Solving Newton's Laws: Mass m Reaches Table in 1.08s

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A mass m=6 kg is released from a height of H=4m on a frictionless table with a mass M=18 kg at an angle of theta=32 degrees. The initial calculation for the time it takes for m to reach the table was found to be t=1.54 s, while the correct answer is t=1.08 s. The discussion highlights the importance of accounting for the acceleration of M, as it is not an inertial frame of reference. The use of conservation of energy and momentum is suggested as a simpler approach to solve the problem. The calculations provided seem to be correct, but the misunderstanding lies in the treatment of the accelerations involved.
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a mass of m=6 kg is free to move without friction on a body with a mass of M=18 kg at an angle of theta=32 deg. M is placed on a friction free table. At the moment t=0 m is released from rest from the top of M at an height of H=4m .

At what moment does m reach to the table?

I'm uploading the question and my solution, which is t=1.54 s, while the correct answer should be t=1.08 s. I'd like to know what I did wrong...
 

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Simon Bridge said:
Compare:
https://www.physicsforums.com/showthread.php?t=66006
Without knowing your reasoning it is difficult to know how to describe the mistake.
The comparison should help you figure it out.

What do you mean "my reasoning"? I can't see why I got the wrong answer and I uploaded a detailed solution... Obviouslly I have a mistake along the way...
 
assaftolko said:
What do you mean "my reasoning"? I can't see why I got the wrong answer and I uploaded a detailed solution... Obviouslly I have a mistake along the way...

At the end of your attempt, you get the acceleration of m w.r.t. M. However, M itself is accelerated. It is not an inertial frame of reference and I do not see you have made any attempt to account for that.

Nor do I think it is required. I think all you need is conservation of energy and horizontal momentum.
 
voko said:
At the end of your attempt, you get the acceleration of m w.r.t. M. However, M itself is accelerated. It is not an inertial frame of reference and I do not see you have made any attempt to account for that.

Nor do I think it is required. I think all you need is conservation of energy and horizontal momentum.

But I did account for that, I got the acceleration of m w.r.t M using the Delambre force on m. And relative to M, m passed the distanc L did it not?
 
You may have tried, indeed. Problem is, I find it difficult to distinguish a_M from a_m in that picture. Could you post the equations here to avoid any misunderstanding?
 
voko said:
You may have tried, indeed. Problem is, I find it difficult to distinguish a_M from a_m in that picture. Could you post the equations here to avoid any misunderstanding?

The first 2 equations are on M and in the second one it's aM. and it says: "aM is the accerleration of M relative to the ground!".

The next equation is the Fy equation on m, and it says:

N+m*aM*sin(theta)-mgcos(theta)=0 where m*aM*sin(theta) is the Delambre force in the y-axis direction of m's coordinate system (drawn at the right side of the picture)

After that linr I simply put N=(M*aM)/sin(theta) and after some calculations you get an expression for aM.

Afterwards the Fx equation for m is written and it says:

m*aM*cos(theta)+mgsin(theta)=m*am where m*aM*cos (theta) is the Delambre force in the x-axis direction of m's coordinate system. After I put the expression I got for aM you can get an expression for am, which is the acceleration of m relative to M.

Hope this helps
 
I have followed your derivation and I cannot spot any problem with it.

Moreover, if your expression for a_m is simplified, it can be seen that in the limit of infinite M it results in a_m = g sin \theta, as it should be for the immovable wedge, and in the limit of \theta → \pi / 2 it results in a_m = g, again as it should be. So I have strong reasons to believe that your solution is correct.
 
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