Calculating KEf for Two Connected Boxes - Frictionless Surface

AI Thread Summary
The discussion revolves around calculating the kinetic energy (KE) of two connected boxes on a frictionless surface, with one box falling 1 meter. The user initially struggles with applying the work-energy theorem and the relationship between potential and kinetic energy. They explore different methods, including conservation of mechanical energy and Newton's second law, to derive the final velocity and subsequently the kinetic energy. The user ultimately finds a negative value for KE due to rounding errors but acknowledges that the kinetic energy should not be zero since the box must have moved. The conversation emphasizes understanding the principles of energy conservation and proper calculations in physics problems.
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Im having trouble with this problem. I know that KE=1/2mv^2 and the Wrok engergy theorm W=KFf-KEo but I am having trouble relating the figure to KE.

Two boxes are connected to each other as show. The system is released from rest and the 1.00 kg box falls 1.00 m. The surface of the table is frictionless. What is the KE of the box before it reaches the floor?

http://dtpcarclub.com/ke.JPG

EDIT-
I was looking itover and I think I kind of know what to do...

I need to find KEf.

KEf=W+KEo

and to find W, W=(F cos 180) s

is that on the right track?
 
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yuuup...sounds right!
 
I got the first part down but now I am having trouble with the basic stuff. I am failing the class right now b/c I know the concepts and the forumulas I just don't know how to work them in problems :frown:

With the W=(F cos 180) 1m How do I find the F? I know F=ma but I don't have the a.

For the Work Engery Theorem, where do I find the vo for 1/2mvo^2
 
Edit: Forgot about the mass of the other block :smile:

I got this with conservation of mechanical energy

m_{b}gh = \frac{1}{2}(m_{a} + m_{b})v^2

If i use Work-Kinetic Energy Principle:

W_{gravity} = \Delta K

Conservative forces work is equal to the change in potential energy caused by them in the system

W_{gravity} = -\Delta \Omega

-\Delta \Omega = \Delta K

0 = \Delta K + \Delta \Omega

which gives:

0 = \frac{1}{2}m_{a}v^2 + \frac{1}{2}m_{b}v^2 - 0 + 0 - m_{b}gh

m_{b}gh = \frac{1}{2}(m_{a} + m_{b})v^2

\sqrt{2 \frac{m_{b}gh}{m_{a} + m_{b}}} = v

Alternatively, you could apply Newton's 2nd Law

\sum_{i=1}^{n} \vec{F}_{i} = m \vec{a}

Analysing our B box it gives

T - m_{b}g = -m_{b}a

m_{b}g - T = m_{b}a

Analysing our A box it gives

T = m_{a}a

Adding both equations

m_{b}g = a(m_{b} + m_{a})

\frac{m_{b}g}{m_{b} + m_{a}} = a

Now using kinematics:

v^2 = v_{o}^2 + 2a \Delta x

v^2 = 0 + 2 \frac{m_{b}g}{m_{b} + m_{a}} \Delta x

\Delta x = h

v^2 = 2 \frac{m_{b}gh}{m_{b} + m_{a}}

v = \sqrt{2 \frac{m_{b}gh}{m_{b} + m_{a}}}
 
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I pluged everything in and found the KEf=-0.01
I think its supposed to be 0, I just rounded wrong. But that can't be right, it has to have some KE before it hits the ground.
and thanks for the help everyone :smile:
 
Why do you say kinetic energy is supposed to be 0??, if the final kinetic energy is 0 then the objet didn't move at all, because it's initial kinetic energy was 0. The gravitational potential energy turned into kinetic energy making the object accelerate and cover a displacement that has a magnitude of 1 meter.

If you want to find the kinetic energy of the B box, just find the speed (magnitude of velocity) in any of the above equations, and then just use

K_{b} = \frac{1}{2}m_{b}v^2
 
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I didnt mean for the KE=0 as in the correct answer, just that with my calculations it came out to -.01 b/c I rounded wrong.

Thanks for the help.
 
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