Radrook said:
We also have to keep in mind that such calculations are based on observations of the detectable universe. The unseen undetectable part has been hypothesized to be like the Earth is to an atom in comparison to the detectable one on which we are basing calculations as if they apply to the whole. So for the sake of accuracy, it's better to use the modifier "detectable" when making these calculations or at least mention a horizon as the previous poster did.
You are right! I didn't emphasize that enough in my post---only got around to it towards the end:
marcus said:
...
So there are two miniscule negligible effects (A) the light travel time would be 1000 years less and (B) the distances would be less by 1/140000 of one percent. They would both have made our particle horizon (radius of observable) slightly less 1000 years ago than it is today, but too little to worry about.
The 46 billion LY that I assumed Termina was talking about is only the radius of the portion that is
currently observable. There is presumably much much more to the universe

One doesn't know how much more.
This radius of the observable universe is called the "particle horizon".
The modifier "detectable" which you suggest would be a good one to use, I think. If anybody wants to read up about the various horizons and the basics of expansion cosmology, the CMB etc, I can't think of anything better than an old (2003) easy-math article by Charley Lineweaver
http://arxiv.org/abs/astro-ph/0305179
You can get it simply by googling "lineweaver inflation"
because inflation is the first word in the title. Radrook if you have an introductory online source you like, please give the link, especially if more recent than this Lineweaver "Inflation and the CMB".
Lineweaver is a worldclass cosmologist who just happens to be able to write clearly at a basic level.