A horizontal straight conductor of mass ‘m’ and length ‘l’ is placed in a uniform vertical magnetic field of magnitude ‘B’. An amount of charge ‘Q’ passes through the rod in a very short time such that the conductor begins to move only after all the charge has passed through it. Its initial velocity will be
BQlm
mv−mu=∫F dt or u=0 & F=ilB=dqdtlB⇒mv=∫q0dqdt⇒v=QlBm