Perspectives on Projective Geometry • Jürgen Richter-Gebert
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Projective Geometry: a Short Introduction
Projective Geometry: A Short Introduction Lecture Notes Edmond Boyer Master MOSIG Introduction to Projective Geometry Contents 1 Introduction 2 1.1 Objective . .2 1.2 Historical Background . .3 1.3 Bibliography . .4 2 Projective Spaces 5 2.1 Definitions . .5 2.2 Properties . .8 2.3 The hyperplane at infinity . 12 3 The projective line 13 3.1 Introduction . 13 3.2 Projective transformation of P1 ................... 14 3.3 The cross-ratio . 14 4 The projective plane 17 4.1 Points and lines . 17 4.2 Line at infinity . 18 4.3 Homographies . 19 4.4 Conics . 20 4.5 Affine transformations . 22 4.6 Euclidean transformations . 22 4.7 Particular transformations . 24 4.8 Transformation hierarchy . 25 Grenoble Universities 1 Master MOSIG Introduction to Projective Geometry Chapter 1 Introduction 1.1 Objective The objective of this course is to give basic notions and intuitions on projective geometry. The interest of projective geometry arises in several visual comput- ing domains, in particular computer vision modelling and computer graphics. It provides a mathematical formalism to describe the geometry of cameras and the associated transformations, hence enabling the design of computational ap- proaches that manipulates 2D projections of 3D objects. In that respect, a fundamental aspect is the fact that objects at infinity can be represented and manipulated with projective geometry and this in contrast to the Euclidean geometry. This allows perspective deformations to be represented as projective transformations. Figure 1.1: Example of perspective deformation or 2D projective transforma- tion. Another argument is that Euclidean geometry is sometimes difficult to use in algorithms, with particular cases arising from non-generic situations (e.g. -
Arxiv:Gr-Qc/0611154 V1 30 Nov 2006 Otx Fcra Geometry
MacDowell–Mansouri Gravity and Cartan Geometry Derek K. Wise Department of Mathematics University of California Riverside, CA 92521, USA email: [email protected] November 29, 2006 Abstract The geometric content of the MacDowell–Mansouri formulation of general relativity is best understood in terms of Cartan geometry. In particular, Cartan geometry gives clear geomet- ric meaning to the MacDowell–Mansouri trick of combining the Levi–Civita connection and coframe field, or soldering form, into a single physical field. The Cartan perspective allows us to view physical spacetime as tangentially approximated by an arbitrary homogeneous ‘model spacetime’, including not only the flat Minkowski model, as is implicitly used in standard general relativity, but also de Sitter, anti de Sitter, or other models. A ‘Cartan connection’ gives a prescription for parallel transport from one ‘tangent model spacetime’ to another, along any path, giving a natural interpretation of the MacDowell–Mansouri connection as ‘rolling’ the model spacetime along physical spacetime. I explain Cartan geometry, and ‘Cartan gauge theory’, in which the gauge field is replaced by a Cartan connection. In particular, I discuss MacDowell–Mansouri gravity, as well as its recent reformulation in terms of BF theory, in the arXiv:gr-qc/0611154 v1 30 Nov 2006 context of Cartan geometry. 1 Contents 1 Introduction 3 2 Homogeneous spacetimes and Klein geometry 8 2.1 Kleingeometry ................................... 8 2.2 MetricKleingeometry ............................. 10 2.3 Homogeneousmodelspacetimes. ..... 11 3 Cartan geometry 13 3.1 Ehresmannconnections . .. .. .. .. .. .. .. .. 13 3.2 Definition of Cartan geometry . ..... 14 3.3 Geometric interpretation: rolling Klein geometries . .............. 15 3.4 ReductiveCartangeometry . 17 4 Cartan-type gauge theory 20 4.1 Asequenceofbundles ............................. -
Feature Matching and Heat Flow in Centro-Affine Geometry
