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Tensors: the mathematics of relativity theory and continuum mechanics PDF

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Tensors Anadijiban Das Tensors The Mathematics of Relativity Theory and Continuum Mechanics AnadijibanDas DepartmentofMathematicsand PacificInstitutefortheMathematicalSciences SimonFraserUniversity 8888UniversityAvenue Burnaby,V5A1S6 BC,Canada ISBN978-0-387-69468-9 e-ISBN978-0-387-69469-6 LibraryofCongressControlNumber:2006939203 (cid:2)c 2007SpringerScience+BusinessMedia,LLC Allrightsreserved.Thisworkmaynotbetranslatedorcopiedinwholeorinpartwithoutthewritten permissionofthepublisher(SpringerScience+BusinessMedia,LLC,233SpringStreet,NewYork, NY10013, USA),exceptforbriefexcerpts inconnection withreviews orscholarly analysis. Use inconnection with any form of information storage and retrieval, electronic adaptation, computer software,orbysimilarordissimilarmethodologynowknownorhereafterdevelopedisforbidden. Theuseinthispublicationoftradenames,trademarks,servicemarksandsimilarterms,evenifthey arenotidentifiedassuch,isnottobetakenasanexpressionofopinionastowhetherornottheyare subjecttoproprietaryrights. Printedonacid-freepaper. 9 8 7 6 5 4 3 2 1 springer.com Dedicated To Sri Sarada Devi Preface Tensor algebra and tensor analysis were developed by Riemann, Christoffel, Ricci, Levi-Civita and others in the nineteenth century. The special theory of relativity, as propounded by Einstein in 1905, was elegantly expressed by Minkowski in terms of tensor fields in a flat space-time. In 1915, Einstein formulated the general theory of relativity, in which the space-time manifold is curved. The theory is aesthetically and intellectually satisfying. The general theory of relativity involves tensor analysis in a pseudo- Riemannian manifold from the outset. Later, it was realized that even the pre-relativistic particle mechanics and continuum mechanics can be elegantly formulatedintermsoftensoranalysisinthethree-dimensionalEuclideanspace. In recent decades, relativistic quantum field theories, gauge field theories, and various unified field theories have all used tensor algebra analysis exhaustively. This book develops from abstract tensor algebra to tensor analysis in vari- ousdifferentiablemanifolds inamathematically rigorousandlogically coherent manner. The material is intended mainly for students at the fourth-year and fifth-year university levels and is appropriate for students majoring in either mathematical physics or applied mathematics. The first chapter deals with tensor algebra, or algebra of multilinear map- pings in a general field F. (The background vector space need not possess an inner product or dot product.). The second chapter restricts the algebraic field to the set of real numbers R. Moreover, it is assumed that the underlying real vector space is endowed with an inner product (or dot product). Chapter 3 defines and investigates a differentiable manifold without imposing any other structure. Chapter 4 discusses tensor analysis in a general differentiable man- ifold. Differential forms are introduced and investigated. Next, a connection formindicatingparalleltransportisbroughtforward. Asalogicalconsequence, the fourth-order curvature tensor is generated. Chapter 5 deals with Rieman- nianandpseudo-Riemannianmanifolds. Tensoranalysis,intermsofcoordinate componentsaswellasorthonormalcomponents,isexhaustivelyinvestigated. In Chapter 6, special Riemannian and pseudo-Riemannian manifolds are studied. Flat manifolds, spaces of constant curvature, Einstein spaces, and conformally flat spaces are explored. Hypersurfaces and submanifolds embedded in higher- dimensional manifolds are discussed in chapter 7. Extrinsic curvature tensors vii viii Preface are defined in all cases. Moreover, Gauss and Codazzi-Mainardi equations are derived. We would like to elaborate on the notation used in this book. The let- ters i, j, k, l, m, n, etc., are used for the subscripts and superscripts of a tensor field in the coordinate basis. However, we use the letters a, b, c, d, e, f, etc., for subscripts and superscripts of the same tensor field rela- tive to an orthonormal basis. The numerical enumeration of coordinate com- ponents vi of a vector field is given by v1,v2,...,vN. However, numerical elaboration of orthonormal components of the same vector field is furnished by v(1),v(2),...,v(N) (toavoidconfusion). Similardistinctionsaremadefortensor fieldcomponents. Theflat metriccomponentsaredenotedeitherby d or d . ij ab (The usual symbol η.. is reserved only for the totally antisymmetric pseudo- tensorofLevi-Civita.) ThegeneralizedLaplacianinthe N-dimensionisdenoted by Δ. I would like to acknowledge my gratitude to several people for various rea- sons. During my stay at the Dublin Institute for Advanced Studies from 1958 to 1961, I learned a lot of classical tensor analysis from the late Professor J. L. Synge, F. R. S.. Professor W. Noll, a colleague of mine at Carnegie- Mellon University from 1963 to 1966, introduced me to the abstract tensor algebra, or the algebra of multilinear mappings. My research projects and teachings on general relativity for many years have consolidated the under- standingoftensors. Dr.AndrewDeBenedictishaskindlyreadtheproof, edited and helped with computer work. Mrs. Judy Borwein typed from chapter 1 to chapter 5 and edited the text diligently and flawlessly. Mrs. Sabine Leb- hart typed the difficult chapter 7 and appendices. She also helped in the final editing. Mr. Robert Birtch drew thirty-four figures of the book. Last but not least, my wife, Mrs. Purabi Das, was a constant source of encourage- ment. Contents Preface vii List of Figures xi 1 Finite-Dimensional Vector Spaces and Linear Mappings 1 1.1 Fields . