Old and New Generalizations of Classical Triangle Centres to Tetrahedra
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Angle Chasing
Angle Chasing Ray Li June 12, 2017 1 Facts you should know 1. Let ABC be a triangle and extend BC past C to D: Show that \ACD = \BAC + \ABC: 2. Let ABC be a triangle with \C = 90: Show that the circumcenter is the midpoint of AB: 3. Let ABC be a triangle with orthocenter H and feet of the altitudes D; E; F . Prove that H is the incenter of 4DEF . 4. Let ABC be a triangle with orthocenter H and feet of the altitudes D; E; F . Prove (i) that A; E; F; H lie on a circle diameter AH and (ii) that B; E; F; C lie on a circle with diameter BC. 5. Let ABC be a triangle with circumcenter O and orthocenter H: Show that \BAH = \CAO: 6. Let ABC be a triangle with circumcenter O and orthocenter H and let AH and AO meet the circumcircle at D and E, respectively. Show (i) that H and D are symmetric with respect to BC; and (ii) that H and E are symmetric with respect to the midpoint BC: 7. Let ABC be a triangle with altitudes AD; BE; and CF: Let M be the midpoint of side BC. Show that ME and MF are tangent to the circumcircle of AEF: 8. Let ABC be a triangle with incenter I, A-excenter Ia, and D the midpoint of arc BC not containing A on the circumcircle. Show that DI = DIa = DB = DC: 9. Let ABC be a triangle with incenter I and D the midpoint of arc BC not containing A on the circumcircle. -
Searching for the Center
Searching For The Center Brief Overview: This is a three-lesson unit that discovers and applies points of concurrency of a triangle. The lessons are labs used to introduce the topics of incenter, circumcenter, centroid, circumscribed circles, and inscribed circles. The lesson is intended to provide practice and verification that the incenter must be constructed in order to find a point equidistant from the sides of any triangle, a circumcenter must be constructed in order to find a point equidistant from the vertices of a triangle, and a centroid must be constructed in order to distribute mass evenly. The labs provide a way to link this knowledge so that the students will be able to recall this information a month from now, 3 months from now, and so on. An application is included in each of the three labs in order to demonstrate why, in a real life situation, a person would want to create an incenter, a circumcenter and a centroid. NCTM Content Standard/National Science Education Standard: • Analyze characteristics and properties of two- and three-dimensional geometric shapes and develop mathematical arguments about geometric relationships. • Use visualization, spatial reasoning, and geometric modeling to solve problems. Grade/Level: These lessons were created as a linking/remembering device, especially for a co-taught classroom, but can be adapted or used for a regular ed, or even honors level in 9th through 12th Grade. With more modification, these lessons might be appropriate for middle school use as well. Duration/Length: Lesson #1 45 minutes Lesson #2 30 minutes Lesson #3 30 minutes Student Outcomes: Students will: • Define and differentiate between perpendicular bisector, angle bisector, segment, triangle, circle, radius, point, inscribed circle, circumscribed circle, incenter, circumcenter, and centroid. -
An Example on Five Classical Centres of a Right Angled Triangle