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 16 (2020), 093, 22 pages Feature Matching and Heat Flow in Centro-Affine Geometry Peter J. OLVER y, Changzheng QU z and Yun YANG x y School of Mathematics, University of Minnesota, Minneapolis, MN 55455, USA E-mail: [email protected] URL: http://www.math.umn.edu/~olver/ z School of Mathematics and Statistics, Ningbo University, Ningbo 315211, P.R. China E-mail: [email protected] x Department of Mathematics, Northeastern University, Shenyang, 110819, P.R. China E-mail: [email protected] Received April 02, 2020, in final form September 14, 2020; Published online September 29, 2020 https://doi.org/10.3842/SIGMA.2020.093 Abstract. In this paper, we study the differential invariants and the invariant heat flow in centro-affine geometry, proving that the latter is equivalent to the inviscid Burgers' equa- tion. Furthermore, we apply the centro-affine invariants to develop an invariant algorithm to match features of objects appearing in images. We show that the resulting algorithm com- pares favorably with the widely applied scale-invariant feature transform (SIFT), speeded up robust features (SURF), and affine-SIFT (ASIFT) methods. Key words: centro-affine geometry; equivariant moving frames; heat flow; inviscid Burgers' equation; differential invariant; edge matching 2020 Mathematics Subject Classification: 53A15; 53A55 1 Introduction The main objective in this paper is to study differential invariants and invariant curve flows { in particular the heat flow { in centro-affine geometry. In addition, we will present some basic applications to feature matching in camera images of three-dimensional objects, comparing our method with other popular algorithms. -
Gravity and Gauge
Gravity and Gauge Nicholas J. Teh June 29, 2011 Abstract Philosophers of physics and physicists have long been intrigued by the analogies and disanalogies between gravitational theories and (Yang-Mills-type) gauge theories. Indeed, repeated attempts to col- lapse these disanalogies have made us acutely aware that there are fairly general obstacles to doing so. Nonetheless, there is a special case (viz. that of (2+1) spacetime dimensions) in which gravity is often claimed to be identical to a gauge theory. We subject this claim to philosophical scrutiny in this paper: in particular, we (i) analyze how the standard disanalogies can be overcome in (2+1) dimensions, and (ii) consider whether (i) really licenses the interpretation of (2+1) gravity as a gauge theory. Our conceptual analysis reveals more subtle disanalogies between gravity and gauge, and connects these to interpretive issues in classical and quantum gravity. Contents 1 Introduction 2 1.1 Motivation . 4 1.2 Prospectus . 6 2 Disanalogies 6 3 3D Gravity and Gauge 8 3.1 (2+1) Gravity . 9 3.2 (2+1) Chern-Simons . 14 3.2.1 Cartan geometry . 15 3.2.2 Overcoming (Obst-Gauge) via Cartan connections . 17 3.3 Disanalogies collapsed . 21 1 4 Two more disanalogies 22 4.1 What about the symmetries? . 23 4.2 The phase spaces of the two theories . 25 5 Summary and conclusion 30 1 Introduction `The proper method of philosophy consists in clearly conceiving the insoluble problems in all their insolubility and then in simply contemplating them, fixedly and tirelessly, year after year, without any -
The Trigonometry of Hyperbolic Tessellations
Canad. Math. Bull. Vol. 40 (2), 1997 pp. 158±168 THE TRIGONOMETRY OF HYPERBOLIC TESSELLATIONS H. S. M. COXETER ABSTRACT. For positive integers p and q with (p 2)(q 2) Ù 4thereis,inthe hyperbolic plane, a group [p, q] generated by re¯ections in the three sides of a triangle ABC with angles ôÛp, ôÛq, ôÛ2. Hyperbolic trigonometry shows that the side AC has length †,wherecosh†≥cÛs,c≥cos ôÛq, s ≥ sin ôÛp. For a conformal drawing inside the unit circle with centre A, we may take the sides AB and AC to run straight along radii while BC appears as an arc of a circle orthogonal to the unit circle.p The circle containing this arc is found to have radius 1Û sinh †≥sÛz,wherez≥ c2 s2, while its centre is at distance 1Û tanh †≥cÛzfrom A. In the hyperbolic triangle ABC,the altitude from AB to the right-angled vertex C is ê, where sinh ê≥z. 1. Non-Euclidean planes. The real projective plane becomes non-Euclidean when we introduce the concept of orthogonality by specializing one polarity so as to be able to declare two lines to be orthogonal when they are conjugate in this `absolute' polarity. The geometry is elliptic or hyperbolic according to the nature of the polarity. The points and lines of the elliptic plane ([11], x6.9) are conveniently represented, on a sphere of unit radius, by the pairs of antipodal points (or the diameters that join them) and the great circles (or the planes that contain them). The general right-angled triangle ABC, like such a triangle on the sphere, has ®ve `parts': its sides a, b, c and its acute angles A and B. -
