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AIME 1989 · 第 10 题

AIME 1989 — Problem 10

专题
Contest Math
难度
L4
来源
AIME

题目详情

Problem

Let aa, bb, cc be the three sides of a triangle, and let α\alpha, β\beta, γ\gamma, be the angles opposite them. If a2+b2=1989c2a^2+b^2=1989c^2, find

cotγcotα+cotβ\frac{\cot \gamma}{\cot \alpha+\cot \beta}
解析

Solution

Solution 1

We draw the altitude hh to cc, to get two right triangles.

AIME diagram

Then cotα+cotβ=ch\cot{\alpha}+\cot{\beta}=\frac{c}{h}, from the definition of the cotangent.

Let KK be the area of ABC.\triangle ABC. Then h=2Kch=\frac{2K}{c}, so cotα+cotβ=c22K\cot{\alpha}+\cot{\beta}=\frac{c^2}{2K}.

By identical logic, we can find similar expressions for the sums of the other two cotangents:

cotα+cotβ=c22Kcotβ+cotγ=a22Kcotγ+cotα=b22K.\begin{aligned} \cot \alpha + \cot \beta &= \frac{c^2}{2K} \\ \cot \beta + \cot \gamma &= \frac{a^2}{2K} \\ \cot \gamma + \cot \alpha &= \frac{b^2}{2K}. \end{aligned} Adding the last two equations, subtracting the first, and dividing by 2, we get

cotγ=a2+b2c24K.\cot \gamma = \frac{a^2 + b^2 - c^2}{4K}. Therefore

cotγcotα+cotβ=(a2+b2c2)/(4K)c2/(2K)=a2+b2c22c2=1989c2c22c2=19882=994.\begin{aligned} \frac{\cot \gamma}{\cot \alpha + \cot \beta} &= \frac{(a^2 + b^2 - c^2)/(4K)}{c^2/(2K)} \\ &= \frac{a^2 + b^2 - c^2}{2c^2} \\ &= \frac{1989 c^2 - c^2}{2c^2} \\ &= \frac{1988}{2} = \boxed{994}. \end{aligned}

Solution 2

By the law of cosines,

cosγ=a2+b2c22ab.\cos \gamma = \frac{a^2 + b^2 - c^2}{2ab}. So, by the extended law of sines,

cotγ=cosγsinγ=a2+b2c22ab2Rc=Rabc(a2+b2c2).\cot \gamma = \frac{\cos \gamma}{\sin \gamma} = \frac{a^2 + b^2 - c^2}{2ab} \cdot \frac{2R}{c} = \frac{R}{abc} (a^2 + b^2 - c^2). Identical logic works for the other two angles in the triangle. So, the cotangent of any angle in the triangle is directly proportional to the sum of the squares of the two adjacent sides, minus the square of the opposite side. Therefore

cotγcotα+cotβ=a2+b2c2(a2+b2+c2)+(a2b2+c2)=a2+b2c22c2.\frac{\cot \gamma}{\cot \alpha + \cot \beta} = \frac{a^2 + b^2 - c^2}{(-a^2 + b^2 + c^2) + (a^2 - b^2 + c^2)} = \frac{a^2 + b^2 - c^2}{2c^2}. We can then finish as in solution 1.

Solution 3

We start as in solution 1, though we'll write AA instead of KK for the area. Now we evaluate the numerator:

cotγ=cosγsinγ\cot{\gamma}=\frac{\cos{\gamma}}{\sin{\gamma}} From the Law of Cosines and the sine area formula,

cosγ=1988c22absinγ=2Aabcotγ=cosγsinγ=1988c24A\begin{aligned}\cos{\gamma}&=\frac{1988c^2}{2ab}\\ \sin{\gamma}&= \frac{2A}{ab}\\ \cot{\gamma}&= \frac{\cos \gamma}{\sin \gamma} = \frac{1988c^2}{4A} \end{aligned} Then cotγcotα+cotβ=1988c24Ac22A=19882=994\frac{\cot \gamma}{\cot \alpha+\cot \beta}=\frac{\frac{1988c^2}{4A}}{\frac{c^2}{2A}}=\frac{1988}{2}=\boxed{994}.