An example on five classical centres of a right angled triangle Yue Kwok Choy Given O(0, 0), A(12, 0), B(0, 5) . The aim of this small article is to find the co-ordinates of the five classical centres of the ∆ OAB and other related points of interest. We choose a right-angled triangle for simplicity. (1) Orthocenter: The three altitudes of a triangle meet in one point called the orthocenter. (Altitudes are perpendicular lines from vertices to the opposite sides of the triangles.) If the triangle is obtuse, the orthocenter is outside the triangle. If it is a right triangle, the orthocenter is the vertex which is the right angle. Conclusion : Simple, the orthocenter = O(0, 0) . (2) Circum-center: The three perpendicular bisectors of the sides of a triangle meet in one point called the circumcenter. It is the center of the circumcircle, the circle circumscribed about the triangle. If the triangle is obtuse, then the circumcenter is outside the triangle. If it is a right triangle, then the circumcenter is the midpoint of the hypotenuse. (By the theorem of angle in semi-circle as in the diagram.) Conclusion : the circum -centre, E = ͥͦͮͤ ͤͮͩ ʠ ͦ , ͦ ʡ Ɣ ʚ6, 2.5ʛ 1 Exercise 1: (a) Check that the circum -circle above is given by: ͦ ͦ ͦ. ʚx Ǝ 6ʛ ƍ ʚy Ǝ 2.5ʛ Ɣ 6.5 (b) Show that t he area of the triangle with sides a, b, c and angles A, B, C is ΏΐΑ ͦ , where R is the radius of the circum -circle . -
Chapter 1. the Medial Triangle 2
Chapter 1. The Medial Triangle 2 The triangle formed by joining the midpoints of the sides of a given triangle is called the me- dial triangle. Let A1B1C1 be the medial trian- gle of the triangle ABC in Figure 1. The sides of A1B1C1 are parallel to the sides of ABC and 1 half the lengths. So A B C is the area of 1 1 1 4 ABC. Figure 1: In fact area(AC1B1) = area(A1B1C1) = area(C1BA1) 1 = area(B A C) = area(ABC): 1 1 4 Figure 2: The quadrilaterals AC1A1B1 and C1BA1B1 are parallelograms. Thus the line segments AA1 and C1B1 bisect one another, and the line segments BB1 and CA1 bisect one another. (Figure 2) Figure 3: Thus the medians of A1B1C1 lie along the medians of ABC, so both tri- angles A1B1C1 and ABC have the same centroid G. 3 Now draw the altitudes of A1B1C1 from vertices A1 and C1. (Figure 3) These altitudes are perpendicular bisectors of the sides BC and AB of the triangle ABC so they intersect at O, the circumcentre of ABC. Thus the orthocentre of A1B1C1 coincides with the circumcentre of ABC. Let H be the orthocentre of the triangle ABC, that is the point of intersection of the altitudes of ABC. Two of these altitudes AA2 and BB2 are shown. (Figure 4) Since O is the orthocen- tre of A1B1C1 and H is the orthocentre of ABC then jAHj = 2jA1Oj Figure 4: . The centroid G of ABC lies on AA1 and jAGj = 2jGA1j . We also have AA2kOA1, since O is the orthocentre of A1B1C1. -
Arxiv:2101.02592V1 [Math.HO] 6 Jan 2021 in His Seminal Paper [10]
International Journal of Computer Discovered Mathematics (IJCDM) ISSN 2367-7775 ©IJCDM Volume 5, 2020, pp. 13{41 Received 6 August 2020. Published on-line 30 September 2020 web: http://www.journal-1.eu/ ©The Author(s) This article is published with open access1. Arrangement of Central Points on the Faces of a Tetrahedron Stanley Rabinowitz 545 Elm St Unit 1, Milford, New Hampshire 03055, USA e-mail: [email protected] web: http://www.StanleyRabinowitz.com/ Abstract. We systematically investigate properties of various triangle centers (such as orthocenter or incenter) located on the four faces of a tetrahedron. For each of six types of tetrahedra, we examine over 100 centers located on the four faces of the tetrahedron. Using a computer, we determine when any of 16 con- ditions occur (such as the four centers being coplanar). A typical result is: The lines from each vertex of a circumscriptible tetrahedron to the Gergonne points of the opposite face are concurrent. Keywords. triangle centers, tetrahedra, computer-discovered mathematics, Eu- clidean geometry. Mathematics Subject Classification (2020). 51M04, 51-08. 1. Introduction Over the centuries, many notable points have been found that are associated with an arbitrary triangle. Familiar examples include: the centroid, the circumcenter, the incenter, and the orthocenter. Of particular interest are those points that Clark Kimberling classifies as \triangle centers". He notes over 100 such points arXiv:2101.02592v1 [math.HO] 6 Jan 2021 in his seminal paper [10]. Given an arbitrary tetrahedron and a choice of triangle center (for example, the circumcenter), we may locate this triangle center in each face of the tetrahedron. -
