A Comparison of Differential Calculus and Differential Geometry in Two
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Riemann's Contribution to Differential Geometry
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Historia Mathematics 9 (1982) l-18 RIEMANN'S CONTRIBUTION TO DIFFERENTIAL GEOMETRY BY ESTHER PORTNOY UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN, URBANA, IL 61801 SUMMARIES In order to make a reasonable assessment of the significance of Riemann's role in the history of dif- ferential geometry, not unduly influenced by his rep- utation as a great mathematician, we must examine the contents of his geometric writings and consider the response of other mathematicians in the years immedi- ately following their publication. Pour juger adkquatement le role de Riemann dans le developpement de la geometric differentielle sans etre influence outre mesure par sa reputation de trks grand mathematicien, nous devons &udier le contenu de ses travaux en geometric et prendre en consideration les reactions des autres mathematiciens au tours de trois an&es qui suivirent leur publication. Urn Riemann's Einfluss auf die Entwicklung der Differentialgeometrie richtig einzuschZtzen, ohne sich von seinem Ruf als bedeutender Mathematiker iiberm;issig beeindrucken zu lassen, ist es notwendig den Inhalt seiner geometrischen Schriften und die Haltung zeitgen&sischer Mathematiker unmittelbar nach ihrer Verijffentlichung zu untersuchen. On June 10, 1854, Georg Friedrich Bernhard Riemann read his probationary lecture, "iber die Hypothesen welche der Geometrie zu Grunde liegen," before the Philosophical Faculty at Gdttingen ill. His biographer, Dedekind [1892, 5491, reported that Riemann had worked hard to make the lecture understandable to nonmathematicians in the audience, and that the result was a masterpiece of presentation, in which the ideas were set forth clearly without the aid of analytic techniques. -
Relativistic Spacetime Structure
Relativistic Spacetime Structure Samuel C. Fletcher∗ Department of Philosophy University of Minnesota, Twin Cities & Munich Center for Mathematical Philosophy Ludwig Maximilian University of Munich August 12, 2019 Abstract I survey from a modern perspective what spacetime structure there is according to the general theory of relativity, and what of it determines what else. I describe in some detail both the “standard” and various alternative answers to these questions. Besides bringing many underexplored topics to the attention of philosophers of physics and of science, metaphysicians of science, and foundationally minded physicists, I also aim to cast other, more familiar ones in a new light. 1 Introduction and Scope In the broadest sense, spacetime structure consists in the totality of relations between events and processes described in a spacetime theory, including distance, duration, motion, and (more gener- ally) change. A spacetime theory can attribute more or less such structure, and some parts of that structure may determine other parts. The nature of these structures and their relations of determi- nation bear on the interpretation of the theory—what the world would be like if the theory were true (North, 2009). For example, the structures of spacetime might be taken as its ontological or conceptual posits, and the determination relations might indicate which of these structures is more fundamental (North, 2018). Different perspectives on these questions might also reveal structural similarities with other spacetime theories, providing the resources to articulate how the picture of the world that that theory provides is different (if at all) from what came before, and might be different from what is yet to come.1 ∗Juliusz Doboszewski, Laurenz Hudetz, Eleanor Knox, J. -
A CONCISE MINI HISTORY of GEOMETRY 1. Origin And
Kragujevac Journal of Mathematics Volume 38(1) (2014), Pages 5{21. A CONCISE MINI HISTORY OF GEOMETRY LEOPOLD VERSTRAELEN 1. Origin and development in Old Greece Mathematics was the crowning and lasting achievement of the ancient Greek cul- ture. To more or less extent, arithmetical and geometrical problems had been ex- plored already before, in several previous civilisations at various parts of the world, within a kind of practical mathematical scientific context. The knowledge which in particular as such first had been acquired in Mesopotamia and later on in Egypt, and the philosophical reflections on its meaning and its nature by \the Old Greeks", resulted in the sublime creation of mathematics as a characteristically abstract and deductive science. The name for this science, \mathematics", stems from the Greek language, and basically means \knowledge and understanding", and became of use in most other languages as well; realising however that, as a matter of fact, it is really an art to reach new knowledge and better understanding, the Dutch term for mathematics, \wiskunde", in translation: \the art to achieve wisdom", might be even more appropriate. For specimens of the human kind, \nature" essentially stands for their organised thoughts about sensations and perceptions of \their worlds outside and inside" and \doing mathematics" basically stands for their thoughtful living in \the universe" of their idealisations and abstractions of these sensations and perceptions. Or, as Stewart stated in the revised book \What is Mathematics?" of Courant and Robbins: \Mathematics links the abstract world of mental concepts to the real world of physical things without being located completely in either". -
