Ich said:
I think you completely missed Naty1's point: the "cosmological proper distance" - which is only dependent on the scale factor for comoving objects - is just one of the infinitely many distances you may define in GR.
Agreed, there are many distances used but that was not what Naty1 said, I'll comment on his post below to clarify.
More importantly the balloon analogy uses one specific definition. In particlular Ned Wright's balloon animations show "photons" crawling over the surface at
constant speed relative to the local rubber which is great for explaining why superluminal rates of expansion don't violate SR. They're not the only balloon illustrations on the web of course but can be taken as representative, for a layman introduction we shouldn't need to be concerned about subtleties of distance definitions.
And, importantly, it is not consistent with the common definitions of distance we encounter outside cosmology.
If I am given two dots drawn on a sheet of paper and asked to find out the distance between them, I would place a ruler passing through the dots and read off the distance. The ruler is on the sheet for the duration of the measurement and I understand that to be a measurement made "now". Cosmological distance is defined as the sum of a set of rulers which happen to be laid exactly end to end at a particular cosmological time which directly corresponds to the ruler on a sheet of paper. I would suggest that is the most common understanding of distance you will find if you ask random members of the public.
On the other hand, if I send a radar pulse to a distant target and measure half the return time, I get "radar distance", the locations of the end points of the path are measured at different times. If you consider
when the distance has the measured value, it was at the instant the signal was reflected, not "now" when it is received and the measurement is obtained.
In fact I inluded this graphic previously to illustrate the loci (past history worldlines) of comoving galaxies and photons on our past light cone:
http://www.astro.ucla.edu/~wright/omega_2.gif
The return path of a radar distance would be measured along the red line so obviously isn't the distance along the circumference of the balloon. One point Naty1 and others have made is that the distances are not measured along geodesics. The average person who is learning about cosmology from the balloon analogy probably has no idea what a geodesic is anyway. Just as for all light-like worldlines, the red line in the graph is a null geodesic.
Naty1 specifically said:
Naty1 said:
So for me, three key concepts from this thread which are not captured by the balloon analogy are that 'expanding space', balloon stretching, is misleading, distance increases are dependent on acceleration, not speed,
That is not true, the "acceleration" is only the rate of change of "speed" and "speed" is only sensibly defined as rate of change of distance anyway.
Naty1 said:
characteristics, and distances are both model and coordinate dependent meaning, observer dependent.
While it is true that they are model dependent, the balloon analogy is only illustrating one specific model, the Friedmann Equations or "FLRW model", just note how often Naty1 used "FLRW" in his reply, there were more in the sections I've omitted:
Naty1 said:
Here is a first draft list [in no particular order] : FLRW is the standard [cosmological] model; FLRW metric [distance measure] is an exact solution to the EFE but only approximates our universe because it assumes the universe is homogeneous and isotropic;
Obviously it is no use for say a steady-state model.
Naty1 said:
superluminal expansion distances are are result of the FLRW model metric; those FLRW distances are NOT great circles nor geodesics on the balloon,
Specifically they
are great circle distances on the balloon. One of the positive features of the balloon analogy is that (in Ned's version at least) you can see how photons move over the surface, always at c while widely separated points can move apart faster thus illustrating how superluminal rates of increasing distance in the FLRW model do NOT contradict SR, a point that puzzles many laymen. You can also see how some photons moving towards a distant galaxy are failing to catch up to it, hence how there can be a horizon to our observable universe.
I kept my reply concise because I didn't want to focus on these few points, the majority of Naty1's reply was on the ball and IMO a very useful contribution but since you have raised the point, I've had to clarify what I was hinting at. Since this is being considered for a web page which may be viewed by many people for many years, and the author has had the courage to open his work to peer review, I think it is important that we should do our best to provide accurate and constructive criticism for him to consider.