(a) State Gauss’s law in electrostatics. Show, with the help of a suitable example along with the figure, that the outward flux due to a point charge ‘q’, in vacuum within a closed surface, is independent of its size or shape and is given by q/εo.
(b) Two parallel uniformly charged infinite plane sheets, ‘1’ and ‘2’, have charge densities +
and –
respectively. Give the magnitude and direction of the net electric field at a point
(i) in between the two sheets and
(ii) outside near the sheet ‘1’.
OR
(a) Define electrostatic potential at a point. Write its S.I. unit. Three point charges q1, q2 and q3 are kept respectively at points A, B and C as shown in the figure. Derive the expression for the electrostatic potential energy of the system.

(b) Depict the equipotential surfaces due to
(i) an electric dipole,
(ii) two identical positive charges separated by a distance.
(a) Gauss Law states that the electric flux linked with a closed surface is equal to 1/ε0 times the net charge enclosed by a closed surface:![]()
Consider two shells, containing same charge = q C. One of the shells is spherical and has a radius 1.5 cm and the other is cubical and has edge length 2 cm.
The flux linked with first spherical shell = q/ε0
The flux linked with second spherical shell = q/ε0
⇒ Both fluxes are same and independent of size and shape of the closed surface.
(b) Let
be the unit vector directed from left to right.
Let P be a point in the region between the two plates. Let Q be a point in the region outside the plates.

Electric field at point P:
![]()
![]()
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Electric field at Q:
![]()
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OR
(a) The electrostatic potential, V at any point in a region with electrostatic field is the work done in bringing a unit positive charge (without acceleration) from infinity to that point. Its S.I. unit is Volt.
The potential energy of a system of three charges q1, q2 and q3 located at
respectively.
To bring q1 first from infinity to
, no work is required.
Next we bring q2 from infinity to
.
![]()
Now, we bring charge q3 from infinity to
.
![]()
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(b) Equipotential surfaces for (i) dipole and (ii)2 identical positive charges separated by a distance.

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