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Question: A particle is moving in a straight line such that its velocity varies according to \(v\left( x \righ...

A particle is moving in a straight line such that its velocity varies according to v(x)=2x3mv\left( x \right) = 2{x^{ - 3m}}, where mm is a constant and xx is the position of the particle. The acceleration of the particle as a function of xx is given by-
(1) 12mx6m+1 - 12m{x^{ - 6m + 1}}
(2) 12mx3m1 - 12m{x^{ - 3m - 1}}
(3) 8mx3m1 - 8m{x^{ - 3m - 1}}
(4) 12mx6m1 - 12m{x^{ - 6m - 1}}

Explanation

Solution

We know that the acceleration is described as the rate of variation of the velocity of an object. If the position of the object is xx then the velocity of the object in the derivative form is given by,
v(x)=dxdtv\left( x \right) = \dfrac{{dx}}{{dt}}
And the acceleration is the derivative of the velocity w.r.t. the time. So, the acceleration of the object in the derivative form is given by,
Acceleration a(x)=dv(x)dta\left( x \right) = \dfrac{{dv\left( x \right)}}{{dt}}
Or, a(x)=ddt(dxdt) a(x)=d2xdt2\begin{array}{l} a\left( x \right) = \dfrac{d}{{dt}}\left( {\dfrac{{dx}}{{dt}}} \right)\\\ a\left( x \right) = \dfrac{{{d^2}x}}{{d{t^2}}} \end{array}

Complete step by step answer:
The expression of variation of the velocity of a particle v(x)=2x3mv\left( x \right) = 2{x^{ - 3m}}
Where mm is a constant and xx is the position of the particle.
In order to find the acceleration of this particle, we have to find the derivative of the functionv(x)=2x3mv\left( x \right) = 2{x^{ - 3m}}.
So, taking derivatives of both sides of the expression w.r.t. time tt we get,
\dfrac{d}{{dt}}\left\\{ {v\left( x \right)} \right\\} = \dfrac{d}{{dt}}\left( {2{x^{ - 3m}}} \right)
We know that acceleration is a(x)=dv(x)dta\left( x \right) = \dfrac{{dv\left( x \right)}}{{dt}}.
So substituting this in the expression we have,
a(x)=2ddt(x3m)a\left( x \right) = 2\dfrac{d}{{dt}}\left( {{x^{ - 3m}}} \right)
We can write ddt(x3m)\dfrac{d}{{dt}}\left( {{x^{ - 3m}}} \right) as-
ddt(x3m)=(ddx(x3m))×dxdt =(ddx(x3m))×v(x)\begin{array}{l} \dfrac{d}{{dt}}\left( {{x^{ - 3m}}} \right) = \left( {\dfrac{d}{{dx}}\left( {{x^{ - 3m}}} \right)} \right) \times \dfrac{{dx}}{{dt}}\\\ = \left( {\dfrac{d}{{dx}}\left( {{x^{ - 3m}}} \right)} \right) \times v\left( x \right) \end{array}
Substituting this value into the expression we get,
a(x)=2(ddx(x3m))×v(x)a\left( x \right) = 2\left( {\dfrac{d}{{dx}}\left( {{x^{ - 3m}}} \right)} \right) \times v\left( x \right)
Substitute v(x)=2x3mv\left( x \right) = 2{x^{ - 3m}} in the expression, we get,
a(x)=2(ddx(x3m))×2x3ma\left( x \right) = 2\left( {\dfrac{d}{{dx}}\left( {{x^{ - 3m}}} \right)} \right) \times 2{x^{ - 3m}}
And we know that ddx(xn)=nxn1\dfrac{d}{{dx}}\left( {{x^n}} \right) = n{x^{n - 1}} so,
a(x)=2×(3m×x3m1)×2x3ma\left( x \right) = 2 \times \left( { - 3{\rm{m}} \times {{\rm{x}}^{ - 3m - 1}}} \right) \times 2{x^{ - 3m}}
Solving this we get,
a(x)=12mx3m13m a(x)=12mx6m1\begin{array}{l} a\left( x \right) = - 12m{x^{ - 3m - 1 - 3m}}\\\ a\left( x \right) = - 12m{x^{ - 6m - 1}} \end{array}
Therefore, the acceleration of the particle as a function of xx is a(x)=12mx6m1a\left( x \right) = - 12m{x^{ - 6m - 1}} and the correct option is (4).

Note: The acceleration of the particle is calculated w.r.t. time but the expression of the velocity is given in form of position x(t)x\left( t \right) so we have to rearrange it in following way-
dv(x)dt=dv(x)dx×dxdt\dfrac{{dv\left( x \right)}}{{dt}} = \dfrac{{dv\left( x \right)}}{{dx}} \times \dfrac{{dx}}{{dt}}