The surface charge density \( \sigma \) of a sphere is defined as: \[ \sigma = \frac{Q}{4 \pi r^2} \] Where \( Q \) is the charge and \( r \) is the radius. Initially, the two spheres have the same surface charge density, so we have: \[ \sigma_1 = \sigma_2 \] Let \( Q_1 \) and \( Q_2 \) be the charges on the spheres initially. Since the surface charge densities are the same: \[ \frac{Q_1}{4 \pi \left( \frac{R}{2} \right)^2} = \frac{Q_2}{4 \pi \left( 2R \right)^2} \] Simplifying this: \[ \frac{Q_1}{\left( \frac{R}{2} \right)^2} = \frac{Q_2}{(2R)^2} \] \[ Q_1 = \frac{Q_2 \cdot R^2}{4R^2} \] So, \( Q_1 = \frac{Q_2}{4} \). When the spheres are brought into contact, the total charge \( Q_1 + Q_2 \) is shared between the two spheres. The charge will distribute according to their radii: \[ \frac{Q_1'}{Q_2'} = \frac{r_1}{r_2} = \frac{R/2}{2R} = \frac{1}{4} \]
Thus, the new surface charge densities are: \[ \sigma_1' = \frac{Q_1'}{4 \pi \left( \frac{R}{2} \right)^2}, \quad \sigma_2' = \frac{Q_2'}{4 \pi (2R)^2} \] Therefore, the ratio of the new surface charge densities is: \[ \frac{\sigma_1'}{\sigma_2'} = \frac{4}{1} \] Thus, the new surface charge density ratio is 4 : 1.
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: