plus, how awesomely beautiful is the idea of tendrils of has connecting the galaxies through space.
plus, how awesomely beautiful is the idea of tendrils of has connecting the galaxies through space.
However, we've only been able to actually detect much less than that 5% contribution of the atomic matter in the Universe, meaning that we expect there's a lot more ordinary matter out there that we can't see. This research indicates that a big chunk of that missing ordinary matter is in the form of huge warm gas clouds on galactic scales.
My understanding is that, up until now, we could only observe half of the 5% expected mass, e.g. 2.5%, and we can now see the rest of it. The rest of the universe is still made up of 25% dark matter and 70% dark energy.
Assuming I'm interpreting this correctly, this means that there's still around 70% of expected baryonic matter unaccounted for.
So, if the stretching thing is true, would there be areas with absolutely no matter or anything at all?
Can anyone clarify how these filaments remain “hot”?
comes to mind
Ott 1963 shows T' = T / {\sqrt{1 - v^2 / c^2}}, or for short T' = \gamma T, where \gamma is the Lorentz factor, T' is the temperature calculated by an observer in a set of coordinates Lorentz boosted with respect to the coordinates in which the system is at rest with a temperature T.
Asymptotically one would expect that as \gamma -> 1 \RightArrow T = T' and \gamma -> \infty \RightArrow T = \infty assuming one is measuring temperature using photocalorimetry (consider a blackbody radiator...).
However, there are different proposals that depend on how and if one makes the first or second laws of thermodynamics Lorentz covariant, and how one goes about measuring a distant object's temperature. All of this is also in the context of Special Relativity; a general relativist could say that the whole matter comes down to a choice of gauge anyway, and temperatures are only directly comparable for two objects at the same point in spacetime (and even there you get a can of worms because they would then be "in contact" at the point p on the manifold, and even then there is a choice of gauge and some interesting cut-offs in which they could equilibriate (T_obj1 = T_obj2), dissipate excess stress-energy (T_{p} > T_obj1 + T_obj2), or collapse gravitationally).
Unfortunately the matter is not wholly settled and there is an absence of firm experimental evidence, and moreover the debate is confined to flat spacetime.
However, one has to do quite a bit of twisting to assume that T = T' (Landsberg did this in 1966 & 1967).
Here is a nice recent set of slides on temperature in GR: http://www.dpg-physik.de/dpg/pbh/aktuelles/pdf/Andersson.pdf
Q. Is a moving body hot/cold? A. Yes/no/maybe. The discussion is "pointless".
There are lots of "cosmic web" renderings from large-scale cosmological simulations of dark mater and the formation of structure in the universe. A major one, now over a decade old is the "Millennium Simulation": http://wwwmpa.mpa-garching.mpg.de/galform/millennium/