Difference between revisions of "1992 USAMO Problems/Problem 2"
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==Solution 4== | ==Solution 4== | ||
− | Let <math>S = \frac{1}{\cos 0\circ\cos 1\circ} + \frac{1}{\cos 1\circ\cos 2\circ} + ... + \frac{1}{\cos 88\circ\cos 89\circ}</math>. | + | Let <math>S = \frac{1}{\cos 0^\circ\cos 1^\circ} + \frac{1}{\cos 1^\circ\cos 2^\circ} + ... + \frac{1}{\cos 88^\circ\cos 89^\circ}</math>. |
− | Multiplying by <math>\sin 1\circ</math> gives | + | Multiplying by <math>\sin 1^\circ</math> gives |
− | <cmath>S \sin 1\circ = \frac{\sin(1\circ-0\circ)}{\cos 0\circ\cos 1\circ} + ... + \frac{\sin(89\circ-88\circ)}{\cos 88\circ\cos 89\circ}</cmath> | + | <cmath>S \sin 1^\circ = \frac{\sin(1^\circ-0^\circ)}{\cos 0^\circ\cos 1^\circ} + ... + \frac{\sin(89^\circ-88^\circ)}{\cos 88^\circ\cos 89^\circ}</cmath> |
− | Notice that <math>\frac{\sin((x+1\circ)-x)}{\cos 0\circ\cos 1\circ} = \tan (x+1\circ) - \tan x</math> after expanding the sine, and so | + | Notice that <math>\frac{\sin((x+1^\circ)-x)}{\cos 0^\circ\cos 1^\circ} = \tan (x+1^\circ) - \tan x</math> after expanding the sine, and so |
− | <cmath>S \sin 1\circ = \tan 1\circ - \tan 0\circ + \tan 2\circ - \tan 1\circ + \tan 3\circ - \tan 2\circ + ... + \tan 89\circ - \tan 88\circ = \tan 89\circ - \tan 0\circ = \cot 1\circ = \frac{\cos 1\circ}{\sin 1\circ}</cmath>, so <cmath>S = \frac{cos 1\circ}{sin^21\circ}.</cmath> | + | <cmath>S \sin 1^\circ = \tan 1^\circ - \tan 0^\circ + \tan 2^\circ - \tan 1^\circ + \tan 3^\circ - \tan 2^\circ + ... + \tan 89^\circ - \tan 88^\circ = \tan 89^\circ - \tan 0^\circ = \cot 1^\circ = \frac{\cos 1^\circ}{\sin 1^\circ}</cmath>, so <cmath>S = \frac{cos 1^\circ}{sin^21^\circ}.</cmath> |
== Resources == | == Resources == |
Revision as of 23:50, 18 April 2014
Problem
Prove
Solution 1
Consider the points in the coordinate plane with origin , for integers .
Evidently, the angle between segments and is , and the length of segment is . It then follows that the area of triangle is . Therefore so as desired.
Solution 2
First multiply both sides of the equation by , so the right hand side is . Now by rewriting , we can derive the identity . Then the left hand side of the equation simplifies to as desired.
Solution 3
Multiply by . We get:
we can write this as:
This is an identity
Therefore;
, because of telescoping.
but since we multiplied in the beginning, we need to divide by . So we get that:
as desired. QED
Solution 4
Let .
Multiplying by gives
Notice that after expanding the sine, and so , so
Resources
1992 USAMO (Problems • Resources) | ||
Preceded by Problem 1 |
Followed by Problem 3 | |
1 • 2 • 3 • 4 • 5 | ||
All USAMO Problems and Solutions |
The problems on this page are copyrighted by the Mathematical Association of America's American Mathematics Competitions.