Physical pendulum of stick swing

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SUMMARY

The discussion centers on calculating the moment of inertia of a physical pendulum, specifically a stick with a mass of 5.90 kg and a center of gravity located 1.2 m from the pivot. The period of the pendulum is given as 3.90 seconds. The moment of inertia was initially calculated using the parallel-axis theorem, yielding a value of 11.328 kgm². However, confusion arose regarding the relationship between the period and the moment of inertia, leading to a reevaluation of the assumptions about the stick's mass distribution.

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  • Understanding of the parallel-axis theorem in physics
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Problem:

A large stick is pivoted about one end and allowed to swing back and forth as a physical penulum. The mass of the stick is 5.90 kg and its center of gravity (found by finding its balance point) is 1.2 m from the pivot. If the period of the swinging stick is 3.90 seconds, what is its moment of inertia, about an axis through the pivot?

I used the parallel-axis theorem (Ip=Icm+Mh^2)...which turns out to be 1/3ML^2 ...so I get 11.328 kgm^2 as the moment of inertia. I am not sure why the period is given. I know T=(2pi)/omega and omega I think is sqrt(MgL/Ip)...so if I solve for Ip given the period, I get a different Ip than my previous calculation. Any enlightenment would be great.
 
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You assumed that the stick could be approximated with a thin rod of uniform mass distribution. Apparently this assumption is wrong, the stick doesn't have to be of uniform material nor does it have to resemble a rod.
The following equation applies to a physical pendulum:

T = 2 \pi \sqrt{\frac{I_A}{mgl}}

where IA is the moment of inertia about the axis through the pivot and l the distance between the pivot and centre of mass.
 
Last edited:
Thanks! :smile:
 

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