The incentral circumconics

Contents

The incentral circumconic
Properties
Construction of axes
Points
The projective map
Point table
Locus definition
Extraversions
Perspectors and Centers

updated: 10-20-06

The incentral circumconic is the isotomic conjugate of the dual of Io, the incenter, with perspector Io. It is a weak conic, coming in four versions, one each generated by ~Ix (x = o,a,b,c), the dual lines of the 4 incenters.

Floor van Lamoen calls this the "billiard conic" since the triangle ABC follows a billiard path. This is true of all 4 conics.

These conics are weakened versions of the circumcircle. We present the Io circumconic as an intermediate case between the Steiner ellipse and the circumcircle.

Notation is here. Generating circumconics as the isotomic conjugate of a line is part of the affine theory of triangle conics.

Figure: The Io-circumconic showing the conic, perspector Io, center Mo, its axes and some points on it. The notation 162o indicates the original version (of 4) for X162, found in the Encyclopedia of Triangle Centers (ETC). The other versions of this point are each on other versions of the conic. The conic is tangent to the exCevian lines of Io at the vertices. The axes are light green lines and are parallel to the asymptotes of the Feuerbach hyperbola.

The "weakened" operation

If the coordinate representation of an object is a function of the squares of the edgelenghs, the substitution b2 –> b, etc,. is known as "weakening" the equation. This operation is outside most traditional triangle geometry and preserves affine and projective properties. It is not usually one to one. Its inverse is called "strengthening."

Properties of the 4 Ix-circumconics

1. The perspector of the central version is Io , which being inside the Steiner ellipse, means it is always an ellipse. The excenters are the perspectors of the other 3, and being outside the Steiner ellipse, are always hyperbolae. The central equation is

a/x + b/y + c/z = 0

This conic is the weakened form of the circumcircle and, as such, shares many of its properties. Since the incenter is always inside the Steiner inellipse, this conic is always an ellipse. The perspector Io has the special algebraic property that its extraversions are the same as its ex-versions, often called harmonic associates. This fact is important below.

2. The four centers are the Mittenpunkts Mx = mtd Ix (x = o,a,b,c).

The Mittenpunkt and its extraversions are desmic. The IxMx lines concur at K.

3. Its tangents at the vertices are the ex-Cevian lines of Ix and analogously for the other versions. The Cevian lines of the Ix are the angle bisectors, two per vertex, making 6, which meet, two at a time, at the triangle edges and 3 at a time at the 4 incenters. The effect of this is that these conics are tangent to eachother, two at each vertex.

Proof: ayz + bzx + cxy = z(ay+bx) + cxy = 0. Since the last term intersects the conic at C twice and z = 0 does not, the factor ay+bx must have a double intersection and hence be the tangent. This is an ex-Cevian line of Io.

4. The axes are parallel to those of the Kiepert hyperbola; also the Mo circumconic and Mo inconic.

4. Its dual is the tIo inconic, an ellipse with center So = mIo.

5. Its switched conics, an ellipse and three hyperbolas, switches the center and perspector, and has perspector Mo and center Io. Its equation is

asa/x + bsb/y + csc/z = 0.

It is generated as the isotomic conjugate of the dual of the Mittenpunkt.

The axes of circumconics whose perspectors are on a line through K are parallel. Hence the axes of the Mx and Ix circumconics are parallel.

6. Its fourth intersection with the Steiner ellipse is wS = 190o = : 1/(c–a) :, a weakened Steiner point, and with the circumcircle wF = 100o = : b/(c–a) :, a weakened Focus point. They have no fourth intesections with eachother, since each is tangent to one of the others at a vertex, making a double intersection there.

Since the incenter, the mittenpunkt, and the symmedian point are colinear, their duals meet at the same point. In conics-world this means that the Io circumconic, the Mo circumconic, and the circumcircle (the K circumconic) meet at the same point as seen in the following picture.

Construction of the axes

 

Points on Io circumconic

Peter Moses has found the ETC points on the original version of this conic. All are weak points except for the last two, which are related to the Euler intersections with the circumcircle. This was a pleasing case where the ETC was almost all information with little noise. It is also a case where the discovered points coincide well with the points the affine theory generates. Point number in red are weak points (almost all of them), green indices fissile or 8-fold. Lightened points are ones that I think should be ignored. I have placed the second barycentric coordinate after each X-number.

