Analyzing the Oscillation of a Plank on a Log

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The discussion focuses on analyzing the oscillation of a plank resting on a log, detailing the relationship between the plank's center of mass and the point of contact. The torque exerted by gravity is calculated, leading to the formulation of the moment of inertia about the point of contact. The angular acceleration is derived from the torque equation, resulting in an expression for angular frequency. The time period of oscillation is ultimately determined as a function of the plank's dimensions and gravitational acceleration. The calculations presented are confirmed as correct.
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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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