Maths Olympiad Prep

Track / Stage 6 / 369 of 400 #1369 of 1964

Problem 1369

National Olympiad, first round
Geometry Difficulty 6.4 Prove it

G7. Let ABCA B C and A′B′C′A^{\prime} B^{\prime} C^{\prime} 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 AA′,BB′A A^{\prime}, B B^{\prime} and CC′C C^{\prime}. Prove that HH, the centre of ω\omega, and the centre of Ω\Omega are collinear.

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.

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Official solution

Solution. In what follows, x(p,q)x(p, q) will denote the directed angle between lines pp and qq, taken modulo 180∘180^{\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 ABCA B C and A′B′C′A^{\prime} B^{\prime} C^{\prime} share the same centroid GG and the midpoints of their sides lie on a circle ρ\rho with centre on OHO H. We will prove that ω,Ω\omega, \Omega, and ρ\rho are coaxial, so in particular it follows that their centres are collinear on OHO H.

Let D=BB′∩CC′,E=CC′∩AA′,F=AA′∩BB′,S=BC′∩B′CD=B B^{\prime} \cap C C^{\prime}, E=C C^{\prime} \cap A A^{\prime}, F=A A^{\prime} \cap B B^{\prime}, S=B C^{\prime} \cap B^{\prime} C, and T=BC∩B′C′T=B C \cap B^{\prime} C^{\prime}. Since D,SD, S, and TT are the intersections of opposite sides and of the diagonals in the quadrilateral BB′CC′B B^{\prime} C C^{\prime} inscribed in ω\omega, by Brocard's theorem triangle DST 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.

First, from DD being the pole of STS T it follows that the inverse D∗D^{*} of DD with respect to ω\omega is the projection of DD onto STS T. In particular, D∗D^{*} lies on the circle with diameter SDS D. If NN denotes the midpoint of SDS D and RR the radius of ω\omega, then the power of OO with respect to this circle is ON2−ND2−OD⋅OD∗−R2O N^{2}-N D^{2}-O D \cdot O D^{*}-R^{2}. By rearranging, we see that ND2N D^{2} is the power of NN with respect to ww.

Second, from TT being the pole of SDS D it follows that OTO T is perpendicular to SDS D. Let MM and M′M^{\prime} denote the midpoints of BCB C and B′C′B^{\prime} C^{\prime}. Then since OM⊥BCO M \perp B C and OM′⊥B′C′O M^{\prime} \perp B^{\prime} C^{\prime} it follows that OMM′TO M M^{\prime} T is cyclic and
x(SD,BC)−x(OT,OM)−x(B′C′,MM′). x(S D, B C)-x(O T, O M)-x\left(B^{\prime} C^{\prime}, M M^{\prime}\right) .

From BB′CC′B B^{\prime} C C^{\prime} being cyclic we also have x(BC,BB′)−x(CC′,B′C′)x\left(B C, B B^{\prime}\right)-x\left(C C^{\prime}, B^{\prime} C^{\prime}\right), hence we obtain
x(SD,BB′)=x(SD,BC)+x(BC,BB′)=x(B′C′,MM′)+x(CC′,B′C′)−x(CC′,MM′). \begin{aligned} x\left(S D, B B^{\prime}\right) & =x(S D, B C)+x\left(B C, B B^{\prime}\right) \\ & =x\left(B^{\prime} C^{\prime}, M M^{\prime}\right)+x\left(C C^{\prime}, B^{\prime} C^{\prime}\right)-x\left(C C^{\prime}, M M^{\prime}\right) . \end{aligned}

Now from the homothety mentioned in the beginning, we know that MM′M M^{\prime} is parallel to AA′A A^{\prime}, hence the above implies that (S D, B B )- * (C C , A A )\text{(S D, B B )- * (C C , A A )}, which shows that Ω\Omega is tangent to SDS D at DD. In particular, ND2N D^{2} is also the power of NN with respect to Ω\Omega.

