Equipotential surfaces
Concept:
Equipotential surfaces are always perpendicular to electric field lines.
Step 1: Direction of electric field
Given:
\[
\vec{E} = E_0 \hat{i}
\]
So electric field is along positive x-direction.
Step 2: Nature of equipotential surfaces
Since electric field is uniform and along x-axis:
• Potential changes only along x-direction
• No change in potential along y and z directions
Therefore equipotential surfaces are:
\[
x = \text{constant}
\]
Step 3: Final representation
Three equipotential surfaces can be represented as:
\[
x = -c,\quad x = 0,\quad x = +c
\]
These are planes parallel to the Y–Z plane.