Differential Geometry Lecture 17: Geodesics and the Exponential
Differential geometry Lecture 17: Geodesics and the exponential map David Lindemann University of Hamburg Department of Mathematics Analysis and Differential Geometry & RTG 1670 3. July 2020 David Lindemann DG lecture 17 3. July 2020 1 / 44 1 Geodesics 2 The exponential map 3 Geodesics as critical points of the energy functional 4 Riemannian normal coordinates 5 Some global Riemannian geometry David Lindemann DG lecture 17 3. July 2020 2 / 44 Recap of lecture 16: constructed covariant derivatives along curves defined parallel transport studied the relation between a given connection in the tangent bundle and its parallel transport maps introduced torsion tensor and metric connections, studied geometric interpretation defined the Levi-Civita connection of a pseudo-Riemannian manifold David Lindemann DG lecture 17 3. July 2020 3 / 44 Geodesics Recall the definition of the acceleration of a smooth curve n 00 n γ : I ! R , that is γ 2 Γγ (T R ). Question: Is there a coordinate-free analogue of this construc- tion involving connections? Answer: Yes, uses covariant derivative along curves. Definition Let M be a smooth manifold, r a connection in TM ! M, 0 and γ : I ! M a smooth curve. Then rγ0 γ 2 Γγ (TM) is called the acceleration of γ (with respect to r). Of particular interest is the case if the acceleration of a curve vanishes, that is if its velocity vector field is parallel: Definition A smooth curve γ : I ! M is called geodesic with respect to a 0 given connection r in TM ! M if rγ0 γ = 0. David Lindemann DG lecture 17 3. -
Math 348 Differential Geometry of Curves and Surfaces Lecture 1 Introduction
Math 348 Differential Geometry of Curves and Surfaces Lecture 1 Introduction Xinwei Yu Sept. 5, 2017 CAB 527, [email protected] Department of Mathematical & Statistical Sciences University of Alberta Table of contents 1. Course Information 2. Before Classical Differential Geometry 3. Classical DG: Upgrade to Calculus 4. Beyond Classical Differential Geometry 1 Course Information Course Organization • Instructor. Xinwei Yu; CAB 527; [email protected]; • Course Webpage. • http://www.math.ualberta.ca/ xinweiyu/348.A1.17f • We will not use eClass. • Getting Help. 1. Office Hours. TBA. 2. Appointments. 3. Emails. 4. It is a good idea to form study groups. 2 Evaluation • Homeworks. 9 HWs; 20%; Worst mark dropped; No late HW. Due dates: 9/22; 9/29; 10/6; 10/20; 10/27; 11/3; 11/10; 12/1; 12/8. 12:00 (noon) in assignment box (CAB 3rd floor) • Midterms. 30%; 10/5; 11/9. One hour. In class. No early/make-up midterms. • Final Exam. Tentative. 50%; 12/14 @9a. Two hours. > 50% =)> D; > 90% =)> A: 3 Resources • Textbook. • Andrew Pressley, Elementary Differential Geometry, 2nd Ed., Springer, 2010. • Reference books. • Most books calling themselves ”Introductory DG”, ”Elementary DG”, or ”Classical DG”. • Online notes. • Lecture notes (updated from Math 348 2016 Notes) • Theodore Shifrin lecture notes. • Xi Chen lecture notes for Math 348 Fall 2015. • Online videos. • Most relevant: Differential Geometry - Claudio Arezzo (ICTP Math). • Many more on youtube etc.. 4 Geometry, Differential • Geometry. • Originally, ”earth measure”. • More precisely, study of shapes.1 • Differential. • Calculus is (somehow) involved. • Classical Differential Geometry. • The study of shapes, such as curves and surfaces, using calculus. -
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. -
Differential Geometry of Manifolds with Density
Rose-Hulman Undergraduate Mathematics Journal Volume 7 Issue 1 Article 2 Differential Geometry of Manifolds with Density Ivan Corwin Harvard University Neil Hoffman, [email protected] Follow this and additional works at: https://scholar.rose-hulman.edu/rhumj Recommended Citation Corwin, Ivan (2006) "Differential Geometry of Manifolds with Density," Rose-Hulman Undergraduate Mathematics Journal: Vol. 7 : Iss. 1 , Article 2. Available at: https://scholar.rose-hulman.edu/rhumj/vol7/iss1/2 Differential Geometry of Manifolds with Density Ivan Corwin, Neil Hoffman, Stephanie Hurder, Vojislav Seˇsum,Yaˇ Xu February 1, 2006 Abstract We describe extensions of several key concepts of differential geometry to manifolds with density, including curvature, the Gauss-Bonnet theorem and formula, geodesics, and constant curvature surfaces. 