Conservation of Energy Physics Olympiad

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SUMMARY

The discussion focuses on the conservation of energy principles applied to a ball of mass M and radius R, which has a moment of inertia I = 2/5MR. The ball rolls down a frictionless ramp and is projected vertically upward, reaching a maximum height ymax. The key equations used include potential energy (PE = mgh), translational kinetic energy (KE = 1/2mv^2), and rotational kinetic energy (Rotational KE = 1/2 I omega^2). The relationship between the maximum height ymax and the initial height h is established through energy conservation, leading to the conclusion that the gravitational potential energy is converted into both translational and rotational energy during the ball's motion.

PREREQUISITES
  • Understanding of potential energy and kinetic energy concepts
  • Familiarity with rotational dynamics and moment of inertia
  • Knowledge of energy conservation principles in physics
  • Ability to relate linear and angular motion (omega and velocity) for rolling objects
NEXT STEPS
  • Study the relationship between linear velocity and angular velocity for rolling objects
  • Learn about the conservation of mechanical energy in different physical systems
  • Explore the derivation of moment of inertia for various shapes
  • Investigate the effects of ramp angles on the motion of rolling objects
USEFUL FOR

Students preparing for physics competitions, educators teaching mechanics, and anyone interested in the principles of energy conservation in rolling motion.

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Homework Statement


A ball of mass M and radius R has a moment of inertia of I =2/5MR. The ball is released from rest and rolls
down the ramp with no frictional loss of energy. The ball is projected vertically upward o a ramp as shown in
the diagram, reaching a maximum height ymax above the point where it leaves the ramp. Determine the maximum
height of the projectile ymax in terms of h
2rwrmud.png


The image is cut off but h is the height from the top of the ramp to the ball

Homework Equations


PE=1/2mv^2
Rotational KE= 1/2 I omega^2
KE= 1/2mv^2

The Attempt at a Solution


Using x as the distance between the bottom and top of the ramp:
mg(h+x) = 1/2mv^2+1/2I omega^2 =1/2mv^2 + 1/2(2/5mr^2)omega^2 = 1/2mv^2 + 1/5mv^2 = 7/10mv^2

7/10mv^2=mgx + 1/2mv'^2

1/2mv'^2 = ymax

im stuck here D: any hints?
 
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Okay so physically the ball rolls down and then exits the ramp spinning and going upward a certain height.

It's energy initially is mgh right? And it's energy afterward will be in the spin and in its motion so if you can determine its rotational energy and subtract it from the mgh you'd have a new mgh right from which to get the final height.

Does that sound right?
 
its energy initally should be mg(h+x), because mgh is just the energy from the top of the ramp to the inital position of the ball
 
I'm not sure why you introduced an x. It rolls from an initial vertical height h, and rises to a height ymax.
 
Don't you need an equation to relate the omega to the ball rolling down with no friction and no slipping? Also do you need the angle of the ramp or does that fall out somewhere? If not I suppose you could choose say 60 degrees or better yet use a variable for it.
 
The clue that is the key to problems like this is to recognize that, by descending without slippage, the rotational speed of the ball is directly related to its linear velocity. When you think about it, it seems obvious, though it may still help if it's spelled out: the ball rotates once in the same time that it rolls a distance 2 Pi R metres.

While you may think the angle of the ramp is needed, it seems not. During the descent, the gravitational potential energy of the ball is totally converted into linear and rotational energy.
 
Sure, however, that still leaves many unknowns. Including the velocity at the bottom and the max y.
 
By equating PE at start to KE + rotational energy on the level, I was able to then obtain a direct proportionality between ymax and h. Recognize that as it rises, the KE is converted into PE while the rotational energy remains as rotational energy.
 

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