Oscillation and Rotation: Can You Solve These Equilibrium and Motion Problems?

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The discussion focuses on two physics problems involving oscillation and rotation. The first problem involves a ruler in equilibrium on a cylindrical body, demonstrating that it undergoes oscillatory motion with a specific period formula. The second problem addresses a sphere rolling down an incline without sliding, deriving the acceleration of its center of mass based on gravitational forces and the sphere's moment of inertia. Participants express confusion over the ruler's behavior and the application of the moment of inertia in the second problem. Overall, the thread highlights the complexities of understanding equilibrium and motion in these scenarios.
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Oscillation and Rotation

Homework Statement



Question nr 1:

You have ruler of length L and thickness 2d resting, in equilibrium , on a cylindrical body of radius r. Slightly unbalancing the ruler, and existing attrition between the surfaces prove that the ruler has a oscillatory motion of period:
T = 2\cdot \pi\cdot \sqrt{\frac{L^2}{12\cdot g\cdot (r-d)}}

SemTtulo.jpg


Question nr 2:

Assuming the sphere roles down without sliding prove that the acceleration of it's center of mass is:

a= \frac{g\cdot \sin(\theta)}{1+\frac{2}{5}\cdot \frac{1}{1-\frac{1}{4}\cdot \alpha^2}}

Where g is the gravitational acceleration and
\alpha= \frac{L}{R}

Note: The moment of inertia of the sphere is:
I= \frac{2}{5}\cdot M\cdot R

SemTtulo-1.jpg


Homework Equations



T=\frac{2\cdot \pi}{\omega}

\tau= F\cdot r\cdot \sin(\varphi)

The Attempt at a Solution



At question nr 1 I can't wrap my mind about the idea that the ruler won't immediately begin to fall and in question nr 2 I get to:
a= \frac{g\cdot \sin(\theta)}{1+\frac{2}{5}\cdot \sqrt{\frac{1}{1-\frac{1}{4}\cdot \alpha^2}}}
 
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moment of inertia of sphere is I=(2/5).M.R^2
 
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