Euclidean Geometry
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Diameter, Width and Thickness in the Hyperbolic Plane
DIAMETER, WIDTH AND THICKNESS IN THE HYPERBOLIC PLANE AKOS´ G.HORVATH´ Abstract. This paper contains a new concept to measure the width and thickness of a convex body in the hyperbolic plane. We compare the known concepts with the new one and prove some results on bodies of constant width, constant diameter and given thickness. 1. Introduction In hyperbolic geometry there are several concepts to measure the breadth of a convex set. In the first section of this paper we introduce a new idea and compare it with four known ones. Correspondingly, we define three classes of bodies, bodies of constant with, bodies of constant diameter and bodies having the constant shadow property, respectively. In Euclidean space more or less these classes are agree but in the hyperbolic plane we need to differentiate them. Among others we find convex compact bodies of constant width which size essential in the fulfilment of this property (see Statement 7) and others where the size dependence is non-essential (see Statementst:circle). We prove that the property of constant diameter follows to the fulfilment of constant shadow property (see Theorem 2), and both of them are stronger as the property of constant width (see Theorem 1). In the last part of this paper, we introduce the thickness of a constant body and prove a variant of Blaschke’s theorem on the larger circle inscribed to a plane-convex body of given thickness. 1.1. The hyperbolic concepts of width (breadth) introduced earlier. 1.1.1. width ( ): Santal´oin his paper [14] developed the following approach. -
AN INSTRUMENT in HYPERBOLIC GEOMETRY P. 290]
AN INSTRUMENT IN HYPERBOLIC GEOMETRY M. W. AL-DHAHIR1 In addition to straight edge and compasses, the classical instru- ments of Euclidean geometry, we have in hyperbolic geometry the horocompass and the hypercompass. By a straight edge, or ruler, we draw the line joining any two distinct points, and by the compasses we construct a circle with given center and radius. The horocompass is used to draw a horocycle through a given point when its diameter through the point with its direction are given. If the central line and radius of a hypercycle are given, we can draw it by the hypercompass. Although ruler and compasses have been generally used in the solutions of construction problems in hyperbolic geometry [l; 2, p. 191, pp. 204-206; 3, p. 394], other instruments have been intro- duced, and the relationships among these instruments, together with some restrictions, have been studied in recent years [2, pp. 289-291]. An important result in this connection is the following theorem [2, p. 290]. Theorem A. In conjunction with a ruler, the three compasses are equivalent. Recently [3, p. 389], a different geometrical tool, called the parallel-ruler, has been considered. For any point 4 and any ray a, not incident to 4, we can draw, with this ruler, a line through 4 parallel to a. As in Euclidean geometry, the parallel-ruler may also be used as an ordinary ruler. Hence the following result has been obtained [3]. Theorem H. Any construction that can be performed by a ruler and compasses can be performed by a parallel-ruler. -
Lectures – Math 128 – Geometry – Spring 2002
Lectures { Math 128 { Geometry { Spring 2002 Day 1 ∼∼∼ ∼∼∼ Introduction 1. Introduce Self 2. Prerequisites { stated prereq is math 52, but might be difficult without math 40 Syllabus Go over syllabus Overview of class Recent flurry of mathematical work trying to discover shape of space • Challenge assumption space is flat, infinite • space picture with Einstein quote • will discuss possible shapes for 2D and 3D spaces • this is topology, but will learn there is intrinsic link between top and geometry • to discover poss shapes, need to talk about poss geometries • Geometry = set + group of transformations • We will discuss geometries, symmetry groups • Quotient or identification geometries give different manifolds / orbifolds • At end, we'll come back to discussing theories for shape of universe • How would you try to discover shape of space you're living in? 2 Dimensional Spaces { A Square 1. give face, 3D person can do surgery 2. red thread, possible shapes, veered? 