Conservation of energy flywheel experiment

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SUMMARY

The discussion centers on a flywheel experiment that demonstrates the conservation of energy principles using different masses. The potential energy (Ep) of the masses is calculated using the formula mgh, and the relationship between Ep and angular velocity (ω) is analyzed through a graph where the gradient equals 1/2I. Participants clarify that the graph does not pass through the origin due to the kinetic energy of the falling mass, which is not fully converted into the rotational energy of the flywheel. Suggestions for improving the experiment include deriving equations connecting the height of the falling mass to ω² and modifying the axle design to minimize kinetic energy loss.

PREREQUISITES
  • Understanding of potential energy (Ep) and its calculation using mgh
  • Basic knowledge of angular velocity and its relationship to rotational motion
  • Familiarity with graphing techniques and interpreting gradients in physics
  • Concept of energy conservation in mechanical systems
NEXT STEPS
  • Derive the equation connecting the change in height (Δh) of the falling mass with the resultant angular velocity (ω²)
  • Experiment with a conically shaped axle to minimize kinetic energy loss during the mass drop
  • Research the principles of energy conversion in mechanical systems, focusing on potential and kinetic energy
  • Explore mathematical models related to rotational dynamics and energy conservation
USEFUL FOR

Physics students, educators, and hobbyists interested in experimental mechanics and energy conservation principles will benefit from this discussion.

jamie3009
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Hi

Ive recently carried out an experiment where different masses are hung from a string and then dropped from the same height. The other end of the string is wrapped around the axle of a flywheel and when the mass hits the ground, the time for ten revolutions of the flywheel is calculated to give angular velocity. The potential energy of each of the masses is calculated using mgh and a graph of Ep vs ω2 is then plotted with the gradient = 1/2I. I am a bit stuck as to how to explain the graph and explain why the graph doesn't go through 0,0. My thoughts are that as the potential energy of the masses is increased, the kinetic energy of the flywheel also increases, as the angular velocity increases. I think the graph doesn't go through 0,0 to show that the flywheel still has some potential energy in the system when the kinetic energy is 0. Am i correct? Sorry for writing loads :)
 
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Welcome to PF.

Ep is the potential energy of the mass and it is on the Y-axis, right? And the graph is crossing above 0 on the Y-axis? Then you are getting an output energy that is below your input energy. This would be because the weight hits the ground with kinetic energy: you aren't converting all of the potential energy to rotational energy in the flywheel.
 
russ_watters said:
Welcome to PF.

Ep is the potential energy of the mass and it is on the Y-axis, right? And the graph is crossing above 0 on the Y-axis? Then you are getting an output energy that is below your input energy. This would be because the weight hits the ground with kinetic energy: you aren't converting all of the potential energy to rotational energy in the flywheel.

Thats correct. So does that mean that because the mass still has kinetic energy when it hits the floor, some is converted into sound etc and not all into rotational energy of the flywheel?
 
jamie3009 said:
Thats correct. So does that mean that because the mass still has kinetic energy when it hits the floor, some is converted into sound etc and not all into rotational energy of the flywheel?
It's simpler than that. The change in potential energy of the falling mass increases both the kinetic energy of the flywheel and the falling mass. (They are connected by a string.) The energy used to increase the KE of the falling mass is energy not available to increase the KE of the flywheel. Doesn't matter what happens when the falling mass hits the ground.

See if you can derive the equation connecting the Δh of the falling mass with the resultant ω2.
 
Another thing to do would be to alter the experiment. Replace your current axle with a conically shaped axle, that will release the weights at ~zero velocity immediately before they touch the ground. This eliminates the dropping mass kinetic energy variable.

cone.jpg

I'm sure there's a mathematical model for this, but my math skills are pretty much gone.
 

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