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Question: A person is at a distance \(x\) from the bus when the bus begins to move with a constant acceleratio...

A person is at a distance xx from the bus when the bus begins to move with a constant acceleration aa . What is the minimum velocity with which the person should run towards the bus so as to catch it?
A)2ax2ax
B)2ax\sqrt {2ax}
C)axax
D)ax\sqrt {ax}

Explanation

Solution

Hint This is a pretty simple question which only requires us to use the equations of motion. These are:
s=ut+12at2s = ut + \dfrac{1}{2}a{t^2}
v2u2=2as{v^2} - {u^2} = 2as
v=u+atv = u + at
Where ss is the displacement.
uu is the initial velocity.
vv is the final velocity.
tt is the time.
aa is the acceleration.

Complete step-by-step solution :Let the distance moved by the bus until the man catches the bus be yy . The only thing common in the motion of the bus and man will be the time taken. Time taken by the man to cover distance (x+y)\left( {x + y} \right) will be equal to the time taken by the bus to cover the distance yy . You can also equate the velocity of the man and bus when the man gets on the bus.
Complete step by step answer:
A pictorial representation to understand this problem well is as follows:

Here, AA is the initial position of man, BB is the initial position of the bus and CC is the position at which man catches the bus.
Try to visualize the situation to proceed. Both the man and the bus start from the rest. Man runs with constant velocity while the bus moves with constant acceleration. Man should have a velocity fast enough such that his velocity matches the velocity of the bus after a certain displacement. Let this distance be yy . We are using the terms distance and displacement interchangeably because the motion is in one direction.
We know that initially the distance between the man and the bus is xx .
Now, let us focus upon the situation at point CC . At point CC, velocity of bus as well as the man attains the same value due to which the man is able to catch the bus. Moreover, time taken by man to reach this point from AA is equal to the time taken by the bus to reach this point from BB . We will make use of these results along with the three equations of motion which are:
s=ut+12at2s = ut + \dfrac{1}{2}a{t^2}
v2u2=2as{v^2} - {u^2} = 2as
v=u+atv = u + at
Where ss is the displacement.
uu is the initial velocity.
vv is the final velocity.
tt is the time.
aa is the acceleration.
Velocity of bus at point CC
Vbus=u+at Vbus=at  {V_{bus}} = u + at \\\ {V_{bus}} = at \\\
(Since, the initial velocity of the bus is zero.)
t=Vbusa or Vmana\Rightarrow t = \dfrac{{{V_{bus}}}}{a}{\text{ or }}\dfrac{{{V_{man}}}}{a}
Because at point CC , the velocity of the bus is equal to the velocity of the man.
So, t=Vmanat = \dfrac{{{V_{man}}}}{a} (1)
Using the relation v2u2=2as{v^2} - {u^2} = 2as for bus at point CC
Vman20=2ay{V_{man}}^2 - 0 = 2ay
y=Vman22ay = \dfrac{{{V_{man}}^2}}{{2a}} (2)
Using relation s=ut+12at2s = ut + \dfrac{1}{2}a{t^2} to describe the motion of man at point CC , we get
x+y=Vmantx + y = {V_{man}}t
(Since man moves with constant velocity.)
Substituting the values of tt and yy from equation (1) and (2) in the above relation, we get
x+Vman22a=(Vman)(Vmana) x=Vman2aVman22a x=Vman22a 2ax=Vman2 Vman=2ax  x + \dfrac{{{V_{man}}^2}}{{2a}} = \left( {{V_{man}}} \right)\left( {\dfrac{{{V_{man}}}}{a}} \right) \\\ x = \dfrac{{{V_{man}}^2}}{a} - \dfrac{{{V_{man}}^2}}{{2a}} \\\ x = \dfrac{{{V_{man}}^2}}{{2a}} \\\ 2ax = {V_{man}}^2 \\\ \Rightarrow {V_{man}} = \sqrt {2ax} \\\
So, option B is correct.

Note: You need to visualize the situation to understand and solve it. This solution is nothing but repeated use of equations of motions keeping in mind the conditions such as equal velocities and time taken at point CC as in this question.