Therefore, It Appears That Aiyars Theorem Is Also to Be Men- Tioned Elementarily, and It May Be Stated As Follows

Total Page:16

File Type:pdf, Size:1020Kb

Therefore, It Appears That Aiyars Theorem Is Also to Be Men- Tioned Elementarily, and It May Be Stated As Follows Elementary Modifications of Rogers' and Alyar's Theorems, Takashi byHAMADA, Urawa. Several geometricians have generalized Feuerbach's theorem, since it was found out more than one hundred years ago. I have also proved its simple extension(1.). Theorem I. A triangle A1A2A3and a point P are given in a plane. Let L1,L2; L3 be the middle points of the sides of A1A2A3and let PM1,PM2, PM3 be the perpendiculars on them. Let a circle S cut the three circles Wthogonally, whose centres are L1, L2, .L3. and their radii L1M1, L2M2, .,Gelds respectively. Then, the circle S touches the nine-point circle of A1A2A3. Moreover, if the radius of S and the distance between , O (the circum-centre of A1A2A3) and P .be denoted by r and ƒÂ respectively, then we have `' Hereby R denotes the• radius of. the circumcircle of A1A2A3.It: is evident that the former part of the theorem is. an extension of Feuerbach's theorem. The latter part is regarded as an extention of Chappel's rela- tion. I saw that this theorem (the former part) is, however, no other than an elementary modification of Rogers' extension of Feuerbach's theorem. And Rogers' theorem is proved geometr ically by the application of Aiyar,s theorem, so we may treat the former as a special case of the latter. Therefore, it appears that Aiyars theorem is also to be men- tioned elementarily, and it may be stated as follows. Theorem, II. A triangle A1A2A3and a line x are given in a,,plane. From any two points P, Q .on x draw perpendiculars PM1,PM2, (1) Tokyo BatsurigakkO Zaashi, No. 561. MODIFCATIONSOFROE ERfS' AND AIYAWS THEOREMS. PM3 and QN1,QN2,QN3 on the sides of A1A2A3respectively. There exists a circle S which cuts three ' eircles, whose centres are N1,N2,N3 and their radii respectively N1M1,N2M2, N3M3,ortho- gonally. Then, Scuts the ortho-polar circle of x with respect to A1A2A3 orthogonally. I was not able to prove Theorem II purely geometrically. But, for. the proof, the following matter is. only. to be shown. The line x cuts the circle Sin Y, Z. From Y and Z draw per-. pendiculars y. and z respectively. Then the 'conic that touches the sides of A1A2A3 and y, z should have the same centre as S, for S must be the joint-director circle of this conic and its confocal conic touching x. I proved the theorem by means of orthogonal coordinates. Proof of Theorem .II. Let the line x be x-axis of orthogonal coordinates and let PQ=m, Q (L,0).(i=1,2,3). Let' ƒ¿ be the angle at which QN1 in- tersects x-axis. hen,T M1M1 is equal to msinƒ¿1, and the equations of A1Ak and QN1, are, A1Ak: (1). (2) The coordinates of N1 are derived from (1) (2). (3) The circle S, cuts these three circles (3) orthogonally. (4) (The second row in the determinant in (4) represents rows from 118 TAKASHI HAMADA Fig. 1. Fig. 6. the second to the fourth). The determinant in (4) is divided into two parts as follows: MODIFICATIONSOF , ROGERS' AND OIYAR'S THEOREMS. 117 (5) Let l 'be fixed and m change, that is, let. Q fix and P move on x Then, S forms a coaxalsystem. This,follows immediately from the form of (5). If we make m infinitely great, then we have the egtia tion of the radical axis of the, system, andit is what the first term in (5) equated to zero: (6) The determinant in (6) is divided into two as follows : (7) The first term in (7) is equal to zero, for its first two columns are equal. The `second term is divided-into two as follows:, (8) (8) is the equation of the radical axis of the system obtained from (6). Finally, let l vary or let Q vary on x, then (8) forms a pencil of