Page 355 - DMTH402_COMPLEX_ANALYSIS_AND_DIFFERENTIAL_GEOMETRY
P. 355

Complex Analysis and Differential Geometry                      Richa Nandra, Lovely Professional University




                    Notes                                   Unit 29: Geodesics




                                     CONTENTS
                                     Objectives

                                     Introduction
                                     29.1 Geodesics
                                     29.2 The Riemann Curvature Tensor
                                     29.3 The Second Variation of Arc length
                                     29.4 Summary

                                     29.5 Keywords
                                     29.6 Self Assessment
                                     29.7 Review Questions

                                     29.8 Further Readings



                                   Objectives

                                   After studying this unit, you will be able to:
                                       Define Geodesics
                                   
                                       Explain the Riemann Curvature Tensor
                                   
                                       Discuss the Second Variation of Arc length
                                   
                                   Introduction

                                   In particular, we will ignore the Gauss map and the second fundamental form. Thanks to Gauss’
                                   Theorema Egregium, we will still be able to take the Gauss curvature into account. In last unit,
                                   you have studied about local intrinsic Geometry of Surfaces.

                                   29.1 Geodesics


                                   Definition 1. Let (U, g) be a Riemannian surface, and let  : I   U  be a curve. A vector field along
                                                            .
                                                            2
                                                                                        i
                                    is a smooth function  Y : I    The covariant derivative of  Y  y   along  is the vector field:
                                                                                         i
                                                                            j
                                                                      y  
                                                                   Y   i  i jk y    k   . i
                                   Note that if Z is any extension of Y, i.e., a any vector field defined on a neighborhood V of the
                                   image    I   of  in U, then we have:
                                                                        Z     i Z .
                                                                     Y      ;i







          348                               LOVELY PROFESSIONAL UNIVERSITY
   350   351   352   353   354   355   356   357   358   359   360