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Question: If \( R \) and \( H \) are the horizontal range and maximum height attained by a projectile then its...

If RR and HH are the horizontal range and maximum height attained by a projectile then its speed of projection is:

& A.\sqrt{2gR+\dfrac{4{{R}^{2}}}{gH}} \\\ & B.\sqrt{2gh+\dfrac{{{R}^{2}}g}{8H}} \\\ & C.\sqrt{2gH+\dfrac{8H}{gR}} \\\ & D.\sqrt{2gH+\dfrac{{{R}^{2}}}{H}} \\\ \end{aligned}$$
Explanation

Solution

A body experiences a projectile motion when the object is projected at an inclination from the ground. Then the body follows a curved path, which is parabolic in nature and is called the ballistic trajectory. Then the distance covered by the body along the x and y-axis respectively is given as, RR and HH which is the maximum horizontal range and maximum height attained by the object.

Formula used:
v2u2=2asv^{2}-u^{2}=2as and s=ut+12at2s=ut+\dfrac{1}{2}at^{2}

Complete step-by-step answer:
Let uu be the initial velocity of the body which is projected at an angle θ\theta from the horizontal. Let HH and RR be the maximum distances along the x and y-axis respectively, during the time of flight TT. Then the initial velocity uu can be resolved into two components along the x and y axis respectively.

Then along the y-axis we have, the maximum height HH , initial velocity uy=usinθu_{y}=usin\theta , final velocity vy=0v_{y}=0 and acceleration ay=ga_{y}=-g
Then we can write, v2u2=2asv^{2}-u^{2}=2as or 0(usinθ)2=2×(g)×H0-(usin\theta)^{2}=2\times (-g)\times H
Or usinθ=2gHusin\theta=\sqrt{2gH}
From s=ut+12at2s=ut+\dfrac{1}{2}at^{2} , let us consider the he half flight, where s=Hs=-H and t=T2t=\dfrac{T}{2}
Then we get, H=0+12(g)(T2)2-H=0+\dfrac{1}{2}(-g)\left(\dfrac{T}{2}\right)^{2}
Or, T=8HgT=\sqrt{\dfrac{8H}{g}}
Similarly, along the x-axis we have, the maximum range RR and the initial velocity ux=ucosθu_{x}=ucos\theta . The time of flight TT can be given as T=RucosθT=\dfrac{R}{ucos\theta}
Or, ucosθ=RTucos\theta=\dfrac{R}{ T}
This is similar to vel=distancetimevel=\dfrac{distance}{time}
Substituting for TT we get, ucosθ=R×g8Hucos\theta=R\times\sqrt{\dfrac{g}{8H}}
Let us square and add (usinθ)2+(ucosθ)2=u2(usin\theta)^{2}+(ucos\theta)^{2}=u^{2} as sin2θ+cos2θ=1sin^{2}\theta+cos^{2}\theta=1
Or u2=(2gH)2+(R×g8H)2u^{2}=(\sqrt{2gH})^{2}+\left(R\times\sqrt{\dfrac{g}{8H}}\right )^{2}
Or, u=2gH+R2g8Hu=\sqrt{2gH+\dfrac{R^{2}g}{8H}}

So, the correct answer is “Option B”.

Note: When the object is on the air,the only force acting on the body is the force due to gravitation, which pulls the object back to the surface at the speed of acceleration due to gravity. Note that the range of the projected body is greater than the distance the body will cover, when dropped from the same height.