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A small mass m is hung at the end of a light string of length 1.5 m and allowed to swing over a small amplitude as a simple p
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Answer #1

The situation is as shown in the figure above.

The total force on the pendulum

F=-mgsin(\theta )-Cv

As

\theta\approx 0 and v=L \dot\theta

F=-mg\theta -CL\dot{\theta}

F=mL\ddot\theta

mL\ddot\theta= -mg\theta-CL\dot{\theta}

\ddot\theta= -\frac{g}{L}\theta-\frac{C}{m}\dot{\theta}

\ddot\theta+\frac{C}{m}\dot{\theta} +\frac{g}{L}\theta=0

This is the require equation of motion.It is second order total differential equation with constat coefficients.

\theta=Aexp(((-C/2m)+\sqrt{(C/2m)^{2}-g/l})t)+Bexp(((-C/2m)-\sqrt{(C/2m)^{2}-g/l})t)

the solution remains periodic for sufficient long only if

(\frac{C}{2m})^{2}< < \frac{g}{L}

which defnitely should be the case here.

Under this assumption the solution can be written as

\theta=D_{0}exp((-C/2m)t)Cos(\sqrt{g/L}t+\phi )

Hence The amplitude

Amplitude ,A=D{_{0}} exp(\frac{-C}{2m})t

decrease exponentially

with g=9.8 ms-2 and L=1.5 m

period,T_{1.5}=2\pi\sqrt{} {L/g}=2\pi\sqrt{1.5/9.8}\approx 2.46 sec

time taken to comple 30 swings

T30=73.8 sec

Amplitude after 30 swings =

.A_{30}=D{_{0}} exp(\frac{-C}{2m})73.8

A_{30}=\frac{D_{0}}{2}

1/2=exp(\frac{-36.9C}{m})

ln(1/2)=\frac{-36.9C}{m}

\frac{C}{m}=.693/36.9=0.0188

Let n  be the no of swings the amplitude will reduce by half if L=2.0m

period,T_{2m}=2\pi\sqrt{} {L/g}=2\pi\sqrt{2/9.8}\approx 2.838 sec

Time for n swings

Tn=2.838 n

soliving

Amplitude ,A=D{_{0}} exp(\frac{-C}{2m})t

with t=2,838n

C/m =0.0188

A=D0/2

we have

\frac{1}{2}= exp(\frac{-0.0188}{2}2.828n)

n\approx 8

Thus the no of swings is 8

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