1 Introduction Riemannian manifolds with density, such as quotients of Riemannian manifolds or Gauss space, of much interest to probabilists, merit more general study. Generalization of mean and Ricci curvature to manifolds with density has been considered by Gromov ([Gr], Section 9.4E), Bakry and Emery,´ and Bayle; see Bayle [Bay]. We consider smooth Riemannian manifolds with a smooth positive density eϕ(x) used to weight volume and perimeter. Manifolds with density arise in physics when considering sur- faces or regions with differing physical density. An example of an important two-dimensional surface with density is the Gauss plane, a Euclidean plane with volume and length weighted by (2π)−1e−r2/2, where r is the distance from the origin. In general, for a manifold with density, in terms of the underlying Riemannian volume dV and perimeter dP , the new weighted volume and area are given by ϕ dVϕ = e dV ϕ dPϕ = e dP. -
Analytic and Differential Geometry Mikhail G. Katz∗
Analytic and Differential geometry Mikhail G. Katz∗ Department of Mathematics, Bar Ilan University, Ra- mat Gan 52900 Israel Email address: [email protected] ∗Supported by the Israel Science Foundation (grants no. 620/00-10.0 and 84/03). Abstract. We start with analytic geometry and the theory of conic sections. Then we treat the classical topics in differential geometry such as the geodesic equation and Gaussian curvature. Then we prove Gauss’s theorema egregium and introduce the ab- stract viewpoint of modern differential geometry. Contents Chapter1. Analyticgeometry 9 1.1. Circle,sphere,greatcircledistance 9 1.2. Linearalgebra,indexnotation 11 1.3. Einsteinsummationconvention 12 1.4. Symmetric matrices, quadratic forms, polarisation 13 1.5.Matrixasalinearmap 13 1.6. Symmetrisationandantisymmetrisation 14 1.7. Matrixmultiplicationinindexnotation 15 1.8. Two types of indices: summation index and free index 16 1.9. Kroneckerdeltaandtheinversematrix 16 1.10. Vector product 17 1.11. Eigenvalues,symmetry 18 1.12. Euclideaninnerproduct 19 Chapter 2. Eigenvalues of symmetric matrices, conic sections 21 2.1. Findinganeigenvectorofasymmetricmatrix 21 2.2. Traceofproductofmatricesinindexnotation 23 2.3. Inner product spaces and self-adjoint endomorphisms 24 2.4. Orthogonal diagonalisation of symmetric matrices 24 2.5. Classification of conic sections: diagonalisation 26 2.6. Classification of conics: trichotomy, nondegeneracy 28 2.7. Characterisationofparabolas 30 Chapter 3. Quadric surfaces, Hessian, representation of curves 33 3.1. Summary: classificationofquadraticcurves 33 3.2. Quadric surfaces 33 3.3. Case of eigenvalues (+++) or ( ),ellipsoid 34 3.4. Determination of type of quadric−−− surface: explicit example 35 3.5. Case of eigenvalues (++ ) or (+ ),hyperboloid 36 3.6. Case rank(S) = 2; paraboloid,− hyperbolic−− paraboloid 37 3.7. -
Teaching General Relativity
Teaching General Relativity Robert M. Wald Enrico Fermi Institute and Department of Physics The University of Chicago, Chicago, IL 60637, USA February 4, 2008 Abstract This Resource Letter provides some guidance on issues that arise in teaching general relativity at both the undergraduate and graduate levels. Particular emphasis is placed on strategies for presenting the mathematical material needed for the formulation of general relativity. 1 Introduction General Relativity is the theory of space, time, and gravity formulated by Einstein in 1915. It is widely regarded as a very abstruse, mathematical theory and, indeed, until recently it has not generally been regarded as a suitable subject for an undergraduate course. In actual fact, the the mathematical material (namely, differential geometry) needed to attain a deep understanding of general relativity is not particularly difficult and requires arXiv:gr-qc/0511073v1 14 Nov 2005 a background no greater than that provided by standard courses in advanced calculus and linear algebra. (By contrast, considerably more mathematical sophistication is need to provide a rigorous formulation of quantum theory.) Nevertheless, this mathematical material is unfamiliar to most physics students and its application to general relativity goes against what students have been taught since high school (or earlier): namely, that “space” has the natural structure of a vector space. Thus, the mathematical material poses a major challenge to teaching general relativity—particularly for a one-semester course. If one take the time to teach the mathematical material properly, one runs the risk of turning the course into a course on differential geometry and doing very little physics. -
Differential Geometry, Part I: Calculus on Euclidean Spaces Jay Havaldar from Wikipedia
