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Forum Geometricorum Volume 6 (2006) 263–268.

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FORUM GEOM ISSN 1534-1178

A Note on the Barycentric Square Roots of Kiepert Perspectors Khoa Lu Nguyen

Abstract. Let P be an interior point of a given triangle ABC. We prove that the orthocenter of the cevian triangle of the barycentric square root of P lies on the Euler line of ABC if and only if P lies on the Kiepert hyperbola.

1. Introduction In a recent Mathlinks message, the present author proposed the following problem. Theorem 1. Given an acute √ triangle ABC with orthocenter H, the orthocenter H  of the cevian triangle of H, the barycentric square root of H, lies on the Euler line of triangle ABC. A

√ H

H

O

H

B

C

Figure 1.

Paul Yiu has subsequently discovered the following generalization. Theorem 2. The locus of point√P for which the orthocenter of the cevian triangle of the barycentric square root P lies on the Euler line is the part of the Kiepert hyperbola which lies inside triangle ABC. Publication Date: October 30, 2006. Communicating Editor: Paul Yiu. The author is grateful to Professor Yiu for his generalization of the problem and his help in the preparation of this paper.

264

K. L. Nguyen

The barycentric square root is defined only for interior points. This is the reason why we restrict to acute angled triangles in Theorem 1 and to the interior points on the Kiepert hyperola in Theorem 2. It is enough to prove Theorem 2. 2. Trilinear polars Let A B  C  be the cevian triangle of P , and A1 , B1 , C1 be respectively the intersections of B C  and BC, C  A and CA, A B  and AB. By Desargues’ theorem, the three points A1 , B1 , C1 lie on a line P , the trilinear polar of P . A

C B

A1

P

B

A

C

B1 C1

Figure 2.

If P has homogeneous barycentric coordinates (u : v : w), then the trilinear polar is the line z x y + + = 0. P : u v w For the orthocenter H = (SBC : SCA : SAB ), the trilinear polar H :

SA x + SB y + SC z = 0.

is also called the orthic axis. Proposition 3. The orthic axis is perpendicular to the Euler line. This proposition is very well known. It follows easily, for example, from the fact that the orthic axis H is the radical axis of the circumcircle and the nine-point circle. See, for example, [2, §§5.4,5]. The trilinear polar P and the orthic axis H intersect at the point (u(SB v − SC w) : v(SC w − SA u) : w(SA u − SB v)). In particular, P and H are parallel, i.e., their intersection is a point at infinity if and only if u(SB v − SC w) + v(SC w − SA u) + w(SA u − SB v) = 0. Equivalently, (SB − SC )vw + (SC − SA )wu + (SA − SB )uv = 0.

(1)

A note on the barycentric square roots of Kiepert perspectors

265

Note that this equation defines the Kiepert hyperbola. Points on the Kiepert hyperbola are called Kiepert perspectors. Proposition 4. The trilinear polar P is parallel to the orthic axis if and only if P is a Kiepert perspector. 3. The barycentric square root of a point Let P be a point inside triangle ABC, with homogeneous barycentric coordinates (u : v : w). We may the barycentric square √ assume u, v, w > 0, and define √ √ √ ( u : v : w). root of P to be the point P with barycentric coordinates √ Paul Yiu [2] has given the following construction of P . (1) Construct the circle CA with BC as diameter. (2) Construct the perpendicular to BC at the trace A of P to intersect CA at X  .  (3) Construct the bisector √ of angle BX C to intersect BC at X. on BC. Similar constructions on the other two sides Then X is the trace of P √ P on CA and AB respectively. The barycentric give the traces Y and Z of √ square root P is the common point of AX, BY , CZ. Proposition 5. If the trilinear polar P intersects BC at A1 , then A1 X 2 = A1 B · A1 C. Proof. Let M is the midpoint of BC. Since A1 , A divide B, C harmonically, we have M B 2 = M C 2 = M A1 · M A (Newton’s theorem). Thus, M X2 = M A1 · M A . It follows that triangles M X A1 and M A X  are similar, and ∠M X  A1 = ∠M A X  = 90◦ . This means that A1 X  is tangent at X  to the circle with diameter BC. Hence, A1 X 2 = A1 B · A1 C. A

X

P

A1

B

Figure 3.