rays. The centre of this pencil is the orthopole T of x with respect to A1A2A3.For, if Q coincides with one of the poiits Q1,02 of intersection of x and the circumcircle of A1A2A3,the coaxal systems correspondingto Q1,Q2,have the Simson lines of Qi,Q2 with respect to, A1A2A3as their radical axes respectively. But it is known that such Simson lines intersect at the ortho- pole T of x with respect to A1A2A3.Therefore, the centre of the pencil is the orthopole T of x Moreover,the pedal, circles of all Q, as it is eapiiy.seen, belong to these systems. And these pedal circles cut the ortho-polar circle of x with respect to A1A2A3ortho- g6nally (Lemoyne'stheorem). Thus, it was proved that all circles which belongto the systems cut the ortho-polar circle of x orthogonally. Q.E.D. 118 HAMADA: ROGERS' AND AIYAR'S THEOREMS. It is evident that -this theorem coincides with Aiyar's, since there are •‡2 cirolep or •‡1 coaxal system generated by P, Q on x. That S forms a coaxal system when P moves and Q is fixed, is shown elementarily as follows:. Let P, P be two positions of P and let S, S1 be two circles cor- responding to P, P1 respectively. Let t1 t2 denote the lengths of tangents drawn to S, 81. from N1. Then we have hence, Therefore, N1 lies on a circle coaxal. with S and S, or the pedal circle N1N2N3of Q is coaxal with S and S'. If we take another point P" on x, we get a circle S" coaxal with N1N2N3and S. Therefore, it is shown that S, S', S" and the pedal circle N1N2N3 form a coaxal system. Q.E.D. What is called as Lemoyne's theorem, is the fact that the pedal circle N1N2N3of a point Q on x belongs to the system. If Q coincides with the circumcentre of A1A2A3,the orthopolar circle S of x reduces to a point T on the nine-point circle of A1A2A3. In this case the coaxal system generated by the variation of P (on OP) is parabolic, and it contains the nine-point circle. Thus Theorem I is obtained by the help of Theorem II. For reference, the original forms of Rogers' and Aiyar's their rems are the following. L. J. Rogers' Theorem. If a conic touches three sides of a triangle, its joint director circle with either confocal drawp through the circumcentre touches the nine-point circle Aiyar's Theorem. The ortho-polar circle of a line x, which touches a conic confocal with another conic touching. the three sides of a given triangle, with respect to the triangle cuts the joint-director circle of these two conics orthogonally. (Receivedthe 31th,January, 1942.) .
Recommended publications
  • A Generalization of the Conway Circle
    Forum Geometricorum b Volume 13 (2013) 191–195. b b FORUM GEOM ISSN 1534-1178 A Generalization of the Conway Circle Francisco Javier Garc´ıa Capitan´ Abstract. For any point in the plane of the triangle we show a conic that be- comes the Conway circle in the case of the incenter. We give some properties of the conic and of the configuration of the six points that define it. Let ABC be a triangle and I its incenter. Call Ba the point on line CA in the opposite direction to AC such that ABa = BC = a and Ca the point on line BA in the opposite direction to AB such that ACa = a. Define Cb, Ab and Ac, Bc cyclically. The six points Ab, Ac, Bc, Ba, Ca, Cb lie in a circle called the Conway circle with I as center and squared radius r2 + s2 as indicated in Figure 1. This configuration also appeared in Problem 6 in the 1992 Iberoamerican Mathematical Olympiad. The problem asks to establish that the area of the hexagon CaBaAbCbBcAc is at least 13∆(ABC) (see [4]). Ca Ca Ba Ba a a a a A A C0 B0 I I r Ab Ac Ab Ac b B s − b s − c C c b B s − b s − c C c c c Bc Bc Cb Cb Figure 1. The Conway circle Figure 2 Figure 2 shows a construction of these points which can be readily generalized. The lines BI and CI intersect the parallel of BC through A at B0 and C0.