Differential Geometry, Part I: Calculus on Euclidean Spaces Jay Havaldar From Wikipedia: Differential geometry is a mathematical discipline that uses the techniques of dif- ferential calculus, integral calculus, linear algebra and multilinear algebra to study problems in geometry. The theory of plane and space curves and surfaces in the three-dimensional Euclidean space formed the basis for development of differential geometry during the 18th century and the 19th century. In short, differential geometry tries to approximate smooth objects by linear approximations. These notes assume prior knowledge of multivariable calculus and linear algebra. Definition: A smooth real-valued function f is one where all partial derivatives and are continu- ous. 0.1 Tangent Vectors The first major concept in differential geometry is that of a tangent space for a given point on a manifold. Loosely, think of manifold as a space which locally looks like Euclidean space; for example, a sphere in R3. The tangent space of a manifold is a generalization of the idea of a tangent plane. Tangent space for a point on a sphere. Image from Wikipedia. Definition: A tangent vector vp consists of a vector v and a point of application p. There is a natural way to add tangent vectors at a point and multiply them by scalars. Definition: If two tangent vectors have the same vector v but different points of application, they are said to be parallel. The best explanation I've seen of tangent vectors is by analogy with the concept of a force in physics. A force applied at different areas of a rod will have different results. -
Differential Geometry and Control
http://dx.doi.org/10.1090/pspum/064 Selected Titles in This Series 64 G. Ferreyra, R. Gardner, H. Hermes, and H. Sussmann, Editors, Differential geometry and control (University of Colorado, Boulder, 1997) 63 Alejandro Adem, Jon Carlson, Stewart Priddy, and Peter Webb, Editors, Group representations: Cohomology, group actions and topology (University of Washington, Seattle, 1996) 62 Janos Kollar, Robert Lazarsfeld, and David R. Morrison, Editors, Algebraic geometry—Santa Cruz 1995 (University of California, Santa Cruz, July 1995) 61 T. N. Bailey and A. W. Knapp, Editors, Representation theory and automorphic forms (International Centre for Mathematical Sciences, Edinburgh, Scotland, March 1996) 60 David Jerison, I. M. Singer, and Daniel W. Stroock, Editors, The legacy of Norbert Wiener: A centennial symposium (Massachusetts Institute of Technology, Cambridge, October 1994) 59 William Arveson, Thomas Branson, and Irving Segal, Editors, Quantization, nonlinear partial differential equations, and operator algebra (Massachusetts Institute of Technology, Cambridge, June 1994) 58 Bill Jacob and Alex Rosenberg, Editors, X-theory and algebraic geometry: Connections with quadratic forms and division algebras (University of California, Santa Barbara, July 1992) 57 Michael C. Cranston and Mark A. Pinsky, Editors, Stochastic analysis (Cornell University, Ithaca, July 1993) 56 William J. Haboush and Brian J. Parshall, Editors, Algebraic groups and their generalizations (Pennsylvania State University, University Park, July 1991) 55 Uwe Jannsen, Steven L. Kleiman, and Jean-Pierre Serre, Editors, Motives (University of Washington, Seattle, July/August 1991) 54 Robert Greene and S. T. Yau, Editors, Differential geometry (University of California, Los Angeles, July 1990) 53 James A. Carlson, C. Herbert Clemens, and David R. -
DIFFERENTIAL GEOMETRY of an M-DIMENSIONAL MANIFOLD in A
DIFFERENTIALGEOMETRY OFAN m-DIMENSIONAL MANIFOLD IN A EUCLIDEANSPACE OF n DIMENSIONS* BY charles e.wilder 1. Introduction This paper had its inspiration in the Einstein Theory. It grew out of an attempt to give geometric interpretation to the Einstein equations for material free space. It was first developed by the methods of Vossf, and BeezJ, but later changed to the simpler notation of Wilson and Moore§, which is a com- bination of vector analysis with the absolute calculus of Ricci and Levi- Civita||. In Voss is to be found the differential geometry of varieties of n— 1 dimensions in a space of n dimensions. In the article of Wilson and Moore is developed the geometry of a two-dimensional manifold in n dimensions. These are the two natural extensions of surface theory to a higher number of dimensions. The object of this paper is to begin the study of the inter- mediate cases. The method of the absolute calculus is developed in great detail in Ricci's Lezioni sulla Teoría délie Superficie, and is there applied to the ordinary surface theory. A sufficient introduction for the purposes of this paper will be found in the paper of Wilson and Moore above mentioned. It is their method that is followed in the deduction of the integrability conditions. It was apparently first given by Ricci in the Lezioni, pp. 87—91. We shall denote by Vm a variety of m dimensions, defined in a euclidean space Pn of n dimensions by means of n—m equations Fa(xx,Xi,...,Xn) = 0 (a = l,2,3,--.,n —1).