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Question: two bodies begin to fall freely from the same height. The second one begins to fall \(\tau s\)after ...

two bodies begin to fall freely from the same height. The second one begins to fall τs\tau safter the first. The time after which the 1st body begins to fall, the distance between bodies equals ll is.
A. lgτ+τ2\dfrac{l}{{g\tau }} + \dfrac{\tau }{2}
B. gτl+τ\dfrac{{g\tau }}{l} + \tau
C. τlg+2τ\dfrac{\tau }{{\lg }} + \dfrac{2}{\tau }
D. glτ+τ2\dfrac{g}{{l\tau }} + \dfrac{\tau }{2}

Explanation

Solution

this question is from the kinematics section, so we will be using the kinematics equation s=ut+12at2s = ut + \dfrac{1}{2}a{t^2} . We have been given two bodies which are at the same height falling freely which means we will take the initial velocity as zero. We will find the distance covered by body 11 and body 22 . We will subtract the distance and will put it equal to ll. Will solve the equation and find our required time.

Complete step by step answer:
Initially it has given that both bodies are at the same height and fall freely.

After τs\tau s body 11 will move, and body 22 would have been moved to t+τt + \tau , it is given in the question that after t+τt + \tau the difference between two bodies is ll , then we have to find the value of tt. See the following diagram,

Here t+T=t+τt + T = t + \tau . We will find the distance covered by body 11 in time t+τt + \tau and by body 22 in time tt . And by subtracting both and putting it equal to ll we will find our required tt. Using the second equation of motion
s=ut+12at2s = ut + \dfrac{1}{2}a{t^2}
We know u=0u = 0 and a=ga = g
So, s=12gt2s = \dfrac{1}{2}g{t^2}

Let distance covered by body 11 be s1{s_1} and distance covered by body 22 be s2{s_2}
Therefore, s1=12g(t+τ)2{s_1} = \dfrac{1}{2}g{\left( {t + \tau } \right)^2}
s2=12gt2{s_2} = \dfrac{1}{2}g{t^2}
Now we have to find the value of tt
So s2s1=l{s_2} - {s_1} = l
Putting values from above
12gt212g(t+τ)2=l\dfrac{1}{2}g{t^2} - \dfrac{1}{2}g{\left( {t + \tau } \right)^2} = l
Solving this we will get
12g[t2(tτ)2]=l\dfrac{1}{2}g\left[ {{t^2} - {{\left( {t - \tau } \right)}^2}} \right] = l
(t+tτ)(tt+τ)=2lg\Rightarrow \left( {t + t - \tau } \right)\left( {t - t + \tau } \right) = \dfrac{{2l}}{g}
2tτ=2lgτ\Rightarrow 2t - \tau = \dfrac{{2l}}{{g\tau }}
t=12[2lgτ+τ]\Rightarrow t = \dfrac{1}{2}\left[ {\dfrac{{2l}}{{g\tau }} + \tau } \right]
t=lgτ+τ2\therefore t = \dfrac{l}{{g\tau }} + \dfrac{\tau }{2}

Therefore, option A is the correct answer.

Note: There are two important motion properties that free-falling objects possess:
-Air resistance does not exist for free-falling objects.
-On Earth, all free-falling objects accelerate downwards.
The time measured is from that instant from which the second body was released. Since both the bodies were initially at zero their initial velocity is taken as zero. Acceleration is due to gravity that is why we have taken a=ga = g.