    [Show full text]
  • Coaxal Pencil of Circles and Spheres in the Pavillet Tetrahedron
    17TH INTERNATIONAL CONFERENCE ON GEOMETRY AND GRAPHICS ©2016 ISGG 4–8 AUGUST, 2016, BEIJING, CHINA COAXAL PENCILS OF CIRCLES AND SPHERES IN THE PAVILLET TETRAHEDRON Axel PAVILLET [email protected] ABSTRACT: After a brief review of the properties of the Pavillet tetrahedron, we recall a theorem about the trace of a coaxal pencil of spheres on a plane. Then we use this theorem to show a re- markable correspondence between the circles of the base and those of the upper triangle of a Pavillet tetrahedron. We also give new proofs and new point of view of some properties of the Bevan point of a triangle using solid triangle geometry. Keywords: Tetrahedron, orthocentric, coaxal pencil, circles, spheres polar 2 Known properties We first recall the notations and properties (with 1 Introduction. their reference) we will use in this paper (Fig.1). • The triangle ABC is called the base trian- gle and defines the base plane (horizontal). The orthocentric tetrahedron of a scalene tri- angle [12], named the Pavillet tetrahedron by • The incenter, I, is called the apex of the Richard Guy [8, Ch. 5] and Gunther Weiss [16], tetrahedron. is formed by drawing from the vertices A, B and 0 0 0 C of a triangle ABC, on an horizontal plane, • The other three vertices (A ,B ,C ) form a three vertical segments AA0 = AM = AL = x, triangle called the upper triangle and define BB0 = BK = BM = y, CC0 = CL = CK = z, a plane called the upper plane. where KLM is the contact triangle of ABC. We As a standard notation, all points lying on the denote I the incenter of ABC, r its in-radius, base plane will have (as much as possible) a 0 0 0 and consider the tetrahedron IA B C .
    [Show full text]
  • Volume 6 (2006) 1–16
    FORUM GEOMETRICORUM A Journal on Classical Euclidean Geometry and Related Areas published by Department of Mathematical Sciences Florida Atlantic University b bbb FORUM GEOM Volume 6 2006 http://forumgeom.fau.edu ISSN 1534-1178 Editorial Board Advisors: John H. Conway Princeton, New Jersey, USA Julio Gonzalez Cabillon Montevideo, Uruguay Richard Guy Calgary, Alberta, Canada Clark Kimberling Evansville, Indiana, USA Kee Yuen Lam Vancouver, British Columbia, Canada Tsit Yuen Lam Berkeley, California, USA Fred Richman Boca Raton, Florida, USA Editor-in-chief: Paul Yiu Boca Raton, Florida, USA Editors: Clayton Dodge Orono, Maine, USA Roland Eddy St. John’s, Newfoundland, Canada Jean-Pierre Ehrmann Paris, France Chris Fisher Regina, Saskatchewan, Canada Rudolf Fritsch Munich, Germany Bernard Gibert St Etiene, France Antreas P. Hatzipolakis Athens, Greece Michael Lambrou Crete, Greece Floor van Lamoen Goes, Netherlands Fred Pui Fai Leung Singapore, Singapore Daniel B. Shapiro Columbus, Ohio, USA Steve Sigur Atlanta, Georgia, USA Man Keung Siu Hong Kong, China Peter Woo La Mirada, California, USA Technical Editors: Yuandan Lin Boca Raton, Florida, USA Aaron Meyerowitz Boca Raton, Florida, USA Xiao-Dong Zhang Boca Raton, Florida, USA Consultants: Frederick Hoffman Boca Raton, Floirda, USA Stephen Locke Boca Raton, Florida, USA Heinrich Niederhausen Boca Raton, Florida, USA Table of Contents Khoa Lu Nguyen and Juan Carlos Salazar, On the mixtilinear incircles and excircles,1 Juan Rodr´ıguez, Paula Manuel and Paulo Semi˜ao, A conic associated with the Euler line,17 Charles Thas, A note on the Droz-Farny theorem,25 Paris Pamfilos, The cyclic complex of a cyclic quadrilateral,29 Bernard Gibert, Isocubics with concurrent normals,47 Mowaffaq Hajja and Margarita Spirova, A characterization of the centroid using June Lester’s shape function,53 Christopher J.
