On 7/23/2020 7:33 AM, Alan Grayson wrote:


On Thursday, July 23, 2020 at 8:27:52 AM UTC-6, Lawrence Crowell wrote:

    Coordinates are not the basis of physics. Curvatures are
    covariant, while connections and coordinates are not. These can be
    imposed in many ways, similar to a gauge choice.

    LC


That right; coordinates are not the basis of physics. That's why Einstein had to cast his GR equation in tensor form, so the laws of physics would be independent of coordinate systems. But you're asserting, or so it seems, that there is a unique coordinate system wherein the external gravitational effect of a BH can be calculated. This is what I object to. AG

Calculations are always done in some coordinate system.   The method is to calculate something, like the curvature tensor or a proper time, that doesn't depend on which coordinate system you used.

Brent



    On Thursday, July 23, 2020 at 6:49:44 AM UTC-5 [email protected]
    wrote:



        On Thursday, July 23, 2020 at 5:41:42 AM UTC-6, Lawrence
        Crowell wrote:

            On Thursday, July 23, 2020 at 5:56:32 AM UTC-5
            [email protected] wrote:



                On Saturday, July 18, 2020 at 6:31:23 AM UTC-6, Alan
                Grayson wrote:



                    On Saturday, July 18, 2020 at 6:18:28 AM UTC-6,
                    Lawrence Crowell wrote:

                        The tortoise coordinates is found from the
                        Schwarzschild metric

                        ds^2 = (1 - 2m/r)dt^2 - (1 - 2m/r)^{-1}dr^2 -
                        r^2dΩ^2

                        where for a signal leaving a point near the
                        black hole with ds = 0 (null path) and
                        propagating radially out, dΩ = 0, we have dt =
                        dr/(1 - 2m/r) which then leads to

                        T = t - t0 - 2m ln|r - 2m|.

                        That is the tortoise coordinate. Please look
                        this up to read further. I can't spend
                        beaucoup time going over this for weeks to come.

                        LC


                    You don't have to. We're done.  But you should IMO
                    address Brent's objection, maybe on another thread. AG


                When it comes to GR, you're a genius; no question
                about it. I wouldn't want to waste your valuable time.
                But consider this; the Schwartzschild metric applies
                to NON-ROTATING masses. Do you really think a massive
                contracting star which forms a BH will be
                non-rotating? Obviously, it will be RAPIDLY rotating,
                like an ice skater who contracts her arms. Brent also
                had some substantive questions about your model. But I
                see you prefer your illusions than to address his
                objections. AG


            The result is similar, but more complex. The same
            calculation can be done for the Kerr solution. It is just
            a lot more complicated mathematically.

            LC


        If you say so. In any event, the idea that an objectively
        existing gravitational field outside a BH should depend on the
        choice of a particular coordinate system, seems a non-starter. AG

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