Zeno said:
I was thinking a bit about the farthest parts of the universe we can see and I came to a few interesting questions that are maybe obvious to more studied physicists but new to me. Is the ~14 billion light year distance we can see in all directions slowly expanding with time? In another billion years will we see 15 billion light years in every direction? If so, does that mean the surface of that observable sphere is always going to look like the very early universe, just after the big bang? That leads to my next thought, from our perspective is the Earth located at the "oldest" point in space we can see?
actual light travel time is not very useful as index of distance because distances are constantly expanding at a constantly changing rate. I suggest you think in terms of "freeze-frame" lightyears, so-called "proper distance". That you would measure if you could PAUSE expansion at some particular moment (like,for example, now) to give time to measure it.
The most distant matter we can see now or could detect with better instruments is matter which is NOW about 46 billion ly. That is proper distance. It is that size because of how much distances expanded while light was in transit.
The most distant matter we will EVER be able to see or detect is matter which is NOW about 63 billion ly from us.
The 46 and 63 are figures from the rightmost column of this table. This gives the PARTICLE HORIZON (the radius of the observable region) multiplied by the scale factor "a". The size to which distances have expanded. So notice that in the bottom row a=100 and the D
par distance (of the farthest particles whose radiation we can have detected) is about 6300. To get the distance to those particles NOW you have to divide by a = 100. so you get 63.
But that is far far in future, the radius of the observable is only gradually increasing as radiation from more distant matter arrives. today the most distant matter we could now be detecting is 46 from us, see the D
par entry in the a=1 row, which refers to the PRESENT DAY situation.
[tex]{\scriptsize\begin{array}{|c|c|c|c|c|c|}\hline R_{0} (Gly) & R_{\infty} (Gly) & S_{eq} & H_{0} & \Omega_\Lambda & \Omega_m\\ \hline 14.4&17.3&3400&67.9&0.693&0.307\\ \hline \end{array}}[/tex] [tex]{\scriptsize\begin{array}{|r|r|r|r|r|r|r|r|r|r|r|r|r|r|r|r|} \hline a=1/S&S&T (Gy)&R (Gly)&D_{now} (Gly)&D_{then}(Gly)&D_{hor}(Gly)&D_{par}(Gly) \\ \hline 0.001&1090.000&0.0004&0.0006&45.332&0.042&0.057&0.001\\ \hline 0.003&339.773&0.0025&0.0040&44.184&0.130&0.179&0.006\\ \hline 0.009&105.913&0.0153&0.0235&42.012&0.397&0.552&0.040\\ \hline 0.030&33.015&0.0902&0.1363&38.052&1.153&1.652&0.249\\ \hline 0.097&10.291&0.5223&0.7851&30.918&3.004&4.606&1.491\\ \hline 0.312&3.208&2.9777&4.3736&18.248&5.688&10.827&8.733\\ \hline 1.000&1.000&13.7872&14.3999&0.000&0.000&16.472&46.279\\ \hline 3.208&0.312&32.8849&17.1849&11.118&35.666&17.225&184.083\\ \hline 7.580&0.132&47.7251&17.2911&14.219&107.786&17.291&458.476\\ \hline 17.911&0.056&62.5981&17.2993&15.536&278.256&17.299&1106.893\\ \hline 42.321&0.024&77.4737&17.2998&16.093&681.061&17.300&2639.026\\ \hline 100.000&0.010&92.3494&17.2999&16.328&1632.838&17.300&6259.262\\ \hline \end{array}}[/tex]
Don't get boggled by the other columns of information. All you want here is the "a" column, and the T column (age of U expansion) and the D
par (radius of observable, particle horizon)
The link to the Lightcone calculator is in my sig. You can make unnecessary columns go away and simplify the table by using the "column selection" menu.