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Question: Prove that the maximum horizontal range is four times the maximum height attained by a projectile wh...

Prove that the maximum horizontal range is four times the maximum height attained by a projectile which is fired along the required oblique direction.

Explanation

Solution

In this question firstly, we will find the time, Maximum horizontal distance and the height of projectile and then accordingly we will put the values in the equation of maximum height to find out at what the range is to the maximum height.

Formula used:
Formula for range of a projectile
R=u2sin2θgR = \dfrac{{{u^2}\sin 2\theta }}{g}
Where, uu is the speed and gg is the acceleration due to gravity.
Formula for height of a projectile
H=u2sin2θ2gH = \dfrac{{{u^2}{{\sin }^2}{\theta ^ \circ }}}{{2g}}

Complete step by step answer:
Let us consider a body, which is projected with the speed um s1um{\text{ }}{s^{ - 1}} which is inclined at θ\theta with the horizontal line.Then we can say that the vertical component of uu , uy=usinθ{u_y} = u\sin \theta and horizontal component of uu , ux=ucosθ{u_x} = u\cos \theta .Acceleration on vertical direction ay=g{a_y} = - g and acceleration on horizontal direction ax=0{a_x} = 0. And we know that,
x=uxt x=ucosθ×t x = {u_x}t \\\ \Rightarrow x = u\cos \theta \times t \\\
t=xucosθ\Rightarrow t = \dfrac{x}{{u\cos \theta }} -----(1)
Similarly,
y=uyt+12ayt2 y=usinθ×t+12(g)t2 y = {u_y}t + \dfrac{1}{2}{a_y}{t^2} \\\ \Rightarrow y = u\sin \theta \times t + \dfrac{1}{2}( - g){t^2} \\\
Now, substituting the value of tt in above equation,
y=usinθ×xucosθ12g×(xucosθ)2 y=xtanθ12gx2u2cos2θ y = u\sin \theta \times \dfrac{x}{{u\cos \theta }} - \dfrac{1}{2}g \times {\left( {\dfrac{x}{{u\cos \theta }}} \right)^2} \\\ \Rightarrow y = x\tan \theta - \dfrac{1}{2}g\dfrac{{{x^2}}}{{{u^2}{{\cos }^2}\theta }} \\\
Which is as similar as the equation of a parabola y=ax+bx2+cy = ax + b{x^2} + c .
As we know that, range equals to, R=u2sin2θgR = \dfrac{{{u^2}\sin 2\theta }}{g}
And RR will be maximum, if
sin2θ=1 2θ=90 θ=45 \sin 2\theta = 1 \\\ \Rightarrow 2\theta = {90^ \circ } \\\ \Rightarrow \theta = {45^ \circ } \\\
Then, Rmax=u2g{R_{\max }} = \dfrac{{{u^2}}}{g}
Therefore, the maximum height will be:
H=u2sin2452gH=u2g×12H=Rmax4 Rmax=4H H = \dfrac{{{u^2}{{\sin }^2}{{45}^ \circ }}}{{2g}} \Rightarrow H = \dfrac{{{u^2}}}{g} \times \dfrac{1}{2} \Rightarrow H = \dfrac{{{R_{\max }}}}{4} \\\ \therefore {R_{\max }} = 4H \\\
Hence, the range is 4 times the maximum height of the projectile.

Note: A projectile is a parabolic motion that is nothing but defined as the superposition of two fundamental forms of motion which are, constant acceleration in one direction and constant velocity in the other. Projectiles include thrown balls, rifle bullets, and falling bombs. Remember all the formulas of maximum height, time of flight and horizontal range of the projectile. It becomes very easy when we solve questions of this type.For easy calculation remember that the horizontal range is maximum when the angle of projection is 45{45^ \circ } .