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AIME 2012 II · 第 13 题

AIME 2012 II — Problem 13

专题
Contest Math
难度
L4
来源
AIME

题目详情

Problem 13

Equilateral ABC\triangle ABC has side length 111\sqrt{111}. There are four distinct triangles AD1E1AD_1E_1, AD1E2AD_1E_2, AD2E3AD_2E_3, and AD2E4AD_2E_4, each congruent to ABC\triangle ABC, with BD1=BD2=11BD_1 = BD_2 = \sqrt{11}. Find k=14(CEk)2\sum_{k=1}^4(CE_k)^2.

解析

Solution 1

Note that there are only two possible locations for points D1D_1 and D2D_2, as they are both 111\sqrt{111} from point AA and 11\sqrt{11} from point BB, so they are the two points where a circle centered at AA with radius 111\sqrt{111} and a circle centered at BB with radius 11\sqrt{11} intersect. Let D1D_1 be the point on the opposite side of AB\overline{AB} from CC, and D2D_2 the point on the same side of AB\overline{AB} as CC.

Let θ\theta be the measure of angle BAD1BAD_1 (also the measure of angle BAD2BAD_2); by the Law of Cosines,

112=1112+11122111111cosθ11=222(1cosθ)\begin{aligned}\sqrt{11}^2 &= \sqrt{111}^2 + \sqrt{111}^2 - 2 \cdot \sqrt{111} \cdot \sqrt{111} \cdot \cos\theta\\ 11 &= 222(1 - \cos\theta)\end{aligned} There are two equilateral triangles with AD1\overline{AD_1} as a side; let E1E_1 be the third vertex that is farthest from CC, and E2E_2 be the third vertex that is nearest to CC.

Angle E1AC=E1AD1+D1AB+BAC=60+θ+60=120+θE_1AC = E_1AD_1 + D_1AB + BAC = 60 + \theta + 60 = 120 + \theta; by the Law of Cosines,

(E1C)2=(E1A)2+(AC)22(E1A)(AC)cos(120+θ)=111+111222cos(120+θ)\begin{aligned}(E_1C)^2 &= (E_1A)^2 + (AC)^2 - 2 (E_1A) (AC)\cos(120 + \theta)\\ &= 111 + 111 - 222\cos(120 + \theta)\end{aligned} Angle E2AC=θE_2AC = \theta; by the Law of Cosines,

(E2C)2=(E2A)2+(AC)22(E2A)(AC)cosθ=111+111222cosθ\begin{aligned}(E_2C)^2 &= (E_2A)^2 + (AC)^2 - 2 (E_2A) (AC)\cos\theta\\ &= 111 + 111 - 222\,\cos\theta\end{aligned} There are two equilateral triangles with AD2\overline{AD_2} as a side; let E3E_3 be the third vertex that is farthest from CC, and E4E_4 be the third vertex that is nearest to CC.

Angle E3AC=E3AB+BAC=(60θ)+60=120θE_3AC = E_3AB + BAC = (60 - \theta) + 60 = 120 - \theta; by the Law of Cosines,

(E3C)2=(E3A)2+(AC)22(E3A)(AC)cos(120θ)=111+111222cos(120θ)\begin{aligned}(E_3C)^2 &= (E_3A)^2 + (AC)^2 - 2 (E_3A) (AC)\cos(120 - \theta)\\ &= 111 + 111 - 222\cos(120 - \theta)\end{aligned} Angle E4AC=θE_4AC = \theta; by the Law of Cosines,

(E4C)2=(E4A)2+(AC)22(E4A)(AC)cosθ=111+111222cosθ\begin{aligned}(E_4C)^2 &= (E_4A)^2 + (AC)^2 - 2 (E_4A) (AC)\cos\theta \\ &= 111 + 111 - 222\cos\theta\end{aligned} The solution is:

