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Question: A particle is executing SHM along the x-axis given by \(x = A\sin ot\). What is the magnitude of the...

A particle is executing SHM along the x-axis given by x=Asinotx = A\sin ot. What is the magnitude of the average acceleration of the particle between t=0t = 0 and tt=T4\dfrac{T}{4}, where TT is the time period of oscillation.
(A) 2ω2Aπ\dfrac{{2{\omega ^2}A}}{\pi }
(B)ω2Aπ\dfrac{{{\omega ^2}A}}{\pi }
(C)4ω2Aπ\dfrac{{4{\omega ^2}A}}{\pi }
(D) None of these

Explanation

Solution

According to the question we need to first calculate the derivative of a given equation to find the velocity of the particle with respect to time. Then we need to calculate the average acceleration by putting the formula from the first law of motion. The average acceleration of a particle is equal to vut\dfrac{{v - u}}{t}

Complete answer:
Any particle executing simple harmonic motion is a special type of periodic motion where the restoring force on the moving object is directly proportional to the magnitude of the object ‘ s displacement and acts towards the equilibrium position .
Here, the motion of the particle is represented by
x(t)=Asinωtx(t) = A\sin \omega t
Where, AAis Amplitude of the motion,ω\omega is the angular frequency of the motion (‘o’ in the question) and tt represents time.
Now, we need to calculate the velocity of the particle by differentiating the given equation with respect to time.
v=dx(t)dt=Aωcosωtv = \dfrac{{dx(t)}}{{dt}} = - A\omega \cos \omega t
Here, vv represents velocity of the particle at any instant of time.
From the first law of motion, we know Average acceleration of any rigid body in motion is given by aa= vut\dfrac{{v - u}}{t}
Here, vv is the velocity of the particle at time = T4\dfrac{T}{4} and
uu is the velocity of the particle at time = 00
Now, putting the respective values of vv and uu after differentiation and putting total time as T4\dfrac{T}{4}
=Aωcosωtt=T4+Aωcosωtt=0T4\dfrac{{ - A\omega \cos \omega {t_{t = \dfrac{T}{4}}} + A\omega \cos \omega {t_{t = 0}}}}{{\dfrac{T}{4}}}
=AωT4\dfrac{{A\omega }}{{\dfrac{T}{4}}}
=Aω2π4ω\dfrac{{A\omega }}{{\dfrac{{2\pi }}{{4\omega }}}}
=4Aωω2π\dfrac{{4A\omega \cdot \omega }}{{2\pi }}
=2Aω2π\dfrac{{2A{\omega ^2}}}{\pi }

Note:
We should take into consideration that the average acceleration of the particle shouldn’t be taken as a double derivative of position with respect to time. Make sure to put the values of time as T4\dfrac{T}{4} in vv and 00in uuafter differentiation.