Kleppner Mechanics: Disk and coil spring

AI Thread Summary
The discussion revolves around a solid disk attached to a coil spring that can undergo simple harmonic motion, with participants analyzing the frequency of this motion. The first part of the problem is solved, confirming the disk's ability to oscillate, but confusion arises in part (b) regarding the effect of added mass from sticky putty on the disk's frequency. Participants emphasize the importance of distinguishing between angular frequency and instantaneous rotation rate, suggesting that the conservation of angular momentum should be applied correctly to find the new frequency. There is a consensus that the calculations need to be clearly laid out to avoid misunderstandings. The overall focus is on accurately determining the new frequency after the putty is added, highlighting the need for careful consideration of rotational dynamics.
MARX
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Homework Statement



A solid disk of mass M and radius R is on a vertical shaft. The shaft is attached to a coil spring that exerts a linear restoring torque of magnitude Cθ, where θ is the angle measured from the static equilibrium position and C is a constant. Neglect the mass of the shaft and the spring, and assume the bearings to be frictionless.

(a) Show that the disk can undergo simple harmonic motion, and find the frequency of the motion.

(b) Suppose that the disk is moving according to θ = θ0 sin (ωt), where ω is the frequency found in part (a). At time t1 = π/ω, a ring of sticky putty of mass M and radius R is dropped concentrically on the disk. Find:

(1) The new frequency of the motion.

Homework Equations


Ei = Ef

The Attempt at a Solution


to get w=w0/√3

I don't understand why if energy is conserved (I know E is always conserved) helps? why just rotational, the putty is moving down with speed and height?! Too many unknowns!
conservation of angular momentum equation has 2 unknowns..
Thanks for any help[/B]
 
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So assume the bearing is tightly clamped on the shaft and only consider the angular motion. You wil need more equations...
 
BvU said:
So assume the bearing is tightly clamped on the shaft and only consider the angular motion. You wil need more equations...
Solution only uses change in I to arrive at w. I did part a no problem there but for frequency I am not convinced. Why not:
Li=Lf then wi*Ii=wf*If. only unknown is wf but then you get w0/3 not w0/√3
 
You forgot your list of symbols.
And to post your steps, not just the outcome.
 
MARX said:
Li=Lf then wi*Ii=wf*If. only unknown is wf but then you get w0/3 not w0/√3
It is not entirely clear what you are doing there.
Perhaps you are confusing the angular frequency, ω, in part b with the instantaneous rate of rotation, dθ/dt, at time t1.
It will become clear if you post all your steps, as BvU asks.
 
haruspex said:
It is not entirely clear what you are doing there.
Perhaps you are confusing the angular frequency, ω, in part b with the instantaneous rate of rotation, dθ/dt, at time t1.
It will become clear if you post all your steps, as BvU asks.
Hello,
Sure attached
IMG-0271.JPG
 

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MARX said:
Hello,
Sure attachedView attachment 228751
If you must post working as an image (images are for diagrams and textbook extracts - read the guidelines), please ensure it is the right way up!

As I suggested, you are confusing the angular frequency with the instantaneous rate of rotation.
The angular momentum at time t is Idθ/dt. This varies. You are asked for the new angular frequency, which will not vary with time.
You can ignore whatever was going on before the putty hit. Just calculate the angular frequency of the disc+putty system from scratch.
 
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