[PM] incentral circumconic, center 9, perspector 1
{
88 b/(c+a–2b), 100 b/(c–a), 162 b/(c2–a2)SB, 190 1/(c–a) , 651 b/(c–a)sb, 653 1/(c–a)sbSB, 655 1/(c–a)sb(4SBB–c2a2) , 658 1/(c–a)sbb, 660 b/(c–a)(b2–ca), 662 b/(c2–a2), 673 1/(c2+a2–ab–bc), 771 , 799 1/b(c2–a2), 823 1/b(c2–a2)SBB, 897 b/(c2+a2–2b2) , 1156, 1492 b/(c–a)(c2+a2+ac),1821 1/bSB2– , 2349 ,2580,2581}

[PM again] let J = OH / R then
X(2580) = a (J–1) SA + 2 SBC /a :: (= X(1113)/a)
X(2581) = a (J + 1) SA – 2 SB SC/a :: (= X(1114)/a)

These points surprisingly turn out to be easy to understand, so here is a little tutorial on centers on a conic curve.

Step 1: We begin with the centers on the line at infinity. These divide into groups, originating with the famous triangle centers. The incenter has its points at infinity, the orthocenter has its points at infinity, and so on. These groups are colored in the chart below.

Step 2: The isotomic conjugate of a point on the line at infinity is on the Steiner circumellipse. These points divide into groups of points associated with triangle centers just as the line at infinity did. The relation of the line at infinity to the Steiner ellipse is grounded in affine invariance.

Step 3: Use the perspector P of a second circumconic to implement the projective map ABCG –> ABCP. Algebraically this map is equivalent to barycentric multiplication by P. Geometrically its implementation is given below. Points on the new circumconic are thus divided into groups associated with triangle centers just as the line at infinity and the Steiner ellipse were.

The view that the structure of the triangle itself is reflected in the distribution of points on a conic is a very heady and pleasing one.

Points originate on the line at infinity and percolate down to the conics through the mechanism of the Steiner ellipse. Hence all conics have contributions from all centers in the plane of the triangle. These families are shown as colors on the following table.

The geometry of this projective mapping.

A point on the line at infinity can be mapped to the Steiner ellipse by the isotomic conjugate. This point can be mapped to the Io-circumellipse using this projective map :y: –> :by: . This same map takes the Io-circumconic to the circumcircle. We call this the Io projective map, since it takes ABCG to ABCIo.

The fourth intersection of two conics allows us to easily implement the mapping of a point from one conic to the other. Simply draw a line from the 4th intersetion through the desired point. The second intersection with the other conic is the projected point. This picture shows the projection from the G-circumconic, the Steiner ellipse, to the Io-circumconic (and vice-versa) and the circumcircle. Numbers like 673o refer to the original version (of 4) of the quartile point X673. There are two projection centers 190o for the Steiner to Io projection and 100o for the Io to circumcircle one.

The following table shows how easy and effective this point generation process is. Each box lists a point, giving its second coordinate and the ETC X-number (if known) in red. Below it is the name of the point and/or the affine invarient constructive notation. The green section represents points that are derived from Io. The orange section, those from the Gergonne point Go. Blue from the symmedian point and purple from the orthocenter.

What is demonstrated here is the easy relation between points on infinity and these three conics and among the conics themselves. There is an equal number of significant points on each. We can also see how various points of the geometry plane contribute to points on the objects of the plane.

The Io-circumconic can be seen to be an intermediate case between the Steiner ellipse and the circumcircle. The motion of a point from Steiner ellipse, to Io-Circumconic, to circumcircle is what I have elsewhere termed an "orbit."

The red mark at the right of a row indicates a point not in the above list of Peter's from ETC.

