Difference between revisions of "1992 USAMO Problems/Problem 2"
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<cmath> \frac{1}{\cos 0^\circ \cos 1^\circ} + \frac{1}{\cos 1^\circ \cos 2^\circ} + \cdots + \frac{1}{\cos 88^\circ \cos 89^\circ} = \frac{\cos 1^\circ}{\sin^2 1^\circ}. </cmath> | <cmath> \frac{1}{\cos 0^\circ \cos 1^\circ} + \frac{1}{\cos 1^\circ \cos 2^\circ} + \cdots + \frac{1}{\cos 88^\circ \cos 89^\circ} = \frac{\cos 1^\circ}{\sin^2 1^\circ}. </cmath> | ||
− | == Solution == | + | == Solution== |
+ | === Solution 1 === | ||
Consider the points <math>M_k = (1, \tan k^\circ)</math> in the coordinate plane with origin <math>O=(0,0)</math>, for integers <math>0 \le k \le 89</math>. | Consider the points <math>M_k = (1, \tan k^\circ)</math> in the coordinate plane with origin <math>O=(0,0)</math>, for integers <math>0 \le k \le 89</math>. | ||
Line 37: | Line 38: | ||
as desired. <math>\blacksquare</math> | as desired. <math>\blacksquare</math> | ||
+ | === Solution 2 === | ||
− | {{ | + | First multiply both sides of the equation by <math>\sin 1</math>, so the right hand side is <math>\frac{\cos 1}{\sin 1}</math>. Now by rewriting <math>\sin 1=\sin((k+1)-k)=\sin(k+1)\cos(k)+\sin(k)\cos(k+1)</math>, we can derive the identity <math>\tan(n+1)-\tan(n)=\frac{\sin 1}{\cos(n)\cos(n+1)}</math>. Then the left hand side of the equation simplifies to <math>\tan 89-\tan 0=\tan 89=\frac{\sin 89}{\cos 89}=\frac{\cos 1}{\sin 1}</math> as desired. |
− | == | + | === Solution 3 === |
+ | Multiply by <math>\sin{1}</math>. We get: | ||
+ | |||
+ | <math>\frac {\sin{1}}{\cos{0}\cos{1}} + \frac {\sin{1}}{\cos{1}\cos{2}} + ... + \frac {\sin{1}}{\cos{88}\cos{89}} = \frac {\cos{1}}{\sin{1}}</math> | ||
+ | |||
+ | we can write this as: | ||
+ | |||
+ | <math>\frac {\sin{1 - 0}}{\cos{0}\cos{1}} + \frac {\sin{2 - 1}}{\cos{1}\cos{2}} + ... + \frac {\sin{89 - 88}}{\cos{88}\cos{89}} = \frac {\cos{1}}{\sin{1}}</math> | ||
+ | |||
+ | This is an identity <math>\tan{a} - \tan{b} = \frac {\sin{(a - b)}}{\cos{a}\cos{b}}</math> | ||
+ | |||
+ | Therefore; | ||
+ | |||
+ | <math>\sum_{i = 1}^{89}[\tan{k} - \tan{(k - 1)}] = \tan{89} - \tan{0} = \cot{1}</math>, because of telescoping. | ||
+ | |||
+ | but since we multiplied <math>\sin{1}</math> in the beginning, we need to divide by <math>\sin{1}</math>. So we get that: | ||
+ | |||
+ | <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 | ||
+ | |||
+ | === 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>. | ||
+ | |||
+ | 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> | ||
+ | |||
+ | 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 = \left(\tan 1^\circ - \tan 0^\circ\right) + \cdots + \left(\tan 89^\circ - \tan 88^\circ\right) = \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> | ||
+ | |||
+ | == See Also == | ||
{{USAMO box|year=1992|num-b=1|num-a=3}} | {{USAMO box|year=1992|num-b=1|num-a=3}} | ||
* [http://www.artofproblemsolving.com/Forum/viewtopic.php?p=356413#p356413 Discussion on AoPS/MathLinks] | * [http://www.artofproblemsolving.com/Forum/viewtopic.php?p=356413#p356413 Discussion on AoPS/MathLinks] | ||
+ | {{MAA Notice}} | ||
[[Category:Olympiad Algebra Problems]] | [[Category:Olympiad Algebra Problems]] |
Latest revision as of 06:41, 19 July 2016
Contents
Problem
Prove
Solution
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
See Also
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.