k=14(CEk)2=(E1C)2+(E3C)2+(E2C)2+(E4C)2=222(1cos(120+θ))+222(1cos(120θ))+222(1cosθ)+222(1cosθ)=222((1(cos120cosθsin120sinθ))+(1(cos120cosθ+sin120sinθ))+2(1cosθ))=222(1cos120cosθ+sin120sinθ+1cos120cosθsin120sinθ+22cosθ)=222(1+12cosθ+1+12cosθ+22cosθ)=222(4cosθ)=666+222(1cosθ)\begin{aligned} \sum_{k=1}^4(CE_k)^2 &= (E_1C)^2 + (E_3C)^2 + (E_2C)^2 + (E_4C)^2\\ &= 222(1 - \cos(120 + \theta)) + 222(1 - \cos(120 - \theta)) + 222(1 - \cos\theta) + 222(1 - \cos\theta)\\ &= 222((1 - (\cos120\cos\theta - \sin120\sin\theta)) + (1 - (\cos120\cos\theta + \sin120\sin\theta)) + 2(1 -\cos\theta))\\ &= 222(1 - \cos120\cos\theta + \sin120\sin\theta + 1 - \cos120\cos\theta - \sin120\sin\theta + 2 - 2\cos\theta)\\ &= 222(1 + \frac{1}{2}\cos\theta + 1 + \frac{1}{2}\cos\theta + 2 - 2\cos\theta)\\ &= 222(4 - \cos\theta)\\ &= 666 + 222(1 - \cos\theta) \end{aligned} Substituting 1111 for 222(1cosθ)222(1 - \cos\theta) gives the solution 666+11=677.666 + 11 = \boxed{677}.

Solution 2

This problem is pretty much destroyed by complex plane geometry, which is similar to vector geometry only with the power of easy rotation. Place the triangle in the complex plane by letting CC be the origin, placing BB along the x-axis, and AA in the first quadrant. Let r=111r=\sqrt{111}. If ω\omega denotes the primative sixth root of unity, eiπ/3e^{i\pi/3}, then we have C=0C=0, B=rB=r, and A=rω.A=r\omega. Recall that counter-clockwise rotation in the complex plane by an angle θ\theta is accomplished by multiplication by eiθe^{i\theta} (and clockwise rotation is multiplication by its conjugate). So, we can find D1D_1 and D2D_2 by rotating BB around AA by angles of θ\theta and θ-\theta, where θ\theta is the apex angle in the isoceles triangle with sides 111\sqrt{111}, 111\sqrt{111}, and 11\sqrt{11}. That is, let z=eiθz=e^{i\theta}, and then:

D1=A+z(BA)D_1=A+z(B-A), and D2=A+z(BA)D_2=A+\overline{z}(B-A). Now notice that BA=AB-A=\overline{A}, so this simplifies further to:

D1=A+zAD_1=A+z\overline{A}, and D2=A+zAD_2=A+\overline{z}\overline{A}.

Similarly, we can write E1E_1, E2E_2, E3E_3, and E4E_4 by rotating D1D_1 and D2D_2 around AA by ±π/3\pm\pi/3:

E1=A+ω(D1A)E_1=A+\omega(D_1-A), E2=A+ω(D1A)E_2=A+\overline{\omega}(D_1-A), E3=A+ω(D2A)E_3=A+\omega(D_2-A), E4=A+ω(D2A)E_4=A+\overline{\omega}(D_2-A). Thus:

E1=A+ωzAE_1=A+\omega z \overline{A}, E2=A+ωzAE_2=A+\overline{\omega} z \overline{A}, E3=A+ωzAE_3=A+\omega\overline{z}\overline{A}, E4=A+ωzAE_4=A+\overline{\omega}\overline{z}\overline{A}.

Now to find some magnitudes, which is easy since we chose CC as the origin:

E12=(A+ωzA)(A+ωzA)=2A2+ωzA2+ωzA2\|E_1\|^2=(A+\omega z \overline{A})(\overline{A}+\overline{\omega z}A)=2\|A\|^2+\omega z \overline{A}^2 + \overline{\omega}\overline{z}A^2,

E22=(A+ωzA)(A+ωzA)=2A2+ωzA2+ωzA2\|E_2\|^2=(A+\overline{\omega} z \overline{A})(\overline{A}+\omega \overline{z}A)=2\|A\|^2+\overline{\omega} z \overline{A}^2 + \omega\overline{z}A^2,

E32=(A+ωzA)(A+ωzA)=2A2+ωzA2+ωzA2\|E_3\|^2=(A+\omega \overline{z} \overline{A})(\overline{A}+\overline{\omega} z A)=2\|A\|^2+\omega \overline{z} \overline{A}^2 + \overline{\omega}zA^2,

E42=(A+ωzA)(A+ωzA)=2A2+ωzA2+ωzA2\|E_4\|^2=(A+\overline{\omega z} \overline{A})(\overline{A}+\omega zA)=2\|A\|^2+\overline{\omega z} \overline{A}^2 + \omega zA^2.

