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Tuesday, June 16, 2015

Cloudy Puzzle: Solution

We want to establish a mathematical relationship between the key variables of the problem: h, R, \theta and \phi.

Consider the triangle PRQ; we can write, \tan\left(\frac{\pi}{2} - \theta \right) = \frac{QP}{RQ} = \frac{QP}{OQ - OR}.
 
Recognizing that the length of the segment OP is R+ h, we can further write:
\tan\left(\frac{\pi}{2} - \theta \right) = \frac{(R+h) \cos \phi}{(R+h) \sin \phi - R}.

Using the variable a = h/R, we can try to solve for \phi, which in this case leads to a quadratic equation. Let us limit \theta < \pi/2, since all other cases are trivial extensions.

If we let,  A = a^{2} \tan^{2} \theta + a^{2} + 2 a \tan^{2}\theta + 2 a + \tan^{2} \theta,
and B = a \tan \theta + \tan \theta - 1,
then the two solutions are: \phi = -2 \tan^{-1} \left( \frac{a + 1 \pm \sqrt{A}}{B} \right).

Due to the geometry, acceptable values of \theta and \phi lie in the region [0, \pi/2]. This constraint may be used to cull out the extraneous root.

It is useful to consider the limit of a = h/R \ll 1. If we take the limit as it goes to zero, then  \phi = -2 \tan^{-1} \left( \frac{ \pm|\tan \theta| + 1}{\tan \theta - 1} \right).


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