In a uniform electric field \( \vec{E} \), the electric potential \(V\) decreases in the direction of \( \vec{E} \).
Equipotential surfaces are perpendicular to the electric field lines.
The figure (interpreted from typical representations for such options) shows the electric field \( \vec{E} \) pointing from left to right.
Option (3) states \( V_C>V_B>V_A \).
For this to be true, if \( \vec{E} \) points in the positive x-direction, then point C must have the smallest x-coordinate, followed by B, and then A having the largest x-coordinate.
That is, \( x_C<x_B<x_A \).
Points further to the left (opposite to the direction of \( \vec{E} \)) will be at a higher potential.
Points further to the right (in the direction of \( \vec{E} \)) will be at a lower potential.
So, if the points are arranged horizontally such that C is to the left of B, and B is to the left of A, with \( \vec{E} \) pointing right, then \( V_C>V_B>V_A \).
The diagram shown in the problem (with C and A vertically aligned and B to their left, E pointing right) leads to \(V_B>V_A = V_C\), which is not among options.
Assuming the configuration that leads to option (3): C is most "upstream" in the field, A is most "downstream", B is in between.
\( x_C<x_B<x_A \).
E field points from left to right.
Then \( V_C \) is highest, \( V_A \) is lowest, \( V_B \) is in between.
So \( V_C>V_B>V_A \).