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:
\[ \boxed{\text{D) Spherical for a point charge}} \]
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Two similar metallic rods of the same length \( l \) and area of cross section \( A \) are joined and maintained at temperatures \( T_1 \) and \( T_2 \) (\( T_1>T_2 \)) at one of their ends as shown in the figure. If their thermal conductivities are \( K \) and \( \frac{K}{2} \) respectively. The temperature at the joining point in the steady state is:

According to equipartition principle, the energy contributed by each translational degree of freedom and rotational degree of freedom at a temperature T are respectively (\( k_B = \text{Boltzmann constant} \)):
Kepler's second law (law of areas) of planetary motion leads to law of conservation of