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Question: A particle is projected vertically upwards and it reaches the maximum height \( H \) in time \( T \)...

A particle is projected vertically upwards and it reaches the maximum height HH in time TT seconds. The height of the particle at any time tt will be
(A) g(tT)2g{(t - T)^2}
(B) H12g(tT)2H - \dfrac{1}{2}g{(t - T)^2}
(C) 12g(tT)2\dfrac{1}{2}g{(t - T)^2}
(D) Hg(tT)2H - g{(t - T)^2}

Explanation

Solution

Hint : At the highest point, the velocity of the particle will be zero and the displacement will have the maximum value, i.e. HH . We will use the formulas of projectile motion in a plane to get the required equations.

Formula used:
v=u+at\Rightarrow v = u + at
where vv is the final velocity of the particle, uu is the initial velocity of the particle, aa is the acceleration acting on the particle, and tt is the time of action and for the calculation of the final velocity.
S=ut+12at2\Rightarrow S = ut + \dfrac{1}{2}a{t^2} ,
where SS is the displacement of the body and the rest of the notations are the same as in the above equation.

Complete step by step answer
Applying the formula v=u+atv = u + at at the topmost point, we get
0=U+(g)T\Rightarrow 0 = U + ( - g)T
U=gT\Rightarrow U = gT ,
where UU is the initial velocity of the particle.
Applying the formula S=ut+12at2S = ut + \dfrac{1}{2}a{t^2} at the topmost point again, we get
H=UT+12(g)T2\Rightarrow H = UT + \dfrac{1}{2}( - g){T^2}
Putting the value of the initial velocity UU as found above, we get
H=(gT)T12gT2\Rightarrow H = (gT)T - \dfrac{1}{2}g{T^2}
H=12gT2\Rightarrow H = \dfrac{1}{2}g{T^2} .
We will use these values in the general equation of motion S=ut+12at2S = ut + \dfrac{1}{2}a{t^2} , so that at a general height hh , we get the required equation as
h=Ut+12(g)t2\Rightarrow h = Ut + \dfrac{1}{2}( - g){t^2} ,
substituting U=gTU = gT , we get
h=gTt12gt2\Rightarrow h = gTt - \dfrac{1}{2}g{t^2}
Adding 0=H12gT20 = H - \dfrac{1}{2}g{T^2} to the above equation we get,
h=gTt12gt2+H12gT2\Rightarrow h = gTt - \dfrac{1}{2}g{t^2} + H - \dfrac{1}{2}g{T^2}
h=H+(gTt12gt212gT2)\Rightarrow h = H + (gTt - \dfrac{1}{2}g{t^2} - \dfrac{1}{2}g{T^2})
On rearranging the equation further, we get,
h=H12g(2Tt+t2+T2)\Rightarrow h = H - \dfrac{1}{2}g( - 2Tt + {t^2} + {T^2})
h=H12g(tT)2\Rightarrow h = H - \dfrac{1}{2}g{(t - T)^2}
Therefore, the correct answer is option (B); H12g(tT)2H - \dfrac{1}{2}g{(t - T)^2} .

Note
The answer obtained is symmetric for a time of TT before and after the value of t=Tt = T . This means that the value of the height of the particle will be the same at t=0t = 0 and at t=2Tt = 2T . This indicated that the displacement of the particle will start from 00 , reach the highest value of HH at t=Tt = T , and then decrease, at the same rate of increase, to 00 at t=2Tt = 2T .