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AIME 2011 I · 第 14 题

AIME 2011 I — Problem 14

专题
Contest Math
难度
L4
来源
AIME

题目详情

Problem

Let A1A2A3A4A5A6A7A8A_1 A_2 A_3 A_4 A_5 A_6 A_7 A_8 be a regular octagon. Let M1M_1, M3M_3, M5M_5, and M7M_7 be the midpoints of sides A1A2\overline{A_1 A_2}, A3A4\overline{A_3 A_4}, A5A6\overline{A_5 A_6}, and A7A8\overline{A_7 A_8}, respectively. For i=1,3,5,7i = 1, 3, 5, 7, ray RiR_i is constructed from MiM_i towards the interior of the octagon such that R1R3R_1 \perp R_3, R3R5R_3 \perp R_5, R5R7R_5 \perp R_7, and R7R1R_7 \perp R_1. Pairs of rays R1R_1 and R3R_3, R3R_3 and R5R_5, R5R_5 and R7R_7, and R7R_7 and R1R_1 meet at B1B_1, B3B_3, B5B_5, B7B_7 respectively. If B1B3=A1A2B_1 B_3 = A_1 A_2, then cos2A3M3B1\cos 2 \angle A_3 M_3 B_1 can be written in the form mnm - \sqrt{n}, where mm and nn are positive integers. Find m+nm + n.

Diagram

AIME diagram

All distances are to scale.

解析

Solution 1

We use coordinates. Let the octagon have side length 22 and center (0,0)(0, 0). Then all of its vertices have the form (±1,±(1+2))(\pm 1, \pm\left(1+\sqrt{2}\right)) or (±(1+2),±1)(\pm\left(1+\sqrt{2}\right), \pm 1).

By symmetry, B1B3B5B7B_{1}B_{3}B_{5}B_{7} is a square. Thus lines B1B3\overleftrightarrow{B_{1}B_{3}} and B5B7\overleftrightarrow{B_{5}B_{7}} are parallel, and its side length is the distance between these two lines. However, this is given to be the side length of the octagon, or 22.

Suppose the common slope of the lines is mm and let m=tanθm=\tan\theta. Then, we want to find

cos2(90θ)=2cos2(90θ)1=2sin2θ1.\cos 2\left(90-\theta\right)=2\cos^{2}\left(90-\theta\right)-1=2\sin^{2}\theta-1. It can easily be seen that the equations of the lines are

B1B3:ymx+m(1+2)=0B5B7:ymxm(1+2)=0.\begin{aligned} B_{1}B_{3}: y-mx+m\left(1+\sqrt{2}\right)=0 \\ B_{5}B_{7}: y-mx-m\left(1+\sqrt{2}\right)=0.\end{aligned} By the distance between parallel lines formula, a corollary of the point to line distance formula, the distance between these two lines is

c2c1a2+b2=2m(1+2)m2+1.\frac{|c_{2}-c_{1}|}{\sqrt{a^{2}+b^{2}}}=\frac{2m\left(1+\sqrt{2}\right)}{\sqrt{m^{2}+1}}. Since we want this to equal 22, we have

2m(1+2)m2+1=24m2(3+22)=4m2+4(12+82)m2=4m2+4(8+82)m2=4m2=48+82m2=tan2θ=sin2θcos2θ=12+22.\begin{aligned}\frac{2m\left(1+\sqrt{2}\right)}{\sqrt{m^{2}+1}}&=2 \\ 4m^{2}\left(3+2\sqrt{2}\right)&=4m^{2}+4 \\ \left(12+8\sqrt{2}\right)m^{2}&=4m^{2}+4 \\ \left(8+8\sqrt{2}\right)m^{2}&=4 \\ m^{2}&=\frac{4}{8+8\sqrt{2}} \\ \Rightarrow m^{2}=\tan^{2}\theta=\frac{\sin^{2}\theta}{\cos^{2}\theta}&=\frac{1}{2+2\sqrt{2}}.\end{aligned} Since sin2θ+cos2θ=1,\sin^{2}\theta+\cos^{2}\theta=1, we have sin2θ=13+22\sin^{2}\theta=\frac{1}{3+2\sqrt{2}}. Thus

2sin2θ1=23+221=1223+22=(122)(322)(3+22)(322)=5421=532.2\sin^{2}\theta-1=\frac{2}{3+2\sqrt{2}}-1=\frac{-1-2\sqrt{2}}{3+2\sqrt{2}}=\frac{\left(-1-2\sqrt{2}\right)\left(3-2\sqrt{2}\right)}{\left(3+2\sqrt{2}\right)\left(3-2\sqrt{2}\right)}=\frac{5-4\sqrt{2}}{1}=5-\sqrt{32}. The answer is 037\boxed{037}.

Solution 2

Let θ=M1M3B1\theta=\angle M_1 M_3 B_1. Thus we have that cos2A3M3B1=cos(2θ+π2)=sin2θ\cos 2 \angle A_3 M_3 B_1=\cos \left(2\theta + \frac{\pi}{2} \right)=-\sin2\theta.

Since A1A2A3A4A5A6A7A8A_1 A_2 A_3 A_4 A_5 A_6 A_7 A_8 is a regular octagon and B1B3=A1A2B_1 B_3 = A_1 A_2, let k=A1A2=A2A3=B1B3k=A_1 A_2 = A_2 A_3 = B_1 B_3.

