Nah, Not pi by 4

The angle of projection that gives the maximum horizontal range of a projectile, if the point of projection is at h = 160 m h=160 m above the point of landing is θ \theta for the speed of projection u = 200 m / s u=\sqrt {200} m/s .

If sin θ = a b \sin \theta =\frac {\sqrt {a}}{b} in simplified form, then find a+b?

Details :

  • ( a , b ) (a, b) are whole numbers.

  • a a has no factor of a perfect square.

  • g = 10 m / s 2 g=10 m/s^2 .Neglect any other force.

  • Horizontal range is the horizontal component of displacement from starting point to landing point.


The answer is 8.

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4 solutions

We have that (i) x = u t c o s θ x = ut*cos\theta and (ii) y = 160 + u t s i n θ 5 t 2 y = 160 + ut*sin\theta - 5*t^{2} .

From (ii) we find that, when y = 0 y = 0 ,

t = ( 1 10 ) ( u s i n θ + u 2 s i n 2 θ + 3200 t = 2 ( s i n θ + s i n 2 θ + 16 ) t = (\frac{1}{10})*(u*sin\theta + \sqrt{u^{2}*sin^{2}\theta + 3200} \Longrightarrow t = \sqrt{2} (sin\theta + \sqrt{sin^{2}\theta + 16}) ,

where I used the fact that u = 200 = 10 2 u = \sqrt{200} = 10\sqrt{2} .

Plugging this result into (i) yields that

x = 20 c o s θ ( s i n θ + s i n 2 θ + 16 ) x = 20*cos\theta (sin\theta + \sqrt{sin^{2}\theta + 16}) .

Taking the derivative of x x with respect to θ \theta yields that

d x d θ = ( s i n θ s i n 2 θ + 16 + 1 ) c o s 2 θ s i n θ ( s i n 2 θ + 16 + s i n θ ) \dfrac{dx}{d\theta} = (\dfrac{sin\theta}{\sqrt{sin^{2}\theta + 16}} + 1) * cos^{2}\theta - sin\theta(\sqrt{sin^{2}\theta + 16} + sin\theta) ,

which, after letting z = s i n θ z = sin\theta , can be simplified to

z + z 2 + 16 z 2 + 16 ( 1 z 2 z z 2 16 ) \dfrac{z + \sqrt{z^{2} + 16}}{\sqrt{z^{2} + 16}} * (1 - z^{2} - z\sqrt{z^{2} - 16}) .

Now since z > 0 z \gt 0 , for the derivative to equal 0 0 we must have that

1 z 2 = z z 2 + 16 ( 1 z 2 ) 2 = z 2 ( z 2 + 16 ) 18 z 2 = 1 z = 2 6 1 - z^{2} = z\sqrt{z^{2} + 16} \Longrightarrow (1 - z^{2})^{2} = z^{2}(z^{2} + 16) \Longrightarrow 18 * z^{2} = 1 \Longrightarrow z = \dfrac{\sqrt{2}}{6} .

Thus a = 2 , b = 6 a = 2, b = 6 and a + b = 8 a + b = \boxed{8} .

Yes, this problem is a bashy subset of a David Morin problem. Nicely written proof. The answer for a general case would be z = 1 2 + ϕ z=\frac{1}{\sqrt{2+\phi}} , where ϕ = 2 g h v 2 \phi=\frac{2gh}{v^{2}} .

Kushal Thaman - 2 years, 6 months ago
Michael Mendrin
Aug 15, 2014

Okay, you can't really say that gcd(a,b) = 1, if a = 2 and b = 6, can't you? Better fix this.

Sorry my mistake

tushar gautam - 6 years, 10 months ago

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You can edit your problem, and say that a is "square free", or "has no square factors", and drop the reference to gcd(a,b) = 1.

Michael Mendrin - 6 years, 10 months ago

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I can't edit second time maybe moderator could help, I really made a big mistake writting that.

tushar gautam - 6 years, 10 months ago

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@Tushar Gautam Ok edited something.

tushar gautam - 6 years, 10 months ago

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@Tushar Gautam I'll report it now as being fixed.

Michael Mendrin - 6 years, 10 months ago
Lu Chee Ket
Oct 18, 2015

There valid with a golden formula year 1993 for this question.

Nice one. Test for application of quadratic equation in reality as well as equation of trajectories nothing else. Simple but maths is required

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