Two charges $ -q $ each are fixed, separated by distance $ 2d $. A third charge $ q $ of mass $ m $ placed at the mid-point is displaced slightly by $ x' (x \ll d) $ perpendicular to the line joining the two fixed charges as shown in the figure. The time period of oscillation of $ q $ will be:
The problem involves three charges: two charges \( -q \) and one charge \( +q \), with the charge \( +q \) displaced slightly from the equilibrium position.
The forces acting on the charge \( q \) due to the two fixed charges \( -q \) will create an electric field, and if we displace the charge \( q \) by a small distance \( x' \), it will experience a restoring force.
We calculate the force acting on the charge \( q \) due to the electric field of the fixed charges. Using Coulomb’s law and the approximation for small displacements, the force \( F \) on \( q \) is: \[ F = -kx' \] Where \( k \) is the effective spring constant related to the electric force.
For the oscillations to occur, the time period \( T \) of the charge is given by: \[ T = 2\pi \sqrt{\frac{m}{k}} \] Since \( k \) is related to the charges and the separation distance, the expression for \( T \) becomes: \[ T = \sqrt{\frac{8 \epsilon_0 m}{q^2}} x^2 \] Thus, the time period of oscillation for the charge \( q \) is \( \sqrt{\frac{8 \epsilon_0 m}{q^2}} x^2 \).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: