Characteristics of Equipotential Surfaces:
1. The electric potential is the same at all points on an equipotential surface, meaning no work is done in moving a charge along the surface.
2. Equipotential surfaces are always perpendicular to the electric field lines.
Since the electric field is uniform and directed along the \( x \)-axis, the potential at any point is given by:
\[
V = V_0 - E \cdot d
\]
Where:
- \( V_0 \) is the potential at the origin,
- \( E \) is the magnitude of the electric field,
- \( d \) is the distance along the \( x \)-axis.
For the given point \( (4m, 3m) \), the distance along the \( x \)-axis is 4 m (since the electric field is along the \( x \)-axis). Therefore, the potential at this point is:
\[
V = 220 \, \text{V} - 50 \, \text{NC}^{-1} \cdot 4 \, \text{m} = 220 \, \text{V} - 200 \, \text{V} = 20 \, \text{V}
\]
Thus, the potential at the point \( (4m, 3m) \) is 20 V.