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AIME 2012 II · 第 15 题

AIME 2012 II — Problem 15

专题
Contest Math
难度
L4
来源
AIME

题目详情

Problem 15

Triangle ABCABC is inscribed in circle ω\omega with AB=5AB=5, BC=7BC=7, and AC=3AC=3. The bisector of angle AA meets side BC\overline{BC} at DD and circle ω\omega at a second point EE. Let γ\gamma be the circle with diameter DE\overline{DE}. Circles ω\omega and γ\gamma meet at EE and a second point FF. Then AF2=mnAF^2 = \frac mn, where mm and nn are relatively prime positive integers. Find m+nm+n.

Quick Solution using Olympiad Terms

Take a force-overlaid inversion about AA and note DD and EE map to each other. As DEDE was originally the diameter of γ\gamma, DEDE is still the diameter of γ\gamma. Thus γ\gamma is preserved. Note that the midpoint MM of BCBC lies on γ\gamma, and BCBC and ω\omega are swapped. Thus points FF and MM map to each other, and are isogonal. It follows that AFAF is a symmedian of ABC\triangle{ABC}, or that ABFCABFC is harmonic. Then (AB)(FC)=(BF)(CA)(AB)(FC)=(BF)(CA), and thus we can let BF=5x,CF=3xBF=5x, CF=3x for some xx. By the LoC, it is easy to see BAC=120\angle{BAC}=120^\circ so (5x)2+(3x)22cos60(5x)(3x)=49(5x)^2+(3x)^2-2\cos{60^\circ}(5x)(3x)=49. Solving gives x2=4919x^2=\frac{49}{19}, from which by Ptolemy's we see AF=3019AF=\frac{30}{\sqrt{19}}. We conclude the answer is 900+19=919900+19=\boxed{919}.

- Emathmaster

Side Note: You might be wondering what the motivation for this solution is. Most of the people who've done EGMO Chapter 8 should recognize this as problem 8.32 (2009 Russian Olympiad) with the computational finish afterwards. Now if you haven't done this, but still know what inversion is, here's the motivation. We'd see that it's kinda hard to angle chase, and if we could, it would still be a bit hard to apply (you could use trig, but it won't be so clean most likely). If you give up after realizing that angle chasing won't work, you'd likely go in a similar approach to Solution 1 (below) or maybe be a bit more insightful and go with the elementary solution above.

Finally, we notice there's circles! Classic setup for inversion! Since we're involving an angle-bisector, the first thing that comes to mind is a force overlaid inversion described in Lemma 8.16 of EGMO (where we invert with radius ABAC\sqrt{AB \cdot AC} and center AA, then reflect over the AA-angle bisector, which fixes B,CB, C). We try applying this to the problem, and it's fruitful - we end up with this solution. -MSC

解析

Solution 1

Use the angle bisector theorem to find CD=218CD=\tfrac{21}{8}, BD=358BD=\tfrac{35}{8}, and use Stewart's Theorem to find AD=158AD=\tfrac{15}{8}. Use Power of Point DD to find DE=498DE=\tfrac{49}{8}, and so AE=8AE=8. Use law of cosines to find CAD=π3\angle CAD = \tfrac{\pi} {3}, hence BAD=π3\angle BAD = \tfrac{\pi}{3} as well, and BCE\triangle BCE is equilateral, so BC=CE=BE=7BC=CE=BE=7.

AIME diagram

In triangle AEFAEF, let XX be the foot of the altitude from AA; then EF=EX+XFEF=EX+XF, where we use signed lengths. Writing EX=AEcosAEFEX=AE \cdot \cos \angle AEF and XF=AFcosAFEXF=AF \cdot \cos \angle AFE, we get

EF=AEcosAEF+AFcosAFE.(1)\begin{aligned}\tag{1} EF = AE \cdot \cos \angle AEF + AF \cdot \cos \angle AFE. \end{aligned} Note AFE=ACE\angle AFE = \angle ACE, and the Law of Cosines in ACE\triangle ACE gives cosACE=17\cos \angle ACE = -\tfrac 17. Also, AEF=DEF\angle AEF = \angle DEF, and DFE=π2\angle DFE = \tfrac{\pi}{2} (DEDE is a diameter), so cosAEF=EFDE=849EF\cos \angle AEF = \tfrac{EF}{DE} = \tfrac{8}{49}\cdot EF.

