Conservation of angular momentum of pucks

AI Thread Summary
The discussion centers on the conservation of angular momentum involving two identical pucks connected by a rod and a third puck striking one of them. The key equation for angular momentum is given as L = Iω, where I is the moment of inertia. The moment of inertia for the system is expressed as I = (1/2)MR^2. Participants are seeking to incorporate the initial and final velocities of the pucks, vi and vf, into the conservation equation without needing to solve for them. Clarification is also sought regarding whether there is a fixed pivot at the center of the rod.
dman_PL
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Homework Statement



Two identical pucks, each of inertia m, are connected to a rod of
length 2r and negligible inertia that is free to rotate about its center. A third puck of inertia m strikes one of the connected pucks perpendicular to the rod with a speed vi

Write the expression for conservation of angular momentum in terms of m, vi, the
final velocity of the puck, vf , and ω, the angular speed of the connected pucks. No I’s should be left. You do not need to solve these for vf and ω


Homework Equations


Well angular momentum is L=Iω
I=(1/2)MR^2



The Attempt at a Solution


I have L=((1/2)MR^2)(ω)

However I don't see where the Velocities should go
 
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dman_PL said:

Homework Statement



Two identical pucks, each of inertia m, are connected to a rod of
length 2r and negligible inertia that is free to rotate about its center. A third puck of inertia m strikes one of the connected pucks perpendicular to the rod with a speed vi
I am not clear about the question. Is there a fixed pivot at the centre of the rod?

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