Rotation and Linear Bonus Problem Help

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The discussion revolves around a physics problem involving two disks connected by a negligible mass rod, rotating about a vertical axis with friction acting to bring the system to rest. Participants are focused on deriving expressions for the frictional torque and the time it takes for the system to stop. Key points include the need to calculate the moment of inertia using the parallel axis theorem and the relationship between angular acceleration and torque. The conversation emphasizes using angular kinematics equations to find the time until the system halts. Overall, the participants are seeking clarity on applying these concepts to solve the problem effectively.
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Homework Statement



A system consists off two small disks of masses m and 2m that are on a plane. The length that connects the two mass is of negligible mass is is 3L long. The rod is free to rotate on a vertical axis P and the mass 2m lies L away from P and the mass m lies 2L away from P. The two disks rest on a horizontal surface and the coefficient of friction is U. At time t = 0, the rod has an initial counterclockwise angular velocity of Wi about P. The system is gradually brought to rest by friction. develop expressions for the following in terms of u, m, L, g, and Wi.
a) the frictional torque acting on the system about axis P
b) the time T at which the system will come to rest.

Homework Equations



T=I(alpha)
Wf= Wi + (alpha)t
0 = Wi + (alpha)t

The Attempt at a Solution



Wi - friction = I (alpha)

what do i use for Inertia?
 
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If I'm seeing this problem right: you have a dumbell with a bar of neglible mass rotating about a center of mass right where one would compute it. You need an eqn for moment of inertia, assuming m1 and m2 are point masses. Thats what's missing and what you are asking about.
 
o okay so u use the parallel axis theorom plus the inertia of the two masses from Point P or the center of mass of dumbell bar?
 
well since you're computing about the CM, not sure that the parallel axis theorum enters it, but I suspect you got the right idea. sums of MR^2
 
thanx for replying. Does anyone have an idea how to find time. my teacher gave me a hint in saying use a angular kinemaics equation, the one i wrote along with the problem.

more info on how to confidently do part a would be appreciated but thanks for replyin
 
last post for the night, so assuming you have computed I by summing the two masses times their radii squared, you have a situation that is analogous to a block of mass M moving at an initial velocity of V and subject to a retarding acceleration of Mg*u,

only here you need to look at the retarding torque which are the sum of the frictional forces times their respective moments/I. Thats the question in (a).

Once there, it becomes a V(t)=Vo+at type of problem as you suggest.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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