Keral Medical Entrance 2009 question paper contained three questions from electrostatics. They are simple except for the first one (given below) which will demand some three dimensional imagination.
(1) The total electric flux through a cube when a charge 8q is placed at one corner of the cube is
(a) ε0 q
(b) ε0 /q
(c) 4πε0 q
(d) q/4πε0
(e) q/ε0
You should remember that the total electric flux originating from a charge q is q/ε0.
[You will definitely remember that the electric field E at a point distant r from a point charge is q/4πε0r2. The electric field is equal to the electric flux through unit area held normal to the direction of the field. If you imagine a spherical surface with the charge q at the centre, the surface area of the sphere is 4πr2 and the total flux passing normally through the spherical surface is (q/4πε0r2) ×4πr2 = q/ε0]
In the question the charge 8q is placed at one corner of the cube. The total electric flux originating from this charge is 8q/ε0. But only one-eigths of the flux passes through the cube. (You can place seven more cubes with their corners touching the charge to cover the entire volume around the charge).
The electric flux through a cube when a charge 8q is placed at one corner of the cube is therefore (1/8)×(8q/ε0) = q/ε0.
(2) A uniform electric field E exists along positive x-axis. The work done in moving a charge 0.5 C through a distance 2 m along a direction making an angle 60º with x-axis is 10 J. Then the magnitude of electric field is
(a) 5 Vm–1
(b) 2 Vm–1
(c) √5 Vm–1
(d) 40 Vm–1
(e) 20 Vm–1
The force (F) acting on charge q in electric field E is given by F = qE along the direction of the field (along the positive x-axis here). Since the displacement (d) of the charge is inclined at 60º with the x-axis, the work done (W) is given by
W = qEd cos 60
Therefore, 10 = 0.5×E×2×½, from which E = 20 Vm–1.
(3) A capacitor of capacitance C is charged to a potential V. If it carries charge Q, then the energy stored in it is
(a) ½ CV
(b) QV
(c) ½ QV2
(d) CV2
(e) ½ QV
The answer is ½ QV which you can obtain from ½ CV2 which is the form most of you will usually remember:
½ CV2 = ½ CV×V = ½ QV
[The capacitor is charged from zero potential to the potential V. The charge Q is therefore transferred to the capacitor at an average potential of (0+V)/2 = V/2. The work done is therefore QV/2.
To be more rigorous, if the charge on the capacitor at any instant of charging is q and the potential at the instant is v, the work done in transferring an additional charge dq is vdq= (q/C)dq. The total work done in transferring the entire charge Q is 0 ∫Q(q/C)dq = Q2/2C = ½ ×Q×(Q/C) = ½ QV].
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