Solution 4

cotα+cotβ=cosαsinα+cosβsinβ=sinαcosβ+cosαsinβsinαsinβ=sin(α+β)sinαsinβ=sinγsinαsinβ\begin{aligned} \cot{\alpha} + \cot{\beta} &= \frac {\cos{\alpha}}{\sin{\alpha}} + \frac {\cos{\beta}}{\sin{\beta}} = \frac {\sin{\alpha}\cos{\beta} + \cos{\alpha}\sin{\beta}}{\sin{\alpha}\sin{\beta}}\\ &= \frac {\sin{(\alpha + \beta)}}{\sin{\alpha}\sin{\beta}} = \frac {\sin{\gamma}}{\sin{\alpha}\sin{\beta}} \end{aligned} By the Law of Cosines,

a2+b22abcosγ=c2=1989c22abcosγ    abcosγ=994c2a^2 + b^2 - 2ab\cos{\gamma} = c^2 = 1989c^2 - 2ab\cos{\gamma} \implies ab\cos{\gamma} = 994c^2 Now

cotγcotα+cotβ=cotγsinαsinβsinγ=cosγsinαsinβsin2γ=abc2cosγ=abc2994c2ab=994\begin{aligned}\frac {\cot{\gamma}}{\cot{\alpha} + \cot{\beta}} &= \frac {\cot{\gamma}\sin{\alpha}\sin{\beta}}{\sin{\gamma}} = \frac {\cos{\gamma}\sin{\alpha}\sin{\beta}}{\sin^2{\gamma}} = \frac {ab}{c^2}\cos{\gamma} = \frac {ab}{c^2} \cdot \frac {994c^2}{ab}\\ &= \boxed{994}\end{aligned}

Solution 5

Use Law of cosines to give us c2=a2+b22abcos(γ)c^2=a^2+b^2-2ab\cos(\gamma) or therefore cos(γ)=994c2ab\cos(\gamma)=\frac{994c^2}{ab}. Next, we are going to put all the sin's in term of sin(a)\sin(a). We get sin(γ)=csin(a)a\sin(\gamma)=\frac{c\sin(a)}{a}. Therefore, we get cot(γ)=994cbsina\cot(\gamma)=\frac{994c}{b\sin a}.

Next, use Law of Cosines to give us b2=a2+c22accos(β)b^2=a^2+c^2-2ac\cos(\beta). Therefore, cos(β)=a2994c2ac\cos(\beta)=\frac{a^2-994c^2}{ac}. Also, sin(β)=bsin(a)a\sin(\beta)=\frac{b\sin(a)}{a}. Hence, cot(β)=a2994c2bcsin(a)\cot(\beta)=\frac{a^2-994c^2}{bc\sin(a)}.

Lastly, cos(α)=b2994c2bc\cos(\alpha)=\frac{b^2-994c^2}{bc}. Therefore, we get cot(α)=b2994c2bcsin(a)\cot(\alpha)=\frac{b^2-994c^2}{bc\sin(a)}.

Now, cot(γ)cot(β)+cot(α)=994cbsinaa2994c2+b2994c2bcsin(a)\frac{\cot(\gamma)}{\cot(\beta)+\cot(\alpha)}=\frac{\frac{994c}{b\sin a}}{\frac{a^2-994c^2+b^2-994c^2}{bc\sin(a)}}. After using a2+b2=1989c2a^2+b^2=1989c^2, we get 994cbcsinac2bsina=994\frac{994c*bc\sin a}{c^2b\sin a}=\boxed{994}.

Solution 6

Let γ\gamma be (180αβ)(180-\alpha-\beta)

cotγcotα+cotβ=tanαtanβtan(α+β)tanα+tanβ=(tanαtanβ)2tanαtanβtan2α+2tanαtanβ+tan2β\frac{\cot \gamma}{\cot \alpha+\cot \beta} = \frac{\frac{-\tan \alpha \tan \beta}{\tan(\alpha+\beta)}}{\tan \alpha + \tan \beta} = \frac{(\tan \alpha \tan \beta)^2-\tan \alpha \tan \beta}{\tan^2 \alpha + 2\tan \alpha \tan \beta +\tan^2 \beta}

WLOG, assume that aa and cc are legs of right triangle abcabc with β=90o\beta = 90^o and c=1c=1

By the Pythagorean theorem, we have b2=a2+1b^2=a^2+1, and the given a2+b2=1989a^2+b^2=1989. Solving the equations gives us a=994a=\sqrt{994} and b=995b=\sqrt{995}. We see that tanβ=\tan \beta = \infty, and tanα=994\tan \alpha = \sqrt{994}.

