返回题库

AIME 2021 I · 第 13 题

AIME 2021 I — Problem 13

专题
Contest Math
难度
L4
来源
AIME

题目详情

Problem

Circles ω1\omega_1 and ω2\omega_2 with radii 961961 and 625625, respectively, intersect at distinct points AA and BB. A third circle ω\omega is externally tangent to both ω1\omega_1 and ω2\omega_2. Suppose line ABAB intersects ω\omega at two points PP and QQ such that the measure of minor arc PQ^\widehat{PQ} is 120120^{\circ}. Find the distance between the centers of ω1\omega_1 and ω2\omega_2.

Quick, Olympiad-Style Solution

Let Dωω1D\equiv\omega\cap\omega_{1} and Eωω2E\equiv\omega\cap\omega_{2}. The solution relies on the following key claim:

Claim. DPEQDPEQ is a harmonic quadrilateral.

Proof. Using the radical axis theorem, the tangents to circle ω\omega at DD and EE are concurrent with line ABPQ\overline{ABPQ} at the radical center, implying that our claim is true by harmonic quadrilateral properties. \blacksquare

Thus, we deduce the tangents to ω\omega at PP and QQ are concurrent at FF with line DE\overline{DE}. Denote by O1,O2,OO_{1}, O_{2}, O the centers of ω1,ω2,ω\omega_{1}, \omega_{2}, \omega respectively.

Now suppose GFDEO1O2G\equiv\overline{FDE}\cap\overline{O_{1}O_{2}}. Note that OFO1O2\overline{OF}\parallel\overline{O_{1}O_{2}} giving us the pairs of similar triangles

O1GDOFD and O2GEOFE.\triangle O_{1}GD\sim\triangle OFD~\text{and}~\triangle O_{2}GE\sim\triangle OFE. We thereby obtain

O1GO1D=OFOD=rsec1202r=sec60=2\dfrac{O_{1}G}{O_{1}D}=\dfrac{OF}{OD}=\dfrac{r\sec\tfrac{120^{\circ}}{2}}{r}=\sec 60^{\circ}=2 since PQ^=120\widehat{PQ}=120^{\circ}, where rr denotes the radius of ω\omega, and

O2GO2E=OFOE=sec60=2\dfrac{O_{2}G}{O_{2}E}=\dfrac{OF}{OE}=\sec 60^{\circ}=2 as well. It follows that

O1O2=O1GO2G=2(O1DO2E)=2(961625)=672.O_{1}O_{2}=O_{1}G-O_{2}G=2(O_{1}D-O_{2}E)=2(961-625)=\textbf{672}. AIME diagram

解析

Solution 1 (Radical Axis)

Let OiO_i and rir_i be the center and radius of ωi\omega_i, and let OO and rr be the center and radius of ω\omega.

Since AB\overline{AB} extends to an arc with arc 120120^\circ, the distance from OO to AB\overline{AB} is r/2r/2. Let X=ABO1O2X=\overline{AB}\cap \overline{O_1O_2}. Consider OO1O2\triangle OO_1O_2. The line AB\overline{AB} is perpendicular to O1O2\overline{O_1O_2} and passes through XX. Let HH be the foot from OO to O1O2\overline{O_1O_2}; so HX=r/2HX=r/2. We have by tangency OO1=r+r1OO_1=r+r_1 and OO2=r+r2OO_2=r+r_2. Let O1O2=dO_1O_2=d.

AIME diagram

Since XX is on the radical axis of ω1\omega_1 and ω2\omega_2, it has equal power with respect to both circles, so

O1X2r12=O2X2r22    O1XO2X=r12r22dO_1X^2 - r_1^2 = O_2X^2-r_2^2 \implies O_1X-O_2X = \frac{r_1^2-r_2^2}{d} since O1X+O2X=dO_1X+O_2X=d. Now we can solve for O1XO_1X and O2XO_2X, and in particular,

O1H=O1XHX=d+r12r22d2r2O2H=O2X+HX=dr12r22d2+r2.\begin{aligned} O_1H &= O_1X - HX = \frac{d+\frac{r_1^2-r_2^2}{d}}{2} - \frac{r}{2} \\ O_2H &= O_2X + HX = \frac{d-\frac{r_1^2-r_2^2}{d}}{2} + \frac{r}{2}. \end{aligned} We want to solve for dd. By the Pythagorean Theorem (twice):