Adding these up, the sum equals 8A2+(A2+A2)(ωz+ωz+ωz+ωz)=8A2+(A2+A2)(z+z)(ω+ω)8\|A\|^2+(\overline{A}^2+A^2)(\omega z + \omega \overline{z} + \overline{\omega}z + \overline{\omega}\overline{z}) = 8\|A\|^2+(\overline{A}^2+A^2)(z + \overline{z})( \omega+ \overline{\omega}).

(Isn't that nice?) Notice that A2+A2=r2(ω2+ω2)=r2\overline{A}^2+A^2 = r^2(\overline{\omega}^2+\omega^2) = -r^2, and ω+ω=1\omega+ \overline{\omega}=1, so that this sum simplifies further to 888111(z+z)888-111(z + \overline{z}).

Finally, z+z=2cosθz + \overline{z} = 2\cos{\theta}, which is found using the law of cosines on that isoceles triangle: 11=111+111222cosθ11=111+111-222\cos{\theta}, so 2cosθ=211/1112\cos{\theta}=211/111.

Thus, the sum equals 888211=677888-211=\boxed{677}.

Solution 3

This method uses complex numbers with AA as the origin. Let A=0A=0, B=111B=\sqrt{111}, C=111θC = \sqrt{111}\theta, where θ=eiπ/3=12+32i\theta = e^{i \pi/3} = \frac{1}{2} + \frac{\sqrt{3}}{2}i.

Also, let xx be D1D_1 or D2D_2. Then

x=111,x111=11|x|=\sqrt{111}, |x-\sqrt{111}|=\sqrt{11}

Therefore, 11=x1112=x2+1112111Re(x)=2222111Re(x)11 = |x-\sqrt{111}|^2 = |x|^2 + 111 -2\sqrt{111}Re(x) = 222 - 2\sqrt{111}Re(x), so

2111Re(x)=211.2\sqrt{111}Re(x) = 211. Since E1E_1, E2E_2 are one of D1θD_1\theta or D1θ1D_1\theta^{-1}, without loss of generality, let E1=D1θE_1=D_1\theta and E2=D1θ1E_2 = D_1\theta^{-1}. Then

CE12=111D12=111x2=11|CE_1|^2 = |\sqrt{111}-D_1|^2 = |\sqrt{111}-x|^2=11 CE22=θ2111D12=2222111Re(D1θ2)|CE_2|^2 = |\theta^2 \sqrt{111} - D_1|^2 = 222-2\sqrt{111} Re(D_1 \theta^2) One can similarly get CE3=11|CE_3|=11 and CE4=2222111Re(D2θ2)|CE_4|=222-2\sqrt{111} Re(D_2 \theta^2), so the desired sum is equal to

22+4442111(Re(D1θ2)+Re(D1θ2))22+444-2\sqrt{111}(Re(D_1 \theta^2)+Re(D_1 \theta^2)) Note that Re(D1,2θ2)=Re((Re(x)±Im(x)i)(1/2+3/2i))=(Re(x)/2±Im(x)3/2)Re(D_{1,2} \theta^2) = Re((Re(x) \pm Im(x)i)(-1/2 + \sqrt{3}/2i)) = - (Re(x)/2 \pm Im(x)\sqrt{3}/2), so the sum of these two is just Re(x)-Re(x). Therefore the desired sum is equal to

22+444+2111Re(x)=22+444+211=677.22+444+2\sqrt{111}Re(x) = 22+444+211 = \boxed{677}.

Solution 4

This method uses the observation that every point is equidistant from AA. Without loss of generality, we can assume CC is on the same side of ABAB as D1D_1.

We can start off by angle chasing the angles around AA. We let BAD1=α\angle BAD_1 = \alpha. Then, we note that BD1=BD2BD_1 = BD_2 and AD1=AB=AD2AD_1 = AB = AD_2. Thus, ABD1ABD2\bigtriangleup ABD_1 \cong \bigtriangleup ABD_2. Thus, BAD2=α\angle BAD_2 = \alpha also.