    [Show full text]
  • Steiner's Theorems on the Complete Quadrilateral
    Forum Geometricorum b Volume 4 (2004) 35–52. bbb FORUM GEOM ISSN 1534-1178 Steiner’s Theorems on the Complete Quadrilateral Jean-Pierre Ehrmann Abstract. We give a translation of Jacob Steiner’s 1828 note on the complete quadrilateral, with complete proofs and annotations in barycentric coordinates. 1. Steiner’s note on the complete quadrilateral In 1828, Jakob Steiner published in Gergonne’s Annales a very short note [9] listing ten interesting and important theorems on the complete quadrilateral. The purpose of this paper is to provide a translation of the note, to prove these theorems, along with annotations in barycentric coordinates. We begin with a translation of Steiner’s note. Suppose four lines intersect two by two at six points. (1) These four lines, taken three by three, form four triangles whose circum- circles pass through the same point F . (2) The centers of the four circles (and the point F ) lie on the same circle. (3) The perpendicular feet from F to the four lines lie on the same line R, and F is the only point with this property. (4) The orthocenters of the four triangles lie on the same line R. (5) The lines R and R are parallel, and the line R passes through the midpoint of the segment joining F to its perpendicular foot on R. (6) The midpoints of the diagonals of the complete quadrilateral formed by the four given lines lie on the same line R (Newton). (7) The line R is a common perpendicular to the lines R and R. (8) Each of the four triangles in (1) has an incircle and three excircles.
    [Show full text]
  • Triangle Circle Limits
    The Journal of Symbolic Geometry Volume 1 (2006) Triangle Circle Limits Walker Ray Lakeside High School Lake Oswego, OR [email protected] Abstract: We examine the limit behavior of various triangle circles, called “limit circles”, as the vertices of the triangle coalesce. Introduction To aid my research I used mathematical software programs, most importantly Geometry Expressions and Maple. The use of technology allowed me to complete this research topic successfully. I was able to visualize the problems I was trying to solve and eliminate a great deal of error from my work by utilizing these programs. This allowed me to use creativity in studying my topic and quickly find solutions to the problems I faced. Limit Circles A “limit circle” is an extension of the concept of single dimension interpolation where two or more points have coalesced. The limit circumcircle is a simple, non- trivial case of multidimensional interpolation through points that have coalesced. We will see that the limit circumcircle has some unexpected properties, especially in terms of its relation to the other triangle circles. Limit Circles 25 Limit Circumradius – Two Coalescing Points: C b A a D c B Figure 1. Triangle ABC with circumcircle We start by examining the limit of the circumradius of a triangle as two of the vertices coalesce. To define the radius of the limit circle, we examine the behavior of the circle as vertices B and C approach one another. Using the Law of Sines, we know that the circumradius R of triangle ABC with a sides a, b, and c opposite the angles A, B, and C is R = .
