Two spheres of electric charges + 2 nC and −8 nC are placed at a distance d apart. If they are allowed to touch each other, what is the new distance between them to get a repulsive force of same magnitude as before ?
d
C.
In the first condition,
Given,
In the second condition,
After touching of sphere to each other the total charge = 2 − 8 = −6 nC
Charge on each sphere = 3 nC
= 3 × 10-9 C
From Eqs. (i) and (ii), we get
Three point charges of + 2q, + 2q and − 4q are placed at the corners A, B and C of an equilateral triangle ABC of side x. The magnitude of the electric dipole moment of this system is
2qx
3qx
64 small drops of mercury, each of radius r and charge q coalesce to form a big drop. The ratio of the surface density of charge of each small drop with of the big drop is
64 : 1
1 : 64
1 : 4
4 : 1
Three point charges are placed at the corners of an equilateral triangle. Assuming only electrostatic forces are acting. Then the system
will be in equilibrium if the charges rotate about the centre of the triangle
can never be in equilibrium
will be in equilibrium if the charges have the same magnitudes but different sign
will be in equilibrium if the charges have different magnitude and different signs.
Two copper balls, each weighing 10 g are kept in air 10 cm apart. If one electron from every 106 atoms is transferred from one ball to the other, the Coulomb force between them is (atomic weight of copperis 63.5)
2.0 × 104 N
2.0 × 1010 N
2.0 × 106 N
2.0 × 106 N
The electric field in a certain region is acting radially outward and is given by E = Ar. A charge contained in a sphere of radius 'a' centred at the origin of the field will be given by
In a coil of resistance 10Ω, the induced current developed by changing magnetic flux through it is shown in the figure as a function of time. The magnitude of change in flux through the coil in weber is
8
2
6
6
What is the flux through a cube of side a if a point charge of q is a one of its corner?
Two thin dielectric slabs of dielectric constants K1 and K2 (K1 < K2) are inserted between plates of a parallel plate capacitor, as shown in the figure. The variation of electric field E between the plates with distance d as measured from plate P is correctly shown by:
A conducting sphere of radius R is given a charge Q. The electric potential and the electric field at the centre of the sphere respectively are:
zero and