Our derived equation equals tan2α\tan^2 \alpha as tanβ\tan \beta approaches infinity. Evaluating tan2α\tan^2 \alpha, we get 994\boxed{994}.

Solution 7

As in Solution 1, drop an altitude hh to cc. Let hh meet cc at PP, and let AP=x,BP=yAP = x, BP = y.

AIME diagram

Then, cotα=1tanα=xh\cot{\alpha} = \frac{1}{\tan{\alpha}} = \frac{x}{h}, cotβ=1tanβ=yh\cot{\beta} = \frac{1}{\tan{\beta}} = \frac{y}{h}. We can calculate cotγ\cot{\gamma} using the tangent addition formula, after noticing that cotγ=1tanγ\cot{\gamma} = \frac{1}{\tan{\gamma}}. So, we find that \begin{align*} \cot{\gamma} &= \frac{1}{\tan{\gamma}} \\ &= \frac{1}{\frac{\frac{x}{h} + \frac{y}{h}}{1 - \frac{xy}{h^2}}} \\ &= \frac{1}{\frac{(x+y)h}{h^2 - xy}} \\ &= \frac{h^2 - xy}{(x+y)h}. \end{align*}

So now we can simplify our original expression: \begin{align*} \frac{\cot{\gamma}}{\cot{\alpha} + \cot{\beta}} &= \frac{\frac{h^2 - xy}{(x+y)h}}{\frac{x + y}{h}} \\ &= \frac{h^2 - xy}{(x+y)^2}. \end{align*}

But notice that x+y=cx+y = c, so this becomes

h2xyc2.\frac{h^2 - xy}{c^2}. Now note that we can use the Pythagorean theorem to calculate h2h^2, we get that

h2=a2y2+b2x22.h^2 = \frac{a^2 - y^2 + b^2 - x^2}{2}. So our expression simplifies to

1989c2(x+y)22c2\frac{1989c^2 - (x+y)^2}{2c^2} since a2+b2=1989c2a^2 + b^2 = 1989c^2 from the problem and that there is another 2xy2-\frac{2xy}{2} after the h2h^2 in our expression. Again note that x+y=cx+y = c, so it again simplifies to 1988c22c2\frac{1988c^2}{2c^2}, or 994\boxed{994}.

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Solution 8 (Quick and Easy)

Since no additional information is given, we can assume that triangle ABC is right with the right angle at B. We can use the Pythagorean theorem to say

c2+a2=b2c^2+a^2=b^2 We can now solve for aa in terms of cc

c2+a2=1989c2a2c^2+a^2=1989c^2-a^2 a2=994c2a^2=994c^2 a=994ca=\sqrt{994}c Using the definition of cotangent

cot(A)=ca=1994cot(A)=\frac{c}{a}=\frac{1}{\sqrt{994}} cot(B)=cot(90)=0cot(B)=cot(90)=0 cot(C)=ac=994cot(C)=\frac{a}{c}=\sqrt{994} Plugging into our desired expression, we get 994\boxed{994}

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Solution 9 (Quick and Easy), similar idea to Solution 8

Assume the triangle is isosceles and c=1c=1. Since a=ba=b, 2a2=19892a^2=1989, a=b=19892\rightarrow a=b=\sqrt{\frac{1989}{2}}

Since this is an isosceles triangle, we can find cot(α)\cot(\alpha), cot(β)\cot(\beta), by just drawing the height. Via Pythagorean Theorem, the height is 39772\frac{\sqrt{3977}}{2}.

Therefore we find that tan(α)=tan(β)=3977\tan(\alpha) = \tan(\beta) = \sqrt{3977}. tan(γ)=tan(180(α+β))=tan(α+β)\tan(\gamma) = \tan(180-(\alpha+\beta)) = -\tan(\alpha+\beta). Via tangent sum formula, tan(α+β)=39771988\tan(\alpha+\beta) = -\frac{\sqrt{3977}}{1988}, so tan(γ)=39771988\tan(\gamma) = \frac{\sqrt{3977}}{1988}.

Since cot(θ)=1tan(θ)\cot(\theta) = \frac{1}{\tan(\theta)}, cot(α)=13977\cot(\alpha) = \frac{1}{\sqrt{3977}}, cot(β)=13977\cot(\beta) = \frac{1}{\sqrt{3977}}, cot(γ)=19883977\cot(\gamma) = \frac{1988}{\sqrt{3977}}.

Plugging this in, almost everything cancels and we get 19882=994\frac{1988}{2} = \boxed{994}.