We can now angle chase the angles about AA. Because D2AE3=60\angle D_2AE_3 = 60, D1AE3=602α\angle D_1AE_3 = 60- 2 \alpha. We can use all the congruent equilateral triangles in a similar manner obtaining:

D1AE3=602α\angle D_1AE_3 = 60- 2 \alpha E3AC=α\angle E_3AC = \alpha CAE1=α\angle CAE_1 = \alpha D2AE2=602α\angle D_2AE_2 = 60- 2 \alpha E2AE4=2α\angle E_2AE_4 = 2 \alpha Now, AE3=AC=111AE_3 = AC = \sqrt{111} and E3AC=α\angle E_3AC = \alpha. Thus, E3ACBAD1\bigtriangleup E_3AC \cong \bigtriangleup BAD_1. Thus, CE32=BD12=11CE_3^2 = BD_1^2 = 11.

Similarly, AC=AE1=111AC = AE_1 = \sqrt{111} and CAE1=α\angle CAE_1 = \alpha. Thus, CAE1BAD1\bigtriangleup CAE_1 \cong \bigtriangleup BAD_1. Thus, CE12=BD12=11CE_1^2 = BD_1^2 = 11.

We can use CAE2\bigtriangleup CAE_2 to find CE22CE_2^2. Law of Cosines yields

CE22=AE22+AC22AE2ACcos(E2AC).CE_2^2 = AE_2^2 + AC^2 - 2 \cdot AE_2 \cdot AC \cdot \cos(\angle E_2AC). Substituting the known lengths and angles gives

CE22=222222cos(120α).CE_2^2 = 222 - 222 \cdot \cos(120- \alpha). Expanding this with the Cosine Subtraction Identity we get

CE22=222222(cos120cosα+sin120sinα).CE_2^2 = 222 - 222(\cos120 \cos \alpha + \sin120 \sin \alpha). We could attempt to calculate this but we can clear it up by simultaneously finding CE42CE_4^2 too. We use Law of Cosines on CAE4\bigtriangleup CAE_4 to get

CE42=AE42+AC22AE4ACcos(E4AC).CE_4^2 = AE_4^2 + AC^2 - 2 \cdot AE_4 \cdot AC \cdot \cos(\angle E_4AC). Substituting the known lengths and angles gives

CE42=222222cos(120+α).CE_4^2 = 222 - 222 \cdot \cos(120 + \alpha). Expanding this with the Cosine Addition Identity we get

CE42=222222(cos120cosαsin120sinα).CE_4^2 = 222 - 222(\cos120 \cos \alpha - \sin120 \sin \alpha). Adding this to our equation for CE22CE_2^2, we get

CE22+CE42=444222(cos120cosαsin120sinα)222(cos120cosα+sin120sinα).CE_2^2 + CE_4^2 = 444 - 222(\cos120 \cos \alpha - \sin120 \sin \alpha) - 222(\cos120 \cos \alpha + \sin120 \sin \alpha). Simplifying we get

CE22+CE42=444444(cos120cosα)CE_2^2 + CE_4^2 = 444 - 444(\cos120 \cos \alpha) We can find cosα\cos \alpha by using Law of Cosines on BAD1\bigtriangleup BAD_1. This gives

11=222222cosα.11 = 222 - 222 \cos \alpha. Thus cosα=211222\cos \alpha = \frac{211}{222}. Substituting it in gives

CE22+CE42=444444(cos120211222).CE_2^2 + CE_4^2 = 444 - 444(\cos120 \cdot \frac{211}{222}). Thus

CE22+CE42=444+211=655.CE_2^2 + CE_4^2 = 444 + 211 = 655. Therefore the desired sum is equal to

11+11+655=677.11+11+655 = \boxed{677}.

