If a charge \( q \) is placed at the centre of a closed hemispherical non-conducting surface, the total flux passing through the flat surface would

Step 1: According to Gauss's Law, the total electric flux \( \Phi_E \) through a closed surface is given by: \[ \Phi_E = \frac{q_{{enc}}}{\epsilon_0} \] where \( q_{{enc}} \) is the enclosed charge and \( \epsilon_0 \) is the permittivity of free space.
Step 2: For a hemispherical surface, if the charge is placed at the center, it will be symmetrically distributed. The flux passing through the entire hemispherical surface will be \( \frac{q}{\epsilon_0} \).
Step 3: Since the flux is symmetrically distributed over the surface, half of the flux will pass through the curved surface, and the other half will pass through the flat surface.
Step 4: The flux passing through the flat surface is zero because the flat surface is in the opposite direction to the field lines, and the flux passing through the flat surface cancels out.

As shown below, bob A of a pendulum having massless string of length \( R \) is released from \( 60^\circ \) to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take \( g \) as acceleration due to gravity):

The magnitude of heat exchanged by a system for the given cyclic process ABC (as shown in the figure) is (in SI units):