3. blue thread, never crossed, possible shapes? 4. what about NE direction? 1 List of possibilities: classification (closed) 1. list them 2. coffee cup vs donut How to tell from inside { view inside small torus 1. old bi-plane game, now spaceship 2. view in each direction (from flat torus point of view) 3. tiling pictures 4. fundamental domain { quotient geometry 5. length spectra can tell spaces apart 6. finite area 7. which one is really you? 8. glueing, animation of folding torus 9. representation, with arrows 10. discuss transformations 11. torus tic-tac-toe, chess on Friday Different geometries (can shorten or lengthen this part) 1. describe each of 3 geometries 2. -
Chapter 1 : the Hyperbolic Plane
Géométrie Hyperbolique 1 M2 Dynamique Chapter 1 : The Hyperbolic plane I Möbius transformations We start with a little bit of geometry on the Riemann sphere using Möbius transformation. A - Definitions Let C^ = C [ f1g be the Riemann sphere. It is the one-point compactification of the usual complex plane. It is homemorphic to the sphere S2 (embedded in R3) through the stereographic projection. It’s also homeomorphic to CP 1, the complex projective line, which is the quotient of C2 n f(0; 0)g by C∗. Definition I.1 A Möbius transformation is a map φ : C^ ! C^ defined by 8 az + b > if z 2 ; z 6= − d < cz + d C c φ(z) = d 1 if z = − c :> a c if z = 1 with a; b; c; d 2 C such that ad − bc 6= 0. Remark : If c = 0, the last two cases are the same We denote by Mob(C^) the set of all Möbius transformations. We can give basic examples of Möbius transformations : • Translations of the form Tb : z 7! z + b with b 2 C. iθ • Rotations. For example Rθ : z 7! e z are the rotations around 0. • Homotheties. For example Sλ : z 7! λz with λ 2 R>0. are the homotheties from 0. 1 • The involution : I : z 7! z Exercise 1: Prove that the group Mob(C^) is generated by the set fTb; b 2 Cg [ fRθ; θ 2 Rg [ fSλ; λ 2 R>0g [ fIg (Try to decompose any map into these elementary elements). Any similarity z 7! az + b with a 2 C∗ and b 2 C is of course a Mobius transformation. -
From 2D Hyperbolic Forests to 3D Euclidean Entangled Thickets
Eur. Phys. J. B 16, 613–630 (2000) THE EUROPEAN PHYSICAL JOURNAL B EDP Sciences c Societ`a Italiana di Fisica Springer-Verlag 2000 From 2D hyperbolic forests to 3D Euclidean entangled thickets S.T. Hyde1 and C. Oguey2,a 1 Applied Mathematics, Research School of Physical Sciences, Australian National University, Canberra, A.C.T. 0200, Australia 2 LPTMb,Universit´e de Cergy Pontoise, 5 Mail G. Lussac, 95031 Cergy-Pontoise, France Received 10 December 1999 Abstract. A method is developed to construct and analyse a wide class of graphs embedded in Euclidean 3D space, including multiply-connected and entangled examples. The graphs are derived via embeddings of infinite families of trees (forests) in the hyperbolic plane, and subsequent folding into triply periodic minimal surfaces, including the P, D,gyroidandH surfaces. Some of these graphs are natural generalisations of bicontinuous topologies to bi-, tri-, quadra- and octa-continuous forms. Interwoven layer graphs and periodic sets of finite clusters also emerge from the algorithm. Many of the graphs are chiral. The generated graphs are compared with some organo-metallic molecular crystals with multiple frameworks and molecular mesophases found in copolymer melts. PACS. 61.50.Ah Theory of crystal structure, crystal symmetry; calculations and modeling – 61.25.Hq Macromolecular and polymer solutions; polymer melts; swelling – 61.30.Cz Theory and models of liquid crystal structure 1 Introduction cutoff at short length scales. Depending on the system at hand, this UV limit is due to e.g. stability limits of Infinite crystalline 3D graphs, consisting of translation- the (meso)phase under study, bonding, hard-core or other ally ordered arrangements of points (vertices) and lines microscopic interactions, effective contributions involving joining them (edges), are relevant to crystalline condensed the curvatures, bending or other geometric parameters. -