Chapter 9 the Geometrical Calculus
Chapter 9 The Geometrical Calculus 1. At the beginning of the piece Erdmann entitled On the Universal Science or Philosophical Calculus, Leibniz, in the course of summing up his views on the importance of a good characteristic, indicates that algebra is not the true characteristic for geometry, and alludes to a “more profound analysis” that belongs to geometry alone, samples of which he claims to possess.1 What is this properly geometrical analysis, completely different from algebra? How can we represent geometrical facts directly, without the mediation of numbers? What, finally, are the samples of this new method that Leibniz has left us? The present chapter will attempt to answer these questions.2 An essay concerning this geometrical analysis is found attached to a letter to Huygens of 8 September 1679, which it accompanied. In this letter, Leibniz enumerates his various investigations of quadratures, the inverse method of tangents, the irrational roots of equations, and Diophantine arithmetical problems.3 He boasts of having perfected algebra with his discoveries—the principal of which was the infinitesimal calculus.4 He then adds: “But after all the progress I have made in these matters, I am no longer content with algebra, insofar as it gives neither the shortest nor the most elegant constructions in geometry. That is why... I think we still need another, properly geometrical linear analysis that will directly express for us situation, just as algebra expresses magnitude. I believe I have a method of doing this, and that we can represent figures and even 1 “Progress in the art of rational discovery depends for the most part on the completeness of the characteristic art. -
PROJECTIVE GEOMETRY Contents 1. Basic Definitions 1 2. Axioms Of
PROJECTIVE GEOMETRY KRISTIN DEAN Abstract. This paper investigates the nature of finite geometries. It will focus on the finite geometries known as projective planes and conclude with the example of the Fano plane. Contents 1. Basic Definitions 1 2. Axioms of Projective Geometry 2 3. Linear Algebra with Geometries 3 4. Quotient Geometries 4 5. Finite Projective Spaces 5 6. The Fano Plane 7 References 8 1. Basic Definitions First, we must begin with a few basic definitions relating to geometries. A geometry can be thought of as a set of objects and a relation on those elements. Definition 1.1. A geometry is denoted G = (Ω,I), where Ω is a set and I a relation which is both symmetric and reflexive. The relation on a geometry is called an incidence relation. For example, consider the tradional Euclidean geometry. In this geometry, the objects of the set Ω are points and lines. A point is incident to a line if it lies on that line, and two lines are incident if they have all points in common - only when they are the same line. There is often this same natural division of the elements of Ω into different kinds such as the points and lines. Definition 1.2. Suppose G = (Ω,I) is a geometry. Then a flag of G is a set of elements of Ω which are mutually incident. If there is no element outside of the flag, F, which can be added and also be a flag, then F is called maximal. Definition 1.3. A geometry G = (Ω,I) has rank r if it can be partitioned into sets Ω1,..., Ωr such that every maximal flag contains exactly one element of each set. -
Euclidean Versus Projective Geometry
