1992 USAMO Problems/Problem 2: Difference between revisions
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<math>\frac {1}{\cos{0}\cos{1}} + \frac {1}{\cos{1}\cos{2}} + \frac {1}{\cos{2}\cos{3}} + .... + \frac {1}{\cos{88}\cos{89}} = \frac {\cos{1}}{\sin^2{1}}</math> | <math>\frac {1}{\cos{0}\cos{1}} + \frac {1}{\cos{1}\cos{2}} + \frac {1}{\cos{2}\cos{3}} + .... + \frac {1}{\cos{88}\cos{89}} = \frac {\cos{1}}{\sin^2{1}}</math> | ||
as desired. QED | as desired. QED | ||
==Solution 4== | |||
Let <math>S = \frac{1}{\cos 0°\cos 1°} + \frac{1}{\cos 1°\cos 2°} + ... + \frac{1}{\cos 88°\cos 89°}</math>. | |||
Multiplying by sin 1° gives | |||
<cmath>S \sin 1° = \frac{\sin(1°-0°)}{\cos 0°\cos 1°} + ... + \frac{\sin(89°-88°)}{\cos 88°\cos 89°}</cmath> | |||
Notice that <math>\frac{\sin((x+1°)-x)}{\cos 0°\cos 1°} = \tan (x+1°) - \tan x</math> after expanding the sine, and so | |||
<cmath>S \sin 1° = \tan 1° - \tan 0° + \tan 2° - tan 1° + \tan 3° - \tan 2° + ... + \tan 89° - \tan 88° = \tan 89° - \tan 0° = \cot 1° = \frac{\cos 1°}{\sin 1°}</cmath>, so <cmath>S = \frac{cos 1°}{sin^21°}.</cmath> | |||
== Resources == | == Resources == | ||
Revision as of 23:46, 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 sin 1° 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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