AY 155 Spring 1989 ___________________________________________________________________________ The Cosmological Framework: * The choice of (meta)physics: physical laws and constants same everywhere and everywhen; generalized gravity the only important interaction on large scales. * The choice of the theory of gravity: probably the GR, more-or-less. (other possibilities: PPNF, Dirac-Canuto, Milgrom-Beckenstein...) * The choice of topology: simple connected at scales >>> Planck (we hope so). * The choice of symmetries: (e.g., the cosmological principle) - Homogeneity (minimum scale = ?) > FRW models - Isotropy (e.g., no global rotation) NB: The universe does not have to be simple for our brains, taste, etc. The Friedman-Robertson-Walker models: Specified by the "scale" = expansion rate, age, H and "form" = curvature, , q , No. of independent parameters = 3 (usually H , or q , ) Possible complication: a pressure term (=zero?) The "scale" (alias H ): still uncertain by ~ 50%. The "form" (alias , ): uncertain by ~ 100% around the critical values.