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

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Homework Help Overview

The discussion revolves around two problems from Goldstein's mechanics, focusing on the dynamics of a point mass and a hoop on a fixed hemisphere under the influence of a gravitational field. Participants explore the conditions under which each object leaves the surface of the hemisphere, specifically comparing the angles at which they do so.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the motion of a point mass versus a hoop, questioning the conceptual reasons behind the differences in the angles at which they leave the hemisphere. There is exploration of energy distribution between translational and rotational motion for the hoop.

Discussion Status

Some participants have provided insights into the mechanics involved, particularly regarding the role of moment of inertia and energy conservation. There is an ongoing exploration of the implications of friction and the conditions under which the hoop may slip, with no explicit consensus reached on the conceptual explanations.

Contextual Notes

Assumptions regarding the rolling condition of the hoop and the effects of friction are under discussion. The potential for slipping at certain angles is noted, which may influence the dynamics of the problem.

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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