On Hyperbolic Analogues of Some Classical Theorems in Spherical Geometry Athanase Papadopoulos, Weixu Su
On hyperbolic analogues of some classical theorems in spherical geometry Athanase Papadopoulos, Weixu Su To cite this version: Athanase Papadopoulos, Weixu Su. On hyperbolic analogues of some classical theorems in spherical geometry. 2014. hal-01064449v1 HAL Id: hal-01064449 https://hal.archives-ouvertes.fr/hal-01064449v1 Preprint submitted on 16 Sep 2014 (v1), last revised 7 Feb 2015 (v2) HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. ON HYPERBOLIC ANALOGUES OF SOME CLASSICAL THEOREMS IN SPHERICAL GEOMETRY ATHANASE PAPADOPOULOS AND WEIXU SU Abstract. We give the hyperbolic analogues of some classical theorems in spherical geometry due to Menelaus, Euler, Lexell, Ceva and Lambert. Some of the spherical results are also made more precise. AMS classification: 01-99 ; 53-02 ; 53-03 ; 53A05 ; 53A35. Keywords: Hyperbolic geometry, spherical geometry, Menelaus Theo- rem, Euler Theorem, Lexell Theorem. The second author is partially supported by NSFC grant No: 11201078. Both authors are partially supported by the French ANR grant FINSLER. They are thankful for Norbert A’Campo discussions on this subject. 1. Introduction We give the hyperbolic analogues of several theorems in spherical geom- etry. The first theorem is due to Menelaus and is contained in his Spherics (cf. -
The Hyperbolic Geometry of Markov's Theorem on Diophantine
The hyperbolic geometry of Markov’s theorem on Diophantine approximation and quadratic forms Boris Springborn Abstract Markov’s theorem classifies the worst irrational numbers with respect to rational approximation and the indefinite binary quadratic forms whose values for integer arguments stay farthest away from zero. The main pur- pose of this paper is to present a new proof of Markov’s theorem using hyperbolic geometry. The main ingredients are a dictionary to translate between hyperbolic geometry and algebra/number theory, and some very basic tools borrowed from modern geometric Teichmüller theory. Simple closed geodesics and ideal triangulations of the modular torus play an im- portant role, and so do the problems: How far can a straight line crossing a triangle stay away from the vertices? How far can it stay away from the vertices of the tessellation generated by the triangle? Definite binary quadratic forms are briefly discussed in the last section. MSC (2010). 11J06, 32G15 Key words and phrases. Diophantine approximation, quadratic form, mod- ular torus, closed geodesic 1 Introduction The main purpose of this article is to present a new proof of Markov’s theo- rem [49, 50] (Secs.2,3) using hyperbolic geometry. Roughly, the following dic- tionary is used to translate between hyperbolic geometry and algebra/number theory: Hyperbolic Geometry Algebra/Number Theory 2 horocycle nonzero vector (p, q) R Sec.5 2 arXiv:1702.05061v2 [math.GT] 7 Aug 2019 geodesic indefinite binary quadratic form f Sec. 10 point definite binary quadratic form f Sec. 16 p1 p2 signed distance between horocycles 2 log det q q (24) 1 2 signed distance between horocycle f (p, q) (29) log p and geodesic/point det f (46) j j ideal triangulation of the modular Markov triple Sec. -
Beltrami's Models of Non-Euclidean Geometry