Solution 5

AIME diagram

We create a diagram. Each of the red quadrilaterals are actually 60 degree rotations about point A. We easily get that CE1=11\overline{C E_1} = \sqrt{11}, and CE3=11\overline{C E_3} = \sqrt{11}. If we set BAD2=θ\angle B A D_2 = \theta, we can start angle chasing. In particular, we will like to find DE4C\angle D E_4 C, and DE2C\angle D E_2 C, since then we will be able to set up some Law Of Cosines. DE4C=DE4A+AE4C=90θ2+30+θ2=120\angle D E_4 C = \angle D E_4 A + \angle A E_4 C = 90 - \frac{\theta}{2} + 30 + \frac{\theta}{2} = 120^{\circ} That was convenient! We can do it with the other angle as well. DE2C=DE2ACE2A=90θ2(30θ2)=60\angle D E_2 C = \angle D E_2 A - \angle C E_2 A = 90 - \frac{\theta}{2} - (30 - \frac{\theta}{2}) = 60^{\circ}. That means we are able to set up Law of Cosines, on triangles DE4C\triangle D E_4 C and DE2C\triangle D E_2 C, with some really convenient angles. Let CE2=xCE_2 = x, and CE4=yCE_4 = y.

333=11+x211x333 = 11 + x^2 - \sqrt{11} x 333=11+y2+11y333 = 11 + y^2 + \sqrt{11} y We subtract and get:

0=(x+y)(xy11)0 = (x+y)(x-y-\sqrt{11}) x+yx+y obviously can't be 0, so xy=11x-y = \sqrt{11} We add and get:

666=22+x2+y2+11(yx)666 = 22 + x^2 + y^2 + \sqrt{11} (y-x) . yx=11y-x = -\sqrt{11}. Thus, we can fill in and solve.

666=22+x2+y211666 = 22 + x^2 + y^2 - 11 655=x2+y2655 = x^2 + y^2 Thus our answer is CE12+CE22+CE22+CE42=11+11+CE22+CE42=11+11+x2+y2=11+11+655=677C E_1^2 + C E_2^2 + C E_2^2 + C E_4^2 = 11 + 11 + C E_2^2 + C E_4^2 = 11 + 11 + x^2 + y^2 = 11 + 11 + 655 = \boxed{677}.

-Alexlikemath

Solution 6

Let D2,E2,E4D_2, E_2, E_4 be on the same side of ABAB as C.C. It is clear that CE2=CE4=11.CE_2=CE_4=\sqrt{11}. Then, consider quadrilateral CE3BD2.CE_3BD_2. Since BD2E3\triangle BD_2E_3 and D2BC\triangle D_2BC are congruent, D2BE3CD_2BE_3C is cyclic because BE3D2BCD2.\angle BE_3D_2\cong\angle BCD_2. By Ptolemy's Theorem, we have CE3=111CD2211.CE_3=\frac{111-CD_2^2}{\sqrt{11}}. Similarly, CE1=CD1211111.CE_1=\frac{CD_1^2-111}{\sqrt{11}}.

Let ABD2AD2B=θ.\angle ABD_2\cong\angle AD_2B=\theta. Then, cosθ=112111,\cos\theta=\frac{\sqrt{11}}{2\sqrt{111}}, so sinθ=4332111.\sin\theta=\frac{\sqrt{433}}{2\sqrt{111}}. Now, LoC on BD2C\triangle BD_2C gives CD22=11+111211111cos(θ60)CD_2^2=11+111-2\sqrt{11}\sqrt{111}\cos (\theta-60^\circ) and LoC on BD1C\triangle BD_1C gives CD12=11+111211111cos(θ+60).CD_1^2=11+111-2\sqrt{11}\sqrt{111}\cos (\theta+60^\circ). By the cosine sum rule, we get \begin{align*} CE_3&=\frac{111-CD_2^2}{\sqrt{11}}\\ &=\frac{2\sqrt{11}\sqrt{111}\cos (\theta-60^\circ)-11}{\sqrt{11}}\\ &=2\sqrt{111}(\cos\theta\cos 60^\circ+\sin\theta\sin 60^\circ)-\sqrt{11}\\ &=2\sqrt{111}\left(\frac{\sqrt{11}+\sqrt{1299}}{4\sqrt{111}}\right)-\sqrt{11}\\ &=\frac{\sqrt{1299}-\sqrt{11}}{2}.\\ \end{align*} Similarly, \begin{align*} CE_1&=\frac{CD_1^2-111}{\sqrt{11}}\\ &=\frac{11-2\sqrt{11}\sqrt{111}\cos (\theta+60^\circ)}{\sqrt{11}}\\ &=\sqrt{11}-2\sqrt{111}(\cos\theta\cos 60^\circ-\sin\theta\sin 60^\circ)\\ &=\sqrt{11}-2\sqrt{111}\left(\frac{\sqrt{11}-\sqrt{1299}}{4\sqrt{111}}\right)\\ &=\frac{\sqrt{1299}+\sqrt{11}}{2}.\\ \end{align*} Therefore, our desired answer is \begin{align*} CE_1^2+CE_2^2+CE_3^2+CE_4^2&=CE_1^2+CE_3^2+11+11\\ &=2\left(\frac{\sqrt{1299}^2+\sqrt{11}^2}{2^2}\right)+22\\ &=\frac{1310}{2}+22\\ &=\boxed{677}.\\ \end{align*}

