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jake jot
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All normal relativists already adapted the point of view of "no metric, no thing"? Who are the relativists who don't?
John Stachel who wrote the book Einstein from B to Z is a veteran 90 year old relativist.
Einstein from 'B' to 'Z' - John Stachel - Google Books
Which textbooks are described as "introducing a global manifold (the points of which are usually identified forthwith with events - I have already discussed that problem), and then put such structures on this manifold as the metric tensor field."?
Who are the lecturers who "we are pulling a swindle when we tell students, as our definitions imply, that you first pick the manifold and then solve the field equations on it.". Why is our current GR not like this? What versions of GR are like this?
John Stachel who wrote the book Einstein from B to Z is a veteran 90 year old relativist.
Einstein from 'B' to 'Z' - John Stachel - Google Books
Even relativists have not yet fully adopted the point of view, "no metric, no nothing". If you look at the way the general theory of relativity is formulated mathematically in even the most careful treatises, for example, you see this clearly. They start out by introducing a global manifold (the points of which are usually identified forthwith with events - I have already discussed that problem), and then put such structures on this manifold as the metric tensor field. Is that the way that anyone of us actually goes about solving the field equations of general relativity? Of course not. One first solves them on a generic patch, and then one tries to maximally extend the local solution (using some criteria for acceptable extensions) from that patch to a global manifold, which is not known ahead of time. Before solving the field equations, one generally doesn't know the global manifold on which the solution will turn out to be maximally extended. So we are pulling a swindle when we tell students, as our definitions imply, that you first pick the manifold and then solve the field equations on it."
Which textbooks are described as "introducing a global manifold (the points of which are usually identified forthwith with events - I have already discussed that problem), and then put such structures on this manifold as the metric tensor field."?
Who are the lecturers who "we are pulling a swindle when we tell students, as our definitions imply, that you first pick the manifold and then solve the field equations on it.". Why is our current GR not like this? What versions of GR are like this?