A stone projected with a velocity u at an angle with the horizontal reaches maximum height h1. When it is projected with velocity u at an angle 2 with the horizontal, it reaches maximum height h2. The relation between the horizontal range r of the projectile, h1 and h2 is
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Let the velocity of projection of the stone be uwith angle of projection θ with the horizontal direction.
The vertical component of the velocity of projection is usinθ and the horizontal component is ucosθ
Now if the time of flight be T then the object will return to the ground after T sec and during this T sec its total vertical displacement h will be zero. So applying the equation of motion under gravity we can write
h=usinθ×T+12gT2
⇒0=usinθT−12×g×T2 where g=acceleration due to gravity
∴T=2usinθg
The horizontal displacement or range during this T sec is
R=ucosθ×T
⇒R=u2sin(2θ)g.......[1]
If H be the maximum height attained by the stone we can write
02=u2sin2θ−2gH
⇒H=u2sin2θ2g....[2]
CALCULATION USING ABOVE RELATIONS
For 1st case
when θ=α,H=h1
So horizontal range
R1=u2sin(2α)g.....[3]
and h1=u2sin2α2g....[4]
For 2nd case
when θ=90−α,H=h2
So horizontal range
R2=u2sin(2(90−α))g
⇒R2=u2sin(180−2α)g
⇒R2=u2sin(2α)g....[5]
and h2=u2sin2(90−α)2g
⇒h2=u2cos2(α)2g....[6]
In both the cases the range is same.So let R1=R2=R
Hence range
R=u2sin(2α)g
Now multiplying [4] and [6] we get
h1h2=u4sin2αcos2α(2g)2
⇒h1h2=(u2×2sinαcosα)2(4g)2
⇒h1h2=(u2×sin2α)2(4g)2
⇒√h1h2=u2×sin2α4g
⇒√h1h2=R4
⇒R=4√h1h2
The vertical component of the velocity of projection is usinθ and the horizontal component is ucosθ
Now if the time of flight be T then the object will return to the ground after T sec and during this T sec its total vertical displacement h will be zero. So applying the equation of motion under gravity we can write
h=usinθ×T+12gT2
⇒0=usinθT−12×g×T2 where g=acceleration due to gravity
∴T=2usinθg
The horizontal displacement or range during this T sec is
R=ucosθ×T
⇒R=u2sin(2θ)g.......[1]
If H be the maximum height attained by the stone we can write
02=u2sin2θ−2gH
⇒H=u2sin2θ2g....[2]
CALCULATION USING ABOVE RELATIONS
For 1st case
when θ=α,H=h1
So horizontal range
R1=u2sin(2α)g.....[3]
and h1=u2sin2α2g....[4]
For 2nd case
when θ=90−α,H=h2
So horizontal range
R2=u2sin(2(90−α))g
⇒R2=u2sin(180−2α)g
⇒R2=u2sin(2α)g....[5]
and h2=u2sin2(90−α)2g
⇒h2=u2cos2(α)2g....[6]
In both the cases the range is same.So let R1=R2=R
Hence range
R=u2sin(2α)g
Now multiplying [4] and [6] we get
h1h2=u4sin2αcos2α(2g)2
⇒h1h2=(u2×2sinαcosα)2(4g)2
⇒h1h2=(u2×sin2α)2(4g)2
⇒√h1h2=u2×sin2α4g
⇒√h1h2=R4
⇒R=4√h1h2
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