Difference between revisions of "2024 AIME I Problems/Problem 10"
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==Problem== | ==Problem== | ||
− | Let <math>ABC</math> be a triangle inscribed in circle <math>\omega</math>. Let the tangents to <math>\omega</math> at <math>B</math> and <math>C</math> intersect at point <math>D</math>, and let <math>\overline{AD}</math> intersect <math>\omega</math> at <math>P</math>. | + | Let <math>ABC</math> be a triangle inscribed in circle <math>\omega</math>. Let the tangents to <math>\omega</math> at <math>B</math> and <math>C</math> intersect at point <math>D</math>, and let <math>\overline{AD}</math> intersect <math>\omega</math> at <math>P</math>. If <math>AB=5</math>, <math>BC=9</math>, and <math>AC=10</math>, <math>AP</math> can be written as the form <math>\frac{m}{n}</math>, where <math>m</math> and <math>n</math> are relatively prime integers. Find <math>m + n</math>. |
+ | |||
+ | ==Diagram== | ||
+ | <asy> | ||
+ | import olympiad; | ||
+ | |||
+ | unitsize(15); | ||
+ | |||
+ | pair A, B, C, D, E, F, P, O; | ||
+ | |||
+ | C = origin; A = (10,0); B = (7.8, 4.4899); | ||
+ | draw(A--B--C--cycle); draw(A..B..C..cycle, red+dotted); | ||
+ | |||
+ | O = circumcenter(A, B, C); | ||
+ | |||
+ | E = rotate(90,B) * (O); | ||
+ | F = rotate(90,C) * (O); | ||
+ | |||
+ | D = IP(B..E + (B-E)*4, C..F + (C-F)*-3); | ||
+ | |||
+ | draw(B--D--C--D--A); | ||
+ | |||
+ | P = IP(D..A, A..B..C); | ||
+ | |||
+ | dot(A); dot(B); dot(C); dot(D); dot(P); | ||
+ | label("$A$", A, dir(335)); | ||
+ | label("$B$", B, dir(65)); | ||
+ | label("$C$", C, dir(200)); | ||
+ | label("$D$", D, dir(135)); | ||
+ | label("$P$", P, dir(235)); | ||
+ | </asy> | ||
==Solution 1== | ==Solution 1== | ||
Line 8: | Line 38: | ||
==Solution 2== | ==Solution 2== | ||
+ | [[File:2024 AIME I problem 10.png|300px|right]] | ||
+ | We know <math>AP</math> is the symmedian,(see [[ Symmedians, Lemoine point | Symmedian and tangents ]]) | ||
− | + | which implies <math>\triangle{ABP}\sim \triangle{AMC}</math> where <math>M</math> is the midpoint of <math>BC</math>. | |
+ | |||
+ | By Appolonius theorem, <math>AM=\frac{13}{2}</math>. | ||
+ | |||
+ | Thus, we have <math>\frac{AP}{AC}=\frac{AB}{AM}, AP=\frac{100}{13}\implies \boxed{113}</math> | ||
~Bluesoul | ~Bluesoul | ||
Line 15: | Line 51: | ||
==Solution 3== | ==Solution 3== | ||
− | Extend sides <math>\overline{AB}</math> and <math>\overline{AC}</math> to points <math>E</math> and <math>F</math>, respectively, such that <math>B</math> and <math>C</math> are the feet of the altitudes in <math>\triangle AEF</math>. Denote the feet of the altitude from <math>A</math> to <math>\overline{EF}</math> as <math>X</math>, and let <math>H</math> denote the orthocenter of <math>\triangle AEF</math>. Call <math>M</math> the midpoint of segment <math>\overline{EF}</math>. By the Three Tangents Lemma, we have that <math>MB</math> and <math>MC</math> are both tangents to <math>(ABC)</math> <math>\implies</math> <math>M = | + | Extend sides <math>\overline{AB}</math> and <math>\overline{AC}</math> to points <math>E</math> and <math>F</math>, respectively, such that <math>B</math> and <math>C</math> are the feet of the altitudes in <math>\triangle AEF</math>. Denote the feet of the altitude from <math>A</math> to <math>\overline{EF}</math> as <math>X</math>, and let <math>H</math> denote the orthocenter of <math>\triangle AEF</math>. Call <math>M</math> the midpoint of segment <math>\overline{EF}</math>. By the Three Tangents Lemma, we have that <math>MB</math> and <math>MC</math> are both tangents to <math>(ABC)</math> <math>\implies</math> <math>M = D</math>, and since <math>M</math> is the midpoint of <math>\overline{EF}</math>, <math>MF = MB</math>. Additionally, by angle chasing, we get that: |
