In Kibble-Berkshire Classical Mechanics there is a problem which says:
A ball is dropped from height $h$ and bounces. The coefficient of restitution at each bounce is $e$. Find the velocity immediately after the first bounce, and immediately after the $n$th bounce. Show that the ball finally comes to rest after a time $$\frac{1+e}{1-e}\sqrt{\frac{2h}{g}}.$$
Even though I did not face any problem proving what I was asked to, the whole problem seems to me irrational. The velocity after the $n$th collision equals $u_n=e^nu_0$. Since the ball never stops how can we find that the ball comes to rest after a certain amount of time?. Any help to my misunderstanding is really appreciated.
(1st Edit: If we could reproduce such an experiment in lab exactly as the conditions of the problem predict, supposing that from the equations above the ball has to stop at time $t_1$ then at time $t_2$: $t_2>t_1$ what would we see? Would we find the ball being between $k$th and $(k+1)$th collision? The maths however of this collision problem would predict that both $k$th and $(k+1)$th collision happened before $t_1$.)
(2nd Edit: Even if we argued that the idealization of physical reality (neglecting the deformation of the ball, neglecting the time interval for which the ball touches the ground, etc) is responsible for the paradox, we would observe the same paradox if we could run a PC simulation with a virtual ball hitting a virtual ground changing its velocity in the way suggested by the excercise.The total time that we would predict mathematicaly that the ball is moving would be finite but an observer of such a simulation would see the ball moving infinitely)