BELTRAMI'S MODELS OF NON-EUCLIDEAN GEOMETRY NICOLA ARCOZZI Abstract. In two articles published in 1868 and 1869, Eugenio Beltrami pro- vided three models in Euclidean plane (or space) for non-Euclidean geometry. Our main aim here is giving an extensive account of the two articles' content. We will also try to understand how the way Beltrami, especially in the first article, develops his theory depends on a changing attitude with regards to the definition of surface. In the end, an example from contemporary mathe- matics shows how the boundary at infinity of the non-Euclidean plane, which Beltrami made intuitively and mathematically accessible in his models, made non-Euclidean geometry a natural tool in the study of functions defined on the real line (or on the circle). Contents 1. Introduction1 2. Non-Euclidean geometry before Beltrami4 3. The models of Beltrami6 3.1. The \projective" model7 3.2. The \conformal" models 12 3.3. What was Beltrami's interpretation of his own work? 18 4. From the boundary to the interior: an example from signal processing 21 References 24 1. Introduction In two articles published in 1868 and 1869, Eugenio Beltrami, at the time pro- fessor at the University of Bologna, produced various models of the hyperbolic ver- sion non-Euclidean geometry, the one thought in solitude by Gauss, but developed and written by Lobachevsky and Bolyai. One model is presented in the Saggio di interpretazione della geometria non-euclidea[5][Essay on the interpretation of non- Euclidean geometry], and other two models are developed in Teoria fondamentale degli spazii di curvatura costante [6][Fundamental theory of spaces with constant curvature]. -
Non-Euclidean Geometry H.S.M
AMS / MAA SPECTRUM VOL AMS / MAA SPECTRUM VOL 23 23 Throughout most of this book, non-Euclidean geometries in spaces of two or three dimensions are treated as specializations of real projective geometry in terms of a simple set of axioms concerning points, lines, planes, incidence, order and conti- Non-Euclidean Geometry nuity, with no mention of the measurement of distances or angles. This synthetic development is followed by the introduction of homogeneous coordinates, begin- ning with Von Staudt's idea of regarding points as entities that can be added or multiplied. Transformations that preserve incidence are called collineations. They lead in a natural way to isometries or 'congruent transformations.' Following a NON-EUCLIDEAN recommendation by Bertrand Russell, continuity is described in terms of order. Elliptic and hyperbolic geometries are derived from real projective geometry by specializing in elliptic or hyperbolic polarity which transforms points into lines GEOMETRY (in two dimensions), planes (in three dimensions), and vice versa. Sixth Edition An unusual feature of the book is its use of the general linear transformation of coordinates to derive the formulas of elliptic and hyperbolic trigonometry. The area of a triangle is related to the sum of its angles by means of an ingenious idea of Gauss. This treatment can be enjoyed by anyone who is familiar with algebra up to the elements of group theory. The present (sixth) edition clari es some obscurities in the fth, and includes a new section 15.9 on the author's useful concept of inversive distance. H.S.M. Coxeter This book presents a very readable account of the fundamental principles of hyperbolic and elliptic geometries. -
Non-Euclidean Geometry Skyler W
The University of Maine DigitalCommons@UMaine Electronic Theses and Dissertations Fogler Library 2000 Non-Euclidean Geometry Skyler W. Ross Follow this and additional works at: http://digitalcommons.library.umaine.edu/etd Part of the Geometry and Topology Commons Recommended Citation Ross, Skyler W., "Non-Euclidean Geometry" (2000). Electronic Theses and Dissertations. 426. http://digitalcommons.library.umaine.edu/etd/426 This Open-Access Thesis is brought to you for free and open access by DigitalCommons@UMaine. It has been accepted for inclusion in Electronic Theses and Dissertations by an authorized administrator of DigitalCommons@UMaine. NON-EUCLIDEAN GEOMETRY By Skyler W. Ross B.S. University of Maine, 1990 A THESIS Submitted in Partial Fulfillment of the Requirements for the Degree of Master of Arts (in Mathematics) The Graduate School University of Maine May, 2000 Advisory Committee: William O. Bray: Chair and Professor of Mathematics, Co-Advisor Eisso J. Atzema: Instructor of Mathematics, Co-Advisor Robert D. Franzosa: Professor of Mathematics