Projective Geometry Projective Geometry Euclidean versus Projective Geometry n Euclidean geometry describes shapes “as they are” – Properties of objects that are unchanged by rigid motions » Lengths » Angles » Parallelism n Projective geometry describes objects “as they appear” – Lengths, angles, parallelism become “distorted” when we look at objects – Mathematical model for how images of the 3D world are formed. Projective Geometry Overview n Tools of algebraic geometry n Informal description of projective geometry in a plane n Descriptions of lines and points n Points at infinity and line at infinity n Projective transformations, projectivity matrix n Example of application n Special projectivities: affine transforms, similarities, Euclidean transforms n Cross-ratio invariance for points, lines, planes Projective Geometry Tools of Algebraic Geometry 1 n Plane passing through origin and perpendicular to vector n = (a,b,c) is locus of points x = ( x 1 , x 2 , x 3 ) such that n · x = 0 => a x1 + b x2 + c x3 = 0 n Plane through origin is completely defined by (a,b,c) x3 x = (x1, x2 , x3 ) x2 O x1 n = (a,b,c) Projective Geometry Tools of Algebraic Geometry 2 n A vector parallel to intersection of 2 planes ( a , b , c ) and (a',b',c') is obtained by cross-product (a'',b'',c'') = (a,b,c)´(a',b',c') (a'',b'',c'') O (a,b,c) (a',b',c') Projective Geometry Tools of Algebraic Geometry 3 n Plane passing through two points x and x’ is defined by (a,b,c) = x´ x' x = (x1, x2 , x3 ) x'= (x1 ', x2 ', x3 ') O (a,b,c) Projective Geometry Projective Geometry -
Research Article Traditional Houses and Projective Geometry: Building Numbers and Projective Coordinates
Hindawi Journal of Applied Mathematics Volume 2021, Article ID 9928900, 25 pages https://doi.org/10.1155/2021/9928900 Research Article Traditional Houses and Projective Geometry: Building Numbers and Projective Coordinates Wen-Haw Chen 1 and Ja’faruddin 1,2 1Department of Applied Mathematics, Tunghai University, Taichung 407224, Taiwan 2Department of Mathematics, Universitas Negeri Makassar, Makassar 90221, Indonesia Correspondence should be addressed to Ja’faruddin; [email protected] Received 6 March 2021; Accepted 27 July 2021; Published 1 September 2021 Academic Editor: Md Sazzad Hossien Chowdhury Copyright © 2021 Wen-Haw Chen and Ja’faruddin. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The natural mathematical abilities of humans have advanced civilizations. These abilities have been demonstrated in cultural heritage, especially traditional houses, which display evidence of an intuitive mathematics ability. Tribes around the world have built traditional houses with unique styles. The present study involved the collection of data from documentation, observation, and interview. The observations of several traditional buildings in Indonesia were based on camera images, aerial camera images, and documentation techniques. We first analyzed the images of some sample of the traditional houses in Indonesia using projective geometry and simple house theory and then formulated the definitions of building numbers and projective coordinates. The sample of the traditional houses is divided into two categories which are stilt houses and nonstilt house. The present article presents 7 types of simple houses, 21 building numbers, and 9 projective coordinates. -
A Survey of the Development of Geometry up to 1870
A Survey of the Development of Geometry up to 1870∗ Eldar Straume Department of mathematical sciences Norwegian University of Science and Technology (NTNU) N-9471 Trondheim, Norway September 4, 2014 Abstract This is an expository treatise on the development of the classical ge- ometries, starting from the origins of Euclidean geometry a few centuries BC up to around 1870. At this time classical differential geometry came to an end, and the Riemannian geometric approach started to be developed. Moreover, the discovery of non-Euclidean geometry, about 40 years earlier, had just been demonstrated to be a ”true” geometry on the same footing as Euclidean geometry. These were radically new ideas, but henceforth the importance of the topic became gradually realized. As a consequence, the conventional attitude to the basic geometric questions, including the possible geometric structure of the physical space, was challenged, and foundational problems became an important issue during the following decades. Such a basic understanding of the status of geometry around 1870 enables one to study the geometric works of Sophus Lie and Felix Klein at the beginning of their career in the appropriate historical perspective. arXiv:1409.1140v1 [math.HO] 3 Sep 2014 Contents 1 Euclideangeometry,thesourceofallgeometries 3 1.1 Earlygeometryandtheroleoftherealnumbers . 