- AAre closer in regions of large electric fields compared to regions of lower electric fields.
- BWill be more crowded near sharp edges of a conductor.
- CWill be more crowded near regions of large charge densities.
- DWill always be equally spaced.
Equipotential surfaces are closer in regions of large electric fields because electric field intensity is inversely proportional to the separation between equipotential surfaces.
As the electric field intensities is large near sharp edges of a charged conductor or near the regions of large charge densities. Therefore, numbers of equipotential surfaces are closer to such places or in other words they are more crowded.
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Magnetic intensity for an axial point due to a short bar magnet of magnetic moment M is given by
|
(a) |
(b) |
(c) |
(d) |
In an induction coil, the secondary e.m.f. is
|
(a) Zero during break of the circuit |
|
(b) Very high during make of the circuit |
|
(c) Zero during make of the circuit |
|
(d) Very high during break of the circuit |
Eight dipoles of charges of magnitude e are placed inside a cube. The total electric flux coming out of the cube will be
|
(a) |
(b) |
(c) |
(d) Zero |
An alternating current of frequency 200 rad/sec and peak value 1A as shown in the figure, is applied to the primary of a transformer. If the coefficient of mutual induction between the primary and the secondary is 1.5 H, the voltage induced in the secondary will be

|
(a) 300 V |
(b) 191 V |
(c) 220 V |
(d) 471 V |