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Question: A thin uniform rod, pivoted at O, is rotating in the horizontal plane with constant angular speed \[...

A thin uniform rod, pivoted at O, is rotating in the horizontal plane with constant angular speed ω\omega , as shown in the figure. At time t = 0, a small insect starts from O and moves with constant speed v, with respect to the rod towards the other end. It reaches the end of the rod at t =T and stops. The angular speed of the system remains ω\omega throughout. The magnitude of the torque (π)\left( \left| {\vec{\pi }} \right| \right) about O, as a function of time is best represented by which plot?

A.
B.
C.

D.

Explanation

Solution

This question is a case of hinged rotational motion. To get the correct answer you have to find out the relationship between τ\tau and time. For that you can proceed by using the formula for τ\tau and moment of inertia. Remember that r=dLdt|\vec{r}|=|\dfrac{d\vec{L}}{dt}|. Also, remember the moment of inertia will be that of rod, i.e., 13ML2\dfrac{1}{3}M{{L}^{2}} plus that of the mx2m{{x}^{2}} for the object where x is an arbitrary distance.

Complete answer:
As we know,
r=dLdt|\vec{r}|=|\dfrac{d\vec{L}}{dt}|
Where
L=IωL=I\omega
So,
Now,
It is obvious from the scenario that the moment of inertia is
The (rod + insect) scheme is increasing.

Let the insect be at a distance xx at any moment in time,' t'
Of O. At this time, the time of the inertia of the moment,
The scheme is
So,
Then
τ=ddt(Iω)=ωdldt\tau =\dfrac{d}{dt}(I\omega )=\omega \dfrac{dl}{dt}
Therefore,
I=13ML2+mx2............I=\dfrac{1}{3}M{{L}^{2}}+m{{x}^{2}}............ ……………. (ii)
Now,
By using the equations (i) and (ii)
We have
τ=ωddt[13ML2+mx2]\tau =\omega \dfrac{d}{dt}[\dfrac{1}{3}M{{L}^{2}}+m{{x}^{2}}]
τ=ωmddtx2\Rightarrow \tau =\omega m\dfrac{d}{dt}{{x}^{2}}
τ=ωm2xdxdt\Rightarrow \tau =\omega m2x\dfrac{dx}{dt}
τ=2ωmxu\Rightarrow \tau =2\omega mxu
τ=2ωmv2t\Rightarrow \tau =2\omega m{{v}^{2}}t
So,
Form the above equation, we can easily conclude that
τt\tau \propto t
At t=T, υ=0.
Therefore, τ=0\tau =0
Hence, the graph between τ\tau and tis a straight line till t=T. Also, for, t>T, τ=0\tau =0
Option - B is the correct option.

Note:
As you can see, the final result was τt\tau \propto t that can be written as τ=kt\tau =ktwhere k is some constant. So, the graph will be that of a straight line. While in exam, you can sometimes save your time by eliminating the options which have any curve other than the straight line.