OH2=O2H2(r+r2)2=O1H2(r+r1)2    (d+rr12r22d)24(r+r2)2=(dr+r12r22d)24(r+r1)2    2dr2(r12r22)8rr24r22=2dr+2(r12r22)8rr14r12    4dr=8rr28rr1    d=2r22r1\begin{aligned} &\qquad -OH^2 = O_2H^2 - (r+r_2)^2 = O_1H^2 - (r+r_1)^2 \\ &\implies \left(d+r-\tfrac{r_1^2-r_2^2}{d}\right)^2 - 4(r+r_2)^2 = \left(d-r+\tfrac{r_1^2-r_2^2}{d}\right)^2 - 4(r+r_1)^2 \\ &\implies 2dr - 2(r_1^2-r_2^2)-8rr_2-4r_2^2 = -2dr+2(r_1^2-r_2^2)-8rr_1-4r_1^2 \\ &\implies 4dr = 8rr_2-8rr_1 \\ &\implies d=2r_2-2r_1 \end{aligned} Therefore, d=2(r2r1)=2(961625)=672d=2(r_2-r_1) = 2(961-625)=\boxed{672}.

Solution 2 (Linearity)

Let O1O_{1}, O2O_{2}, and OO be the centers of ω1\omega_{1}, ω2\omega_{2}, and ω\omega with r1r_{1}, r2r_{2}, and rr their radii, respectively. Then, the distance from OO to the radical axis AB\ell\equiv\overline{AB} of ω1,ω2\omega_{1}, \omega_{2} is equal to 12r\frac{1}{2}r. Let x=O1O2x=O_{1}O_{2} and OO^{\prime} the orthogonal projection of OO onto line \ell. Define the function f:R2Rf:\mathbb{R}^{2}\rightarrow\mathbb{R} by

f(X)=Powω1(X)Powω2(X).f(X)=\text{Pow}_{\omega_{1}}(X)-\text{Pow}_{\omega_{2}}(X). Then

f(O1)=r12(xr2)(x+r2)=x2+r22r12,f(O2)=(xr1)(x+r1)(r22)=x2+r22r12,f(O)=r(r+2r1)r(r+2r2)=2r(r1r2),f(O)=0.\begin{aligned} f(O_{1})=-r_{1}^{2}-(x-r_{2})(x+r_{2})&=-x^{2}+r_{2}^{2}-r_{1}^{2}, \\ f(O_{2})=(x-r_{1})(x+r_{1})-(-r_{2}^{2})&=x^{2}+r_{2}^{2}-r_{1}^{2}, \\ f(O)=r(r+2r_{1})-r(r+2r_{2})&=2r(r_{1}-r_{2}), \\ f(O^{\prime})&=0. \end{aligned} By linearity,

f(O2)f(O1)f(O)f(O)=O1O2OO=x12r=2xr.\frac{f(O_{2})-f(O_{1})}{f(O)-f(O^{\prime})}=\frac{O_{1}O_{2}}{OO^{\prime}}=\frac{x}{\tfrac{1}{2}r}=\frac{2x}{r}. Notice that f(O2)f(O1)=x2(x2)=2x2f(O_{2})-f(O_{1})=x^{2}-(-x^{2})=2x^{2} and f(O)f(O)=2r(r1r2)f(O)-f(O^{\prime})=2r(r_{1}-r_{2}), thus

2x22r(r1r2)=2xr\begin{aligned}\frac{2x^{2}}{2r(r_{1}-r_{2})}&=\frac{2x}{r}\end{aligned} Dividing both sides by 2xr\frac{2x}{r} (which is obviously nonzero as xx is nonzero) gives us

x2(r1r2)=1\begin{aligned}\frac{x}{2(r_{1}-r_{2})}&=1\end{aligned} so x=2(r1r2)x=2(r_{1}-r_{2}). Since r1=961r_{1}=961 and r2=625r_{2}=625, the answer is x=2(961625)=672x=2\cdot(961-625)=\boxed{672}.

Solution 3

Denote by O1O_1, O2O_2, and OO the centers of ω1\omega_1, ω2\omega_2, and ω\omega, respectively. Let R1=961R_1 = 961 and R2=625R_2 = 625 denote the radii of ω1\omega_1 and ω2\omega_2 respectively, rr be the radius of ω\omega, and \ell the distance from OO to the line ABAB. We claim that

r=R2R1d,\dfrac{\ell}{r} = \dfrac{R_2-R_1}{d}, where d=O1O2d = O_1O_2. This solves the problem, for then the PQ^=120\widehat{PQ} = 120^\circ condition implies r=cos60=12\tfrac{\ell}r = \cos 60^\circ = \tfrac{1}{2}, and then we can solve to get d=672d = \boxed{672}.