line at infinity
Steiner ellipse
Io-Circumconic
Circumcircle
(:m:)
(:1/m:)
(:b/m:)
(:b2/m:)
From the Incenter
514 c–a
twS =
∞•~Io
190 1/(c–a)
wS = t(
∞•~Io)
100 b/(c–a)
wF intersection
with circumcircle
101 b2/(c–a)
519 c+a–2b
∞•(G—Io)
903 1/(c+a–2b)
t(
∞•(G—Io))
88 b/(c+a–2b)
106 b2/(c+a–2b)
513 b(c–a)
∞•~tIo
668 1/b(c–a)
t(
∞•~tIo)
190 1/(c–a)
wS
100 b/(c–a)
wF = focus of Yff parabola
900 (c–a)(c+a–2b)
(
∞•~190o)
t900 1/(c–a)(c+a–2b)
t(
∞•~190o)
? b/(c–a)(c+a–2b)
901 b2/(c–a)(c+a–2b)
812 (c–a)(b2–ca)
? 1/(c–a)(b2–ca)
660 b/(c–a)(b2–ca)
813 b2/(c–a)(b2–ca)
? (c+a)(b2–ca)
∞•(Io—tIo)
? 1/(c+a)(b2–ca)
t(
∞•(Io—tIo))
g2238 b/(c+a)(b2–ca)
? b2/(c+a)(b2–ca)
g(
∞•(Io—tIo))
(a2–bc+c2–ab)(c–a)
? b(c2+a2–ab–bc)
? 1/b(c2+a2–ab–bc)
673 1/(c2+a2–ab–bc)
wT
105 b/(c2+a2–ab–bc)
? b(c–a)sbb,
? 1/b(c–a)sbb,
658 1/(c–a)sbb,
? b/(c–a)sbb,
From the Gergonne point
also the Mittenpunkt
g109 (c–a)sb
∞•~Go
r109 1/(c–a)sb
651 b/(c–a)sb
109 b2/(c–a)sb
? csc+asa–2bsb
∞•(G—Go)
? 1/(csc+asa–2bsb)
t(
∞•(G—Go))
? b/(csc+asa–2bsb)
? b2/(csc+asa–2bsb)
From the Symmedian point
523 c2–a2
tS =
∞•~K
99 1/(c2–a2)
t(
∞•~K)
the Steiner point
662 b/(c2–a2)
110 b2/(c2–a2)
the focus of the Kiepert Parabola
524 c2+a2–2b2
∞•(G—K)
671 1/(c2+a2–2b2)
t(
∞•(G—K))
897 b/(c2+a2–2b2)
111 b2/(c2+a2–2b2)
isogonal of G—K endpoint
512 b2(c2–a2)
gS =
∞•~tK
670 1/b2(c2–a2)
rS = t(
∞•~tK)
799 1/b(c2–a2)
t of Io–Mineur conic perspector
99 1/(c2–a2)
Steiner point
g98 b2SB2–
gT
r98 1/b2SB2–
rT
1821 1/bSB2–
98 1/SB2–
Tarry point T
From the Orthocenter
also the Circumcenter
? (c2–a2)SB
∞•~H = ∞•~O
? 1/(c2–a2)SB
162 b/(c2–a2)SB
? b2/(c2–a2)SB
30 SBC+SAB–2SCA
∞•(G—H)
infinite point on Euler line
1494 1/(SBC+SAB–2SCA)
isotomic of Euler endpoint
b/(SBC+SAB–2SCA)
74 b2/(SBC+SAB–2SCA)
isotomic of Euler endpoint
? b2(c2–a2)SBB
? 1/b2(c2–a2)SBB
823 1/b(c2–a2)SBB
? 1/(c2–a2)SBB
Fissile points
r1113, r1114 b2(J–1)SB+2bSCA
D–tO meets Steiner ellipse
2580,2581 b (J–1) SB+2SCA / b
Wo—tWo meets Io circumonic
1113,1114 b (J–1) SB + 2 SCA Euler meets circumcircle
not so sure what to make of these
? b(c–a)sb(4SBB–c2a2)
? 1/b(c–a)sb(4SBB–c2a2)
655 1/(c–a)sb(4SBB–c2a2)
b/(c–a)sb(4SBB–c2a2)
1492 b/(c–a)(c2+a2+ac)

Locus property

If a point is on an Ix-circumconic, the Newton line of its Cevian quadrilateral is tangent to the circumcircle.

All four circumconics

These conics are generated as the isotomic conjugates of ~Ix, the duals of the four incenters. These four lines intersect 6 times, two on each triangle edge, a given line meeting each of the others at a different edge. These conics only intersect at vertices.The fourth intersections of the conics are double intersections at a vertex. Each conic is tangent to the the 3 others, each at a different vertex.

Since each conic is tangent to an internal or external bisector at a vertex, and since at a vertex these bisectors are perpendicular, these conics meet orthogonally or parallelly at the vertices, each conic being orthogonal to two and parallel to one.

The endpoints of the lines map onto the intersections of these conics with the Steiner ellipse.

Figure: Each version of the 4 Ix-circumconics is given a different color. The 4 generating lines, the duals of the Ix, are shown dashed. The points are shown in all versions of these conics. The quartile points are shown, each on its version of the conic.

Perspectors and Centers

The perspectors are the extraversions of Io = (:b:) which are harmonic associates as shown in the picture below. The harmonic associates are one each in each region of the plane; hence only one perspector can be inside the triangle and inside the Steiner inellipse. Hence it is only possible for one conic to be an ellipse.

The lines IxMx concur at K.

The ~Io lines meet at the traces of the isotomic conjugates of the perspectors.

The centers are the Mittenpunkts, obtained by operations mtd of the perspectors, an harmonic set of 4, which guarantees that they will be desmic . Here Mabc = : b/sb : is the desmic mate of Mo = : b sb : .