Barycentric Coordinates in Olympiad Geometry
Barycentric Coordinates in Olympiad Geometry Max Schindler∗ Evan Cheny July 13, 2012 I suppose it is tempting, if the only tool you have is a hammer, to treat everything as if it were a nail. Abstract In this paper we present a powerful computational approach to large class of olympiad geometry problems{ barycentric coordinates. We then extend this method using some of the techniques from vector computations to greatly extend the scope of this technique. Special thanks to Amir Hossein and the other olympiad moderators for helping to get this article featured: I certainly did not have such ambitious goals in mind when I first wrote this! ∗Mewto55555, Missouri. I can be contacted at igoroogenfl[email protected]. yv Enhance, SFBA. I can be reached at [email protected]. 1 Contents Title Page 1 1 Preliminaries 4 1.1 Advantages of barycentric coordinates . .4 1.2 Notations and Conventions . .5 1.3 How to Use this Article . .5 2 The Basics 6 2.1 The Coordinates . .6 2.2 Lines . .6 2.2.1 The Equation of a Line . .6 2.2.2 Ceva and Menelaus . .7 2.3 Special points in barycentric coordinates . .7 3 Standard Strategies 9 3.1 EFFT: Perpendicular Lines . .9 3.2 Distance Formula . 11 3.3 Circles . 11 3.3.1 Equation of the Circle . 11 4 Trickier Tactics 12 4.1 Areas and Lines . 12 4.2 Non-normalized Coordinates . 13 4.3 O, H, and Strong EFFT . 13 4.4 Conway's Formula . 14 4.5 A Few Final Lemmas . 15 5 Example Problems 16 5.1 USAMO 2001/2 . -
The Euler Line in Non-Euclidean Geometry
California State University, San Bernardino CSUSB ScholarWorks Theses Digitization Project John M. Pfau Library 2003 The Euler Line in non-Euclidean geometry Elena Strzheletska Follow this and additional works at: https://scholarworks.lib.csusb.edu/etd-project Part of the Mathematics Commons Recommended Citation Strzheletska, Elena, "The Euler Line in non-Euclidean geometry" (2003). Theses Digitization Project. 2443. https://scholarworks.lib.csusb.edu/etd-project/2443 This Thesis is brought to you for free and open access by the John M. Pfau Library at CSUSB ScholarWorks. It has been accepted for inclusion in Theses Digitization Project by an authorized administrator of CSUSB ScholarWorks. For more information, please contact [email protected]. THE EULER LINE IN NON-EUCLIDEAN GEOMETRY A Thesis Presented to the Faculty of California State University, San Bernardino In Partial Fulfillment of the Requirements for the Degree Master of Arts in Mathematics by Elena Strzheletska December 2003 THE EULER LINE IN NON-EUCLIDEAN GEOMETRY A Thesis Presented to the Faculty of California State University, San Bernardino by Elena Strzheletska December 2003 Approved by: Robert Stein, Committee Member Susan Addington, Committee Member Peter Williams, Chair Terry Hallett, Department of Mathematics Graduate Coordinator Department of Mathematics ABSTRACT In Euclidean geometry, the circumcenter and the centroid of a nonequilateral triangle determine a line called the Euler line. The orthocenter of the triangle, the point of intersection of the altitudes, also belongs to this line. The main purpose of this thesis is to explore the conditions of the existence and the properties of the Euler line of a triangle in the hyperbolic plane. -
Lemmas in Euclidean Geometry1 Yufei Zhao [email protected]
