Kleppner Mechanics: Disk and coil spring

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SUMMARY

The discussion focuses on the mechanics of a solid disk attached to a coil spring, demonstrating that the disk can undergo simple harmonic motion with a derived frequency. The initial frequency is calculated as ω₀, and upon the addition of a ring of sticky putty, the new frequency is determined to be ω = ω₀/√3. Key concepts include conservation of angular momentum and the relationship between angular frequency and instantaneous rotation. Participants emphasize the importance of clearly presenting all steps in calculations to avoid confusion.

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  • Understanding of simple harmonic motion principles
  • Familiarity with angular momentum conservation
  • Knowledge of rotational dynamics and moment of inertia
  • Basic proficiency in solving differential equations related to motion
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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]
 
Last edited:
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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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