Plugging in all our values into equation (1)(1), we get:

EF=6449EF17AFEF=715AF.EF = \tfrac{64}{49} EF -\tfrac{1}{7} AF \quad \Longrightarrow \quad EF = \tfrac{7}{15} AF. The Law of Cosines in AEF\triangle AEF, with EF=715AFEF=\tfrac 7{15}AF and cosAFE=17\cos\angle AFE = -\tfrac 17 gives

82=AF2+49225AF2+215AF2=225+49+30225AF28^2 = AF^2 + \tfrac{49}{225} AF^2 + \tfrac 2{15} AF^2 = \tfrac{225+49+30}{225}\cdot AF^2 Thus AF2=90019AF^2 = \frac{900}{19}. The answer is 919\boxed{919}. ~Shen Kislay Kai

Solution 2

Let a=BCa = BC, b=CAb = CA, c=ABc = AB for convenience. Let MM be the midpoint of segment BCBC. We claim that MAD=DAF\angle MAD=\angle DAF.

Proof\textit{Proof}. Since AEAE is the angle bisector, it follows that EB=ECEB = EC and consequently EMBCEM\perp BC. Therefore, MγM\in \gamma. Now let X=FDωX = FD\cap \omega. Since EFX=90\angle EFX=90^\circ, EXEX is a diameter, so XX lies on the perpendicular bisector of BCBC; hence EE, MM, XX are collinear. From DAG=DMX=90\angle DAG = \angle DMX = 90^\circ, quadrilateral ADMXADMX is cyclic. Therefore, MAD=MXD\angle MAD = \angle MXD. But MXD\angle MXD and EAF\angle EAF are both subtended by arc EFEF in ω\omega, so they are equal. Thus MAD=DAF\angle MAD=\angle DAF, as claimed.

AIME diagram

As a result, CAM=FAB\angle CAM = \angle FAB. Combined with BFA=MCA\angle BFA=\angle MCA, we get ABFAMC\triangle ABF\sim\triangle AMC and therefore

cAM=AFbAF2=b2c2AM2=152AM2\frac c{AM}=\frac {AF}b\qquad \Longrightarrow \qquad AF^2=\frac{b^2c^2}{AM^2} = \frac{15^2}{AM^2} By Stewart's Theorem on ABC\triangle ABC (with cevian AMAM), we get

AM2=12(b2+c2)14a2=194,AM^2 = \tfrac 12 (b^2+c^2)-\tfrac 14 a^2 = \tfrac{19}{4}, so AF2=90019AF^2 = \tfrac{900}{19}, so the answer is 900+19=919900+19=\boxed{919}.

-Solution by thecmd999

Solution 3

Use the angle bisector theorem to find CD=218CD=\tfrac{21}{8}, BD=358BD=\tfrac{35}{8}, and use Stewart's Theorem to find AD=158AD=\tfrac{15}{8}. Use Power of Point DD to find DE=498DE=\tfrac{49}{8}, and so AE=8AE=8. Then use the Extended Law of Sine to find that the length of the circumradius of ABC\triangle ABC is 733\tfrac{7\sqrt{3}}{3}.

AIME diagram

Since DEDE is the diameter of circle γ\gamma, DFE\angle DFE is 9090^\circ. Extending DFDF to intersect circle ω\omega at XX, we find that XEXE is the diameter of ω\omega (since DFE\angle DFE is 9090^\circ). Therefore, XE=1433XE=\tfrac{14\sqrt{3}}{3}.