    [Show full text]
  • Ptolemy-Copernican Debate - Is the Astro Ver
    Ptolemy-Copernican Debate - Is the Astro Ver. 1.0 Earth or the Sun the center of solar system? In 1600 C.E., educated but reasonable minds disagreed as to whether the Earth or the Sun was the center of the Solar System. Trignometry played a role in the debate by showing that the apparent motion of the planets is explained in models by the same equations. (Note Sun has no retrograde motion.) Mars Mars 1.5 a.u Earth Sun 1.0 a.u Sun 1.0 a.u Earth Earth-centered Ptolemy Sun-centered Coperincus Fig. 1 Fig. 2 Slide 1 Ptolemy-Copernican Debate - The best minds of 1600 C.E. disagreed on . Earth-centered Ptolemy Sun-centered Copernicus Earth at center doesnot rotate. The Sun The Earth rotates and revolves around revolves around Earth. Based on their Sun. Requires acceptance of Newtonian physical senses, people were unwilling to physics. The model is consistent with accept that the Earth's surface is moving observed motions of Venus and Mercury. at 1,500km. The model is inconsistent Equation of time rises from solar orbit. with observed motions of Venus and The model does not simulate the non- Mercury. Unable to measure length of linear planetary albedo effect at year accurately. The model better opposition well. The accuracy of simulates the albedo effect of planets at predicted positions of planets is no opposition. The accuracy of predicted significantly better. The model does not positions of planets is moderate. The need "anti-gravity" to work. model needs "antigravity" to work. Slide 2 Ptolemy-Copernican debate - Apparent retrograde motion of the planets Fig.
    [Show full text]
  • Antiorthocorrespondents of Circumconics
    Forum Geometricorum b Volume 3 (2003) 231–249. bbb FORUM GEOM ISSN 1534-1178 Antiorthocorrespondents of Circumconics Bernard Gibert Abstract. This note is a complement to our previous paper [3]. We study how circumconics are transformed under antiorthocorrespondence. This leads us to consider a pencil of pivotal circular cubics which contains in particular the Neu- berg cubic of the orthic triangle. 1. Introduction This paper is a complement to our previous paper [3] on the orthocorrespon- dence. Recall that in the plane of a given triangle ABC, the orthocorrespondent of a point M is the point M⊥ whose trilinear polar intersects the sidelines of ABC at the orthotraces of M.IfM =(p : q : r) in homogeneous barycentric coordinates, then 1 ⊥ 2 M =(p(−pSA + qSB + rSC)+a qr : ···: ···). (1) The antiorthocorrespondents of M consists of the two points M1 and M2, not ⊥ ⊥ necessarily real, for which M1 = M = M2 . We write M = {M1,M2}, and say that M1 and M2 are orthoassociates. We shall make use of the following basic results. Lemma 1. Let M =(p : q : r) and M = {M1,M2}. 2 (1) The line M1M2 has equation SA(q − r)x + SB(r − p)y + SC (p − q)z =0. It always passes through the orthocenter H, and intersects the line GM at the point (b2 − c2)/(q − r):··· : ··· on the Kiepert hyperbola. (2) The perpendicular bisector M of the segment M1M2 is the trilinear polar of the isotomic conjugate of the anticomplement of M, i.e., (q + r − p)x +(r + p − q)y +(p + q − r)z =0.
    [Show full text]
  • EDUCATIONAL ACTIVITY 2. Calculating the Latitude of the Observation Site from Images of the Midnight Sun
    EDUCATIONAL ACTIVITY 2. Calculating the Latitude of the observation site from images of the Midnight Sun. Mr. Miguel Ángel Pío Jiménez. Astronomer Instituto de Astrofísica de Canarias, Tenerife. Dr. Miquel Serra-Ricart. Astronomer Instituto de Astrofísica de Canarias, Tenerife. Mr. Juan Carlos Casado. Astrophotographer tierrayestrellas.com, Barcelona. Dr. Lorraine Hanlon. Astronomer University College Dublin, Irland. Dr. Luciano Nicastro. Astronomer Istituto Nazionale di Astrofisica, IASF Bologna. 1 – Objectives of the activity. In this activity we will learn to calculate the latitude of an observer from digital images and calculating in them the height the Sun on the horizon. The goals of this activity are to: - Explain the phenomenon of the midnight Sun. - Apply a methodology for the calculation of a physical parameter (Geographycal Latitude) from an observable (digital images). - Support the teaching and learning of mathematics and physics by applying knowledge of mathematics (algebra and trigonometry) and basic physics (kinematics) to solve a practical problem. - Understand and apply basic techniques of image analysis (angular scale, distance measurement, etc.). - Work cooperatively as a team, valuing individual contributions and expressing democratic attitudes. 2 – Instrumentation. The activity will use digital images obtained from northern Europe during the transit of Venus on June 6, 2012 (see sky-live.tv). 3 – Phenomenon. 3.1. Midnight Sun. The Midnight Sun is a natural phenomenon that occurs in its fullness only north of the Arctic Circle and south of the Antarctic Circle. Since in the southern hemisphere there are no permanent settlements sufficiently close to the pole (except in the Antarctic bases which are inhabited by a few scientists and military personnel), inhabited regions that can enjoy with this phenomenon are all in the Northern Hemisphere: Alaska, Canada, Greenland, Norway, Sweden, Finland, Russia and northern end of Iceland.