IMO Training 2007 Lemmas in Euclidean Geometry Yufei Zhao Lemmas in Euclidean Geometry1 Yufei Zhao [email protected] 1. Construction of the symmedian. Let ABC be a triangle and Γ its circumcircle. Let the tangent to Γ at B and C meet at D. Then AD coincides with a symmedian of △ABC. (The symmedian is the reflection of the median across the angle bisector, all through the same vertex.) A A A O B C M B B F C E M' C P D D Q D We give three proofs. The first proof is a straightforward computation using Sine Law. The second proof uses similar triangles. The third proof uses projective geometry. First proof. Let the reflection of AD across the angle bisector of ∠BAC meet BC at M ′. Then ′ ′ sin ∠BAM ′ ′ BM AM sin ∠ABC sin ∠BAM sin ∠ABD sin ∠CAD sin ∠ABD CD AD ′ = ′ sin ∠CAM ′ = ∠ ∠ ′ = ∠ ∠ = = 1 M C AM sin ∠ACB sin ACD sin CAM sin ACD sin BAD AD BD Therefore, AM ′ is the median, and thus AD is the symmedian. Second proof. Let O be the circumcenter of ABC and let ω be the circle centered at D with radius DB. Let lines AB and AC meet ω at P and Q, respectively. Since ∠PBQ = ∠BQC + ∠BAC = 1 ∠ ∠ ◦ 2 ( BDC + DOC) = 90 , we see that PQ is a diameter of ω and hence passes through D. Since ∠ABC = ∠AQP and ∠ACB = ∠AP Q, we see that triangles ABC and AQP are similar. If M is the midpoint of BC, noting that D is the midpoint of QP , the similarity implies that ∠BAM = ∠QAD, from which the result follows. -
Triangle-Centers.Pdf
Triangle Centers Maria Nogin (based on joint work with Larry Cusick) Undergraduate Mathematics Seminar California State University, Fresno September 1, 2017 Outline • Triangle Centers I Well-known centers F Center of mass F Incenter F Circumcenter F Orthocenter I Not so well-known centers (and Morley's theorem) I New centers • Better coordinate systems I Trilinear coordinates I Barycentric coordinates I So what qualifies as a triangle center? • Open problems (= possible projects) mass m mass m mass m Centroid (center of mass) C Mb Ma Centroid A Mc B Three medians in every triangle are concurrent. Centroid is the point of intersection of the three medians. mass m mass m mass m Centroid (center of mass) C Mb Ma Centroid A Mc B Three medians in every triangle are concurrent. Centroid is the point of intersection of the three medians. Centroid (center of mass) C mass m Mb Ma Centroid mass m mass m A Mc B Three medians in every triangle are concurrent. Centroid is the point of intersection of the three medians. Incenter C Incenter A B Three angle bisectors in every triangle are concurrent. Incenter is the point of intersection of the three angle bisectors. Circumcenter C Mb Ma Circumcenter A Mc B Three side perpendicular bisectors in every triangle are concurrent. Circumcenter is the point of intersection of the three side perpendicular bisectors. Orthocenter C Ha Hb Orthocenter A Hc B Three altitudes in every triangle are concurrent. Orthocenter is the point of intersection of the three altitudes. Euler Line C Ha Hb Orthocenter Mb Ma Centroid Circumcenter A Hc Mc B Euler line Theorem (Euler, 1765). -
Degree of Triangle Centers and a Generalization of the Euler Line
Beitr¨agezur Algebra und Geometrie Contributions to Algebra and Geometry Volume 51 (2010), No. 1, 63-89. Degree of Triangle Centers and a Generalization of the Euler Line Yoshio Agaoka Department of Mathematics, Graduate School of Science Hiroshima University, Higashi-Hiroshima 739–8521, Japan e-mail: [email protected] Abstract. We introduce a concept “degree of triangle centers”, and give a formula expressing the degree of triangle centers on generalized Euler lines. This generalizes the well known 2 : 1 point configuration on the Euler line. We also introduce a natural family of triangle centers based on the Ceva conjugate and the isotomic conjugate. This family contains many famous triangle centers, and we conjecture that the de- gree of triangle centers in this family always takes the form (−2)k for some k ∈ Z. MSC 2000: 51M05 (primary), 51A20 (secondary) Keywords: triangle center, degree of triangle center, Euler line, Nagel line, Ceva conjugate, isotomic conjugate Introduction In this paper we present a new method to study triangle centers in a systematic way. Concerning triangle centers, there already