Since the tension is always perpendicular to the velocity vector, the work done by the tension force will be zero. Hence, according to the work energy theorem, the kinetic eneigy or velocity of the disc will remain constant during it’s motion. Hence, the sought time t=s/v0 where s is the total distance traversed by the small disc during it's motion.
It should be clearly understood that the only uncompensated force acting on the disc A, in this case, is the tension T, of the thread. It is easy to see that there is no point here, relative to which the moment of force T is invariable in the process of motion. Hence conservation of angular momentum is not applicable here