    [Show full text]
  • Triangle and Its Circles from the Standpol T of Modern
    View metadata, citationbrought and to similar you by papersCORE at core.ac.uk provided by K-State... A TRIANGLE A*D ITS CIRCLES nCLU MAT COOK Hlrtn ., College, 1913» B.8., Phillips Uhivoraity, 1925 i wmaa submitted In partial fuirillwmt ©f the requlreBenta for the of MatKB OF SCIXSCB XAR8A8 STAK AORICaLTORAL COLLEGE 1920 —— — ——- DoccP rncn+ C65 ttMM OF UWIUM 3 I fetation 4 ELK* BR1ST SBVZSW 0FCIRCLB8 WOM 20 TO A TMAWLB in mrntscr asoBuwr ——— 6 THK TrUASBLB AHD ITS CIRCLES FROM THK STAKDPOT?IT OF QDKM 0K1KETHY 7 Properties of • Triangle used In Connection with Circles Pedsl or Siraeon Line e n s — — 8 8 i —— — . ntlperallela — SjRaaedlon Line end Synwedien Point —— 10 Isogoml Conjugates ~ 12 Appolonius' Theoren lb Circles 18 Pe<:el Circle » — —— lusscribcd and Inscribed -—————-- 21 Zaerlbeu sad Inscribed — — — 28 Hine-polnt Circle » »— 30 "~ 34 P Circle — Feuerbach's Theorem » ' -~ 37 T-emoine's First Circle or Triplicate Satlo 40 Leaoine's Leeond Circle or Cosine Circle ~ Broeard Circle i Circle cr Circle - ?olar Circle «» •s Circle Other Properties of the irlangle lev Um — 71 telner's Point — 74 Terry's Point — it Inversion of a Triangle (a) With Bespeet to Inscribed Circle — 76 ith nespeot to Clrcwsseribod Clrele — 7« (e) If eapeot to Kserlbed Circle -—»-— 77 ACKWOWLKDOFEHT 81 MM Mi 82 ItTRODUCTIOl This dissertation Is an attempt to present a consistent and systematic account of son* of the various theories of the triangle and Its circles from the standpol t of modern geometry end to solve a number of original exercises in connection with these theorem*.
