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Question: A boy is sitting on the seat of a merry-go-round with a constant angular velocity. At \(t=0\), the b...

A boy is sitting on the seat of a merry-go-round with a constant angular velocity. At t=0t=0, the body is at position AA, as shown in the figure. Which of the following graphs are correct? All graphs are sinusoidal.

A)FyA){{F}_{y}} is the yy- component of the force keeping the boy moving in a circle

B)xB)x is the xx-component of the boy’s position

C)θC)\theta is the angle that the position vector of the boy makes with the positive xx-axis

D)VxD){{V}_{x}} is the xx-component of the boy’s velocity

Explanation

Solution

Each option is scrutinized by taking the position of the boy at a particular time tt. When the boy moves from his initial position at t=0t=0 to a position at time tt, the angular displacement of the boy is taken as θ\theta . Then, the required equations are derived and checked with the given graphs, one by one.

Complete step-by-step solution
We are given that a boy is sitting on the seat of a merry-go-round with a constant angular velocity. At t=0t=0, the body is at position AA. We are also provided with four graphs, which talks about different parameters with respect to the movement of boys in the merry-go-round. We are required to mark the correct graphs from these options.
For this, let us assume that the boy has already started moving in the merry-go-round and is at a position BB now, as shown in the figures given below. Let tt be the time at which the boy is at BB, as shown.
Now, let us go through the provided options one by one.
A)FyA){{F}_{y}} is the yy- component of the force keeping the boy moving in a circle

Here, we are told that Fy{{F}_{y}} is the yy- component of the force keeping the boy moving in a circle. From the graph, it is clear that Fy{{F}_{y}} is in the form of a negative sinusoidal wave, moving with respect to time.
Now, let’s have a look at the figure given below.

Clearly, the boy is at BB, when the time is tt. We know that force acting on the boy is the centripetal force, which is given by
F=mω2rF=m{{\omega }^{2}}r
where
FF is the centripetal force acting on the boy at time tt
mm is the mass of the boy
ω\omega is the angular frequency of motion of the boy
rr is the radius of the merry-go-round
Clearly, the centripetal force is acting along the position vector of the boy at BB, as shown.
Now, the yy-component of this centripetal force is given by
Fy=mω2rsinθ=mω2rsin(ωt){{F}_{y}}=-m{{\omega }^{2}}r\sin \theta =-m{{\omega }^{2}}r\sin (\omega t)
where
Fy{{F}_{y}} is the yy-component of the centripetal force
θ=ωt\theta =\omega t is the angular displacement of the boy
Clearly, this component of force is acting along the negative yy-direction
Also, if we draw a graph between Fy{{F}_{y}} and tt, it is of the form of a negative sine wave.
The graph given in option AA satisfies this condition and hence, we can conclude that option AA is correct.
B)xB)x is the xx-component of the boy’s position

xx-component of the position vector of the boy at BB can be deduced from the right triangle CEBCEB, as shown below.

Clearly, xx-component of the position vector of the boy at BB is given by
x=rcosθ=rcos(ωt)x=r\cos \theta =r\cos (\omega t)
where
xx is the xx-component of the position vector of the boy at BB
rr is the radius of the merry-go-round
θ=ωt\theta =\omega t is the angular displacement of the motion of the boy
Now, if we draw a graph between xx and tt, it will have the shape of a cosine wave. Since the graph provided in the option is in the form of a sine wave, the given option is concluded as wrong.
C)θC)\theta is the angle that the position vector of the boy makes with the positive xx-axis

We know that angular frequency is defined as angular displacement per unit time. If ω\omega represents the angular frequency of the boy rotating in merry-go-round at time tt, then, ω\omega is given by
ω=θtθ=ωt\omega =\dfrac{\theta }{t}\Rightarrow \theta =\omega t
where
ω\omega is the angular frequency of the boy at time tt
θ\theta is the angular displacement of the boy at time tt
Clearly, angular displacement is directly proportional to time. Therefore, if we draw a graph between θ\theta and tt, it will look similar to the graph provided in the option, as given above.
Hence, option CC is also correct.
D)VxD){{V}_{x}} is the xx-component of the boy’s velocity

Here, we are said that Vx{{V}_{x}} is the xx-component of the boy’s velocity xx-component of the velocity vector of the boy at BB can be deduced from the right triangle CFBCFB, where <B=θ< B = \theta , as shown below.

Here, the velocity of the boy at BB is given by
V=ωrV=\omega r
where
VV is the velocity of the boy at BB
ω\omega is the angular frequency of the motion of boy at time tt
rr is the radius of the merry-go-round
Clearly, this velocity is acting along the tangent drawn at BB, as shown in the figure.
Now, the xx-component of this velocity is given by
Vx=ωrsinθ=ωrsin(ωt){{V}_{x}}=-\omega r\sin \theta =-\omega r\sin (\omega t)
where
Vx{{V}_{x}} is the xx-component velocity of the boy at BB
θ=ωt\theta =\omega t is the angular displacement of the boy at tt
Clearly, this component of velocity acts in the negative xx-direction. If we draw a graph between Vx{{V}_{x}}
and tt, it will have the shape of a negative sine wave.
Since the provided option has the shape of a negative cosine wave, option DD can be concluded as wrong.
Therefore, option AA and option CC is correct while option BB and option DD are incorrect for a boy moving in a merry-go-round.

Note: Such questions are asked to evaluate the visualizing capabilities of students. Therefore, students need to be thorough with the shapes of a positive sine wave, a negative sine wave, a positive cosine wave, and a negative cosine wave. Deducing the correct waveform from an equation is also important, which students should practice from time to time.