benf.stokes
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Oscillation and Rotation
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)}}
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
T=\frac{2\cdot \pi}{\omega}
\tau= F\cdot r\cdot \sin(\varphi)
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}}}
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)}}
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
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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