Physical pendulum of stick swing

AI Thread Summary
The discussion centers on calculating the moment of inertia for a physical pendulum, specifically a stick pivoted at one end. The stick has a mass of 5.90 kg and a center of gravity located 1.2 m from the pivot, with a swinging period of 3.90 seconds. The initial calculation using the parallel-axis theorem yields a moment of inertia of 11.328 kgm², but this conflicts with results derived from the period. The correct formula for the period of a physical pendulum is provided, emphasizing the need to consider the moment of inertia about the pivot and the distance to the center of mass. The conversation highlights the importance of assumptions regarding the stick's mass distribution in these calculations.
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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.
 
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Thanks! :smile:
 
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