On 12/22/2017 3:43 AM, [email protected] wrote:


On Friday, December 22, 2017 at 7:45:42 AM UTC, Brent wrote:



    On 12/21/2017 11:06 PM, [email protected] <javascript:> wrote:


    On Friday, December 22, 2017 at 4:46:10 AM UTC, Brent wrote:



        On 12/21/2017 4:22 PM, [email protected] wrote:


        On Thursday, December 21, 2017 at 11:03:53 PM UTC, Brent wrote:



            On 12/21/2017 2:04 PM, [email protected] wrote:


            On Tuesday, December 19, 2017 at 8:51:51 PM UTC, Brent
            wrote:



                On 12/18/2017 11:44 PM, [email protected] wrote:

                    Invariants are always the important things in
                    physics because they are what we can have
                    intersubjective agreement on.

                    Brent


                *IIUC, the field equations are covariant, which
                means coordinate system independent. *

                Right.  Covariant means that something that changes
                in such a way that invariant things remain the
                same.  So vectors components transform covariantly
                so that they keep the vector physically the same.

                *Isn't Newton's Law of Gravitation also coordinate
                independent? That is, if we use Newton to
                calculate the planetary orbits, won't we get the
                same results in different coordinate systems? *
                Right.

            *
            If Newton's Law of Gravitation is covariant -- that is,
            coordinate frame independent -- I'd expect it to to be
            invariant between inertial frames, but I don't believe
            it is. That is, I don't think a LT between inertial
            frames will leave the form of the law unchanged. How do
            you resolve this problem? TIA, AG
            *

            Don't use a Lorentz transform between frames in a
            Galilean invariant theory.


        *OK, So why didn't Einstein do what he did for classical
        mechanics which is not Lorentz invariant, and directly
        modify Newton's Law of Gravitation? AG*

        (a) I don't read minds, and especially not Einstein's  and
        (b) I don't know what "directly modify" means.

        Brent


    *He changed (= directly modified) the laws of mechanics to make
    them Lorentz invariant. So why can't that be done for Newton's
    Law of Gravitation? Does that law work for any inertial frame? AG*

    Newton's gravity is a field theory.  It implies an infinite speed
    of changes in the gravitational field.  That wasn't consistent
    with relativity.  What you're calling "directly modified" was just
    local mechanics, not fields.

    Brent


*When you think about it, it's apriori highly improbable that Newtonian gravity would work as well as it does, say for planetary orbits, given the substantial light times between the Sun and the planets, and between the planets. AG
*

It's an interesting point that if you just take Newton's theory and allow for the finite travel time of gravitational fields, so each body is attracted toward the point another body was in past, the theory doesn't work at all.

Brent

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