Energy Conservation in Angular motion / Moment of Inertia

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Homework Help Overview

The discussion revolves around the conservation of energy in the context of angular motion and moment of inertia, specifically involving a large sphere and a rolling ball. Participants are examining the assumptions made regarding the motion of the sphere and the conditions necessary for analyzing the problem.

Discussion Character

  • Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants are questioning the necessity of assuming that the sphere of radius R remains at rest. There is a focus on understanding the implications of this assumption for solving the problem.

Discussion Status

Some participants have provided insights into why the assumption of the sphere remaining at rest may be valid, suggesting that it simplifies the problem given the lack of information about the sphere's moment of inertia and the ground conditions. Others express a desire for more clarity on the author's intentions and the problem's setup.

Contextual Notes

There is an acknowledgment that the problem may not provide all necessary details, which influences the assumptions participants feel compelled to make. The discussion reflects a mix of interpretations regarding the setup and the role of the sphere in the energy conservation analysis.

EEristavi
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Homework Statement
A uniform ball of radius r rolls without slipping down from
the top of a sphere of radius R. Find the angular velocity of the ball
at the moment it breaks off the sphere. The initial velocity of the
ball is negligible.
Relevant Equations
K = I w^2 / 2
T = F R
U = m g h
I write Conservation of Energy:

Potential Energy loss(change):
U = m g ##\Delta##h = m g (R+r) (1-cos##\alpha##)

kinetic Energy gain(change):
K = (##\frac {m v^2} 2## + ##\frac {I \omega^2} 2##) + (##\frac {M v_2^2} 2## + ##\frac {I_2 \omega_2^2} 2##)

U = K
m g (R+r) (1-cos##\alpha##) = (##\frac {m v^2} 2## + ##\frac {I \omega^2} 2##) + (##\frac {M v_2^2} 2## + ##\frac {I_2 \omega_2^2} 2##)

-----------------

However,
In the solution we have:

m g (R+r) (1-cos##\alpha##) = ##\frac {m v^2} 2## + ##\frac {I \omega^2} 2##

-----------------

As I understand,
big ball doesn't roll (Or we don't consider it's rolling and movement).Need help here..
 
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Assume that the sphere of radius R is and stays at rest. At some point you need to write down the condition for separation of the rolling ball from the sphere.
 
kuruman said:
At some point you need to write down the condition for separation of the rolling ball from the sphere.
Agreed, but first I need to understand what I asked above.

kuruman said:
Assume that the sphere of radius R is and stays at rest
That's my question - why I must consider (or assume) that sphere of radius R stays at rest
 
EEristavi said:
That's my question - why I must consider (or assume) that sphere of radius R stays at rest
There are no hard and fast rules for such. I would assume that it remains at rest because any other assumption would require that we have enough information to calculate the moment of inertia of the sphere whose radius is R and the slipperiness of the ground on which it rests.

Since we do not know those things and since the question is supposed to be answerable, they must not matter. The simplest explanation for why they do not matter is that the sphere whose radius is R remains at rest.

I would expect that it never dawned on the person setting the question that someone might worry whether the sphere underneath could move.
 
EEristavi said:
That's my question - why I must consider (or assume) that sphere of radius R stays at rest
As @jbriggs444 already indicated, you need to make enough assumptions to be able to solve the problem with what is given. It also helps to have encountered a problem and its variants enough times so that you can understand the author's intentions. The standard formulation of this kind of problem has the mass either sliding without friction or rolling without slipping on a hemisphere that is firmly attached to the Earth.
 
Ok, Thank you.
I expected more from the Author... :D
 
EEristavi said:
Ok, Thank you.
I expected more from the Author... :D
If you care to try the case where the large ball can move I'm sure you will get help from this forum. But note that it will make the centripetal acceleration tricky.
 

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