<cmath>\angle ABC \cong \angle AHC \cong \angle EHX</cmath> | <cmath>\angle ABC \cong \angle AHC \cong \angle EHX</cmath> | ||
Also, | Also, | ||
Line 24: | Line 60: | ||
<cmath>\cos(A) = \frac{10^2 + 5^2 - 9^2}{2 \cdot 10 \cdot 5} = \frac{11}{25}</cmath> | <cmath>\cos(A) = \frac{10^2 + 5^2 - 9^2}{2 \cdot 10 \cdot 5} = \frac{11}{25}</cmath> | ||
Thus, we can find that the side lengths of <math>\triangle AEF</math> are <math>\frac{250}{11}, \frac{125}{11}, \frac{225}{11}</math>. Then, by Stewart's theorem, <math>AM = \frac{13 \cdot 25}{22}</math>. By Power of a Point, | Thus, we can find that the side lengths of <math>\triangle AEF</math> are <math>\frac{250}{11}, \frac{125}{11}, \frac{225}{11}</math>. Then, by Stewart's theorem, <math>AM = \frac{13 \cdot 25}{22}</math>. By Power of a Point, | ||
− | <cmath>\overline{MB} \cdot \overline{MB} = \overline{MA} \cdot \overline{ | + | <cmath>\overline{MB} \cdot \overline{MB} = \overline{MA} \cdot \overline{MP}</cmath> |
− | <cmath>\frac{225}{22} \cdot \frac{225}{22} = \overline{ | + | <cmath>\frac{225}{22} \cdot \frac{225}{22} = \overline{MP} \cdot \frac{13 \cdot 25}{22} \implies \overline{MP} = \frac{225 \cdot 9}{22 \cdot 13}</cmath> |
Thus, | Thus, | ||
− | <cmath> | + | <cmath>AP = AM - MP = \frac{13 \cdot 25}{22} - \frac{225 \cdot 9}{22 \cdot 13} = \frac{100}{13}</cmath> |
Therefore, the answer is <math>\boxed{113}</math>. | Therefore, the answer is <math>\boxed{113}</math>. | ||
Line 36: | Line 72: | ||
\begin{align*} | \begin{align*} | ||
81&=x^2+4x^2-4x^2\cos(180-\angle BAC) \\ | 81&=x^2+4x^2-4x^2\cos(180-\angle BAC) \\ | ||
− | &= 5x^2+4x^2\cos( | + | &= 5x^2+4x^2\cos(BAC). \\ |
\end{align*} | \end{align*} | ||
Line 45: | Line 81: | ||
~evanhliu2009 | ~evanhliu2009 | ||
+ | |||
+ | ==Solution 5== | ||
+ | |||
+ | Following from the law of cosines, we can easily get <math>\cos A = \frac{11}{25}</math>, <math>\cos B = \frac{1}{15}</math>, <math>\cos C = \frac{13}{15}</math>. | ||
+ | |||
+ | Hence, <math>\sin A = \frac{6 \sqrt{14}}{25}</math>, <math>\cos 2C = \frac{113}{225}</math>, <math>\sin 2C = \frac{52 \sqrt{14}}{225}</math>. | ||
+ | Thus, <math>\cos \left( A + 2C \right) = - \frac{5}{9}</math>. | ||
+ | |||
+ | Denote by <math>R</math> the circumradius of <math>\triangle ABC</math>. | ||
+ | In <math>\triangle ABC</math>, following from the law of sines, we have <math>R = \frac{BC}{2 \sin A} = \frac{75}{4 \sqrt{14}}</math>. | ||
+ | |||
+ | Because <math>BD</math> and <math>CD</math> are tangents to the circumcircle <math>ABC</math>, <math>\triangle OBD \cong \triangle OCD</math> and <math>\angle OBD = 90^\circ</math>. | ||
+ | Thus, <math>OD = \frac{OB}{\cos \angle BOD} = \frac{R}{\cos A}</math>. | ||
+ | |||
+ | In <math>\triangle AOD</math>, we have <math>OA = R</math> and <math>\angle AOD = \angle BOD + \angle AOB = A + 2C</math>. | ||
+ | Thus, following from the law of cosines, we have | ||
+ | |||
+ | \begin{align*} | ||
+ | AD & = \sqrt{OA^2 + OD^2 - 2 OA \cdot OD \cos \angle AOD} \\ | ||
+ | & = \frac{26 \sqrt{14}}{33} R. | ||
+ | \end{align*} | ||
+ | |||
+ | |||
+ | Following from the law of cosines, | ||
+ | |||
+ | \begin{align*} | ||
+ | \cos \angle OAD & = \frac{AD^2 + OA^2 - OD^2}{2 AD \cdot OA} \\ | ||
+ | & = \frac{8 \sqrt{14}}{39} . | ||
+ | \end{align*} | ||
+ | |||
+ | |||
+ | Therefore, | ||
+ | |||
+ | \begin{align*} | ||
+ | AP & = 2 OA \cos \angle OAD \\ | ||
+ | & = \frac{100}{13} . | ||
+ | \end{align*} | ||
+ | |||
+ | |||
+ | Therefore, the answer is <math>100 + 13 = \boxed{\textbf{(113) }}</math>. | ||
+ | |||
+ | ~Steven Chen (Professor Chen Education Palace, www.professorchenedu.com) | ||
==Video Solution 1 by OmegaLearn.org== | ==Video Solution 1 by OmegaLearn.org== | ||
https://youtu.be/heryP002bp8 | https://youtu.be/heryP002bp8 | ||
+ | ==Video Solution== | ||
+ | |||
+ | https://youtu.be/RawwQmVYyaw | ||
