Lucky Bird Hunter

A stone is projected from a point on the ground, so as to hit a bird on the top of a vertical pole of height "h" and then attains a max height "2h" above the ground.

If at the instant of projection, the bird flies in the horizontal direction with a uniform speed and if the stone hits the bird while descending, the ratio of the speed of the bird to the horizontal speed of the stone can be represented as:

a/(b+c).

Find the value of a^2 + b^2 + c^2


The answer is 7.

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2 solutions

Ayan Jain
Feb 25, 2015

Let Vy be the vertical component of the stone's velocity and Vx be it's horizontal velocity.

Max height = 2H = (Vy^2)/2g

Vy^2 = 4gH

Now, the time at which the stone reaches height H. There will be two such times. Let them be T and T', where T > T'.

H = (Vy)t - g(t^2)/2

Solutions of this are T, T'.

T = Vy + sqrt[Vy^2 - 2gH]/g

We need T - T' for the time between the 2 heights.

T - T' = 2sqrt{Vy^2 - 2gH}/g

Finally, (velocity of bird)/(Vx) = (T - T')/T = 2/[(sqrt2) + 1]

Sorry for non-formatting, I am unable to do so properly.

Kushal Thaman
Nov 19, 2018

The bird would be at a height h h twice during it's motion. The total time from the point of projection to the point where stone and bird collide can be given by the bigger root of h = v 0 sin α t A B 1 2 g t A B 2 h= v_{0} \sin{\alpha} t_{AB} - \frac{1}{2} g {t_{AB}}^{2} Now, we know that v 0 sin α = 2 g h v_{0} \sin{\alpha} = 2 \sqrt{gh} by writing its maximum height. Hence, substituting this in the first equation and solving quadratic gives us t A B = 2 h g ( 2 ± 1 ) t_{AB} = \sqrt{\frac{2h}{g}} (\sqrt{2} \pm 1) . Of course, the total time from the point of projection to the point where stone and bird collide would be T = 2 h g ( 2 + 1 ) T= \boxed{\sqrt{\frac{2h}{g}} (\sqrt{2} + 1)} . Since the bird is moving with a constant velocity (Let it be v b v_{b} ), we can write: R B D v b = T \frac{R_{BD}}{v_{b}} = T , where R B D R_{BD} is the distance the bird travels. This can of course be written as 2 v 0 cos α 2 h g 2v_{0} \cos{\alpha} \cdot \sqrt{\frac{2h}{g}} , considering it to be the range of a smaller projectile thrown with vertical velocity 2 g h \sqrt{2gh} and horizontal velocity v 0 cos α v_{0} \cos{\alpha} . Now, using R B D v b = T \frac{R_{BD}}{v_{b}} = T , we get

v 0 cos α v b = 2 2 + 1 {\boxed{\boxed{\frac{v_{0} \cos{\alpha}}{v_{b}} = \frac{2}{\sqrt{2} +1}}}}

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