A uniform rod can rotate freely about one end. Rod is in equilibrium with the
help of massless spring in horizontal position. Then
(mass of rod=m; length of rod =/; spring constant=k).
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Explanation:
If the rod is rotated through an angle θ, extension in one spring = compression in the other spring,
i.e.,x=lθ/2
Therefore, force acting on each of the ends of the rod,
F=kx=k(lθ/2)
Restoring torque on the rod,
T=−Fl=−k( θ/2)l=−kl
2
(θ/2)
As T=Iα=(Ml
2
/12)α
or α=−
M
6k
θ,α∝theta.
Thus, the motion of the rod is simple harmonic with
ω
2
=
M
6k
orω=
M
6k
orv=
2π
1
M
6k
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