Natural Period of Vibration for Mass with Torque

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Homework Help Overview

The problem involves determining the natural period of vibration for a body of arbitrary shape that is hanging and pinned at the top. The body has a mass, a mass center, and a radius of gyration, and the discussion centers around the dynamics of its motion when displaced from equilibrium.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive the natural period using torque equations and the small angle approximation. Some participants question the definition of the radius of gyration and the correctness of the derivation. Others suggest comparing the derived differential equation to that of a harmonic oscillator to identify parameters.

Discussion Status

The discussion is active, with participants providing hints and clarifications. There is acknowledgment of potential confusion regarding the derivation, but some guidance has been offered regarding the comparison to the harmonic oscillator equation. The original poster expresses gratitude for the assistance received.

Contextual Notes

There is a noted lack of definition for the radius of gyration, which may affect the clarity of the derivation. The discussion also reflects a typical homework context where participants are navigating through assumptions and mathematical relationships.

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Homework Statement



A body of arbitrary shape has a mass m, mass center at G with a distance of D and a radius of gyration about G of K. It is hanging, and pinned at the top. If it is displaced a slight amount of angle P from it's equilibrium position and released, determine the natural period of vibration.

Homework Equations


The Attempt at a Solution



Sum of Torques = Ia. Hence, I = K2m

The torque applied by gravity: -mgDSinP = K2ma

Hence, mgDSinP + K2ma = 0
By the small angle approximation..

mgDP + K2mP'' = 0

Is this correct so far? I am lost at what to do next,

Cheers,
Adrian
 
Last edited:
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I just have to ask, you have not defined K so I'm not sure your derivation is correct.

Assuming it is correct, you just got your answer. HINT: Compare your final differential equation with the harmonic oscillator differential equation.

i.e.Compare
<br /> \ddot{x} + \omega^{2}x = 0<br />

with yours:

<br /> \ddot{P} + \frac{K^{2}}{g D} P = 0<br />
the rest is just identification.

Tell me if this was helpful, good luck.
 
Last edited:
Hello,

Thanks for that! I am a little confused about how the K2 coefficient moved from the angular acceleration to the angle, though? ^^
 
Oh my bad, just a typo. Here's the good one:

<br /> P + \frac{K^{2}}{g D} \ddot{P} = 0<br />

Just got the P miced up with the P'' for a second.
 
Cheers, thanks for that, I got it! :)

Thanks very much for that, I appreciate your help
Adrian
 

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