Let EF=xEF=x, XD=uXD=u, and DF=vDF=v. Then XE2XF2=EF2=DE2DF2XE^2-XF^2=EF^2=DE^2-DF^2, so we get

(u+v)2v2=1963240164(u+v)^2-v^2=\frac{196}{3}-\frac{2401}{64} which simplifies to

u2+2uv=5341192.u^2+2uv = \frac{5341}{192}. By Power of Point DD, uv=BDDC=735/64uv=BD \cdot DC=735/64. Combining with above, we get

XD2=u2=931192.XD^2=u^2=\frac{931}{192}. Note that XDEADF\triangle XDE\sim \triangle ADF and the ratio of similarity is ρ=AD:XD=158:u\rho = AD : XD = \tfrac{15}{8}:u. Then AF=ρXE=158uRAF=\rho\cdot XE = \tfrac{15}{8u}\cdot R and

AF2=22564R2u2=90019.AF^2 = \frac{225}{64}\cdot \frac{R^2}{u^2} = \frac{900}{19}. The answer is 900+19=919900+19=\boxed{919}.

-Solution by TheBoomBox77

Solution 4

Use Law of Cosines in ABC\triangle ABC to get BAC=120\angle BAC=120^\circ. Because AEAE bisects A\angle A, EE is the midpoint of major arc BCBC so BE=CE,BE=CE, and BEC=60.\angle BEC=60^\circ. Thus BEC\triangle BEC is equilateral. Notice now that BFC=BFE=60.\angle BFC=\angle BFE= 60^\circ. But DFE=90\angle DFE=90^\circ so FDFD bisects BFC.\angle BFC. Thus,

BFCF=BDCD=BACA=53.\frac{BF}{CF}=\frac{BD}{CD}=\frac{BA}{CA}=\frac{5}{3}. Let BF=5k,CF=3k.BF=5k, CF=3k. Use Law of Cosines on BFC\triangle BFC to get

25k2+9k215k2=49k=71925k^2+9k^2-15k^2 = 49 \qquad \Longrightarrow\qquad k=\frac 7{\sqrt{19}} Use Ptolemy's Theorem on BFCABFCA, to get

15k+15k=7AF,AF=3019,15k+15k=7\cdot AF, \qquad \Longrightarrow\qquad AF= \frac{30}{\sqrt{19}}, so AF2=90019AF^2=\frac{900}{19} and the answer is 900+19=919900+19=919

~Shen Kislay Kai

Solution 5

AIME diagram

Denote AB=c,BC=a,AC=b,A=2α.AB = c, BC = a, AC = b, \angle A = 2 \alpha. Let M be midpoint BC. Let θ\theta be the circle centered at AA with radius ABAC=bc.\sqrt{AB \cdot AC} =\sqrt{bc}.

We calculate the length of some segments. The median AM=b22+c22a24.AM = \sqrt{\frac {b^2}{2} + \frac {c^2}{2} - \frac {a^2}{4}}. The bisector AD=2bccosαb+c.AD = \frac {2 b c \cos \alpha}{b+c}. One can use Stewart's Theorem in both cases.

ADAD is bisector of A    BD=acb+c,CD=abb+c    \angle A \implies BD = \frac {a c}{b + c}, CD = \frac {a b}{b + c} \implies

BDCD=a2bc(b+c)2.BD \cdot CD = \frac {a^2 bc }{(b+c)^2}. We use Power of Point DD and get ADDE=BDCD.AD \cdot DE = BD \cdot CD.

AE=AD+DE=AD+BDCDAD,AE = AD + DE = AD + \frac {BD \cdot CD}{AD}, AE=2bccosαb+c+a2bc(b+c)(b+c)22bccosα=AE =\frac {2 b c \cos \alpha}{b+c} + \frac {a^2 bc \cdot (b+c) }{(b+c)^2 \cdot 2 b c \cos \alpha} = =bccos2α+a22(b+c)cosα=4bccos2α+b2+c22bccos2α2(b+c)cosα=b+c2    ADAE=2bccosα.= \frac {b c \cos^2 \alpha + a^2}{2(b+c)\cos \alpha} =\frac {4bc \cos^2 \alpha + b^2 +c^2 -2 b c \cos 2\alpha}{2(b+c) \cos \alpha} = \frac {b+c}{2} \implies AD \cdot AE = 2 bc \cos \alpha. We consider the inversion with respect θ.\theta.