-pieMax2713

Solution 7

AIME diagram

WLOG assume CD2>CD1,CE2>CE1,CE4>CE3CD_2>CD_1, CE_2>CE_1, CE_4>CE_3.

We first know that CE1=CE3=11CE_1=CE_3=\sqrt{11}.

The supplementary angle of E1CE2\angle E_1CE_2 is half the value of E2AE1\angle E_2AE_1. Also, E2AE1=D1AE1+D1AE2=120\angle E_2AE_1=\angle D_1AE_1 + \angle D_1AE_2 = 120^{\circ}, so E1CE2=1801202=120\angle E_1CE_2=180^{\circ}-\frac{120^{\circ}}{2}=120^{\circ}.

We now use Law of Cosines on ΔCE1E2\Delta CE_1E_2 and E1CE2\angle E_1CE_2:

(E1E2)2=(CE1)2+(CE2)22(CE1)(CE2)cos(120)(E_1E_2)^2=(CE_1)^2+(CE_2)^2-2(CE_1)(CE_2)\cos(120^{\circ}) 333=(CE2)2+112(CE2)(11)(12)333=(CE_2)^2+11-2(CE_2)(\sqrt{11})(-\frac{1}{2}) 333=(CE2)211(CE2)+11333=(CE_2)^2-\sqrt{11}(CE_2)+11 CE2=1299112CE_2=\frac{\sqrt{1299}-\sqrt{11}}{2} AIME diagram

Let FF be the midpoint of E3CE_3C. Since ΔAE3C\Delta AE_3C is isosceles, AFAF is the altitude of E4CE_4C. Then

E3E4C=12E3AC=E3AF\angle E_3E_4C=\frac{1}{2}\angle E_3AC=\angle E_3AF sin(E3E4C)=sin(E3AF)=112111=112111\sin(\angle E_3E_4C)=\sin(\angle E_3AF)=\frac{\frac{\sqrt{11}}{2}}{\sqrt{111}}=\frac{\sqrt{11}}{2\sqrt{111}} cos(E3E4C)=1sin(E3E4C)2=4332111\cos(\angle E_3E_4C)=\sqrt{1-\sin(\angle E_3E_4C)^2}=\frac{\sqrt{433}}{2\sqrt{111}} Now the Law of Cosines on ΔCE3E4\Delta CE_3E_4 and E3E4C\angle E_3E_4C:

(CE3)2=(CE4)2+(E3E4)22(CE4)(E3E4)cos(E3E4C)(CE_3)^2=(CE_4)^2+(E_3E_4)^2-2(CE_4)(E_3E_4)\cos(\angle E_3E_4C) 11=(CE4)2+3332(CE4)(333)(4332111)11=(CE_4)^2+333-2(CE_4)(\sqrt{333})(\frac{\sqrt{433}}{2\sqrt{111}}) 11=(CE4)21299(CE4)+33311=(CE_4)^2-\sqrt{1299}(CE_4)+333 CE4=1299+112CE_4=\frac{\sqrt{1299}+\sqrt{11}}{2} Finally,

k=14(CEk)2\sum_{k=1}^4(CE_k)^2 =((CE2)2+(CE4)2)+(CE1)2+(CE3)2=((CE_2)^2+(CE_4)^2)+(CE_1)^2+(CE_3)^2 =(655)+(11)+(11)=(655)+(11)+(11) =677=\boxed{677} -Marchk26

Video Solution by MOP 2024

https://youtu.be/IUOqCEGgG0g

~r00tsOfUnity