In: Physics
A uniform thin rod of length 0.812 m is hung from a horizontal nail passing through a small hole in the rod located 0.043 m from the rod\'s end. When the rod is set swinging about the nail at small amplitude, what is the period of oscillation?
The basic equation of motion is
I d^2ϕ/dt^2 = τ
where ϕ is the angle, I the moment of inertia and τ the torque. Let
h denote the distance between the hole and the top of the rod
(h<L/2).
The moment of inertia of a uniform rod about its end is 1/3 M L^2.
Invoking the Parallel Axes Theorem therefore gives us that the
moment of inertia for rotation about the hole s 1/3ML^2 -
Mh^2.
The net torque from gravity is::
τ = -M(1-h/L)g (L-h)/2 sin(ϕ) + M h/L g h/2 sinϕ)
= -1/2 Mg/L * ( (L-h)^2 - h^2 ) sin(ϕ)
= -1/2 M g (L-2h) sin(ϕ)
As usual the small angle approximation uses sin(ϕ) ~ ϕ. The
equation of motion therefore becomes
(1/3ML^2 - Mh^2) ϕ“ + 1/2 Mg(L-2h) ϕ = 0
which can be written as
ϕ“ + 3g(L-2h)/(2L^2-6h^2) ϕ = 0
From this we read off
ω^2 = 3g(L-2h)/(2L^2-6h^2)
and so a period
T = 2π/ω
= 2π √︎ ( (2L^2-6h^2)/(3g(L-2h)) )
= 2*3.14*SQRT((2*.812^2-6*0.043^2)/3g(0.812-2*.043)))
Here it calculates to
T = 1.55s
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