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Question: A particle is projected vertically upwards from a point A on the ground. It takes time \( {t_1} \) ,...

A particle is projected vertically upwards from a point A on the ground. It takes time t1{t_1} , to reach a point B, but it still continues to move up. It takes further time t2{t_2} to reach the ground from point B. the height of point B from the ground is-

Explanation

Solution

Hint : The total time of flight is equal to the sum of the time to get to point B and the time to go from point B back to the ground. The final height from the ground should only be expressed in terms of all known values (i.e. constants and variables given)

Formula used: In this solution we will be using the following formula;
h=ut±12gt2h = ut \pm \dfrac{1}{2}g{t^2} where hh is the height of an upwardly projected object above the ground, uu is the initial velocity of projection, tt is the particular considered, and gg is the acceleration due to gravity.
T=2ugT = \dfrac{{2u}}{g} where TT is the time of flight.

Complete step by step answer
A particular particle is projected vertically upwards from point A on the ground. It is said to reach point B after a time t1{t_1} , we are to calculate the height of B above the ground.
The height above the ground of such motion is given as
h=ut±12gt2h = ut \pm \dfrac{1}{2}g{t^2} where uu is the initial velocity of projection, tt is the particular consideration, and gg is the acceleration due to gravity. Hence, for our particle at point B it is
hB=ut112gt12{h_B} = u{t_1} - \dfrac{1}{2}g{t_1}^2 ( on assuming downward is negative)
All variables, except the initial velocity of projection uu , is known. Hence, we need to find uu .
The time of flight (time taken to complete whole journey) is given as
T=2ugT = \dfrac{{2u}}{g} , hence, making uu subject of formula, we have that
u=Tg2u = \dfrac{{Tg}}{2}
But according to question, it takes a time t2{t_2} to go from point B back to the ground, hence, the total time of flight is
T=t1+t2T = {t_1} + {t_2} , thus by insertion,
u=g(t1+t2)2u = \dfrac{{g({t_1} + {t_2})}}{2} , then finally, substituting into hB=ut1+12gt12{h_B} = u{t_1} + \dfrac{1}{2}g{t_1}^2 , we have
hB=g(t1+t2)2t112gt12{h_B} = \dfrac{{g({t_1} + {t_2})}}{2}{t_1} - \dfrac{1}{2}g{t_1}^2
By simplifying
hB=gt12[(t1+t2)t1]{h_B} = \dfrac{{g{t_1}}}{2}\left[ {({t_1} + {t_2}) - {t_1}} \right]
hB=gt12(t2)\Rightarrow {h_B} = \dfrac{{g{t_1}}}{2}\left( {{t_2}} \right)
Thus,
hB=gt1t22\therefore {h_B} = \dfrac{{g{t_1}{t_2}}}{2} .

Note
For clarity, the time of flight can be derived from the equation of the velocity
v=ugtv = u - gt where vv is the final velocity at a time tt . Hence, the for time of flight t=Tt = T , the final velocity is equal to negative of the initial velocity (since they are in opposite direction) i.e. v=uv = - u
Hence, u=ugT- u = u - gT
2u=gT\Rightarrow 2u = gT
By dividing both sides by gg , we have
T=2ugT = \dfrac{{2u}}{g} .