Extend A1A2\overline{A_1 A_2} and A3A4\overline{A_3 A_4} until they intersect. Denote their intersection as I1I_1. Through similar triangles & the 45459045-45-90 triangles formed, we find that M1M3=k2(2+2)M_1 M_3=\frac{k}{2}(2+\sqrt2).

We also have that M7B7M1=M1B1M3\triangle M_7 B_7 M_1 =\triangle M_1 B_1 M_3 through ASA congruence (B7M7M1=B1M1M3\angle B_7 M_7 M_1 =\angle B_1 M_1 M_3, M7M1=M1M3M_7 M_1 = M_1 M_3, B7M1M7=B1M3M1\angle B_7 M_1 M_7 =\angle B_1 M_3 M_1). Therefore, we may let n=M1B7=M3B1n=M_1 B_7 = M_3 B_1.

Thus, we have that sinθ=nkk2(2+2)\sin\theta=\frac{n-k}{\frac{k}{2}(2+\sqrt2)} and that cosθ=nk2(2+2)\cos\theta=\frac{n}{\frac{k}{2}(2+\sqrt2)}. Therefore cosθsinθ=kk2(2+2)=22+2=22\cos\theta-\sin\theta=\frac{k}{\frac{k}{2}(2+\sqrt2)}=\frac{2}{2+\sqrt2}=2-\sqrt2.

Squaring gives that sin2θ2sinθcosθ+cos2θ=642\sin^2\theta - 2\sin\theta\cos\theta + \cos^2\theta = 6-4\sqrt2 and consequently that 2sinθcosθ=542=sin2θ-2\sin\theta\cos\theta = 5-4\sqrt2 = -\sin2\theta through the identities sin2θ+cos2θ=1\sin^2\theta + \cos^2\theta = 1 and sin2θ=2sinθcosθ\sin2\theta = 2\sin\theta\cos\theta.

Thus we have that cos2A3M3B1=542=532\cos 2 \angle A_3 M_3 B_1=5-4\sqrt2=5-\sqrt{32}. Therefore m+n=5+32=037m+n=5+32=\boxed{037}.

Solution 3

Let A1A2=2A_1A_2 = 2. Then B1B_1 and B3B_3 are the projections of M1M_1 and M5M_5 onto the line B1B3B_1B_3, so 2=B1B3=M1M5cosx2=B_1B_3=-M_1M_5\cos x, where x=A3M3B1x = \angle A_3M_3B_1. Then since M1M5=2+22,cosx=22+22=12M_1M_5 = 2+2\sqrt{2}, \cos x = \dfrac{-2}{2+2\sqrt{2}}= 1-\sqrt{2}, cos2x=2cos2x1=542=532\cos 2x = 2\cos^2 x -1 = 5 - 4\sqrt{2} = 5-\sqrt{32}, and m+n=037m+n=\boxed{037}.

Solution 4

Notice that R3R_3 and R7R_7 are parallel (B1B3B5B7B_1B_3B_5B_7 is a square by symmetry and since the rays are perpendicular) and B1B3=B3B5=s=B_1B_3=B_3B_5=s= the distance between the parallel rays. If the regular hexagon as a side length of ss, then M3M7M_3M_7 has a length of s+s2s+s\sqrt{2}. Let XX be on R3R_3 such that M7XM_7X is perpendicular to M3XM_3X, and ϕ=M7M3X\phi=\angle M_7M_3X. The distance between R3R_3 and R7R_7 is s=M7Xs=M_7X, so sinϕ=ss+s2=11+2\sin\phi=\frac{s}{s+s\sqrt{2}}=\frac{1}{1+\sqrt{2}}.

Since we are considering a regular hexagon, M3M_3 is directly opposite to M7M_7 and A3M3B1=90+ϕ\angle A_3M_3B_1=90 ^\circ +\phi. All that's left is to calculate cos2A3M3B1=cos2(90+ϕ)sin2(90+ϕ)=sin2ϕcos2ϕ\cos 2\angle A_3M_3B_1=\cos^2(90^\circ+\phi)-\sin^2(90^\circ+\phi)=\sin^2\phi-\cos^2\phi. By drawing a right triangle or using the Pythagorean identity, cos2ϕ=2+223+22\cos^2\phi=\frac{2+2\sqrt2}{3+2\sqrt2} and cos2A3M3B1=1223+22=542=532\cos 2\angle A_3M_3B_1=\frac{-1-2\sqrt2}{3+2\sqrt2}=5-4\sqrt2=5-\sqrt{32}, so m+n=037m+n=\boxed{037}.

Solution 5

Assume that A1A2=1.A_1A_2=1. Denote the center OO, and the midpoint of B1B_1 and B3B_3 as B2B_2. Then we have that

cosA3M3B1=cos(A3M3O+OM3B1)=sin(OM3B1)=OB2OM3=1/21/2+2/2=12+1=12.\cos\angle A_3M_3B_1=\cos(\angle A_3M_3O+\angle OM_3B_1)=-\sin(\angle OM_3B_1)=-\frac{OB_2}{OM_3}=-\frac{1/2}{1/2+\sqrt2/2}=-\frac{1}{\sqrt2+1}=1-\sqrt2. Thus, by the cosine double-angle theorem,

cos2A3M3B1=2(12)21=532,\cos2\angle A_3M_3B_1=2(1-\sqrt2)^2-1=5-\sqrt{32}, so m+n=037m+n=\boxed{037}.

Video Solution

2011 AIME I #14

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