Przyk, I must correct this:
GNUFDL image by Johnstone, see wikipedia
It isn't flat, just as a mountain isn't flat. Yes, this "rubber-sheet" depiction isn't ideal, but it isn’t totally wrong. Imagine you’ve placed a whole lot of parallel-mirror light-clocks in an equatorial slice through the Earth and the surrounding space. When you plot all the clock rates, your plot looks like the picture above. It's from the Wikipedia Riemann curvature tensor article. And the crucial point is this: The "Riemann manifold" is curved because the speed of light is not constant. If it was constant throughout the room you're in, those NIST optical clocks would stay synchronised, and your pencil wouldn't fall down. Light wouldn't curve down either, because "a curvature of rays of light can only occur when the speed of light varies with position". Look again at Ned Wright's deflection and delay of light: "In a very real sense, the delay experienced by light passing a massive object is responsible for the deflection of the light". Light doesn't curve because spacetime is curved. Light curves because the speed of light varies with position. Spacetime is curved because the speed of light varies with position. Because a concentration of energy in the guise of a star "conditions" the surrounding space. It doesn't curve it, it renders it inhomogenous. See Baez: "Note: not the curvature of space, but of spacetime. The distinction is crucial". Space isn't curved in the room you're in, it's "neither homogeneous nor isotropic".
Spacetime is not what space is. It's an abstract thing, a mathematical model in which motion does not occur. The "Riemann manifold" is similarly abstract. Here's a depiction of it:The infinitesimal local gravitational field doesn't have any effect on a local measurement of the speed of light. Tangent to every point on the riemann manifold the spacetime is flat. Same as at boundary. Flat...
GNUFDL image by Johnstone, see wikipedia
It isn't flat, just as a mountain isn't flat. Yes, this "rubber-sheet" depiction isn't ideal, but it isn’t totally wrong. Imagine you’ve placed a whole lot of parallel-mirror light-clocks in an equatorial slice through the Earth and the surrounding space. When you plot all the clock rates, your plot looks like the picture above. It's from the Wikipedia Riemann curvature tensor article. And the crucial point is this: The "Riemann manifold" is curved because the speed of light is not constant. If it was constant throughout the room you're in, those NIST optical clocks would stay synchronised, and your pencil wouldn't fall down. Light wouldn't curve down either, because "a curvature of rays of light can only occur when the speed of light varies with position". Look again at Ned Wright's deflection and delay of light: "In a very real sense, the delay experienced by light passing a massive object is responsible for the deflection of the light". Light doesn't curve because spacetime is curved. Light curves because the speed of light varies with position. Spacetime is curved because the speed of light varies with position. Because a concentration of energy in the guise of a star "conditions" the surrounding space. It doesn't curve it, it renders it inhomogenous. See Baez: "Note: not the curvature of space, but of spacetime. The distinction is crucial". Space isn't curved in the room you're in, it's "neither homogeneous nor isotropic".