How Fast Will Box A Hit the Floor in a Pulley System?

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The discussion revolves around calculating the speed of Box A when it hits the floor in a pulley system involving two boxes with different masses. The initial potential energy of Box A is calculated, but the mistake occurs by not accounting for the kinetic energy of Box B, which is also in motion. The conservation of energy principle is emphasized, indicating that the total energy change must consider both boxes. The relationship between the speeds of the two boxes, connected by a rope, is crucial for solving the problem correctly. Understanding these energy dynamics is essential for accurately determining the final speed of Box A upon impact.
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Homework Statement


Two boxes are connected over a pulley and hel AT REST. Box A has a mass of 15kg and box B has a mass of 12kg. If the bottom of box A is originally 85cm above the floor, with what speed will it contact the floor when the system is released? Use conservation of energy and assume that friction is negligible. (Hint: Think abou the total energy of the system before and after the block A is released)


Homework Equations


ET= mgh + 1/2mv squared
Ek=1/2mv squared
Ep=mgh


The Attempt at a Solution


Before released: Eta= (15)(9.8)(.85)
Eta= 124.95J
After released: Etb= mgh
Etb= 12(9.8)(.85)

up to this point, the test says I have it write (as seen from the teachers marking)

then this is where i somehow went wrong: 124.95-99.96= Change in Energy
*at this point, the marker said, "B HAS Ek TOO!"

then i did: 24.99= Change in Energy
24.99= 1/2mv squared
24.99= 1/2(15)v squared
3.332m/s=v
3.3m/s=v

This is unfortunately not the correct answer. If anyone can assist me in where i went wrong that would be great!
 
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I think block B is still moving when A hits the floor. That's probably what your teacher was talking about (there's no floor to stop B).

So

U_A = K_A+K_B+U_B

Dorothy
 
what is that?

what does U stand for Dorothy?
 
Not only is B moving, but what is the relationship between the speeds of A and B? (They are connected by a rope!)

A useful way to view conservation of energy is in terms of changes:
\Delta{E} = \Delta{KE} + \Delta{PE} = 0

Remember: You want the change in energy of the system--both boxes.

(Dorothy is using U to stand for potential energy.)
 
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