Henrik Bresinsky: Professor of Mathematics Acknowledgments The Author would like to express his gratitude to the members of the thesis advisory committee for their time, effort and contributions, to Dr. Grattan Murphy who first introduced the author to non-Euclidean geometries, and to Jean-Marie Laborde for his permission to include the demonstration version of his software, Cabri II, with this thesis. Thanks also to Euclid, Henri Poincaré, Felix Klein, Janos Bolyai, and all other pioneers in the field of geometry. And thanks to those who wrote the texts studied by the author in preparation for this thesis. A special debt of gratitude is due Dr. -
Lobachevski Illuminated: Content, Methods, and Context of the Theory of Parallels
University of Montana ScholarWorks at University of Montana Graduate Student Theses, Dissertations, & Professional Papers Graduate School 2007 Lobachevski Illuminated: Content, Methods, and Context of the Theory of Parallels Seth Braver The University of Montana Follow this and additional works at: https://scholarworks.umt.edu/etd Let us know how access to this document benefits ou.y Recommended Citation Braver, Seth, "Lobachevski Illuminated: Content, Methods, and Context of the Theory of Parallels" (2007). Graduate Student Theses, Dissertations, & Professional Papers. 631. https://scholarworks.umt.edu/etd/631 This Dissertation is brought to you for free and open access by the Graduate School at ScholarWorks at University of Montana. It has been accepted for inclusion in Graduate Student Theses, Dissertations, & Professional Papers by an authorized administrator of ScholarWorks at University of Montana. For more information, please contact [email protected]. LOBACHEVSKI ILLUMINATED: CONTENT, METHODS, AND CONTEXT OF THE THEORY OF PARALLELS By Seth Philip Braver B.A., San Francisco State University, San Francisco, California, 1999 M.A., University of California at Santa Cruz, Santa Cruz, California, 2001 Dissertation presented in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Mathematical Sciences The University of Montana Missoula, MT Spring 2007 Approved by: Dr. David A. Strobel, Dean Graduate School Dr. Gregory St. George, Committee Co-Chair Department of Mathematical Sciences Dr. Karel Stroethoff, Committee Co-Chair Department of Mathematical Sciences Dr. James Hirstein Department of Mathematical Sciences Dr. Jed Mihalisin Department of Mathematical Sciences Dr. James Sears Department of Geology Braver, Seth, Ph.D., May 2007 Mathematical Sciences Lobachevski Illuminated: The Content, Methods, and Context of The Theory of Parallels. -
Hypercycles and Horocycles
Chapter 10 Hypercycles and Horocycles There is a curve peculiar to hyperbolic geometry, called the horocycle. Consider two limiting parallel lines, ` and m, with a common direction, say . Let P be a point on one of these lines P 2 `. If there exists a point Q 2 m such that the singly asymptotic triangle, 4PQ, has the property that \PQ =» \QP then we say that Q corresponds to P . If the singly asymptotic triangle 4PQ has the above property we shall say that it is equiangular. Note that it is obvious from the de¯nition that if Q corresponds to P , then P corresponds to Q. The points P and Q are called a pair of corresponding points. Theorem 10.1 If points P and Q lie on two limiting parallel lines in the direction of the ideal point, , they are corresponding points on these lines if and only if the perpendicular bisector of PQ is limiting parallel to the lines in the direction of . Theorem 10.2 Given any two limiting parallel lines, there exists a line each of whose points is equidistant from them. The line is limiting parallel to them in their common direction. Proof: Let ` and m be limiting parallel lines with common direction . Let A 2 ` and B 2 m. The bisector of \BA in the singly asymptotic triangle 4AB meets side B in a point X and the bisector of \AB meets side AX of the triangle 4ABX in a point C. Thus the bisectors of the angles of the singly asymptotic triangle 4AB meet in a point C.