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Question: A body is projected vertically upwards. The times corresponding to height \[H\] while ascending and ...

A body is projected vertically upwards. The times corresponding to height HH while ascending and while descending are t1{t_1} and t2{t_2} respectively. Then, the velocity of projection will be (take gg as acceleration due to gravity)
(A) gt1t22\dfrac{{g\sqrt {{t_1}{t_2}} }}{2}
(B) g(t1+t2)2\dfrac{{g\left( {{t_1} + {t_2}} \right)}}{2}
(C) gt1t2g\sqrt {{t_1}{t_2}}
(D) gt1t2(t1+t2)g\dfrac{{{t_1}{t_2}}}{{\left( {{t_1} + {t_2}} \right)}}

Explanation

Solution

We need to use the second equation of motion to find the times at which the body will be at height HH. With time as the unknown variable, the second equation of motion is a quadratic equation.
Formula used: In this solution we will be using the following formulae;
h=ut+12gt2h = ut + \dfrac{1}{2}g{t^2} where hh is the height of an object thrown vertically upward, uu is the initial velocity of projection, gg is the acceleration due to gravity, and tt is the instantaneous time when at the height.
x=b±b24ac2ax = \dfrac{{ - b \pm \sqrt {{b^2} - 4ac} }}{{2a}} for an equation ax2+bx+c=0a{x^2} + bx + c = 0

Complete Step-by-Step solution:
Generally, when a body is thrown upwards, any particular height is crossed twice, while going up and while coming down. The second equation of motion can be used to calculate the times when it crosses a particular height. This is given as
h=ut+12gt2h = ut + \dfrac{1}{2}g{t^2} where hh is the height of an object thrown vertically upward, uu is the initial velocity of projection, gg is the acceleration due to gravity, and tt is the instantaneous time when at the height.
By inserting known values, we have
H=ut12gt2H = ut - \dfrac{1}{2}g{t^2}
gt22ut+2H=0\Rightarrow g{t^2} - 2ut + 2H = 0 which is a quadratic equation.
Hence, using the quadratic formula given by
x=b±b24ac2ax = \dfrac{{ - b \pm \sqrt {{b^2} - 4ac} }}{{2a}} for an equation ax2+bx+c=0a{x^2} + bx + c = 0.
Hence, we have
t=2u±(2u)24(g)(2H)2g=2u±4u28gH2gt = \dfrac{{2u \pm \sqrt {{{\left( {2u} \right)}^2} - 4\left( g \right)\left( {2H} \right)} }}{{2g}} = \dfrac{{2u \pm \sqrt {4{u^2} - 8gH} }}{{2g}}
By simplification, we have
t=u±u22gHgt = \dfrac{{u \pm \sqrt {{u^2} - 2gH} }}{g}
Then the two different values of tt are
t1=uu22gHg{t_1} = \dfrac{{u - \sqrt {{u^2} - 2gH} }}{g}
and
t2=u+u22gHg{t_2} = \dfrac{{u + \sqrt {{u^2} - 2gH} }}{g}
By adding the two times, we have
t1+t2=u+u22gHg+uu22gHg=2ug{t_1} + {t_2} = \dfrac{{u + \sqrt {{u^2} - 2gH} }}{g} + \dfrac{{u - \sqrt {{u^2} - 2gH} }}{g} = \dfrac{{2u}}{g}
By making uu subject, we have
u=g(t1+t2)2u = \dfrac{{g\left( {{t_1} + {t_2}} \right)}}{2}

Hence, the correct option is B

Note: For clarity, the equation H=ut12gt2H = ut - \dfrac{1}{2}g{t^2} has been derived by allowing downward to be negative. This is a matter of choice, and hence upward can be taken as negative instead. However, note that when upward is negative the height h=Hh = - H, and not HH, since the height is measured upward from the ground.