A highly conducting ring of radius R is perpendicular to and concentric with the axis of a long solenoid as shown in fig. The ring has a narrow gap of width d in its circumference. The solenoid has cross sectional area A and a uniform internal field of magnitude B0. Now beginning at t=0,the solenoid current is steadily increased so that the field magnitude at any time t is given by B(t)=B0+α where α>0. Assuming that no change can flow across the gap, the end of ring which has excess of positive charge and the magnitude of induced e.m.f in the ring are respectively