Page 8 - Nature Of Space And Time
P. 8

ought to be a globally hyperbolic region in which there ought to be conjugate points on
               every geodesic between two points. This establishes a contradiction which shows that the
               assumption of geodesic completeness, which can be taken as a de nition of a non singular
               spacetime, is false.
                    The reason one gets conjugate points in spacetime is that gravity is an attractive force.

               It therefore curves spacetime in such a way that neighbouring geodesics are bent towards
               each other rather than away. One can see this from the Raychaudhuri or Newman-Penrose
               equation, which I will write in a uni ed form.



                          Raychaudhuri - Newman - Penrose equation


                                           d         2        ij         1     a b
                                                =       +     ij +        R abl l
                                           dv                            n

                       where n = 2 for null geodesics
                               n = 3 for timelike geodesics




               Here v is an a ne parameter along a congruence of geodesics, with tangent vector l           a
               which are hypersurface orthogonal. The quantity   is the average rate of convergence of
                                                                           a b
               the geodesics, while   measures the shear. The term R abl l gives the direct gravitational
               e ect of the matter on the convergence of the geodesics.


                          Einstein equation


                                                          1
                                                R ab −     g abR =8 T ab
                                                          2


                          Weak Energy Condition


                                                           a b
                                                      T abv v    ≥ 0

                                                   a
                          for any timelike vector v .


                                                                                        a
               By the Einstein equations, it will be non negative for any null vector l if the matter obeys
               the so called weak energy condition. This says that the energy density T 00 is non negative
               in any frame. The weak energy condition is obeyed by the classical energy momentum
               tensor of any reasonable matter, such as a scalar or electro magnetic  eld or a 
uid with


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