Solving Goldstein Problems: Point Mass vs. Hoop on Fixed Hemisphere

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SUMMARY

The discussion centers on solving Goldstein problems involving a point mass and a hoop on a fixed hemisphere under the influence of a gravitational field (g). It is established that the point mass detaches from the hemisphere at a smaller angle relative to the vertical compared to the hoop. This difference is attributed to the hoop's moment of inertia, which causes it to convert some energy into rotational kinetic energy, resulting in slower translational speed. The presence of friction affects the hoop's ability to roll without slipping, complicating the dynamics further.

PREREQUISITES
  • Understanding of classical mechanics principles, specifically dynamics and motion.
  • Familiarity with Goldstein's classical mechanics problems.
  • Knowledge of moment of inertia and its impact on rotational motion.
  • Concept of centripetal force in gravitational fields.
NEXT STEPS
  • Study the equations of motion for rigid bodies in classical mechanics.
  • Explore the concept of moment of inertia and its effects on rolling objects.
  • Research the dynamics of friction and its role in rolling without slipping.
  • Investigate the implications of frictionless surfaces on motion dynamics.
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Students and professionals in physics, particularly those focusing on classical mechanics, as well as educators seeking to explain complex motion dynamics involving rigid bodies.

robb_
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I just solved two of Goldstein problems. let me give you the gist.
1. A point mass is on a fixed hemisphere under the influence of a g field.
2. A hoop is on a fixed hemisphere under the influence of a g field.

I have found the equations of motion, etc... no probs there.
I found that the point mass will leave the sphere at a smaller angle than the hoop. Here the angle is measured w.r.t the vertical.
I would not have guesed this and am wondering if anyone has a good conceptual explanation for this. thanks
 
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I presume the hoop is rolling without slipping down the hemisphere (there is friction present).

In any case, gravity provides the centripetal force. But at some point the object is going too fast for the radial component of gravity to provide enough force to keep it in contact with the sphere. But note that the hoop rolls as well as translates--thus it takes longer to build up enough speed. (It's change in gravitational PE must support rotation as well as translation.)
 
robb_ said:
I just solved two of Goldstein problems. let me give you the gist.
1. A point mass is on a fixed hemisphere under the influence of a g field.
2. A hoop is on a fixed hemisphere under the influence of a g field.

I have found the equations of motion, etc... no probs there.
I found that the point mass will leave the sphere at a smaller angle than the hoop. Here the angle is measured w.r.t the vertical.
I would not have guesed this and am wondering if anyone has a good conceptual explanation for this. thanks

I would say that this is reasonable given that at any given angle, the point mass is moving faster than the hoop. The reason is of course th emoment of inertia of the hoop, some energy goes into kinetic energy of rotation, leaving less for kinetic energy of translation. In the case of the point mass, all the energy goes into kinetic energy of translation.

My two cents.

Patrick
 
The hoop rolls without slipping as stated in the problem. (Funny though, it turns out that friction will not be large enough to keep it from slipping after a certain angle which can be less than the angle at which the hoop leaves the surface.)
So if I follow the reasoning above, I would guess that for a frictionless hemisphere the angles would be equal?
 
robb_ said:
The hoop rolls without slipping as stated in the problem. (Funny though, it turns out that friction will not be large enough to keep it from slipping after a certain angle which can be less than the angle at which the hoop leaves the surface.)
Right--slipping complicates things, but doesn't change the fact that at any given angle the hoop will be moving slower than the point mass.

So if I follow the reasoning above, I would guess that for a frictionless hemisphere the angles would be equal?
That's what I'd say. Without friction the hoop will not rotate, so its speed will match that of the point mass.
 
Thank you greatly.
 

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