The gravitational force acting on the spheres is given by:
\( F_g = \rho_B V g \),
where \( \rho_B \) is the density of the spheres, \( V \) is the volume of the sphere, and \( g \) is the acceleration due to gravity.
The electric force acting between the spheres is:
\( F_e = \frac{Q^2}{4 \pi \epsilon_0 d^2} \),
where \( Q \) is the charge on the spheres, \( d \) is the distance between the centers of the spheres, and \( \epsilon_0 \) is the permittivity of free space.
The buoyant force acting on the spheres in the liquid is:
\( F_b = \rho_L V g \),
where \( \rho_L \) is the density of the liquid.
In equilibrium, the tension in the strings balances both the horizontal and vertical forces. The vertical and horizontal components of the tension are:
\( T \cos \theta = F_g - F_b \),
\( T \sin \theta = F_e \).
The ratio of these equations gives:
\( \tan \theta = \frac{F_e}{F_g - F_b} \).
For the spheres in the liquid, substituting the expressions for \( F_g \) and \( F_b \):
\( \tan \theta = \frac{F_e}{(\rho_B - \rho_L) V g} \).
When the spheres are in air, the buoyant force is negligible, and the force balance becomes:
\( \tan \theta = \frac{F_e}{\rho_B V g} \).
Equating the two expressions for \( \tan \theta \), we get:
\( \frac{F_e}{\rho_B V g} = \frac{F_e}{(\rho_B - \rho_L) V g} \).
Simplifying:
\( \rho_B V g = (\rho_B - \rho_L) V g \).
Cancelling \( V g \) from both sides:
\( \rho_B = \rho_B - \rho_L \Rightarrow \rho_B - \rho_L = k \cdot \rho_B \).
Substituting the given values:
\( \rho_B = 1.4 \, g/cm^3 \), \( \rho_L = 0.7 \, g/cm^3 \).
From the ratio:
\( k = \frac{\rho_B}{\rho_L} = \frac{1.4}{0.7} = 2 \).
Final Answer: The dielectric constant of the liquid is: \( k = 2 \).
A point charge $ +q $ is placed at the origin. A second point charge $ +9q $ is placed at $ (d, 0, 0) $ in Cartesian coordinate system. The point in between them where the electric field vanishes is:
A small bob of mass 100 mg and charge +10 µC is connected to an insulating string of length 1 m. It is brought near to an infinitely long non-conducting sheet of charge density \( \sigma \) as shown in figure. If the string subtends an angle of 45° with the sheet at equilibrium, the charge density of sheet will be :
Consider two infinitely large plane parallel conducting plates as shown below. The plates are uniformly charged with a surface charge density \( +\sigma \) and \( -\sigma \). The force experienced by a point charge \( +q \) placed at the mid point between the plates will be:
Match List-I with List-II.