BB swap B    AB=AC,BAB    BB' \implies AB' = AC, B' \in AB \implies B' is symmetric to CC with respect to AE.AE.

CC swap C    AC=AB,CC' \implies AC' = AB, C' lies on line AC    CAC \implies C' is symmetric to BB with respect to AE.AE.

BC2=AB2+AC2+ABBC    α=60    ADAE=bc    DBC^2 = AB^2 + AC^2 + AB \cdot BC \implies \alpha = 60^\circ \implies AD \cdot AE = bc \implies D swap E.E.

Points DD and EE lies on Γ    Γ\Gamma \implies \Gamma swap Γ.\Gamma.

DEDE is diameter Γ,DME=90    MΓ.\Gamma, \angle DME = 90^\circ \implies M \in \Gamma. Therefore MM is crosspoint of BCBC and Γ.\Gamma.

Let Ω\Omega be circumcircle ABC.ΩAB'C'. \Omega is image of line BC.BC. Point MM maps into M    M=ΓΩ.M' \implies M' = \Gamma \cap \Omega.

Points A,B,A, B', and CC' are symmetric to A,C,A, C, and B,B, respectively.

Point MM' lies on Γ\Gamma which is symmetric with respect to AEAE and on Ω\Omega which is symmetric to ω\omega with respect to AE    AE \implies

MM' is symmetric FF with respect to AE    AM=AF.AE \implies AM' = AF.

We use Power of Point AA and get

AF=AM=ADAEAM=4bc2b2+2c2a2=43550+1849=3019    919.AF = AM' = \frac {AD \cdot AE}{AM} = \frac {4b c}{\sqrt{2 b^2 + 2 c^2 – a^2}} = \frac {4 \cdot 3 \cdot 5}{\sqrt{ 50 + 18 – 49}} = \frac {30}{\sqrt{19}} \implies \boxed{\textbf{919}}. vladimir.shelomovskii@gmail.com, vvsss

Solution 6:

To do this, we first define the intersection of EFEF and BCBC to be KK.

Lemma 1: (K,C,D,B)(K, C, D, B) are harmonic. First of all, define the midpoint of BCBC to be MM. Then, we have that angle FMD is 9090 degrees, and as a result, MM lies on this circle. By Power of a Point, (KD)(KM)=(KE)(KF)=(KB)(KC)(KD)(KM) = (KE)(KF) = (KB)(KC). As a result, (K,C,D,B)(K, C, D, B) are harmonic from another famous harmonic lemma.

As a result, since EFD=90\angle EFD = 90^{\circ}, by another Harmonic Lemma, FDFD is the angle bisector of BFCBFC. Since BDCD=53\frac{BD}{CD} = \frac{5}{3} by angle bisector theorem, BFCF=53\frac{BF}{CF} = \frac{5}{3}. Since BAC\angle BAC is 120120^{\circ} by Law of Cosines (LOC), we can use LOC to finish off. Call BF=5aBF = 5a, and CF=3aCF = 3a, (5a)2+(3a)215a2=49(5a)^2+(3a)^2-15a^2 = 49, so a=719a = \frac{7}{\sqrt{19}}. We do Ptolemy's Theorem on ABFCABFC. Our answer is:

(3)(35)+(5)(21)719=3019.\frac{(3)(35)+(5)(21)}{7\sqrt{19}} = \frac{30}{\sqrt{19}}. As a result, the final answer is 919\boxed{919}.

-sepehr2010

Minor edits ~Zhenghua

Video Solution by mop 2024

https://youtu.be/mIFUuY4ybeg

~r00tsOfUnity