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Question: A particle moving on a straight line so that its distance \(s\)from a fixed point at any time \(t\) ...

A particle moving on a straight line so that its distance ssfrom a fixed point at any time tt is proportional to tn{t^n}. If vv be the velocity and aathe acceleration at any time then nasn1=\dfrac{{nas}}{{n - 1}} =
A) vv
B) v2{v^2}
C) v3{v^3}
D) 2v2v

Explanation

Solution

Velocity and acceleration both describe motion, but there is an important difference between them. The velocity is the rate of change of position and acceleration is rate of change of velocity.

Complete step by step answer:
We know that, velocity is the rate of change of displacement with respect to time
v=dsdt\Rightarrow v = \dfrac{{ds}}{{dt}} . . . (1)
And acceleration is rate of change of velocity
a=dvdt\Rightarrow a = \dfrac{{dv}}{{dt}} . . . (2)
It is given that displacement ssis directly proportional to time by the relation,
sαtns\alpha {t^n}
We would add a constant to remove the proportionality sign
s=βtn\Rightarrow s = \beta {t^n} . . . . . (3)
Where β=\beta = Constant
By putting the value of displacement in equation (1), we get
v=ddt(βtn)v = \dfrac{d}{{dt}}(\beta {t^n})
v=nβtn1v = n\beta {t^{n - 1}} . . . . (4) (ddxxn=nxn1)\left( {\because \dfrac{d}{{dx}}{x^n} = n{x^{n - 1}}} \right)
By putting the value of velocity from equation (4) in equation (2), we get
a=ddt(nβtn)a = \dfrac{d}{{dt}}(n\beta {t^n})
a=n×(n1)βtn2\Rightarrow a = n \times (n - 1)\beta {t^{n - 2}} . . . . (5) (ddxxn=nxn1)\left( {\because \dfrac{d}{{dx}}{x^n} = n{x^{n - 1}}} \right)
Therefore, by putting the value of displacement and acceleration in nas(n1)\dfrac{{nas}}{{(n - 1)}}
We get,
nas(n1)=n×n(n1)βt(n2)×βtn(n1)\dfrac{{nas}}{{(n - 1)}} = \dfrac{{n \times n(n - 1)\beta {t^{(n - 2)}} \times \beta {t^n}}}{{(n - 1)}}
We can simplify it as
nas(n1)=n2β2tn2+n\dfrac{{nas}}{{(n - 1)}} = {n^2}{\beta ^2}{t^{n - 2 + n}}
=n2β2t2n2= {n^2}{\beta ^2}{t^{2n - 2}}
=n2β2t2(n1)= {n^2}{\beta ^2}{t^{2(n - 1)}}
Since, all the terms are squares, we can write them together and get
nas(n1)=(nβt(n1))2\dfrac{{nas}}{{(n - 1)}} = {\left( {n\beta {t^{(n - 1)}}} \right)^2}
nas(n1)=v2\dfrac{{nas}}{{(n - 1)}} = {v^2} (v=nβtn1)\left( {\because v = n\beta {t^{n - 1}}} \right)
Therefore, From the above explanation option (B) v2{v^2}is correct.

Note: Not knowing the basics and formulae of derivatives can lead to a problem while solving such questions. It is important that you study basic calculus before starting to solve the questions of kinematics. Due to the lack of knowledge about derivatives, if you try to attempt it using the laws of motion, the answer will be incorrect as no information is given about initial velocity of the particle.