A ball is bouncing elastically with a speed of between walls of a railway compartment of size in a direction perpendicular to walls. The train is moving at a constant velocity of parallel to the direction of motion of the ball. As seen from the ground
The direction of motion of the ball changes every seconds.
Speed of ball changes every seconds.
Average speed of ball over any second interval is fixed.
The acceleration of ball is the same when observed either from ground or train.
This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try
refreshing the page, (b) enabling javascript if it is disabled on your browser and,
finally, (c)
loading the
non-javascript version of this page
. We're sorry about the hassle.
To answer properly, let us make the assumption that the ball is moving along one axis only (parallel to the speed of the train). This means that the ball is rather rolling (or sliding with no friction) on the ground than "boucing" through the compartment.
In this case, the speed pattern as seen from the ground is the following (please let us ignore relativity effects !)
speed 1 1 m / s on the way from back wall to front wall (wich takes 10 seconds)
speed 9 m / s on the way from front wall to back wall (10 seconds)
This gives a 20 seconds periodicity of the speed pattern.
In conclusion :
(A) the direction of the motion never changes from the ground (always in the direction of the train speed)
(B) speed of ball changes every 10 seconds
(C) Average speed of ball over any 20 seconds interval is fixed, as a directe consequence of the 20 seconds periodicity of speed
(D) The acceleration of the ball is the same in train / ground, since the train has a uniform motion in straight line.
Remark : the problem could be better stated, in particular precise the absence of vertical motion, otherwise:
(A) remains fasle, but for different reason: speed direction changes continuously
(B) becomes fasle (continuous change)
(C) is not possible to assess (vertical movment are periodic bounces, with a period depending on the maximum height of the trajectory)
(D) remains true