What is the angular speed of a ball sliding on a rotating ring at a given angle?

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SUMMARY

The discussion centers on calculating the angular speed of a ball sliding on a rotating ring at an angle of θ = π/4. The initial angular speed of the ring is denoted as ω₀. By applying the conservation of angular momentum, the final angular speed (ω₂) is derived as ω₂ = (M/(M+m))ω₁ when substituting θ = 45 degrees. The inertia contributions from both the ring and the ball are considered, confirming that angular momentum remains conserved throughout the motion.

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  • Understanding of angular momentum conservation principles.
  • Familiarity with rotational dynamics and inertia calculations.
  • Knowledge of the parallel axis theorem in physics.
  • Basic trigonometry, particularly sine functions for angle calculations.
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Homework Statement


A thin ring of mass M and radius R rotates around its vertical axis. A small ball of mass m can slide, without constraint nor friction, on the ring. If the angular speed of the ring when the ball is at the top is [\tex]\omega_0[\tex], what is the angular speed when the ball is at [tex]\theta=\pi/4[/tex].
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Homework Equations


This is what I can't find. The problem seems easy enough, provided the right path of solution.


The Attempt at a Solution



I tried working with the angular momentum conservation law. That gives:

[tex]L = I\omega[/tex]
where
[tex]I= MR^2[/tex]

The contribution of the ball to the inertia is null, because it is on the axis of rotation at that instant. Hence, we have

[tex]\omega_0 = \frac{L}{MR^2}[/tex]

However, if we include a dependence on [tex]\theta[/tex], we obtain

[tex]L = (I_{ring} + I_{ball})\omega[/tex]
[tex]L = (MR^2 + mR^2\sin^2\theta)\omega[/tex]

Now, that seems bad to me, because (1) it's a bad application of the parallel axes theorem because I can't write the inertia of the ball relative to the center of mass since I do not have its radius and (2) it does give an answer as a fraction of the initial angular speed.

Any ideas?
 
Last edited:
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Since there is no net external torque on the system, angular momentum is conserved
apply conservation of angular momentum.
initially L= {(MR^2)/2}w1 (applying perpendicular axis theorem)
finally, L = {MR^2 + mR^2sin^2(theta)}w2
substitute theta=45
and you get w2= M/(M+m) w1
 
Thank you. I just arrived at the same solution.
 

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