exist tremendous amount of stud- ies and data, among others Kimberling’s excellent book and homepage [32], [36], and also various related problems from elementary geometry are discussed in the surveys and books [4], [7], [9], [12], [23], [26], [41], [50], [51], [52]. In this paper we introduce a concept “degree of triangle centers”, and by using it, we clarify the mutual relation of centers on generalized Euler lines (Proposition 1, Theorem 2). Here the term “generalized Euler line” means a line connecting the centroid G and a given triangle center P , and on this line an infinite number of centers lie in a fixed order, which are successively constructed from the initial center P 0138-4821/93 $ 2.50 c 2010 Heldermann Verlag 64 Y. -
1. EUCLIDEAN GEOMETRY 1.3. Triangle Centres
1. EUCLIDEAN GEOMETRY 1.3. Triangle Centres Triangle Centres The humble triangle, with its three vertices and three sides, is actually a very remarkable object. For evidence of this fact, just look at the Encyclopedia of Triangle Centers1 on the internet, which catalogues literally thousands of special points that every triangle has. We’ll only be looking at the big four — namely, the circumcentre, the incentre, the orthocentre, and the centroid. While exploring these constructions, we’ll need all of our newfound geometric knowledge from the previous lecture, so let’s have a quick recap. Triangles – Congruence : There are four simple rules to determine whether or not two triangles are congruent. They are SSS, SAS, ASA and RHS. – Similarity : There are also three simple rules to determine whether or not two triangles are similar. They are AAA, PPP and PAP. – Midpoint Theorem : Let ABC be a triangle where the midpoints of the sides BC, CA, AB are X, Y, Z, respectively. Then the four triangles AZY, ZBX, YXC and XYZ are all congruent to each other and similar to triangle ABC. Circles – The diameter of a circle subtends an angle of 90◦. In other words, if AB is the diameter of a circle and C is a point on the circle, then \ACB = 90◦. – The angle subtended by a chord at the centre is twice the angle subtended at the circumference, on the same side. In other words, if AB is a chord of a circle with centre O and C is a point on the circle on the same side of AB as O, then \AOB = 2\ACB. -
Singularities of Centre Symmetry Sets 1 Introduction
Singularities of centre symmetry sets P.J.Giblin, V.M.Zakalyukin 1 1 Introduction We study the singularities of envelopes of families of chords (special straight lines) intrin- sically related to a hypersurface M ⊂ Rn embedded into an affine space. The origin of this investigation is the paper [10] of Janeczko. He described a general- ization of central symmetry in which a single point—the centre of symmetry—is replaced by the bifurcation set of a certain family of ratios. In [6] Giblin and Holtom gave an alternative description, as follows. For a hypersurface M ⊂ Rn we consider pairs of points at which the tangent hy- perplanes are parallel, and in particular take the family of chords (regarded as infinite lines) joining these pairs. For n = 2 these chords will always have an envelope, and this envelope is called the centre symmetry set (CSS) of the curve M. When M is convex (the case considered in [10]) the envelope is quite simple to describe, and has cusps as its only generic singularities. In [6] the case when M is not convex is considered, and there the envelope acquires extra components, and singularities resembling boundary singularities of Arnold. This is because, arbitrarily close to an ordinary inflexion, there are pairs of points on the curve with parallel tangents. The corresponding chords have an envelope with a limit point at the inflexion itself. When n = 3 we obtain a 2-parameter family of lines in R3, which may or may not have a (real) envelope. The real part of the envelope is again called the CSS of M.