Physics, asked by tamnaypal3510, 9 months ago

Show that the maximum range of a projectile in any direction is described in the same time in which it would fall freely under gravity through this distance starting from rest.

Answers

Answered by nirman95
7

To Prove:

Maximum range of a projectile is described in the same time in which it takes to fall freely under gravity through the same distance starting from rest.

Proof:

For Projectile:

Let range be R , initial velocity of projectile be u , gravity be g and \theta be angle of Projection.

 \therefore \: R =  \dfrac{ {u}^{2}  \sin(2 \theta) }{g}

For maximum value of R , the value of sine function should be maximum

 \therefore \:  \sin(2 \theta)  = 1

 =  > 2 \theta = 90 \degree

 =  >  \theta = 45 \degree

So maximum range is obtained at 45° angle of Projection.

Time taken for maximum range be T

 \therefore \: T =  \dfrac{2u \sin( \theta) }{g}

  =  >  \: T =  \dfrac{2u \sin( 45 \degree) }{g}

  =  >  \: T =  \dfrac{2u \times  ( \frac{1}{ \sqrt{2} })  }{g}

 =  > T =  \dfrac{u \sqrt{2} }{g}

For Vertical Free Fall:

Height = Max range = u²/g

 \therefore \: H =  \dfrac{1}{2} g {t}^{2}

 =  >  \dfrac{ {u}^{2} }{g}  =  \dfrac{1}{2} g {t}^{2}

 =  >  {t}^{2}  =  \dfrac{2 {u}^{2} }{ {g}^{2} }

 =  > t =  \dfrac{u \sqrt{2} }{g}

So , in both cases , t and T are same

[Hence Proved]

Answered by Arceus02
3

Question:-

Show that the maximum range of a projectile in any direction is described in the same time in which it would fall freely under gravity through this distance starting from rest.

Answer:-

\bold{Finding \:\theta\: for\: which\: range\: is\: maximum:-}

\sf{R\:=\:\dfrac{{u}^{2}sin(2\theta)}{g}}

R is maximum when \bf{sin(2\theta)} is maximum

\bf{sin(90)} = 1 is maximum value possible

Then \bf{2\theta } = 90°

So \bf{\theta} = 45°

Range:-

\sf{R\:=\:\dfrac{{u}^{2}sin(2\theta)}{g}}

\sf{\implies\:R\:=\:\dfrac{{u}^{2}1}{g}}

\sf{\implies\:R\:=\:\dfrac{{u}^{2}}{g}}

Time of flight:-

\bf{Time\:of\:flight\:for\:\theta\:=\:45°:-}

\sf{T\:=\:\dfrac{2usin(\theta)}{g}}

\sf{\implies\:T=\dfrac{2u*\dfrac{1}{\sqrt{2}}}{g}}

\sf{\implies\:=\:T=\dfrac{\sqrt{2}u}{g}}

\rule{400}{4}

Vertical free fall:-

Given: Height = max range = u²/g

Height = H

Apply s = ut + 1/2(a)(t²)

=> -H = 0 - 1/2(g)(t²)

=> H = 1/2(g)t²

Given: H = u²/g

=> \sf{\dfrac{{u}^{2}}{g}\:=\:\dfrac{1}{2}(g){t}^{2}}

=> \sf{\dfrac{2{u}^{2}}{{g}^{2}}\:=\:{t}^{2}}

=> \sf{t\:=\:\sqrt{\dfrac{2{u}^{2}}{{g}^{2}}}}

=> \sf{t\:=\:\dfrac{\sqrt{2}u}{g}}

T = t

Hence, proved

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