+ | |||
+ | ~Steven Chen (Professor Chen Education Palace, www.professorchenedu.com) | ||
+ | |||
+ | ==Solution 6== | ||
+ | |||
+ | Note that since P is a symmedian, <math>(AP;BC)</math> are harmonic. As a result, <math>\frac{BP}{PC} = \frac{BA}{CA}</math>. As a result, <math>2(BP) = PC</math>. Call <math>BP = x</math>. Then, <math>PC = 2x</math>. Since <math>cos A = \frac{11}{25}</math>, <math>cos BPC = - \frac{11}{25}</math>. Use LOC to find <math>x = \frac{45}{13}</math>. Finish with Ptolemy on ABPC, and finish to get <math>\frac{100}{13}</math>. | ||
==See also== | ==See also== |
Latest revision as of 14:03, 5 October 2024
Contents
Problem
Let be a triangle inscribed in circle . Let the tangents to at and intersect at point , and let intersect at . If , , and , can be written as the form , where and are relatively prime integers. Find .
Diagram
Solution 1
From the tangency condition we have . With LoC we have and . Then, . Using LoC we can find : . Thus, . By Power of a Point, so which gives . Finally, we have .
~angie.
Solution 2
We know is the symmedian,(see Symmedian and tangents )
which implies where is the midpoint of .
By Appolonius theorem, .
Thus, we have
~Bluesoul
Solution 3
Extend sides and to points and , respectively, such that and are the feet of the altitudes in . Denote the feet of the altitude from to as , and let denote the orthocenter of . Call the midpoint of segment . By the Three Tangents Lemma, we have that and are both tangents to , and since is the midpoint of , . Additionally, by angle chasing, we get that: Also, Furthermore, From this, we see that with a scale factor of . By the Law of Cosines, Thus, we can find that the side lengths of are . Then, by Stewart's theorem, . By Power of a Point, Thus, Therefore, the answer is .
~mathwiz_1207
Solution 4 (LoC spam)
Connect lines and . From the angle by tanget formula, we have . Therefore by AA similarity, . Let . Using ratios, we have Similarly, using angle by tangent, we have , and by AA similarity, . By ratios, we have However, because , we have so Now using Law of Cosines on in triangle , we have Solving, we find . Now we can solve for . Using Law of Cosines on we have \begin{align*} 81&=x^2+4x^2-4x^2\cos(180-\angle BAC) \\ &= 5x^2+4x^2\cos(BAC). \\ \end{align*}
Solving, we get Now we have a system of equations using Law of Cosines on and ,
Solving, we find , so our desired answer is .
~evanhliu2009
Solution 5
Following from the law of cosines, we can easily get , , .
Hence, , , . Thus, .
Denote by the circumradius of . In , following from the law of sines, we have .
Because and are tangents to the circumcircle , and . Thus, .
In , we have and . Thus, following from the law of cosines, we have
\begin{align*} AD & = \sqrt{OA^2 + OD^2 - 2 OA \cdot OD \cos \angle AOD} \\ & = \frac{26 \sqrt{14}}{33} R. \end{align*}
Following from the law of cosines,
\begin{align*} \cos \angle OAD & = \frac{AD^2 + OA^2 - OD^2}{2 AD \cdot OA} \\ & = \frac{8 \sqrt{14}}{39} . \end{align*}
Therefore,
\begin{align*} AP & = 2 OA \cos \angle OAD \\ & = \frac{100}{13} . \end{align*}
Therefore, the answer is .
~Steven Chen (Professor Chen Education Palace, www.professorchenedu.com)
Video Solution 1 by OmegaLearn.org
Video Solution
~Steven Chen (Professor Chen Education Palace, www.professorchenedu.com)
Solution 6
Note that since P is a symmedian, are harmonic. As a result, . As a result, . Call . Then, . Since , . Use LOC to find . Finish with Ptolemy on ABPC, and finish to get .
See also
2024 AIME I (Problems • Answer Key • Resources) | ||
Preceded by Problem 9 |
Followed by Problem 11 | |
1 • 2 • 3 • 4 • 5 • 6 • 7 • 8 • 9 • 10 • 11 • 12 • 13 • 14 • 15 | ||
All AIME Problems and Solutions |
The problems on this page are copyrighted by the Mathematical Association of America's American Mathematics Competitions.