ideasrule said:
Alright, a detailed explanation. Let's consider all galaxies that are 11 billion light years away (measured by the travel time of light).
...
If you want to give clear explanations of the kind of thing OP asked about, I would advise you to use proper distance which is what you'd measure if you could freeze expansion.
What beeres, the OP, asked about was essentially the angular size and angular separation of stuff that we see from early times---that is, high redshifts.
What that depends on, a lot, is how far the matter was from our matter
then.
As a real distance. (the relation between light travel time and real distance is very irregular due to different rates of expansion during travel, it depends on when the trip was made, better not to use traveltime as measure of distance in this situations)
Ned Wright's calculator gives you angular size conversion numbers for the various redshifts.
But a good way to understand is with a simple example. Back around 380,000 some matter (call it "A") radiated some light which we are now receiving as microwave. The actual distance to A then, if you could have frozen expansion, was only 41 million LY! That's fairly close.
Matter A and our matter (which became our galaxy and us) were only 41 million LY apart.
Now we are 45 billion LY apart. The conventional figure for the microwave background redshift is z = 1090. That's how much the distances have expanded and also the wavelengths, while the light was traveling.
So when we look back in time----to high redshifts like z = 1090----we really are examining a very dense universe where the material which eventually became millions of galaxies was arrayed around us on a sphere with radius only a measely 41 million LY.
So dense in fact that sound waves could travel through it and did so, contributing overdense and underdense regions that became part of the cobwebby structure of vast strands and clusters of galaxies which we can observe. We observe the (effects of the) soundwaves in that denser gaseous universe.
You can do the same with smaller redshifts like z = 7, where we can already see protogalaxies, quasars. Ned Wright's calculator will tell you the angular-size distance, which was the distance
then (real distance measured by light travel if you could have frozen expansion then).
Thanks for explaining the angular separation of the stars to beer-research. I'm just suggesting how to improve/sharpen the concepts, not any basic change.
The physical meaning of angular separation in the sky depends on the distance that you attribute, which should be the distance
then. You should always be prepared to grab the wright calculator and find out what distance then corresponds to a given redshift.
For people who aren't familiar with the wright calculator---just google "wright calculator" and you will get
http://www.astro.ucla.edu/~wright/CosmoCalc.html
and if you put in z=7 you will get that the distance then was 3.6 billion LY, and of course the distance now is 7 times farther. It also tells the travel time. (but not the travel time "distance", which is a concept for kiddies.)