Angular Oscillation of a rod in a circle

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SUMMARY

The discussion focuses on calculating the angular frequency of small oscillations for a uniform rod constrained to move in a vertical circle. The rod's moment of inertia is derived using the formula I = I_{cm} + Md^2, where I_{cm} = ML^2/12. The mechanical energy equation is established as E = mgd(1 - cosθ) + (1/2)Iθ̇². By applying the small angle approximation, the angular acceleration is expressed as θ̈ = - (mgd/I)θ, confirming the approach to be correct for analyzing the rod's oscillatory motion.

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  • Understanding of rotational dynamics and moment of inertia
  • Familiarity with the principles of conservation of mechanical energy
  • Knowledge of small angle approximations in physics
  • Basic calculus for differentiation and solving differential equations
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Tanya Sharma
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Homework Statement



A uniform rod moves in a vertical circle .Its ends are constrained to move on the track without friction.Find the angular frequency of small oscillation .

Homework Equations


The Attempt at a Solution



Suppose the rod of length L moves in a circle of radius R .
Let the equilibrium position of the rod be AB .X be the mid point .CD is the position of the rod when it displaced by an angle θ .Y is the mid point.

The mechanical energy of the rod in position CD is denoted by E .

The moment of inertia of the rod about its CM (the middle point) is Icm
The moment of inertia of the rod about O is I .

[itex]I_{cm} = ML^2/12[/itex]

[itex]I=I_{cm} + Md^2[/itex]

[itex]I=M(R^2-\frac{L^2}{6})[/itex]

[itex]E= mgd(1-cos\theta)+(1/2)I\dot\theta^2[/itex]

Differentiating E w.r.t time ,we get

[itex]dE/dt = mgdsin\theta\dot\theta+(1/2)I(2\dot\theta\ddot\theta)[/itex]

Since Mechanical energy remains conserved ,

Putting dE/dt=0 ,we get

[itex]\ddot\theta = -\frac{mgdsin\theta}{I}[/itex]

Using small angle approximation , sinθ≈θ

[itex]\ddot\theta = -\frac{mgd\theta}{I}[/itex]

Is my approach correct ?
 

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Looks right to me. (It's clearly the same as making a pendulum out of the rod by attaching a light bar length d rigidly, at right angles, to its centre.)
 

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