    [Show full text]
  • The Mathematical Gazette Index for 1894 to 1908
    The Mathematical Gazette Index for 1894 to 1908 AUTHOR TITLE PAGE Issue Category C.W.Adams Stability of cube floating in liquid p. 388 Dec 1908 MNote 285 V.Ramaswami Aiyar Extension of Euclid I.47 to n-sided regular polygons p. 109 June 1897 MNote 41 V.Ramaswami Aiyar On a fundamental theorem in inversion p. 88 Oct 1904 MNote 153 V.Ramaswami Aiyar On a fundamental theorem in inversion p. 275 Jan 1906 MNote 183 V.Ramaswami Aiyar Note on a point in the demonstration of the binomial theorem p. 276 Jan 1906 MNote 185 V.Ramaswami Aiyar Note on the power inequality p. 321 May 1906 MNote 192 V.Ramaswami Aiyar On the exponential inequalities and the exponential function p. 8 Jan 1907 Article V.Ramaswami Aiyar The A, B, C of the higher analysis p. 79 May 1907 Article V.Ramaswami Aiyar On Stolz and Gmeiner’s proof of the sine and cosine series p. 282 June 1908 MNote 259 V.Ramaswami Aiyar A geometrical proof of Feuerbach’s theorem p. 310 July 1908 MNote 264 A.O.Allen On the adjustment of Kater’s pendulum p. 307 May 1906 Article A.O.Allen Notes on the theory of the reversible pendulum p. 394 Dec 1906 Article Anonymous Proof of a well-known theorem in geometry p. 64 Oct 1896 MNote 30 Anonymous Notes connected with the analytical geometry of the straight line p. 158 Feb 1898 MNote 49 Anonymous Method of reducing central conics p. 225 Dec 1902 MNote 110B (note) Anonymous On a fundamental theorem in inversion p.
    [Show full text]
  • A Treatise on the Circle and the Sphere
    A TREATISE ON THE CIRCLE AND THE SPHERE BY JULIAN LOWELL COOLIDGE, Ph.D. ASSISTANT PROFESSOR OF MATHEMATICS IN HARVARD UNIVERSITY OXFORD AT THE CLARENDON PRESS 1916 i Eh OXFOED UNIVEESITY PEESS LONDON EDINBURGH GLASGOW NEW YORK TORONTO MELBOURNE BOMBAY HUMPHREY MILFORD PUBLISHER TO THE UNIVERSITY PREFACE Every beginner in the science of geometry knows that the circle and the sphere have always played a central rdle, yet few people realize that the reasons for this are many and various. Attention was first called to these figures by their mechanical simplicity and importance, and the fortunate position thus won was further strengthened by the Euclidean tradition of limiting geometry, on the constructive side, to those operations which can be carried out with the aid of naught but ruler and compass. Yet these'facts are far from sufficient to account for the commanding position which the circle and the sphere occupy to-day. To begin with, there would seem no a 'priori reason why those curves which are the simplest from the mechanical point of view should have the greatest wealth of beautiful properties. Had Euclid started, not with the usual parallel postulate, but with the different assumption either of Lobachevski or Riemann, he would have been unable to prove that all angles inscribed in the same circular arc are equal, and a large proportion of our best elementary theorems about the circle would have been lacking. Again, there is no a priori reason why a curve with attractive geometric properties should be blessed with a peculiarly simple cartesian equation; the cycloid is particularly unmanageable in pure cartesian form.
    [Show full text]
  • Article 17 Harmonic Ranges in a Coaxal System of Circles Christopher J Bradley
    Article 17 Harmonic ranges in a coaxal system of circles Christopher J Bradley 1. Introduction Suppose we are given a circle that cuts the sides BC, CA, AB of a triangle ABC at pairs of points on each side, say P and L on BC, Q and M on CA and R and N on AB, in each case in the specified order working around the triangle in an anticlockwise direction. Now let P' and L' be the harmonic conjugates of P and L with respect to B and C, Q' and M' the harmonic conjugates of Q and M with respect to C and A and R' and N' the harmonic conjugates of R and N with respect to A and B. First we prove that P', L', Q', M', R' and N' always lie on a conic. We then investigate the conditions on the given circle for this conic also to be a circle. We define such a pair of circles as a harmonic pair of circles and it turns out that each such pair belongs to the coaxal system of circles of which the polar circle, centre the orthocentre H of ABC and the circumcircle, centre the circumcentre O of ABC may be regarded as defining members. Since the polar circle is real only when ABC is obtuse we remark that other circles in this coaxal system are the nine-point circle, centre T, the midpoint of OH, and the orthocentroidal circle based on GH as diameter, where G is the centroid of ABC. If a harmonic pair S and S' have centres at X and X', then X and X' divide O and H harmonically.
    [Show full text]