Simple Harmonic Motion of a Rigid Body

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SUMMARY

The discussion focuses on calculating the period of oscillation for a rigid rod of length 0.570 m suspended from a pivot. The relevant equations include the angular frequency formula, omega = (Mgd/I)^(1/2), and the relationship between angular frequency and period, omega = 2π/period. The moment of inertia for the rod is derived using I = (1/3)ML² and the parallel axis theorem, which adds Md² to account for the pivot's location. The correct period of oscillation calculated is 2.15 seconds, confirming the application of the moment of inertia and the distance from the center of mass to the pivot.

PREREQUISITES
  • Understanding of Simple Harmonic Motion (SHM)
  • Familiarity with the moment of inertia and its calculations
  • Knowledge of the parallel axis theorem
  • Basic grasp of angular frequency and its relation to oscillation period
NEXT STEPS
  • Study the derivation of the moment of inertia for various shapes
  • Learn about the applications of the parallel axis theorem in physics
  • Explore the effects of mass distribution on oscillation periods
  • Investigate advanced topics in oscillatory motion, such as damping and resonance
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators seeking to clarify concepts related to rigid body dynamics.

Cintdrix
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Homework Statement



A very light, rigid rod with a length of 0.570 m extends straight out from one end of a meter stick. The stick is suspended from a pivot at the far end of the rod and is set into oscillation. Determine the period of oscillation.


Homework Equations



omega = (Mgd/I)^1/2
omega = 2pi/period.

The Attempt at a Solution



I solved this question, but I was just looking for clarification as to why it was right. The moment of inertia of the rod would be 1/3 ML^2 and using the parallel axis theorem I would have to add Md^2 on top of that.

The masses cancel in the first equation, but I was wondering about the "d" in the numerator. What does it represent? I originally thought it was the distance from the centre of mass to the pivot but it wasn't the case for this problem. Any insight is appreciated.

I when i subbed d=0.57 into the equation i got the correct answer of 2.15s, but I don't understand why.
 
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Cintdrix said:

The Attempt at a Solution



I solved this question, but I was just looking for clarification as to why it was right. The moment of inertia of the rod would be 1/3 ML^2 and using the parallel axis theorem I would have to add Md^2 on top of that.

The parallel axes theorem says that the moment of inertia about distance d from the center of mass is given by

I = ICM + md2, where ICM = (1/12)mL2 for a uniform rod not (1/3)mL2. If you got the right answer, you must have made two errors that canceled each other.
 
True. I was using the moment of inertia about one end of the stick, which is indeed (1/3)mL2. In my case i guess the D was still the distance from the old axis to the new axis. In using the moment of inertia about the CM, and making d the distance between the pivot and the CM, I was able to again get the correct answer.

Thanks for your help
 

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