Additionally, from BB′CC′B B^{\prime} C C^{\prime} being cyclic it follows that triangles DBCD B C and DC′B′D C^{\prime} B^{\prime} are inversely similar, so x(BB′,DM′)−x(DM,CC′)x\left(B B^{\prime}, D M^{\prime}\right)-x\left(D M, C C^{\prime}\right). This yields
x(SD,DM′)=x(SD,BB′)+x(BB′,DM′)=x(CC′,MM′)+x(DM,CC′)−x(DM,MM′), \begin{aligned} x\left(S D, D M^{\prime}\right) & =x\left(S D, B B^{\prime}\right)+x\left(B B^{\prime}, D M^{\prime}\right) \\ & =x\left(C C^{\prime}, M M^{\prime}\right)+x\left(D M, C C^{\prime}\right)-x\left(D M, M M^{\prime}\right), \end{aligned}
which shows that the circle DMM′D M M^{\prime} is also tangent to SDS D. Since N,MN, M, and M′M^{\prime} are collinear on the Newton-Gauss line of the complete quadrilateral determined by the lines BB′,CC′,BC′B B^{\prime}, C C^{\prime}, B C^{\prime}, and B′CB^{\prime} C, it follows that ND2−NM⋅NM′N D^{2}-N M \cdot N M^{\prime}. 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,Ω\omega, \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,Ω\omega, \Omega, and ρ\rho. Hence the three circles are coaxial, as desired.

Comment 1. Instead of invoking the Newton-Gauss line, one can also use a nice symmetry argument: If from the beginning we swapped the labels of B′B^{\prime} and C′C^{\prime}, then in the proof above the labels of DD and SS would be swapped while the labels of MM and M′M^{\prime} do not change. The consequence is that the circle SMM′S M M^{\prime} is also tangent to SDS D. Since NN is the midpoint of SDS D it then has the same power with respect to circles DMM′D M M^{\prime} and SMM′S M M^{\prime}, so it lies on their radical axis MM′M M^{\prime}.

Comment 2. There exists another triple of points on the common radical axis of ω,Ω\omega, \Omega, and ρ\rho which can be used to solve the problem. We outline one such solution.

Let LL and L′L^{\prime} denote the feet of the altitudes from AA and A′A^{\prime} in triangle ABCA B C and A′B′C′A^{\prime} B^{\prime} C^{\prime}, respectively. Since ρ\rho is the nine-point circle of the two triangles it contains both LL and L′L^{\prime}. Furthermore, HA⋅HLH A \cdot H L and HA′⋅HL′H A^{\prime} \cdot H L^{\prime} both equal twice the power of HH with respect to ρ\rho, so A,A′,L,L′A, A^{\prime}, L, L^{\prime} are concyclic as well.

Now let ℓ=AA′\ell=A A^{\prime} and denote P=LL′∩ℓ,K=BC∩ℓP=L L^{\prime} \cap \ell, K=B C \cap \ell, and K′=B′C′∩ℓK^{\prime}=B^{\prime} C^{\prime} \cap \ell. As MM′∥ℓM M^{\prime} \| \ell (shown in the previous solution) and LL′MM′L L^{\prime} M M^{\prime} is cyclic
(B C, )= (B C, M M )= (L L , B C )\text{(B C, )= (B C, M M )= (L L , B C )}
so K,K′,LK, K^{\prime}, L, and L′L^{\prime} are also concyclic. From the cyclic quadrilaterals AA′LL′A A^{\prime} L L^{\prime} and KK′LL′K K^{\prime} L L^{\prime} we get PA⋅PA′=PL⋅PL′=PK⋅PK′P A \cdot P A^{\prime}=P L \cdot P L^{\prime}=P K \cdot P K^{\prime}. This implies that PP is the centre of the (unique) involution σ\sigma on ℓ\ell that swaps A,A′A, A^{\prime} and K,K′K, K^{\prime}. On the other hand, by Desargues' involution theorem applied to the line ℓ\ell, the quadrilateral BB′CC′B B^{\prime} C C^{\prime}, and its circumcircle ω\omega, the involution σ\sigma also swaps EE and FF. Hence
PA⋅PA′=PL⋅PL′=PE⋅PF.  P A \cdot P A^{\prime}=P L \cdot P L^{\prime}=P E \cdot P F \text {. }

However, this means that PP has the same power with respect to ω,Ω\omega, \Omega, and ρ\rho, and by the same arguments there exist points on BB′B B^{\prime} and CC′C C^{\prime} with this property.

Source: NuminaMath-1.5, licensed Apache-2.0. Statement reproduced verbatim; metadata (topic, difficulty, ordering) added by this project.