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benf.stokes
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Homework Statement
Assuming the sphere roles down without sliding prove that the acceleration of it's center of mass is:
[tex] a= \frac{g\cdot \sin(\theta)}{1+\frac{2}{5}\cdot \frac{1}{1-\frac{1}{4}\cdot \xi^2}}[/tex]
[tex]Where \ \xi=\frac{L}{R}[/tex]
Note that the moment of inertia of the sphere is:
[tex]I_{sphere}=\frac{2}{5}\cdot M\cdot R^2[/tex]
Homework Equations
[tex]\tau= F\cdot r\cdot \sin(\varphi)[/tex]
[tex]\alpha\cdot R=a[/tex]
The Attempt at a Solution
The forces acting on the sphere are: the normal force, the force of gravity and the frictional force. The sum of the y components of the normal force will be equal to [tex]M\cdot g[/tex] and the sum of the x components will be 0. So that the sum of torques due to the normal force is zero as well as torques due to the sphere's weight.
[tex]\tau_{a}=F_{a}\cdot R\cdot \sin(\varphi)[/tex]
Where we have by the figure:
[tex]\sin(\varphi)= \frac{\sqrt{R^2-(\frac{L}{2}^2)}}{R}= \sqrt{1-\frac{1}{4}\cdot \xi^2}[/tex]
So we have that:
[tex] \left\{ \begin{array}{ccc} 2\cdot F_{a}\cdot R\cdot \sqrt{1-\frac{1}{4}\cdot \xi^2} & = & I\cdot \alpha \\ -2\cdot F_{a} + M\cdot g\cdot \sin(\theta) & = & M\cdot a \end{array} \right. [/tex]
Which will yield:
[tex]F_{a}= \frac{I\cdot a}{2\cdot R^2\cdot \sqrt{1-\frac{1}{4}\cdot \xi^2}}[/tex]
After some manipulation you arive to
[tex]a=\frac{M\cdot g\cdot \sin(\theta)}{M+\frac{I}{R^2\cdot \sqrt{1-\frac{1}{4}\cdot \xi^2}}}[/tex]
Which after substituting I for it's value leads to:
[tex]a= \frac{g\cdot \sin(\theta)}{1+\frac{2}{5}\cdot \sqrt{\frac{1}{1-\frac{1}{4}\cdot \xi^2}}}[/tex]
Can somebody please tell me where I've gone wrong
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