What is the Speed of a Falling Object Attached to a Rotating Spherical Shell?

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Homework Help Overview

The problem involves a uniform spherical shell rotating about a vertical axis, with a light cord attached to a small object that falls under gravity. The objective is to determine the speed of the falling object after it has descended a distance h, utilizing the work-energy theorem.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of the work-energy theorem and the relationship between gravitational potential energy and kinetic energy for both the falling object and the rotating shell. There are questions about the correct moment of inertia for the spherical shell and the pulley, as well as the relationship between linear and angular speeds.

Discussion Status

Participants are actively engaging with the problem, exploring different interpretations of the equations involved. Some have provided clarifications regarding the moment of inertia and the relationship between linear and angular velocities, while others express confusion about their calculations and the expected results.

Contextual Notes

There is a lack of specific information regarding the masses of the objects involved, which has led to some uncertainty in the calculations. Participants are also questioning the assumptions made about the moment of inertia for the pulley and the spherical shell.

CoreanJesus

Homework Statement


A uniform spherical shell rotates about a vertical axis on frictionless bearings. A light cord passes around the equator of the shell, over a light, frictionless pulley, and is attached to a small object that is otherwise free to fall under the influence of gravity. Calculate the speed of the object after is has fallen a distance h from rest. Use the work-energy theorem.
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2woiith-png.png

2woiiTh

2woiiTh

Homework Equations


2woiiTh

Well the Work-energy Theorem :P and the Rotational Inertia for a Sphere and disk

The Attempt at a Solution


So assuming that the rotational inertia is given, I used the right equations but one step confuses me. I set the Gravitational potential energy of block m equal to the kinetic energy of the block m, rotational kinetic energy of M and I.
To take into account the kinetic energy of the disk, I tried to do the same thing I did for the sphere but it didn't work. Am I missing something?
The answer is
ffZLnox.png
 

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Are the masses of the sphere, pulley, and the falling object given?
 
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No all variables
and the link should work... (hopefully)
 
This is the figure (just copy and paste)
2woiiTh.png

Determine the speed of the falling object in terms of the mass and radius of the sphere, the moment of inertia and radius of the pulley and the mass of the falling object. You have to know how the linear speed of the falling object is related to the angular speeds of the sphere and pulley.
 

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mgh=1/2 I(s)*w^2 + 1/2 I(p)*w^2 + 1/2 mv^2 right?
 
CoreanJesus said:
mgh=1/2 I(s)*w^2 + 1/2 I(p)*w^2 + 1/2 mv^2 right?
Not quite. The string moves with certain linear velocity, and it does not slip neither on the pulley nor on the sphere. So the linear speed of the perimeters is the same as the speed of the falling object, but the angular speeds are different. How is the angular speed and linear speed related?
 
V=rW?
 
CoreanJesus said:
V=rW?
Yes, V=radius times ω. The radius of the sphere is R, that of the pulley is r.
 
But the answer that I get using this method is wrong...
I don't get 3I as the denominator
 
  • #10
CoreanJesus said:
But the answer that I get using this method is wrong...
I don't get 3I as the denominator
The given answer can be wrong. What did you get?
 
  • #11
CoreanJesus said:
But the answer that I get using this method is wrong...
I don't get 3I as the denominator
I get the given answer. Please post your working.
 
  • #12
CoreanJesus said:
But the answer that I get using this method is wrong...
I don't get 3I as the denominator
3I is not the denominator. What did you use as the moment of inertia for the spherical shell?
 
  • #13
ehild said:
3I is not the denominator. What did you use as the moment of inertia for the spherical shell?
I assumed CoreanJ meant 3I in the denominator.
 
  • #14
So I set mgh=1/2 I(s)*w^2 + 1/2 I(p)*w^2 + 1/2 mv^2
So mgh=(1/2)(2/3)mR^2(V/R)^2 + (1/2)(1/2)(IR^2)(V/R)^2 + (1/2)mV^2
Simplifying 6mgh=2mV^2 + (3/2)IV^2 + 3mV^2 And I know that this can't simplify into the proper answer...
Why does r remain for the kinetic energy of the the disk as I'm assuming that must be the case for the answer to be what it is... And what is wrong with my equation for the inertia for a pulley? is it not a solid disk?
 
  • #15
CoreanJesus said:
(2/3)mR^2
M, not m.
CoreanJesus said:
(1/2)(IR^2)
I is the moment of inertia of the pulley, not the mass.
Also, you have the wrong angular speed for the pulley. The radius is r, not R.
 
  • #16
Wait WHAT? so the I that's given by the pulley is the inertia given to you?
 
  • #17
CoreanJesus said:
Wait WHAT? so the I that's given by the pulley is the inertia given to you?
Yes. You do not know its mass, or whether it is a uniform disk.
Also note the edit I just made at the end of my previous post.
 
  • #18
Well... That makes this problem easier and solvable :P Thank you for the clarification!
 
  • #19
CoreanJesus said:
Well... That makes this problem easier and solvable :P Thank you for the clarification!
Ok.
The question statement should have made it clear, but the use of the symbol I was a clue, and dimensional analysis of the supposed answer makes it certain.
 

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