Maths Olympiad Prep

Track / Stage 8 / 130 of 180 #1830 of 1964

Problem 1830

IMO Shortlist mid-range; USAMO P2/P5
Geometry Difficulty 8.4 Prove it International Mathematical Olympiad · IMO

Let ABCABC and ABCA'B'C' be two triangles having the same circumcircle ω\omega, and the same orthocentre HH. Let Ω\Omega be the circumcircle of the triangle determined by the lines AAAA', BBBB', and CCCC'. Prove that HH, the centre of ω\omega, and the centre of Ω\Omega are collinear.
(Denmark)

This one wants a proof. Work it on paper, then read the official solution and mark yourself. Be honest about it: the record is only any use to you if it is.

Official solution

In what follows, \Varangle(p,q)\Varangle(p, q) will denote the directed angle between lines pp and qq, taken modulo 180180^\circ. Denote by OO the centre of ω\omega. In any triangle, the homothety with ratio 12-\frac{1}{2} centred at the centroid of the triangle takes the vertices to the midpoints of the opposite sides and it takes the orthocentre to the circumcentre. Therefore the triangles ABCABC and ABCA'B'C' share the same centroid GG and the midpoints of their sides lie on a circle ρ\rho with centre on OHOH. We will prove that ω\omega, Ω\Omega, and ρ\rho are coaxial, so in particular it follows that their centres are collinear on OHOH.

Let D=BBCCD = BB' \cap CC', E=CCAAE = CC' \cap AA', F=AABBF = AA' \cap BB', S=BCBCS = BC' \cap B'C, and T=BCBCT = BC \cap B'C'. Since DD, SS, and TT are the intersections of opposite sides and of the diagonals in the quadrilateral BBCCBB'CC' inscribed in ω\omega, by Brocard's theorem triangle DSTDST is self-polar with respect to ω\omega, i.e. each vertex is the pole of the opposite side. We apply this in two ways.

Figure 1

First, from DD being the pole of STST it follows that the inverse DD^* of DD with respect to ω\omega is the projection of DD onto STST. In particular, DD^* lies on the circle with diameter SDSD. If NN denotes the midpoint of SDSD and RR the radius of ω\omega, then the power of OO with respect to this circle is ON2ND2=ODOD=R2ON^2 - ND^2 = OD \cdot OD^* = R^2. By rearranging, we see that ND2ND^2 is the power of NN with respect to ω\omega.

Second, from TT being the pole of SDSD it follows that OTOT is perpendicular to SDSD. Let MM and MM' denote the midpoints of BCBC and BCB'C'. Then since OMBCOM \perp BC and OMBCOM' \perp B'C', it follows that OMMTOMM'T is cyclic and
\Varangle(SD,BC)=\Varangle(OT,OM)=\Varangle(BC,MM). \Varangle(SD, BC) = \Varangle(OT, OM) = \Varangle(B'C', MM').
From BBCCBB'CC' being cyclic we also have \Varangle(BC,BB)=\Varangle(CC,BC)\Varangle(BC, BB') = \Varangle(CC', B'C'), hence we obtain
\Varangle(SD,BB)=\Varangle(SD,BC)+\Varangle(BC,BB)=\Varangle(BC,MM)+\Varangle(CC,BC)=\Varangle(CC,MM). \begin{aligned} \Varangle(SD, BB') &= \Varangle(SD, BC) + \Varangle(BC, BB') \\ &= \Varangle(B'C', MM') + \Varangle(CC', B'C') = \Varangle(CC', MM'). \end{aligned}
Now from the homothety mentioned in the beginning, we know that MMMM' is parallel to AAAA', hence the above implies that \Varangle(SD,BB)=\Varangle(CC,AA)\Varangle(SD, BB') = \Varangle(CC', AA'), which shows that Ω\Omega is tangent to SDSD at DD. In particular, ND2ND^2 is also the power of NN with respect to Ω\Omega.

Additionally, from BBCCBB'CC' being cyclic it follows that triangles DBCDBC and DCBDC'B' are inversely similar, so \Varangle(BB,DM)=\Varangle(DM,CC)\Varangle(BB', DM') = \Varangle(DM, CC'). This yields
\Varangle(SD,DM)=\Varangle(SD,BB)+\Varangle(BB,DM)=\Varangle(CC,MM)+\Varangle(DM,CC)=\Varangle(DM,MM), \begin{aligned} \Varangle(SD, DM') &= \Varangle(SD, BB') + \Varangle(BB', DM') \\ &= \Varangle(CC', MM') + \Varangle(DM, CC') = \Varangle(DM, MM'), \end{aligned}
which shows that the circle DMMDMM' is also tangent to SDSD. Since NN, MM, and MM' are collinear on the Newton-Gauss line of the complete quadrilateral determined by the lines BBBB', CCCC', BCBC', and BCB'C, it follows that ND2=NMNMND^2 = NM \cdot NM'. Hence NN has the same power with respect to ω\omega, Ω\Omega, and ρ\rho.

By the same arguments there exist points on the tangents to Ω\Omega at EE and FF which have the same power with respect to ω\omega, Ω\Omega, and ρ\rho. The tangents to a given circle at three distinct points cannot be concurrent, hence we obtain at least two distinct points with the same power with respect to ω\omega, Ω\Omega, and ρ\rho. Hence the three circles are coaxial, as desired.

Source: MathNet, licensed CC-BY-4.0. Statement and solution reproduced as published; topic, difficulty and ordering added by this site.