4 1.1.1 Geometric algebra, constructivism, and the real numbers 7 1.1.2 Thedownfalloftheancientgeometry . 8 ∗This monograph was written up in 2008-2009, as a preparation to the further study of the early geometrical works of Sophus Lie and Felix Klein at the beginning of their career around 1870. The author apologizes for possible historiographic shortcomings, errors, and perhaps lack of updated information on certain topics from the history of mathematics. -
Kiepert Conics in Regular CK-Geometries
Journal for Geometry and Graphics Volume 17 (2013), No. 2, 155{161. Kiepert Conics in Regular CK-Geometries Sybille Mick, Johann Lang Institute of Geometry, Graz University of Technology Kopernikusgasse 24, A-8010 Graz, Austria emails: [email protected], [email protected] Abstract. This paper is a contribution to the concept of Kiepert conics in reg- ular CK -geometries. In such geometries a triangle ABC determines a quadruple of first Kiepert conics and, consequently, a quadruple of second Kiepert conics. Key Words: Cayley-Klein geometries, geometry of triangle, Kiepert conics, pro- jective geometry MSC 2010: 51M09, 51N30 1. Introduction Hyperbolic geometry obeys the axioms of Euclid except for the Euclidean parallel postulate which is replaced by the hyperbolic parallel postulate: Any line g and any point P not on g determine at least two distinct lines through P which do not intersect g. Axiomatic hyperbolic geometry H can be visualized by the disk model. It is defined by an absolute conic m (regular curve of 2nd order) with real points in the real projective plane. The points of the model are the inner points of m, the lines are the open chords of m (see [1, 2, 4]). In a real projective plane the conic m also defines the hyperbolic Cayley-Klein geometry CKH ([6, 9]). All points of the plane not on m | not only the inner points of m | are points of CKH. All lines of the real projective plane are lines of CKH. The second type of regular CK -geometry is the elliptic Cayley-Klein geometry CKE which is determined by a real conic m without real points. -
The Rise of Projective Geometry II
The Rise of Projective Geometry II The Renaissance Artists Although isolated results from earlier periods are now considered as belonging to the subject of projective geometry, the fundamental ideas that form the core of this area stem from the work of artists during the Renaissance. Earlier art appears to us as being very stylized and flat. The Renaissance Artists Towards the end of the 13th century, early Renaissance artists began to attempt to portray situations in a more realistic way. One early technique is known as terraced perspective, where people in a group scene that are further in the back are drawn higher up than those in the front. Simone Martini: Majesty The Renaissance Artists As artists attempted to find better techniques to improve the realism of their work, the idea of vertical perspective was developed by the Italian school of artists (for example Duccio (1255-1318) and Giotto (1266-1337)). To create the sense of depth, parallel lines in the scene are represented by lines that meet in the centerline of the picture. Duccio's Last Supper The Renaissance Artists The modern system of focused perspective was discovered around 1425 by the sculptor and architect Brunelleschi (1377-1446), and formulated in a treatise a few years later by the painter and architect Leone Battista Alberti (1404-1472). The method was perfected by Leonardo da Vinci (1452 – 1519). The German artist Albrecht Dürer (1471 – 1528) introduced the term perspective (from the Latin verb meaning “to see through”) to describe this technique and illustrated it by a series of well- known woodcuts in his book Underweysung der Messung mit dem Zyrkel und Rychtsscheyed [Instruction on measuring with compass and straight edge] in 1525.