What Angle Causes a Mass to Leave a Frictionless Sphere?

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Homework Help Overview

The problem involves a point mass sliding down a frictionless sphere and seeks to determine the angle at which the mass leaves the surface of the sphere. The context is rooted in classical mechanics, specifically focusing on forces acting on the mass and energy conservation principles.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the conditions under which the normal force becomes zero and the application of Newton's second law in the radial direction. There are attempts to relate potential energy changes to kinetic energy and to express velocity as a function of position.

Discussion Status

The discussion is active, with participants exploring various equations and concepts related to energy conservation and forces. Some guidance has been offered regarding the relationships between potential and kinetic energy, and there is a collaborative atmosphere as participants share insights and hints.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can use or the methods they can apply. There is an emphasis on deriving relationships rather than applying direct solutions.

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Homework Statement


A point mass m starts from rest (at the top of a sphere) and slides down the surface of the frictionless solid sphere of radius r.

Find the angle at which the mass flies off the sphere.




Homework Equations






The Attempt at a Solution



Well, all I know is that at that point, the Normal force will be zero. Also, that it is moving in a circular way.. so that we will have mv^2/r for its radial components and some other tangential components..

please help.. thanks
 
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Start by drawing a free body diagram at an angle θ
 
I have a free body diagram, I don't know what equations to use :S

thanks
 
Now, write out Newton's second law for the radial direction.
 
okay, so m v^2/ r = mgsintheta - N? When it falls off, N will be 0

thanks
 
holezch said:
okay, so m v^2/ r = mgsintheta - N? When it falls off, N will be 0

thanks

Yes so now find what mv2/r works out to be using conservation of energy.
 
hmm.. so should I express v in terms of kinetic energy and stuff? like from 1/2mv^2.. et c

thanks
 
holezch said:
hmm.. so should I express v in terms of kinetic energy and stuff? like from 1/2mv^2.. et c

thanks

yes that will help.
 
okay, so I got -mgr(1-cos theta) as the change in PE in this case.. I'm having trouble expressing the KE though.. any hints? I need to express the velocity as the function of the position.. the angle..

thanks
 
  • #10
holezch said:
okay, so I got -mgr(1-cos theta) as the change in PE in this case.. I'm having trouble expressing the KE though.. any hints? I need to express the velocity as the function of the position.. the angle..

thanks

mgr(1-cosθ) = kinetic energy at the angle θ

So you can find what mv2 is equal to.
 
  • #11
rock.freak667 said:
mgr(1-cosθ) = kinetic energy at the angle θ

So you can find what mv2 is equal to.

ah right, of course.. do you mean by the conversation of energy, K = mgr(1-cos theta) at some point?

Thanks! (rats, I should've known)

By the way, thanks for replying back constantly :) there's nothing better than real-time help
 
  • #12
holezch said:
ah right, of course.. do you mean by the conversation of energy, K = mgr(1-cos theta) at some point?

Thanks! (rats, I should've known)

By the way, thanks for replying back constantly :) there's nothing better than real-time help

Well the change in potential energy= change in kinetic energy. Initially there is no kinetic energy so just the change in potential energy is 1/2mv2
 
  • #13
rock.freak667 said:
Well the change in potential energy= change in kinetic energy. Initially there is no kinetic energy so just the change in potential energy is 1/2mv2

ah, I see so:

change in KE = - change in PE..

there is no initial KE, so 1/2 mv^2 = - change in PE

but - change in PE = mgr(1-cos theta)

so 1/2mv^2 = mgr(1-cos theta)

:) woohoo
 
  • #14
awesome, I solved it.. just used mv^2/r and plugged in v from here 1/2mv^2 = mgr(1-cos theta) ...et c :)

Oh.. I had a question, if the tangential part of a force overcomes the radial force, will the object fling out of the orbit?

Thanks
 

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