Solving Exchange of Momentum by Conserving Energy & Momentum

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SUMMARY

The discussion centers on the mechanics of a block of wood shot upwards from two different points: the center and near the support ends. Using conservation of momentum and energy, it is established that the center of mass (COM) rises to the same height in both scenarios, despite the rotational effects introduced when the block is shot off-center. The key takeaway is that while the energy is conserved, the distribution between translational and rotational kinetic energy varies, leading to different dynamics in energy transfer. The equation 1/2 mu² + 1/2 Iω² = (m+M)gh accurately describes the energy conservation in both cases.

PREREQUISITES
  • Understanding of conservation of momentum and energy principles
  • Familiarity with translational and rotational kinetic energy concepts
  • Knowledge of center of mass (COM) and its significance in mechanics
  • Basic grasp of angular momentum and its effects on motion
NEXT STEPS
  • Explore the implications of rotational dynamics in mechanical systems
  • Study the conservation of angular momentum in various physical scenarios
  • Investigate the differences between translational and rotational kinetic energy
  • Watch educational videos on similar mechanics problems for visual understanding
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in the principles of dynamics and energy conservation in physical systems.

pukb
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Imagine a block of wood resting on two supports at each end. You point a gun upward under the block and shoot the block upwards.

One scenario is you shoot the block upwards in the exact center. Another scenario is you shoot upwards near one of the support ends. The block is thick enough that in both cases the bullet comes to rest inside the block.

Question: in which case does the centre of mass of the block rise the highest?

I could quantify the first case (both for velocity and distance rise of cog) using conservation of momentum and conservation of energy as follows:
mu = (m+M)V
1/2(mu^2) = (m+M)gh

Can somebody help me in the second case?
 
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hi pukb! :smile:

hint: in the second case, why does 1/2 mu2 = (m+M)gh not work? :wink:
 
yes, it does apply - what i meant was the heights to which cog is lifted are not same when force is applied at center and at corner because the latter case will cause some rotation as well. The problem is to quantify that
 
hi pukb! :smile:

(btw, it's better to say centre of mass, com, than centre of gravity, cog :wink:)
pukb said:
…the latter case will cause some rotation as well.

yes! … so the kinetic energy will be the "translational" kinetic energy 1/2 mv2 plus the rotational kinetic energy 1/2 Iω2 :wink:
 
There's a video of this very problem on YouTube. The results are not exactly what you'd expect. The video does compare two wooden blocks, one shot thru the CG and the other shot off-center. Both went the same height into the air. Of course, this raises the question of what happened to the conservation of energy. The block that's spinning should not go as high into the air due to energy being transferred as angular momentum. But it does. What gives?

The video proposed an answer that both blocks must go the same height in order to conserve linear momentum. The difference in energy is due to the bullet not traveling as far into the wood (doing work in the process) and that difference in work is getting translated into angular energy.

Yes, it's not a comforting explanation. But it does seem to be correct.
 
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Hi Ryoko! :smile:

Yes, I didn't think this through fully :redface:: the energy equation which I said didn't work …
tiny-tim said:
hint: in the second case, why does 1/2 mu2 = (m+M)gh not work? :wink:

should be 1/2 mu2 + 1/2 Iω2 = (m+M)gh + 1/2 Iω2,

which of course is the same equation, with the same u (since u is fixed by conservation of momentum, irrespective of ω and of the slight difference in I).

So h (the height) will be the same in both cases.

Thanks, Ryoko. :smile:
 

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