What is the final angular velocity when two rotating disks are pushed together?

AI Thread Summary
The discussion centers on determining the final angular velocity of two rotating disks when they are pushed together. The first disk has a moment of inertia I and angular velocity ω, while the second disk has a moment of inertia 2I and angular velocity ω/2. Participants clarify that the conservation of angular momentum applies, leading to the equation I1ω1 + I2ω2 = (I1 + I2)ωc for calculating the common angular velocity ωc. There is a correction regarding the initial misunderstanding that involved energy equations, emphasizing that heat dissipation occurs when the disks contact. The final approach correctly focuses on angular momentum conservation to solve the problem.
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Homework Statement


Two disks are rotating about an axis common to both. The first disk has moment of inertia I and angular velocity ω. The second disk has moment of inertia 2I and angular velocity \frac{ω}{2}
Both rotate in same direction
If both disks are pushed into each other what is the angular velocity of the larger disk when both are rotating together?

xa9TyS2.png


The Attempt at a Solution


I don't know how to solve this.
I was thinking in I+2I = \frac{ω}{2} + ω but that doesn't make sense.
Any idea in how to start solving this?
 
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duplaimp said:

Homework Statement


Two disks are rotating about an axis common to both. The first disk has moment of inertia I and angular velocity ω. The second disk has moment of inertia 2I and angular velocity \frac{ω}{2}
Both rotate in same direction
If both disks are pushed into each other what is the angular velocity of the larger disk when both are rotating together?

xa9TyS2.png


The Attempt at a Solution


I don't know how to solve this.
I was thinking in I+2I = \frac{ω}{2} + ω but that doesn't make sense.
Any idea in how to start solving this?

Conservation of angular momentum.
 
[1/2 Iω^2]1 + [1/2 Iω^2]2 = 1/2 (I1 + I2)ωc^2
Where ωc is the common angular velocity
 
siddharth23 said:
[1/2 Iω^2]1 + [1/2 Iω^2]2 = 1/2 (I1 + I2)ωc^2
Where ωc is the common angular velocity

EDIT:
this is not conservation of angular momentum. It's an energy equation which is invalid since heat is dissipated when the two disks conjoin.
 
Last edited:
rude man said:
EDIT:
this is not conservation of angular momentum. It's an energy equation which is invalid since heat is dissipated when the two disks conjoin.

Oh my bad. That's a very specific case. Sorry.

I1ω1 + I2ω2 = (I1 + I2)ωc
 
siddharth23 said:
Oh my bad. That's a very specific case. Sorry.

I1ω1 + I2ω2 = (I1 + I2)ωc

That is correct.
 
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