The conservation of energy applying to TWO objects

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Homework Help Overview

The discussion revolves around the conservation of energy in a system involving a pulley and a block. The original poster references a specific problem from an AP Physics exam, focusing on calculating the rotational inertia of the pulley while questioning the application of energy conservation principles to both objects involved.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the kinetic energy of the block and the pulley, questioning why the rotational inertia is attributed solely to the pulley. There is a discussion about the conservation of mechanical energy and whether it can be applied separately to the block and the pulley.

Discussion Status

Participants are actively engaging with the problem, raising questions about the assumptions made in the solution. Some guidance has been offered regarding the application of conservation of energy to the entire system rather than isolating the block or pulley. The discussion remains open with no clear consensus reached.

Contextual Notes

There are references to external links that are not functioning, which may limit access to the original problem statement. Participants are also navigating the complexities of rotational versus translational kinetic energy in the context of the problem.

flyingpig
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Homework Statement



http://www.collegeboard.com/prod_downloads/ap/students/physics/ap04_frq_physics_cm.pdf

Question 2 part c)

"Calculate the rotational inertia of the pulley"




Answer Key: http://www.collegeboard.com/prod_downloads/ap/students/physics/ap04_frq_physics_cm.pdf



The Attempt at a Solution



Something about the alternative solution makes no sense to me

½m(v² - v₀²) + mg(h - h₀) + ½I(ω² - ω₀²) = 0

½m(v² - 0) + mg(0 - D) + ½I(ω² - 0) = 0

-mgD = -½Iω² - ½mv²

Now here comes the problem the solution said the kinetic energy is the CHANGE for the block, not the pulley, so how come when I is solved, it is assumed that I is for the pulley? Since the energy is calculated for the CHANGE for the block and not the pulley.
 
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The links don't work for me. Maybe they work for someone else.
 
It's on collegeobard AP Physics C 2004 EXAM
 
flyingpig said:
It's on collegeobard AP Physics C 2004 EXAM
OK, but this is no link. If you are requesting our help, you should make it easy for us to provide it.
 
please help...
 
flyingpig said:
Now here comes the problem the solution said the kinetic energy is the CHANGE for the block, not the pulley, so how come when I is solved, it is assumed that I is for the pulley? Since the energy is calculated for the CHANGE for the block and not the pulley.
Only the block changes its gravitational PE, but both the block and pulley change their kinetic energies. The decrease in the block's PE equals the increase in total KE. It's total mechanical energy that is conserved, not just the energy of the block.
 
Doc Al said:
Only the block changes its gravitational PE, but both the block and pulley change their kinetic energies. The decrease in the block's PE equals the increase in total KE. It's total mechanical energy that is conserved, not just the energy of the block.

But shouldn't I be both the pulley and the block, not just the pulley alone?
 
flyingpig said:
But shouldn't I be both the pulley and the block, not just the pulley alone?
What do you mean by 'the pulley alone'? The conservation of energy applies to both together.
 
  • #10
flyingpig said:
But shouldn't I be both the pulley and the block, not just the pulley alone?
I think I see what you're asking now: Why should the rotational inertia (I) apply only to the pulley? Well, the pulley is the only thing rotating. The pulley rotates but doesn't translate, so it has rotational KE only; the block translates but doesn't rotate, so it has translational KE only.
 
  • #11
Doc Al said:
I think I see what you're asking now: Why should the rotational inertia (I) apply only to the pulley? Well, the pulley is the only thing rotating. The pulley rotates but doesn't translate, so it has rotational KE only; the block translates but doesn't rotate, so it has translational KE only.

Is it possible to break the equation into two parts? One for the conservation of energy for the pulley and one for the block? Can you show me if is possible?
 
  • #12
flyingpig said:
Is it possible to break the equation into two parts? One for the conservation of energy for the pulley and one for the block? Can you show me if is possible?
I would not recommend that. To apply conservation of energy to the block alone, you'd have to consider the work done by the external force of the rope.

Applying conservation of mechanical energy to the system as a whole is the easy way, since no external work is done on the system.
 
  • #13
Wait, I just thought of a better solution, but I am not sure how it works mathematically or is it even right.

Since the block isn't rotating, no moment of inertia exists?
 
  • #14
flyingpig said:
Since the block isn't rotating, no moment of inertia exists?
It has a moment of inertia, but it's irrelevant since the block isn't rotating. As I said in post #10, the block has no rotational KE.
 

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