Analyzing the Oscillation of a Plank on a Log

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SUMMARY

The discussion focuses on the analysis of the oscillation of a plank resting on a log, detailing the mechanics involved. The torque due to gravity is calculated as Mgxcosθ, simplifying to Mgaθ under small angle approximations. The moment of inertia about the contact point C is derived as Mb²/3, leading to the angular acceleration α = -3gaθ/b². The final formulas for angular frequency ω and time period T are established as ω = √(3ga)(1/b) and T = 2πb/√(3ga), respectively.

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Homework Statement


shm1.png

plank.png


Homework Equations

The Attempt at a Solution



C is the point of contact and G is the CM of the plank . x be the distance between G and C .Since plank always remain in contact , x=aθ

When the line joining the point of contact C with the center makes an angle θ with the vertical ,the force due to gravity mg acts vertically down and exerts a torque about the point of contact C.

Torque due to Mg = Mgxcosθ

Since θ is small , cosθ ≈ 1 and using x=aθ

Mgxcosθ ≈ Mgaθ

Moment of inertia about C = M(2b)2/12 + Mx2 =Mb2/3+Ma2θ2

Since θ is small , θ2≈0

Moment of inertia about C = Mb2/3

Writing torque equation about C ,

-Mgaθ = (Mb2/3)α ( α is angular acceleration )

α = -3gaθ/b2

Angular frequency of oscillation ω = √(3ga)(1/b)

Time period = 2π/ω = 2πb/√(3ga)

Is my work correct ?
 

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Jahnavi said:
correct ?
Looks good.
 
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Thanks !
 

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