(i) Let H be the maximum height reached by the projectile in time t1 For vertical motion,
The initial velocity = u sinθ
The final velocity = 0
Acceleration = - g
∴ using, v2 = u2 + 2as
0 = u2sin2 θ - 2gH
2gH = u2sin2 θ
H = \(\frac {u^2 sin^2 \theta}{2g}\)
(ii) Let t, be the time taken by the projectile to reach the maximum height H.
For vertical motion,
initial velocity = usin θ
Final velocity at the maximum height = 0
Acceleration a = - g
Using the equation v = u + at1
0 = usin θ - gt1
gt1 = usin θ
t1 = \(\frac {usin\theta} {g}\)
Let t2 be the time of descent.
But t1 = t2
i.e. time of ascent = time of descent.
∴ Time of flight T = t1 + t2 = 2t1
∴ T = \(\frac {2usin \theta}{g}\)
(iii) Let R be the range of the projectile in a time T. This is covered by the projectile with a constant velocity ucos θ.
Range = horizontal component of
velocity × Time of flight
i.e, R = ucos θ. T
R = ucos θ. \(\frac{2usin\theta}{g}\)
R = \(\frac{u^2sin2\theta}{g}\)
∵ 2 sin θ.cos θ = sin2 θ.