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Question: A car starting from rest accelerates at rate\(\alpha \)through a distance \(x\) then continues at co...

A car starting from rest accelerates at rateα\alpha through a distance xx then continues at constant speed for time t and then decelerates at a rate of α2\dfrac{\alpha }{2} to come to rest. If the total distance travelled is 15x15x. Then
A.x=14αt2x=\dfrac{1}{4}\alpha {{t}^{2}}
B.x=12αt2x=\dfrac{1}{2}\alpha {{t}^{2}}
C.x=18αt2x=\dfrac{1}{8}\alpha {{t}^{2}}
D.x=172αt2x=\dfrac{1}{72}\alpha {{t}^{2}}

Explanation

Solution

While dealing with problems based on one dimensional Motion of an object in a straight line, we usually come across three kinematic variables namely velocity(v)\left( v \right) , position(s)\left( s \right) and time(t)\left( t \right) and to find one when others are already provided , we use the three equations of motion that are basically equations that describe the behavior of a physical system in terms of the given variables and each could be characterized by an entanglement of two.
The three equations of motion are:
v=u+gtv=u+gt
h=ut+12gt2h=ut+\dfrac{1}{2}g{{t}^{2}}
v2u2=2gh{{v}^{2}}-{{u}^{2}}=2gh
Where u=Initial velocityu=Initial\text{ }velocity
v=Final velocityv=Final\text{ }velocity
g=acceleration due to gravityg=acceleration\text{ }due\text{ }to\text{ }gravity
h=heighth=height
t=timet=time
It is with the help of these three equations of motion that we are going to solve and give appropriate solutions to the given question.

Complete answer:
The total distance covered by the car = 15x15x
\therefore 15x=x+x1+x215x=x+{{x}_{1}}+{{x}_{2}}
Where, x is the displacement covered during the first phase of travel
x1{{x}_{1}} is the displacement covered during the second phase of travel
x2{{x}_{2}}is the displacement covered during the third phase of travel
Lett0'{{t}_{0}}', t1'{{t}_{1}}',t2'{{t}_{2}}'be the time duration for covering x, x1{{x}_{1}},x2{{x}_{2}} displacements respectively.
For phase 1:
x=ut+12αt02\Rightarrow x=ut+\dfrac{1}{2}\alpha t_{0}^{2}
x=12αt02\Rightarrow x=\dfrac{1}{2}\alpha t_{0}^{2}
\left\\{ \because u=0 \right\\}
v=u+αt0\Rightarrow v=u+\alpha {{t}_{0}}
v=αt0\Rightarrow v=\alpha {{t}_{0}}
Where ‘v’ stands for the final velocity in this phase.
For phase 2:
x1=vt1{{x}_{1}}=v{{t}_{1}}
x1=(αt0)t1{{x}_{1}}=(\alpha {{t}_{0}}){{t}_{1}}
For phase 3:
v32u32=2(α2x3)\Rightarrow v_{3}^{2}-u_{3}^{2}=2\left( \dfrac{\alpha }{2}{{x}_{3}} \right)
0(αt0)2=2(α2x3)\Rightarrow 0-{{(\alpha {{t}_{0}})}^{2}}=2\left( \dfrac{\alpha }{2}{{x}_{3}} \right)
x3=αt02\Rightarrow {{x}_{3}}=\alpha t_{0}^{2}
15x=12αt02+(αt0)t1+αt02\Rightarrow 15x=\dfrac{1}{2}\alpha t_{0}^{2}+(\alpha {{t}_{0}}){{t}_{1}}+\alpha t_{0}^{2}
15x=x+(αt0)t1+2x\Rightarrow 15x=x+(\alpha {{t}_{0}}){{t}_{1}}+2x
12x=αt0t1\Rightarrow 12x=\alpha {{t}_{0}}{{t}_{1}}
From phase 1:
x=12αt02\Rightarrow x=\dfrac{1}{2}\alpha t_{0}^{2}
12xx=(αt0)t112αt02\Rightarrow \dfrac{12x}{x}=\dfrac{(\alpha {{t}_{0}}){{t}_{1}}}{\dfrac{1}{2}\alpha t_{0}^{2}}
t0=t16\Rightarrow {{t}_{0}}=\dfrac{{{t}_{1}}}{6}
After substituting the value of t0{{t}_{0}}
12x=(αt16)×t1\Rightarrow 12x=\left( \alpha \dfrac{{{t}_{1}}}{6} \right)\times {{t}_{1}}
x=αt1272\Rightarrow x=\dfrac{\alpha t_{1}^{2}}{72}

Therefore, the correct option would be (D) x=172αt2x=\dfrac{1}{72}\alpha t_{{}}^{2}

Note:
It is advised to be accurate and be attentive while performing substitution of different values in several equations. And also, the usage of the three equations of motion should also be done carefully and also values must be given appropriately especially the values of initial velocity and final velocity otherwise the student might resultantly get an incorrect solution.