AIME diagram

Denote by O1O_1 and O2O_2 the centers of ω1\omega_1 and ω2\omega_2 respectively. Set XX as the projection of OO onto O1O2O_1O_2, and denote by YY the intersection of ABAB with O1O2O_1O_2. Note that =XY\ell = XY. Now recall that

d(O2YO1Y)=O2Y2O1Y2=R22R12.d(O_2Y-O_1Y) = O_2Y^2 - O_1Y^2 = R_2^2 - R_1^2. Furthermore, note that

d(O2XO1X)=O2X2O1X2=O2O2O1O2=(R2+r)2(R1+r)2=(R22R12)+2r(R2R1).\begin{aligned}d(O_2X - O_1X) &= O_2X^2 - O_1X^2= O_2O^2 - O_1O^2 \\ &= (R_2 + r)^2 - (R_1+r)^2 = (R_2^2 - R_1^2) + 2r(R_2 - R_1).\end{aligned} Substituting the first equality into the second one and subtracting yields

2r(R2R1)=d(O2XO1X)d(O2YO1Y)=2dXY,2r(R_2 - R_1) = d(O_2X - O_1X) - d(O_2Y - O_1Y) = 2dXY, which rearranges to the desired.

Solution 4 (Quick)

Suppose we label the points as shown below.

AIME diagram

By radical axis, the tangents to ω\omega at DD and EE intersect on ABAB. Thus PDQEPDQE is harmonic, so the tangents to ω\omega at PP and QQ intersect at XDEX \in DE. Moreover, OXO1O2OX \parallel O_1O_2 because both OXOX and O1O2O_1O_2 are perpendicular to ABAB, and OX=2OPOX = 2OP because POQ=120\angle POQ = 120^{\circ}. Thus

O1O2=O1YO2Y=29612625=672O_1O_2 = O_1Y - O_2Y = 2 \cdot 961 - 2\cdot 625 = \boxed{672} by similar triangles.

~mathman3880

Solution 5 (Official MAA)

Like in other solutions, let OO be the center of ω\omega with rr its radius; also, let O1O_{1} and O2O_{2} be the centers of ω1\omega_{1} and ω2\omega_{2} with R1R_{1} and R2R_{2} their radii, respectively. Let line OPOP intersect line O1O2O_{1}O_{2} at TT, and let u=TO2u=TO_{2}, v=TO1v=TO_{1}, x=PTx=PT, where the length O1O2O_{1}O_{2} splits as u+vu+v. Because the lines PQPQ and O1O2O_{1}O_{2} are perpendicular, lines OTOT and O1O2O_{1}O_{2} meet at a 6060^{\circ} angle.

Applying the Law of Cosines to O2PT\triangle O_{2}PT, O1PT\triangle O_{1}PT, O2OT\triangle O_{2}OT, and O1OT\triangle O_{1}OT gives

O2PT:O2P2=u2+x2uxO1PT:O1P2=v2+x2+vxO2OT:(r+R2)2=u2+(r+x)2u(r+x)O1OT:(r+R1)2=v2+(r+x)2+v(r+x)\begin{aligned}\triangle O_{2}PT&:O_{2}P^{2}=u^{2}+x^{2}-ux \\ \triangle O_{1}PT&:O_{1}P^{2}=v^{2}+x^{2}+vx \\ \triangle O_{2}OT&:(r+R_{2})^{2}=u^{2}+(r+x)^{2}-u(r+x) \\ \triangle O_{1}OT&:(r+R_{1})^{2}=v^{2}+(r+x)^{2}+v(r+x)\end{aligned} Adding the first and fourth equations, then subtracting the second and third equations gives us

(O2P2O1P2)+(R12R22)+2r(R1R2)=r(u+v)\left(O_{2}P^{2}-O_{1}P^{2}\right)+\left(R_{1}^{2}-R_{2}^{2}\right)+2r(R_{1}-R_{2})=r(u+v) Since PP lies on the radical axis of ω1\omega_{1} and ω2\omega_{2}, the power of point PP with respect to either circle is

O2P2R22=O1P2R12.O_{2}P^{2}-R_{2}^{2}=O_{1}P^{2}-R_{1}^{2}. Hence 2r(R1R2)=r(u+v)2r(R_{1}-R_{2})=r(u+v) which simplifies to

u+v=2(R1R2).u+v=2(R_{1}-R_{2}). The requested distance

O1O2=O1T+O2T=u+vO_{1}O_{2}=O_{1}T+O_{2}T=u+v is therefore equal to 2(961625)=6722\cdot(961-625)=\boxed{672}.

