Conservation laws (tricky, conceptual,not homework)

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SUMMARY

The discussion focuses on the application of conservation laws in a physics problem involving two masses, m and M, where mass m is pushed on mass M and eventually breaks off. The participants clarify that energy conservation is applicable when the entire system, including both masses and the ground, is considered. The correct equation derived for the speed of the smaller mass upon breaking off is x² = [(M² + Mm + m²)/(M + m)²]v² - 2gh, confirming that the normal force does not perform work in this frictionless scenario.

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f(x)
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Homework Statement
Consider a small body of mass m placed over a larger body of mass M whose surface is horizontal near the smaller mass and gradually curves to become vertical at height h.

f_figure1m_feb2fa4.jpg


The smaller mass is pushed on the longer one at speed v and the system is left to itself.
Assuming all surfaces to be frictionless, find the speed of the smaller mass when it breaks off the larger mass.

My attempt
This problem has been frustrating me for quite some time now. :rolleyes:
I start by assuming the bigger block is moving at speed V to the left when the smaller block is on the vertical and just about to break off.
Then by conserving momentum in horizontal direction : V=\frac{mv}{M+m}
since the small block is also having a velocity component V to the left wrt ground

Now, i am going to use conservation of energy, and this is where I have doubts.
I am not sure whether to choose only the small block & ground as the system , or to choose both blocks & ground as the system. (I am getting answer in neither)

I think that in choosing only the small block and ground as system, an external force by the large block is acting (normal reaction) and thus i cannot use conservation of energy directly. Is this hypothesis correct ?

So, choosing the both blocks and ground as system :
The small block is having a velocity component upwards and velocity component left wards which is V. Let the required speed of the small block at the time of breaking off be x
Since F_{ext}=0
\frac{1}{2}mv^2 = \frac{1}{2}MV^2 + mgh + \frac{1}{2}mx^2
Plz verify whether this equation is correct

Solving, i get x^2=\frac{(v^2-2gh)(m+M)^2-mMv^2}{(m+M)^2}

while the answer is printed as x^2=\frac{(M^2+Mm+m^2)}{(M+m)^2}v^2-2gh

Sorry for the length, but i desperately need some input :cry:
Thx a lot !
 
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Energy is conserved, as you noted. The normal force never causes motion in the direction of that force, therfore, the normal force does not do any work and does not need to be considered in the CoE formulae

But you need another equation, since you have two unkowns.

What else is always conserved?
Edit: oops, you already noted this.

Edit again: TinyTim caught it first. Dang.
 
Last edited:
f(x) said:
Sorry for the length, but i desperately need some input

Hi f(x)! :smile:

The length is fine … you've explained the problem admirably clearly.
Now, i am going to use conservation of energy, and this is where I have doubts.
I am not sure whether to choose only the small block & ground as the system , or to choose both blocks & ground as the system. (I am getting answer in neither)

I think that in choosing only the small block and ground as system, an external force by the large block is acting (normal reaction) and thus i cannot use conservation of energy directly. Is this hypothesis correct ?


ah, I expect you're thinking of am ordinary frictionless roller-coaster or pendulum-type situation, where energy is conserved even though the mass is constrained to move along a curve …

that works because the work done is zero … since there's no friction, the external force is normal to the surface, while the motion is by definition parallel to it …

but here, the force is still normal to the surface, but the motion (relative to the Earth) isn't parallel to it, because the whole system is moving.

So: general principle: energy is conserved only if work done is zero: and in this case you're right (but for the wrong reason … a normal force usually is ok): you must use the whole system. :smile:
Solving, i get x^2=\frac{(v^2-2gh)(m+M)^2-mMv^2}{(m+M)^2}

while the answer is printed as x^2=\frac{(M^2+Mm+m^2)}{(M+m)^2}v^2-2gh

erm … they're the same! :redface:

(M2 + mM + m2) = (M + m)2 - mM :rolleyes:
 
Thx a lot tinytim and Chi Meson for your help :)

tiny-tim said:
but here, the force is still normal to the surface, but the motion (relative to the Earth) isn't parallel to it, because the whole system is moving.
Ah ok thanks

tiny-tim said:
So: general principle: energy is conserved only if work done is zero: and in this case you're right (but for the wrong reason … a normal force usually is ok): you must use the whole system. :smile:

tiny-tim said:
erm … they're the same! :redface:

(M2 + mM + m2) = (M + m)2 - mM :rolleyes:
Oh
I thought the answer meant \frac{(M^2+Mm+m^2)(v^2-2gh)}{M+m)^2} but i was unsure about the reasoning, still wanted to confirm
Thx a lot for those corrections tinytim :)
 

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