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

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SUMMARY

The discussion focuses on two physics problems related to oscillation and rotation. The first problem involves a ruler of length L and thickness 2d resting on a cylindrical body, demonstrating oscillatory motion with a period defined by the formula T = 2π√(L²/(12g(r-d))). The second problem examines a sphere rolling down an incline without sliding, with the acceleration of its center of mass given by a = (g sin(θ))/(1 + (2/5)(1/(1 - (1/4)α²))), where α = L/R and I = (2/5)MR² represents the moment of inertia of the sphere.

PREREQUISITES
  • Understanding of oscillatory motion and its mathematical representation
  • Knowledge of rotational dynamics and moment of inertia
  • Familiarity with gravitational acceleration and its effects on motion
  • Basic proficiency in trigonometric functions and their applications in physics
NEXT STEPS
  • Study the derivation of oscillation formulas in classical mechanics
  • Explore the concepts of rolling motion and friction in physics
  • Learn about the applications of moment of inertia in rotational systems
  • Investigate the relationship between angular acceleration and linear acceleration in rolling objects
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Students studying classical mechanics, physics educators, and anyone interested in understanding the principles of oscillation and rotation in physical systems.

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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:
[tex]T = 2\cdot \pi\cdot \sqrt{\frac{L^2}{12\cdot g\cdot (r-d)}}[/tex]

SemTtulo.jpg


Question nr 2:

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 \alpha^2}}[/tex]

Where g is the gravitational acceleration and
[tex]\alpha= \frac{L}{R}[/tex]

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

SemTtulo-1.jpg


Homework Equations



[tex]T=\frac{2\cdot \pi}{\omega}[/tex]

[tex]\tau= F\cdot r\cdot \sin(\varphi)[/tex]

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:
[tex]a= \frac{g\cdot \sin(\theta)}{1+\frac{2}{5}\cdot \sqrt{\frac{1}{1-\frac{1}{4}\cdot \alpha^2}}}[/tex]
 
Last edited:
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moment of inertia of sphere is I=(2/5).M.R^2
 

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