Naty1 said:
yes, I agree with your explanation...
but how does one calculate the velocity as in the above example in the FRW model?? It never occurred to me previosuly that the Doppler calculation was for flat spacetime...I never thought about it...
As I understand it, the scale factor is unique to the FRW model, and found some aspects of it here:
http://en.wikipedia.org/wiki/Friedmann-Lemaître-Robertson-Walker_metric
All I understand so far is that the scale factor is a non uniform one wrsp to time...
Thanks.
Here, I'll summarize a little bit about what I know about it. I recently got a writing pad and heard about this Jing software. It's kind of nice, for a change, since I can't read my own notes most of the time, I could watch these videos and actually remember what in the world I was doing.
http://screencast.com/t/PTSKqy01uNVI
Looking up the FLRW metric on Wikipedia, I "imagine" that dSIGMA is sort of a volume element, then scroll down to the definition of dSIGMA, and find it's sort of a modified form of a volume element. I'm not entirely confident in the concept of "Reduced circumference." An aside about the tangent function.
http://screencast.com/t/gnazhwpw5hFU
Trying to convert dSIGMA from
spherical into cartesian Coordinates. (I'm not well-practiced at differential equations, by the way, so I'm not entirely sure this approach will get you very far). derivatives of arc-cosine and arc-tangents found at:
http://www.themathpage.com/acalc/inverse-trig.htm. This video starts the problem but doesn't finish it.
http://screencast.com/t/ui4UQ63mhvn
I remembered that when I've tried this problem before, I was converting from
cartesian-to-spherical, which may be easier to do, but still quite time-consuming. Again, this video only starts the problem. It would take much longer than five minutes to do the whole thing.
http://screencast.com/t/apU5PpGn
Here are Einstein Field Equations, and two solutions to it; the FLRW metric, and the Schwarzschild metric, Coefficients in front of dr^2 and dt^2. Effect of setting k=0 and a(t)=1 in the FLRW metric. This video asks a couple of questions that I really never have figured out. (1) how can you plug these metrics into the EFE's and actually see that they are "solutions" and (2) How can you have a function of r as a coefficient of the dr^2 term, and still be a homogeneous metric?