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Question: Jerk is defined as the rate of change of acceleration of a particle. The velocity of a particle is \...

Jerk is defined as the rate of change of acceleration of a particle. The velocity of a particle is v=v0sinωtv = {v_0}\sin \omega t , where v0{v_0}and ω\omega are constant, Find jerk as a function of time.
a. v0ω2sinωt{v_0}{\omega ^2}\sin \omega t
b. v0ω2cosωt - {v_0}{\omega ^2}\cos \omega t
c. v0ω2sinωt - {v_0}{\omega ^2}\sin \omega t
d. v0ω2cosωt{v_0}{\omega ^2}\cos \omega t

Explanation

Solution

The rate of change of acceleration is called jerk. This rate of change of acceleration can be calculated by differentiating the acceleration with respect to time. Since acceleration is the rate of change of velocity, it can be calculated by differentiating the velocity with respect to time. Therefore, to get the function for jerk the expression for velocity must be double differentiated.

Complete step by step answer:
It is given in the question that, the velocity of the particle is-
v=v0sinωtv = {v_0}\sin \omega t
Here, the velocity vvis a function of time tt. It is given that the terms v0{v_0}and ω\omega are constant. The term v0{v_0} generally refers to the initial velocity of the object, whereas ω\omega refers to the frequency or the angular speed of the particle. At an instant, ω\omega multiplied with the instantaneous time tt gives the amount of angle covered by the object.

Therefore the acceleration of this particle can be determined by differentiating this function with respect to time,
a=dvdta = \dfrac{{dv}}{{dt}}
a=ddt(v0sinωt)\Rightarrow a = \dfrac{d}{{dt}}\left( {{v_0}\sin \omega t} \right)
The equation for derivative of sinx\sin x is,
ddx(sinx)=cosx\dfrac{d}{{dx}}\left( {\sin x} \right) = \cos x
Using this value in the above equation we get,
a=v0(cosωt)×ωa = {v_0}(\cos \omega t) \times \omega
a=v0ωcosωt\Rightarrow a = {v_0}\omega \cos \omega t

Now, to calculate the jerk of the object, the expression of acceleration needs to be differentiated with respect to time.
Therefore,
j=dadtj = \dfrac{{da}}{{dt}}or j=d2vdt2j = \dfrac{{{d^2}v}}{{d{t^2}}}
j=ddt(v0ωcosωt)\Rightarrow j = \dfrac{d}{{dt}}\left( {{v_0}\omega \cos \omega t} \right)
The term v0ω{v_0}\omega is constant. Therefore,
j=v0ωddt(cosωt)j = {v_0}\omega \dfrac{d}{{dt}}\left( {\cos \omega t} \right)
The equation for derivative of cosx\cos x is,
ddx(cosx)=sinx\dfrac{d}{{dx}}\left( {\cos x} \right) = - \sin x

Using this value in the above equation we get,
j=v0ω(sinωt)×ωj = {v_0}\omega \left( { - \sin \omega t} \right) \times \omega
j=v0ω2sinωt\Rightarrow j = - {v_0}{\omega ^2}\sin \omega t
The function defining the jerk of the particle is given by,
j=v0ω2sinωtj = - {v_0}{\omega ^2}\sin \omega t

Hence, the correct answer is option (C).

Note: To calculate the jerk produced in a particle, the velocity must be double differentiated. Since velocity refers to the displacement of an object per unit time, the displacement of the object can also be used to calculate jerk. For this, the displacement of the particle must be differentiated three times. Thus, Jerk is the third derivative of displacement with respect to time.