Solving Rotational Kinetic Energy with Mass M2 Added

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Homework Help Overview

The discussion revolves around a problem involving rotational kinetic energy in a system of particles connected by a rod. The setup includes two fixed masses (M1 and M3) and a movable mass (M2) that slides along the rod, with a focus on the implications of adding M2 on the moment of inertia and the center of mass.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the addition of mass M2 and its effect on the center of mass and moment of inertia. Questions arise about the treatment of the masses independently and the definition of the center of mass for the system.

Discussion Status

Some participants have provided clarifications regarding the definitions of the center of mass and the moment of inertia, suggesting that the axis of rotation is fixed and does not change with the addition of M2. There is an acknowledgment of the need to consider the rotational kinetic energy of the masses separately.

Contextual Notes

Participants note that the problem is derived from a textbook on Lagrangian Dynamics, indicating a focus on theoretical understanding rather than practical homework. There is a recognition of the constraints imposed by the definitions used in the problem.

H_man
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Hi,

I am rather perplexed by the solution to the following problem.

Particles of mass M1 and M3 are fastened to the ends of a light rod having a length l. A bead of mass M2 is free to slide along the rod between M1 and M3. Point p is the center of mass of M1 and M3, not including M2.

I is the moment of inertia of the M1, M3 rod arrangement about an axis perpendicular to the rod and passing through p . All motion is considered in a plane.

Now the translational aspect of the KE is very simple. But it was the rotational part that had me confused.

In my humble opinion we cannot use I and p coz as we add M2 the center of mass changes.

However in the answer for the rot. KE they have

[tex]\frac{1}{2}[/tex] I @theta/@dt + [tex]\frac{1}{2}[/tex] M2[.........]

The thing that bothers me is that surely with the addition of M2, the value of p and hence I would change. So how can they treat the other masses independently from the third?

:confused:


I hope I have been fairly clear and am not being too silly.

Thanks guys!
 
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hmmm, I see this has been moved.

In fairness to me I should point out that this is not my homework and I am not at college.

The problem comes from a textbook on Lagrangian Dynamics I thought I would work through for interest.

:redface: :redface: :redface: :redface: :redface: :redface:
 
The thing that bothers me is that surely with the addition of M2, the value of p and hence I would change. So how can they treat the other masses independently from the third?

Adding M2 does change the total CoM, but you should recall the superposition principle. The center of mass of the whole system relies on where M2 is placed, but 'p' is defined to be the CM of M1 and M3, which are not moving. The axis of rotation is through this point and is also fixed. Adding M2 to a point on the beam does change the total center of mass, but it does not affect 'p' by definition.
 
Yes you are right. They can't use same I and P if they consider all the three masses as a single system, but I think they are calculating the rotational kinetic energy of M1, M3 system and M2 separately and then adding them, and therefore no question for I of the system with M1,M2 and M3.
 
Thanks Whozum,

Seeing it put in other words makes things a lot clearer!

I did not realize that the axis was a constraint on the system.

cheers to u too Mukundpa,

H_Man
 
Last edited:

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