QUESTION: An object, 2 m above the floor, tethered by a chain which is attached to a brake (a constant force spring) is released and falls vertically under the influence of gravity under it reaches the end of its tether and then is deaccelerated by the ``brake'' which can, in the absence of any other effect (gravity included) has an acceleration of 14.7 m/s2. How long should the tether chain be so that the falling object just ``kisses'' the floor?
As the figure below shows there are two regimes to the fall.
![\includegraphics [height=3.1in]{pd_fig1.eps}](img1.gif)
To solve the problem:
![\includegraphics [height=4.1in]{pd_fig2.eps}](img2.gif)
Of the three motion equations:
![]()
v = v0 t + a t
v2 = v02 + 2 a (x-x0)
only the last doesn't require a knowledge of the temporal aspect of the problem. Using a space-time to establish the motion and facts you should find that you obtain two useful expressions:| Time regime one: | v2 = (0)2 + 2 (-g) x |
| Time regime two: | 0 = v2 + 2 (g/2) y |
|
with |
Substituting gives 0 = 2 (-g) x + 2 (g/2) (s - x) and solving gives x = s/3 = -0.67 meters.