Solution 6 (Geometry)

AIME diagram

Let circle ω\omega tangent circles ω1\omega_1 and ω2,\omega_2, respectively at distinct points CC and DD. Let O,O1,O2(r,r1,r2)O, O_1, O_2 (r, r_1, r_2) be the centers (the radii) of ω,ω1\omega, \omega_1 and ω2,\omega_2, respectively. WLOG r1<r2.r_1 < r_2. Let FF be the point of OO2OO_2 such, that OO1=OF.OO_1 =OF. Let MM be the midpoint FO1,OEAB,CTFO_1, OE \perp AB, CT be the radical axes of ω1\omega_1 and ω,TAB.\omega, T \in AB.

Then TT is radical center of ω,ω1\omega, \omega_1 and ω2,TD=CT.\omega_2, TD = CT.

In OFO1(OF=OO1)OT\triangle OFO_1 (OF = OO_1) OT is bisector of O,OM\angle O, OM is median

    O,T,\hspace{10mm} \implies O,T, and MM are collinear.

OCT=ODT=OET=90    \angle OCT = \angle ODT = \angle OET = 90^\circ \implies OCTDEOCTDE is cyclic (in Ω),OT\Omega), OT is diameter Ω.\Omega. O1O2AB,OMFO1    FO1O2=OTEO_1O_2 \perp AB, OM \perp FO_1 \implies \angle FO_1O_2 = \angle OTE OTE=ODE\angle OTE = \angle ODE as they intercept the same arc OE\overset{\Large\frown}{OE} in Ω.\Omega.

OEAB,O1O2AB    O1O2OE    OE \perp AB, O_1O_2 \perp AB \implies O_1 O_2 || OE \implies OO2O1=O2OE    ODEO2O1F    \angle OO_2O_1 = \angle O_2 OE \implies \triangle ODE \sim \triangle O_2 O_1 F \implies OEOD=O2FO1O2    cos1202=r2+rr1rO1O2    O1O2=2r2r1.\frac {OE}{OD} = \frac {O_2F}{O_1O_2} \implies \cos \frac {120^\circ}{2} = \frac{r_2 + r - r_1 -r} {O_1O_2}\implies {O_1O_2}= 2|r_2 – r_1|. Since r1=625r_{1}=625 and r2=961r_{2}=961, the answer is 2961625=6722\cdot|961-625|=\boxed{672}.

vladimir.shelomovskii@gmail.com, vvsss

Solution 7

We are not given the radius of circle ww, but based on the problem statement, that radius isn't important. We can set ww to have radius infinity (solution 8), but if you didn't observe that, you could also set the radius to be 2r2r so that the line containing the center of ww, call it WW, and w2w_2, call it W2W_2, is perpendicular to the line containing the center of w1w_1, call it W1W_1 and w2w_2. Let AB=2hAB = 2h and W1W2=xW_1W_2 = x. Also, let the projections of WW and W1W_1 onto line ABAB be XX and YY, respectively.

By Pythagorean Theorem on WW1W2\triangle WW_1W_2, we get

x2+(625+2r)2=(961+2r)2  (1)x^2+(625+2r)^2=(961+2r)^2 \;(1) Note that since PWQ=120\angle PWQ = 120, PWX=60\angle PWX = 60. So, WX=2r/2=r=W1YWX = 2r/2 = r = W_1Y. We now get two more equations from Pythag:

h2+r2=6252  (2)h^2+r^2 = 625^2 \; (2) h2+(xr)2=9612  (3)h^2+(x-r)^2 = 961^2 \; (3) From subtracting (2)(2) and (3)(3), x22rx=96126252  (4)x^2-2rx=961^2-625^2 \; (4). Rearranging (1)(1) yields x21344r=96126252x^2-1344r = 961^2-625^2. Plugging in our result from (4)(4), x21344r=x22rx    1344r=2rx    x=672x^2-1344r= x^2-2rx \implies 1344r = 2rx \implies x=\boxed{672}.

~sml1809

Solution 8 (Cheese)

Let the circle ω\omega be infinitely big (a line). Then for it to be split into an arc of 120120^{\circ}, PQ\overline{PQ} must intersect at a 6060^{\circ} with line ω\omega.

Notice the 30-60-90 triangle in the image. O1R=961625O_1R = 961 - 625.

Thus, the distance between the centers of ω1\omega_1 and ω2\omega_2 is 2(961625)=6722(961-625)=\boxed{672}

AIME diagram

picture by afly

Video Solution by MOP 2024

https://youtu.be/GQT73xqvtXA

~r00tsOfUnity

Video Solution

https://youtu.be/gN7Ocu3D62M

~Math Problem Solving Skills

Video Solution

Who wanted to see animated video solutions can see this. I found this really helpful.

https://youtu.be/YtZ8_7i833E

P.S: This video is not made by me. And solution is same like below solutions.

≈@rounak138