For a given velocity, a projectile has the same range R for two angles of projection, if t1 and t2 are the times of flight in the two cases then
t1t2 ∝R
As we know for complementary angles will have the same range for a projectile with a given velocity.
Therefore,
t1=2u×sinθ1g
t2=2u×sinθ2g
sinθ1+sinθ2=90o
t1t2=2Rg ∴ t1t2∝ R
Where,
R=(u)2×sin 2 θg