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 1.2 Finite-Dimensional Vector Spaces . . . . . . . . . . . . . . . . . . 3 1.3 Linear Mappings of a Vector Space . . . . . . . . . . . . . . . . . 9 1.4 Dual or Covariant Vector Spaces . . . . . . . . . . . . . . . . . . 11 2 Tensor Algebra 16 2.1 Second-Order Tensors . . . . . . . . . . . . . . . . . . . . . . . . 16 2.2 Higher-Order Tensors . . . . . . . . . . . . . . . . . . . . . . . . 24 2.3 Exterior or Grassmann Algebra . . . . . . . . . . . . . . . . . . . 31 2.4 Inner Product Vector Spaces and the Metric Tensor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42 3 Tensor Analysis on a Differentiable Manifold 52 3.1 Differentiable Manifolds . . . . . . . . . . . . . . . . . . . . . . . 52 3.2 Tangent Vectors, Cotangent Vectors, and Parametrized Curves . . . . . . . . . . . . . . . . . . . . . . . . . 60 3.3 Tensor Fields over Differentiable Manifolds . . . . . . . . . . . . 69 3.4 Differential Forms and Exterior Derivatives . . . . . . . . . . . . 80 4 Differentiable Manifolds with Connections 92 4.1 The Affine Connection and Covariant Derivative . . . . . . . . . 92 4.2 Covariant Derivatives of Tensors along a Curve . . . . . . . . . . 101 4.3 Lie Bracket, Torsion, and Curvature Tensor . . . . . . . . . . . . 107 ix x Contents 5 Riemannian and Pseudo-Riemannian Manifolds 121 5.1 Metric Tensor, Christoffel Symbols, and Ricci Rotation Coefficients . . . . . . . . . . . . . . . . . . . 121 5.2 Covariant Derivatives and the Curvature Tensor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 135 5.3 Curves, Frenet-Serret Formulas, and Geodesics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 157 5.4 Special Coordinate Charts . . . . . . . . . . . . . . . . . . . . . . 181 6 Special Riemannian and Pseudo-Riemannian Manifolds 200 6.1 Flat Manifolds . . . . . . . . . . . . . . . . . . . . . . . . . . . . 200 6.2 The Space of Constant Curvature . . . . . . . . . . . . . . . . . . 205 6.3 Einstein Spaces . . . . . . . . . . . . . . . . . . . . . . . . . . . . 214 6.4 Conformally Flat Spaces . . . . . . . . . . . . . . . . . . . . . . . 216 7 Hypersurfaces, Submanifolds, and Extrinsic Curvature 225 7.1 Two-Dimensional Surfaces Embedded in a Three-Dimensional Space . . . . . . . . . . . . . . . . . . . . 225 7.2 (N −1)-Dimensional Hypersurfaces . . . . . . . . . . . . . . . . 233 7.3 D-Dimensional Submanifolds . . . . . . . . . . . . . . . . . . . . 245 Appendix 1 Fibre Bundles 257 Appendix 2 Lie Derivatives 263 Answers and Hints to Selected Exercises 271 References 277 List of Symbols 280 Index 285 List of Figures 3.1 A chart (χ,U) and projection mappings. . . . . . . . . . . . . . 53 3.2 Two charts in M and a coordinate transformation. . . . . . . . . 54 3.3 Spherical polar coordinates. . . . . . . . . . . . . . . . . . . . . . 57 3.4 A function from U ⊂M into R. . . . . . . . . . . . . . . . . . . 57 3.5 A Ck-diffeomorphism F. . . . . . . . . . . . . . . . . . . . . . . 58 3.6 Tangent vector in E and R3. . . . . . . . . . . . . . . . . . . . 60 3 3.7 A curve γ into M. . . . . . . . . . . . . . . . . . . . . . . . . . . 65 3.8 Reparametrization of a curve. . . . . . . . . . . . . . . . . . . . . 67 3.9 The Jacobian mapping of tangent vectors. . . . . . . . . . . . . . 74 3.10 A star-shaped domain in R2. . . . . . . . . . . . . . . . . . . . . 85 3.11 A star-shaped domain D∗ in R3. . . . . . . . . . . . . . . . . . . 87 2 4.1 Parallel propagation of a vector along a curve.. . . . . . . . . . . 102 4.2 Parallel transport along a closed curve.. . . . . . . . . . . . . . . 117 5.1 Deformation of a cubical surface into a spherical one. . . . . . . . 154 5.2 A circular helix in R3. . . . . . . . . . . . . . . . . . . . . . . . . 163 5.3 Two-dimensional surface generated by geodesics. . . . . . . . . . 172 5.4 Geodesic deviation between two neighboring longitudes. . . . . . 175 5.5 An incomplete manifold R2−{(0,0)}. . . . . . . . . . . . . . . . 177 5.6 The exponential mapping. . . . . . . . . . . . . . . . . . . . . . . 183 5.7 A normal coordinate x(cid:2)N. . . . . . . . . . . . . . . . . . . . . . . 189 6.1 The normal section of M along (cid:4)t(x). . . . . . . . . . . . . . . . 206 2 6.2 (i) A plane, (ii) a sphere, and (iii) a saddle-shaped surface. . . . 206 (cid:3) 7.1 A two-dimensional surface embedded in R3. . . . . . . . . . 226 2 7.2 A smooth surface of revolution. . . . . . . . . . . . . . . . . . . . 231 (cid:3) 7.3 The image of a parametrized hypersurface ξ. . . . . . . . 234 N−1 7.4 Coordinate transformation and reparametrization of hypersurface ξ. . . . . . . . . . . . . . . . . . . . . . . . . . . 235 7.5 Change of normal vector due to extrinsic curvature. . . . . . . . 241 xi

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