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Question: If a person can through a stone upto a maximum height of h metre vertically, then the maximum distan...

If a person can through a stone upto a maximum height of h metre vertically, then the maximum distance through which it can be thrown horizontally by the same person is,
A) h2\dfrac{h}{2}metres.
B) h metres.
C) 2h metres.
D) 3h metres.

Explanation

Solution

Hint
Find out the relation between u and H using the condition of Maximum vertical height. At maximum height v=0v = 0. And then for maximum horizontal range use the formula for range which is given by R=u2sin2θgR = \dfrac{{{u^2}\sin 2\theta }}{g} and put the value of θas45\theta \,{\text{as}}\,{45^{^ \circ }}and solve for R to find out the answer.

Complete step by step answer
Let the person throw the stone with an initial velocity u and when the stone reaches the maximum height, its final velocity becomes zero. So, using the third law of motion we have,
v2=u2+2aS{v^2} = {u^2} + 2aS
Putting the values as mentioned we have,
02=u22gH\Rightarrow {0^2} = {u^2} - 2gH
H=u22g\Rightarrow H = \dfrac{{{u^2}}}{{2g}}
u2=2gH\Rightarrow {u^2} = 2gH
Now for the maximum distance to be covered (horizontal) the angle with which the stone should be thrown must be 45{45^{^ \circ }}.
In case of a projectile to attain maximum range, angle must be 45{45^{^ \circ }}.
So, the maximum horizontal range is given by,
R=u2sin2θgR = \dfrac{{{u^2}\sin 2\theta }}{g}
On putting the appropriate values we have,
R=u2sin(2×45)g\Rightarrow R = \dfrac{{{u^2}\sin (2 \times {{45}^{^ \circ }})}}{g}
R=u2sin(90)g\Rightarrow R = \dfrac{{{u^2}\sin ({{90}^{^ \circ }})}}{g}
On further solving we have,
R=2gHg\Rightarrow R = \dfrac{{2gH}}{g}
R=2H\Rightarrow R = 2H
Therefore the maximum range through which the stone travels is 2H.
Hence the correct answer is option (C).

Note
At both angles θand(90θ)\theta \,{\text{and}}\,(90 - \theta )the horizontal range is the same. This can be proved by inverting the value of θ\theta as θand(90θ)\theta \,{\text{and}}\,(90 - \theta )in the formula, R=u2sin2θgR = \dfrac{{{u^2}\sin 2\theta }}{g}. By using the simple trigonometric identity like sin2(90θ)=sin(1802θ)=sin2θ\sin 2(90 - \theta ) = \sin (180 - 2\theta ) = \sin 2\theta , we can prove the following statement.