∮→E.−→dA=qenc∈0
Where →E is the electric field and
−→dA is the elemental area vector for any small elemental area on the gaussian surfae.
∮|→E||−→dA|cosθ=qenc∈0...(1)
Given that the formula
|→E|=qenc∈0|A|
is applicable.
|→E||A|=qenc∈0
(Using equation 1)
|→E||A|=∮|→E||−→dA|cosθ...(2)
For constant E ∮|→E||−→dA|cosθ
becomes |→E|∮|−→dA|cosθ=|→E||A|cosθ Hence, the given relation will be valid when →E is a constant throughout the gaussian surface and angle (θ) between the area vector and the Electric field vector is same at all points and equal to 0°
For constant E∮|→E||−→dA|cosθ
becomes |→E|∮|−→dA|=|→E||A|.
The condition θ=0° means that the components of the electric field parallel to the surface is zero.
Since, E=dvdx, Where V is the Electric potential.
The potential gradient over the surface is zero. Hence the surface is equipotential.
Hence, option (d) is correct.