Solveeit Logo

Question

Question: A particle of unit mass undergoes one-dimensional motion such that its velocity varies according to ...

A particle of unit mass undergoes one-dimensional motion such that its velocity varies according to v(x)=βx2nv(x) = \beta {x^{ - 2n}}, where, β\beta and nn are constant and xx is the position of the particle. The acceleration of the particle as the function of xx, is given by:
A) 2β2x2n+1-2{\beta ^2}{x^{ - 2n + 1}}
B) 2nβ2x4n+1-2n{\beta ^2}{x^{ - 4n + 1}}
C) 2nβ2x2n1-2n{\beta ^2}{x^{ - 2n - 1}}
D) 2nβ2x4n1-2n{\beta ^2}{x^{ - 4n - 1}}

Explanation

Solution

In order to find the value of acceleration in terms of xx from the velocity as a function of xx, we should be able to differentiate velocity with respect to xx. For that add dxdx\dfrac{{dx}}{{dx}} in the equation for the acceleration and do the further differentiation.

Complete step by step solution:
From the question, we know that,
A particle undergoes one-dimensional motion such that the velocity of the object varies according to:
v(x)=βx2nv(x) = \beta {x^{ - 2n}}
Where, β\beta and nn are constant
xx is the position of the particle
We are asked to find the acceleration of the particle in terms of xx
We know, acceleration, a=dvdta = \dfrac{{dv}}{{dt}}
We know that the acceleration is a function of velocity and time.
Hence, we need the acceleration as a function of xx, we need to multiply the equation with dxdx\dfrac{{dx}}{{dx}}
That is, a=dvdt×dxdxa = \dfrac{{dv}}{{dt}} \times \dfrac{{dx}}{{dx}} ……………………. (1)
We know, velocity,v=dxdtv = \dfrac{{dx}}{{dt}}
Thus, equation (1) will become,
a=vdvdxa = v\dfrac{{dv}}{{dx}}……………(2)
Now we are finding the value of dvdx\dfrac{{dv}}{{dx}}
We are given velocity as function of xx,
v(x)=βx2nv(x) = \beta {x^{ - 2n}}
Differentiating vv with respect to xx, we get,
dvdx=2nβx2n1\dfrac{{dv}}{{dx}} = - 2n\beta {x^{ - 2n - 1}}
Now we have the value of both terms dvdx\dfrac{{dv}}{{dx}} and vv for the equation (2)
Applying these values in the equation (2), we get,
a=vdvdxa = v\dfrac{{dv}}{{dx}}
a=βx2n×(2nβx2n1)\Rightarrow a = \beta {x^{ - 2n}} \times \left( { - 2n\beta {x^{ - 2n - 1}}} \right)
a=2nβ2x2n12n\Rightarrow a = - 2n{\beta ^2}{x^{ - 2n - 1 - 2n}}
a=2nβ2x4n1\Rightarrow a = - 2n{\beta ^2}{x^{ - 4n - 1}}
That is, the acceleration of the particle which have a velocity, v(x)=βx2nv(x) = \beta {x^{ - 2n}} in terms of xx given by,
a=2nβ2x4n1a = - 2n{\beta ^2}{x^{ - 4n - 1}}

So the final answer is option (D), 2nβ2x4n1 - 2n{\beta ^2}{x^{ - 4n - 1}}.

Note: The velocity of an object is the rate of change of that object’s position with respect to a frame of reference, and is a function of time.
In mechanics, acceleration is defined as the rate of change of the velocity of the object with respect to time. Acceleration has the dimensions of velocity (LT1)\left( {L{T^{ - 1}}} \right) divided by time, i.e. LT2L{T^{ - 2}}.