1992 USAMO Problems/Problem 2: Difference between revisions
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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> | <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 | ||
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