Moment of inertia and angular velocity of a uniform disk

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Homework Help Overview

The problem involves determining the moment of inertia and angular velocity of a system consisting of a uniform circular disk and two particles attached to its diameter. The disk has a mass of 4m and radius a, and the system rotates about a horizontal axis through a point on the diameter. The system is released from rest when the diameter is horizontal.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the application of the parallel axis theorem to calculate the moment of inertia. Some express uncertainty about relating the moment of inertia to angular velocity and the energy conservation principles involved. Others question the clarity of the problem setup and the assumptions made regarding the initial conditions.

Discussion Status

Participants have shared their calculations and interpretations of the moment of inertia. Some have provided hints regarding the use of conservation of energy to approach the second part of the problem. There is an ongoing exploration of the relationship between kinetic energy and the moment of inertia, with some participants expressing uncertainty about the energy calculations.

Contextual Notes

There is mention of a diagram that aids in understanding the problem, but initial posts indicate confusion about the orientation of the disk and the setup of the system. Participants are working within the constraints of the problem as stated, with a focus on deriving relationships between the physical quantities involved.

Sara583
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Homework Statement



Two particles, each of mass m, are attached one to each end of a diameter PQ of a uniform circular disk, of mass 4m, radius a with its centre at O. The system is free to rotate about a horizontal axis through A, a point on PQ such that OA = b as indicated in the diagram below. The system is released from rest when PQ is horizontal.[/B]
Determine the Moment of Inertia of the system about the axis A, in terms of integer constants, a , b and m.
Determine the angular velocity of the disk plus masses when PQ is vertical. Enter your answer in terms of integer constants, a, b and the acceleration due to gravity g.

Homework Equations


I=ma^2
parallel axis equation I=Icentre of mass + md^2

The Attempt at a Solution


I already calculated the moment of inertia using the parallel axis theorem, which gave me 4ma^2+6mb^2, but now I'm not entirely sure how to relate the acceleration to the moment of inertia to find the angular velocity. Any suggestions very welcome.

Thanks
 
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Welcome to PF;
Hint: describe what sort of motion you expect.
See also: Newtons laws and/or conservation of energy.
 
Last edited:
Sara583 said:
Two particles, each of mass m, are attached one to each end of a diameter PQ of a uniform circular disk, of mass 4m, radius a with its centre at O. The system is free to rotate about a horizontal axis through A, a point on PQ such that OA = b as indicated in the diagram below. The system is released from rest when PQ is horizontal.
Determine the Moment of Inertia of the system about the axis A, in terms of integer constants, a , b and m.
Determine the angular velocity of the disk plus masses when PQ is vertical. Enter your answer in terms of integer constants, a, b and the acceleration due to gravity g.
I don't see a diagram, and the description does not make clear whether the disk starts in a vertical plane or in a horizontal plane.
Sara583 said:
I already calculated the moment of inertia using the parallel axis theorem, which gave me 4ma^2+6mb^2
Whichever interpretation I use, I don't get that formula. Please post your working.
 
here is the diagram for the problem:
My working for part a was)
parallel axis theorem: Icentre of mass + md^2
d= b , total mass = 6m
(ma^2 + ma^2+ 1/2(4m)a^2)+ 6m(b)^2
2ma^2+2ma^2+6mb^2
4ma^2+6mb^2
Hopefully it makes more sense with the diagram now. The program has marked my answer has correct so I assumed I hadn't misapplied the above theorem but if I have, please tell me.
 

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Sara583 said:
here is the diagram for the problem:
My working for part a was)
parallel axis theorem: Icentre of mass + md^2
d= b , total mass = 6m
(ma^2 + ma^2+ 1/2(4m)a^2)+ 6m(b)^2
2ma^2+2ma^2+6mb^2
4ma^2+6mb^2
Hopefully it makes more sense with the diagram now. The program has marked my answer has correct so I assumed I hadn't misapplied the above theorem but if I have, please tell me.
Ah yes, my mistake.
So have you done the whole question now, or are you still stuck on the second part? Did you try conservation of energy as Simon suggested?
 
I know that K = 1/2 Iω^2 but I'm still a bit unsure how to calculate the total energy beforehand. Am I missing something?
 
Sara583 said:
I know that K = 1/2 Iω^2 but I'm still a bit unsure how to calculate the total energy beforehand. Am I missing something?
The gain in KE has come from a loss of energy somewhere else. What is the nature of that loss and how can you calculate it?
 
Thank you very much! I did manage to solve it in the end using your hints about energy loss.
 

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