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Question: In case of simple harmonic motion, if the velocity is plotted along the X-axis and the displacement ...

In case of simple harmonic motion, if the velocity is plotted along the X-axis and the displacement (from the equilibrium position) is plotted along the Y-axis, the resultant curve happens to be an ellipse with the ratio:
majoraxis(alongX)minoraxis(alongY)=20π\dfrac{{majoraxis(alongX)}}{{\min oraxis(alongY)}} = 20\pi . What is the frequency of the simple harmonic motion?
A) (A) 100Hz\left( {\text{A}} \right){\text{ }}100Hz
B) (B) 20Hz\left( {\text{B}} \right){\text{ }}20Hz
C) (C) 10Hz\left( {\text{C}} \right){\text{ }}10Hz
D) (D) 110Hz\left( {\text{D}} \right){\text{ }}\dfrac{1}{{10}}Hz

Explanation

Solution

First we have to assume the variables on the given data.
Then we defined the simple harmonic function and found the velocity by using the elliptical curve on the velocity displacement graph.
Finally we get the frequency of the simple harmonic function.

Complete step by step answer:
In case of Simple harmonic motion(S.M.H) be M,
Let VV is the velocity and displacement from equilibrium position is xx .
The displacement from equilibrium position is defined as a function of time tt,
We can write it as,x=Asinωtx = A\sin \omega t.
Here, AA= Amplitude of the S.H.M and ω\omega = Angular frequency = 2π×frequency2\pi \times {\text{frequency}}
The velocity of the S.H.M is calculated by differentiating the displacement,
V=dxdtV = \dfrac{{dx}}{{dt}}=AωcosωtA\omega \cos \omega t.
Now we know an elliptical equation in X-Y axis should be,
x2a2+y2b2=1\dfrac{{{x^2}}}{{{a^2}}} + \dfrac{{{y^2}}}{{{b^2}}} = 1 .
The elliptical equation diagram is as follows,

where, the major axis =2a2a and the minor axis = 2b2b.
Here, The velocity is plotted along X-axis and the displacement is plotted along Y-axis, and the resultant curve is an ellipse as the figure drawn is as follows:

Therefore, V2A2ω2+x2A2=1\dfrac{{{V^2}}}{{{A^2}{\omega ^2}}} + \dfrac{{{x^2}}}{{{A^2}}} = 1 - Elliptical equation.
Here the major axis is 2ωA2\omega A and the minor axis is 2A2A .
In this question stated as, majoraxis(alongX)minoraxis(alongY)=20π\dfrac{{majoraxis(alongX)}}{{\min oraxis(alongY)}} = 20\pi
Putting the values an we get,
2ωA2A=20π\Rightarrow \dfrac{{2\omega A}}{{2A}} = 20\pi
Cancelling the same term we get,
ω=20π\Rightarrow \omega = 20\pi
Now, we have to find out the frequency.
ω=2π×frequency\omega = 2\pi \times {\text{frequency}}
ω=2π×f\Rightarrow \omega = 2\pi \times f
Let us take the ff as LHS and remaining as in divide term we get
f=ω2π\Rightarrow f = \dfrac{\omega }{{2\pi }}
Putting the value of ω\omega and we get,
f=20π2π\Rightarrow f = \dfrac{{20\pi }}{{2\pi }}
On divide the term we get,
f=10\Rightarrow f = 10
Therefore the frequency is f=10Hzf = 10Hz.

Hence, the right answer is in option (C).

Note: In the case of an S.H.M of a particle if the displacement from the equilibrium position is xx,
Here dxdt\dfrac{{dx}}{{dt}} is the change in displacement per unit time which defines the Velocity of that particle.
If we represent the displacement as,x=Asinωtx = A\sin \omega t
The velocity should be, V=dxdt=ωAcosωtV = \dfrac{{dx}}{{dt}} = \omega A\cos \omega t
V=ωAsin(ωt+π2)\Rightarrow V = \omega A\sin (\omega t + \dfrac{\pi }{2})
Hence, the phase difference between the displacement and velocity of a particle in S.H.M is π2\dfrac{\pi }{2}.