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Question: The initial velocity of a particle is \(u\)(at \({\text{t = 0}}\) ) and the acceleration \(a\) is gi...

The initial velocity of a particle is uu(at t = 0{\text{t = 0}} ) and the acceleration aa is given by αt32\alpha {t^{\dfrac{3}{2}}} . Which of the following relations is valid?
A) V=u+αt32V = u + \alpha {t^{\dfrac{3}{2}}}
B) V=u+3rt32V = u + \dfrac{{3r{t^3}}}{2}
C) V=u+25αt52V = u + \dfrac{2}{5}\alpha {t^{\dfrac{5}{2}}}
D) V=u+αt52V = u + \alpha {t^{\dfrac{5}{2}}}

Explanation

Solution

In this question, we are asked to find out the valid relation. We use the simple formula of the acceleration and integrate that equation with applying proper limits. As acceleration is a function of time, we get the correct relation.

Formula used:
a=dvdt\vec a = \dfrac{{dv}}{{dt}}
Here, a  {{\vec a}}\;is the acceleration,
dv{\text{dv}} is the velocity (small)
dt{\text{dt}} is the time (small)

Complete step by step answer:
Let’s define all the terms which are given in the question.
We have given the initial velocity of the particle i.e. uu at(t = 0)\left( {{\text{t = 0}}} \right).
The acceleration is given by αt32\alpha {t^{\dfrac{3}{2}}}.
That is, a=αt32\vec a = \alpha {t^{\dfrac{3}{2}}}
Here, the acceleration is dependent on time
Hence, we can say acceleration is a function of time.
Now, from the formula of acceleration,
That is,
\Rightarrow a=dvdt\vec a = \dfrac{{dv}}{{dt}}
adt  =  dv  \Rightarrow \vec adt\; = \;dv\; ………………………………… (1)
We know, acceleration is a function of time. The velocity is changing from u{\text{u}} to v{\text{v}} at time interval t = 0{\text{t = 0}} to t = t.{\text{t = t}}{\text{.}}
Hence, integrating equation (1) with applying these values as limit, we get
0tadt=uvdv\int_0^t {adt} = \int_u^v {dv}
Now, we are substituting the value of a{\text{a}},
We get,
0tαt32dt=uvdv\Rightarrow \int_0^t {\alpha {t^{\dfrac{3}{2}}}dt = \int_u^v {dv} }
α[t32+132+1]0t=[V]uv\Rightarrow \alpha \left[ {\dfrac{{{t^{\dfrac{3}{2} + 1}}}}{{\dfrac{3}{2} + 1}}} \right]_0^t = \left[ V \right]_u^v
α25t52=vu\Rightarrow \alpha \dfrac{2}{5}{t^{\dfrac{5}{2}}} = v - u
So, vu  =  25αt52v - u\; = \;\dfrac{2}{5}\alpha {t^{\dfrac{5}{2}}}
v=  u+25αt52v = \;u + \dfrac{2}{5}\alpha {t^{\dfrac{5}{2}}}
This is the final relation for velocity.

Hence, the final answer is option (C) i.e. v=  u+25αt52v = \;u + \dfrac{2}{5}\alpha {t^{\dfrac{5}{2}}}.

Additional Information:
a=ΔvΔta = \dfrac{{\Delta v}}{{\Delta t}} Where Δv=vfvi\Delta v = {v_f} - {v_i} and Δt  =tfti\Delta t\; = {t_f} - {t_i}.
The equation for acceleration may be written as
a = \dfrac{{\Delta v}}{{\Delta t}} = \dfrac{{{v_f} - {v_i}}}{{{t_f} - {t_i}}}\;\\_\\_\left( 1 \right)
Note that, tfti{t_f} - {t_i} is always positive as tf>  ti{t_f} > \;{t_i} and it is called ‘elapsed time’.
Equation (1)\left( 1 \right) becomes
a=vfvita = \dfrac{{{v_f} - {v_i}}}{t}

Note: Velocity is defined as the rate of change of distance with respect to time, whereas acceleration is defined as the rate of change of Speed. And both of them are vector quantities. To solve these types of questions, simply use the equation of motion, & if the quantity is changing at t=0t = 0 to t=t,t = t, then integrate it with respect to proper limits. This way you are able to solve such Questions.