 2\vec{b}) $.