The set-up, shown in the figure, is present in a uniform magnetic field, B, directed perpendicular to the plane of this ‘set-up’. The rod, PQ, of length L, is allowed to slide down vertically, under its own weight, on the (shaded) conducting rods. The terminal velocity, acquired by the sliding rod (of mass m), would equal
(1) \((\frac{m^2g^2R}{Bl})\)
(2) \((\frac{Bl}{m^2g^2R})\)
(3) \((\frac{B^2l^2}{mgR})\)
(4) \((\frac{mgR}{B^2l^2})\)