Calculate phenomena.....like what?
Are you being serious? When experiments are performed to test GR what do you think they studying? The phenomena of light and matter and their respective motions. What else do you think those experiments do???
A metric describing the phenomena of light and matter rather. Because, and correct me if I am wrong here, but what experiment done to verify this metric didn’t observe phenomena? None?
And it's not flat no matter what coordinate system you choose to represent it in.
I never claimed it wasn’t Mr Spinkles.
Its curvature is specified by the spacetime metric tensor, g which essentially gives us rules for calculating distances and so forth between events A and B, which are points in spacetime by definition.
Defining it so doesn’t make it so. Especially when the experimental evidence to hand is testing phenomena within spacetime.
Now, you can argue that, actually, there is some higher space that is the "real" spacetime, and it is indeed flat....
That’s not what I’m arguing. It would be an example illustrating the difference between a metric measuring spacetime and a metric measuring the geometry of phenomena within that spacetime.
but if it is above and beyond the 3 spatial and 1 time coordinate physicists know and love, and we can't measure it, its very existence is mere speculation, much less its flatness vs. its curvature.
Last I checked the 3+1 spacetime hasn’t been measured either. Phenomena within it have been measured, but not the spacetime itself.
Meanwhile, we do need words to describe the 4D space we can actually measure and that word is "spacetime" and it is a curved space.
If you are doing this then you are defining spacetime to be the geometrical set in which light and matter move through. Fair enough but that is different that defining spacetime to be the points (t,x,y,z) and then claiming it is curved on the basis of observing and measuring phenomena within that set.
No no, the metric metric in tensor form is an abstract object, just like a vector in its abstract form, it is its own, independent thing and unaffected no matter what coordinate system you choose.
Exactly which part of the following do you disagree with?:
Different coordinate systems give different metrics though, but these metrics should be [/u]isomorphic to each other. You want to disagree in this point with then fine – but you will be disagreeing with a well known fact of metric spaces.
Like a vector, only its representation changes when you express it explicitly in terms of a chosen coordinate system.
That’s what isomorphic means here….
The abstract metric tells you the curvature of space,
Or rather the curvature of the phenomena’s geometry.
However, you could say the same thing about light itself.
…
So you could say there really is no such thing as the EM field, and therefore no light, it is all just charges interacting with each other, and the mathematics of the EM field is just a trick to capture this interaction.
This analogy isn’t really capturing what is going on here. I don’t have a problem that the EM field exists, and the equations represent the EM interactions through that field, etc. – I don’t buy the next step which is to equate the EM field with spacetime. That’s the step that I don’t as being justified – particularly when spacetime is previously defined in manner independent of the phenomena within it being measured.
But one picture is useful and predictive and the other is not.
This isn’t the case. None of the predictions you can make with GR require extrapolating spacetime further than is justifiable. Not even gravity waves.
The idea that the set of points (t,x,y,z) is the spacetime of the phenomena represented by the metrics seems intuitive – but what evidence is there really that this is so? Galilean relativity was intuitive too until GR came along.