A X M

C

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K. L. Nguyen

To complete the proof it is enough to show that A1 X = A1 X  , i.e., triangle A1 XX  is isosceles. This follows easly from ∠A1 X  X =∠A1 X  B + ∠BX  X =∠X  CB + ∠XX  C =∠X  XA1 .  Corollary 6. If X1 is the intersection of Y Z and BC, then A1 is the midpoint of XX1 . Proof. If X1 is the intersection of Y Z and BC, then X, X1 divide B, C harmonically. The circle through X, X1 , and with center on BC is orthogonal to the circle CA . By Proposition 5, this has center A1 , which is therefore the midpoint of  XX1 . 4. Proof of Theorem 2 Let P be an interior point √ of triangle ABC, and XY Z the cevian triangle of its barycentric square root P . Proposition 7. If H  is the orthocenter of XY Z, then the line OH is perpendicular to the trilinear polar P . Proof. Consider the orthic triangle DEF of XY Z. Since DEXY , EF Y Z, and F DZX are cyclic, and the common chords DX, EY , F Z intersect at H , H  is the radical center of the three circles, and H  D · H  X = H  E · H  Y = H  F · H  Z.

(2)

Consider the circles ξA , ξB , ξC , with diameters XX1 , Y Y1 , ZZ1 . These three √ circles are coaxial; they are the generalized Apollonian circles of the point P . See [3]. As shown in the previous section, their centers are the points A1 , B1 , C1 on the trilinear polar P . See Figure 4. Now, since D, E, F lie on the circles ξA , ξB , ξC respectively, it follows from (2) that H  has equal powers with respect to the three circles. It is therefore on the radical axis of the three circles. We show that the circumcenter O of triangle ABC also has the same power with respect to these circles. Indeed, the power of O with respect to the circle ξA is A1 O2 − A1 X 2 = OA21 − R2 − A1 X 2 + R2 = A1 B · A1 C − A1 X 2 + R2 = R2 by Proposition 5. The same is true for the circles ξB and ξC . Therefore, O also lies on the radical axis of the three circles. It follows that the line OH is the radical axis of the three circles, and is perpendicular to the line P which contains their centers.  The orthocenter H  of XY Z lies on the Euler line of triangle ABC if and only if the trilinear polar P is parallel to the Euler line, and hence parallel to the orthic axis by Proposition 3. By Proposition 4, this is the case precisely when P lies on the Kiepert hyperbola. This completes the proof of Theorem 2.

A note on the barycentric square roots of Kiepert perspectors

267

B1

A

Y D

Z P



A1

B

O

H F

E X1

P

X

C

C1

Z1

Figure 4.

√ Theorem 8. The orthocenter of the cevian triangle of P lies on the Brocard axis if and only if P is an interior point on the Jerabek hyperbola. Proof. The Brocard axis OK is orthogonal to the Lemoine axis. The locus of points whose trilinear polars are parallel to the Brocard axis is the Jerabek hyperbola. 

5. Coordinates In homogeneous barycentric coordinates, the orthocenter of the cevian triangle of (u : v : w) is the point

268

K. L. Nguyen





1 1 SB + w u  : ··· : ··· .



 + SC

1 1 + u v

 

 −SA

1 1 + v w

2

 + SB

1 1 − 2 u2 w



 + SC

1 1 − 2 u2 v



2 2 2  to the square root of the orthocenter, with (u : v : w ) =  Applying this 1 1 1 SA : SB : SC , we obtain  

a2 SA · SABC + SBC a2 SA : · · · : · · ·  , cyclic

H

in Theorem 1. which is the point More generally, if P is the Kiepert perspector   1 1 1 K(θ) = : : , SA + Sθ SB + Sθ SC + Sθ √ the orthocenter of the cevian triangle of P is the point 

a2 SA (SA + Sθ )(SB + Sθ )(SC + Sθ ) +SBC

cyclic

a2



SA + Sθ + a2 Sθ



SA





SA + Sθ : · · · : · · ·  .

cyclic

References [1] R. A. Johnson, Advanced Euclidean Geometry, 1925, Dover reprint. [2] P. Yiu, Introduction to the Geometry of the Triangle, Florida Atlantic University lecture notes, 2001. [3] P. Yiu, Generalized Apollonian circles, Journal of Geometry and Graphics, 8 (2004) 225–230. Khoa Lu Nguyen: Massachusetts Institute of Technology, student, 77 Massachusetts Avenue, Cambridge, MA, 02139, USA E-mail address: [email protected]

A Note on the Barycentric Square Roots of Kiepert ...

Oct 30, 2006 - The trilinear polar lP and the orthic axis lH intersect at the point. (u(SBv − SCw) : v(SCw − SAu) : w(SAu − SBv)). In particular, lP and lH are parallel, i.e., their intersection is a point at infinity if and only if u(SBv − SCw) + v(SCw − SAu) + w(SAu − SBv)=0. Equivalently,. (SB − SC)vw + (SC − SA)wu + (SA ...

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