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Question: The velocity of a particle moving in a positive direction of the x-axis varies as \(v = \alpha \sqrt...

The velocity of a particle moving in a positive direction of the x-axis varies as v=αxv = \alpha \sqrt x , where a is a positive constant. If at t=0t = 0 , x=0x = 0, the velocity and acceleration as a function of time tt will be.
A. α2t2,α2\dfrac{{{\alpha ^2}t}}{2},\,{\alpha ^2}
B. α2t,α2t2{\alpha ^2}t,\,\dfrac{{{\alpha ^2}t}}{2}
C. α2t2,α22\dfrac{{{\alpha ^2}t}}{2},\,\dfrac{{{\alpha ^2}}}{2}
D. α2t,α2{\alpha ^2}t,\,{\alpha ^2}

Explanation

Solution

The difference between the final and initial velocity with respect to time is called acceleration. And it is denoted by ‘a’ and SI unit is ms2m{s^{ - 2}}. Acceleration is a vector quantity, it means it has direction as well as magnitude. There are two types of acceleration: uniform acceleration and non-uniform accelerations.

Complete step by step answer:
Given, v=αxv = \alpha \sqrt x …(1)
We know that
dVdT=a\dfrac{{dV}}{{dT}} = a…(2)
Differentiate equation 1 w.r.t to T
dVdT=αddTx\dfrac{{dV}}{{dT}} = \alpha \dfrac{d}{{dT}}\sqrt x
dVdT=α2xdxdT\Rightarrow \dfrac{{dV}}{{dT}} = \dfrac{\alpha }{{2\sqrt x }}\dfrac{{dx}}{{dT}}
But dxdT=v\dfrac{{dx}}{{dT}} = v is velocity gradient
Put the values in equation 2 we get.
a=α2x×αx\Rightarrow a = \dfrac{\alpha }{{2\sqrt x }} \times \alpha \sqrt x
a=α22\Rightarrow a = \dfrac{{{\alpha ^2}}}{2}

Now, relationship between velocity and displacement
v=αxv = \alpha \sqrt x
dxdt=αx\Rightarrow \dfrac{{dx}}{{dt}} = \alpha \sqrt x
dxx=αdt\Rightarrow \dfrac{{dx}}{{\sqrt x }} = \alpha dt
Integrate
dxx=αdt\Rightarrow \int {\dfrac{{dx}}{{\sqrt x }}} = \alpha \int {dt}
x12+112+1=αt+c\Rightarrow \dfrac{{{x^{ - \dfrac{1}{2} + 1}}}}{{ - \dfrac{1}{2} + 1}} = \alpha t + c
Since t=0,x=0t = 0,\,x = 0
We get
c=0c = 0

So, 2x=αt2\sqrt x = \alpha t
Squaring both side
4x=a2t2\Rightarrow 4x = {a^2}{t^2}
x=α2t24\Rightarrow x = \dfrac{{{\alpha ^2}{t^2}}}{4}
Differentiate w.r.t. ‘t’
dxdt=α24ddt(t2)\Rightarrow \dfrac{{dx}}{{dt}} = \dfrac{{{\alpha ^2}}}{4}\dfrac{d}{{dt}}({t^2})
We know that
dxdt=v\dfrac{{dx}}{{dt}} = v
v=α2t2\therefore v = \dfrac{{{\alpha ^2}t}}{2}

Hence, the correct answer is option C.

Note: Force is the product of mass and acceleration. Application acceleration improves the application performances using techniques like compression, caching and transmission control protocol. When the velocity of any moving is changed it is said to be a change in acceleration. Change in acceleration may be positive or negative.