
(a) When the sphere 1 is released from horizontal position, then from energy conservation, potential energy at height $l_{0} =$ kinetic energy at bottom
Or $mgl_{0} = \frac{1}{2}mv^{2}$
Or $v = \sqrt{2gl_{0}}$
Since, all collisions are elastic, so velocity of sphere 1 is transferred to sphere 2, then from 2 to 3 and finally from 3 to 4. Hence, just after collision, the sphere 4 attains a velocity equal to $\sqrt{2gl_{0}}$