connorp said:
Thanks all. I mostly understand now. Just one more question now. So as I understand (or at least think I do), if the space between us and a galaxy is expanding faster than c, those photons will never be able to reach us and the galaxy will effectively "wink out" and disappear. And space expands faster as you go out over larger distances, correct? So if distant galaxies can disappear due to space expanding faster than c, why won't the CMB since its even farther out? If expansion truly is unbounded, the CMB will eventually be redshifted beyond detection. But why won't it "wink out" well before that?
Connor, at any given time there is a "safe range" within which distances are NOT growing faster than light.
There are plenty of of galaxies which are today OUTSIDE that range but which have already sent us thousands of years worth of photons which are already WITHIN safe range and which will be able to eventually make it here to us.
I wouldn't expect any galaxy that is visible today to abruptly "wink out". But you are right that the light from objects can "eventually be redshifted beyond detection". You mention this in connection with the CMB but it is a more general expectation. The light we will be receiving from the galaxies (outside our immediate group) will be taking longer and longer to get here and will arrive more and more wave-stretched until the once-visible light is all radio waves and until the waves are so long that no practical-size antenna can pick them up. the galaxies we can now see (outside our local group) will very slowly, over billions of years, RED OUT, but they will not wink out.
How are you with numbers? I simplified the earlier table by eliminating unnecessary columns and increasing the number of steps and narrowing the time-span covered. I want to illustrate how the "safe range" changes over time. If you go to the "Lightcone" link you will see how you can change the number of steps or rows in the table, eliminate columns etc.
R is the "safe range" within which photons can make forward progress because distances grow < c
T is the year, the table starts with year 545 million, goes to present around year 13.8 billion, and on into future.
a is the scale of distances with present distance called "1". So back in year 545 million at the start of the table distances were ONE TENTH what they are today. and by the end of the table, the last row, those same distances will be ten times what they are today.
{\scriptsize\begin{array}{|r|r|r|r|r|r|r|r|r|r|r|r|r|r|r|r|} \hline a=1/S&T (Gy)&R (Gly) \\ \hline 0.100&0.545&0.820\\ \hline 0.126&0.771&1.157\\ \hline 0.158&1.089&1.631\\ \hline 0.200&1.536&2.294\\ \hline 0.251&2.165&3.213\\ \hline 0.316&3.041&4.463\\ \hline 0.398&4.250&6.105\\ \hline 0.501&5.883&8.135\\ \hline 0.631&8.015&10.403\\ \hline 0.794&10.669&12.602\\ \hline 1.000&13.787&14.400\\ \hline 1.259&17.257&15.649\\ \hline 1.585&20.956&16.410\\ \hline 1.995&24.789&16.836\\ \hline 2.512&28.694&17.063\\ \hline 3.162&32.638&17.180\\ \hline 3.981&36.601&17.240\\ \hline 5.012&40.575&17.270\\ \hline 6.310&44.553&17.285\\ \hline 7.943&48.534&17.292\\ \hline 10.000&52.516&17.296\\ \hline \end{array}}
The technical name for what I called the "safe range" is actually "Hubble radius". at any given time in history, the Hubble radius is the size of distances which are growing exactly at speed c. the others grow proportionately. So if a distance is half R then it is growing at half c speed.
Any distance less than R is growing at less than c speed. So a photon coming towards us which has made it within that range is safe, it will not be swept back.
There is even an additional help to photons which comes from R gradually increasing so that it reaches out to some ones that were getting swept back and takes them in too. But that is a fine point. the real "safe" zone is actually slightly larger than the radius R indicates, because R is growing over time.