A point charge placed in a cavity of a conducting sphere does not experience a force from the sphere's charge, but it can induce a charge on the cavity wall that affects it. If the point charge is off-center, it creates a non-radial force on the induced charges on the inner surface, leading to a redistribution that shields the charge. This results in a net force pulling the point charge toward the wall, and if movable, it will ultimately spread over the outer surface of the sphere. The electric field within the metal remains zero, indicating that while charge density is zero inside, induced charges can exist on the inner and outer surfaces. Thus, the charge distribution maintains equilibrium while allowing for the presence of surface charges.