Anonymous wrote:Well maybe it's seems simple, but (in my point of view) it's definitely not
Let's take it in an simple and intuitive (but wrong) way
:
Let's imagine that after the big bang, the Universe is always expanding at light speed, then imagine we are at the border of the expanding Universe. Then we always have this equation:
our distance to this center (in light years) = time for the first big bang light to come to us (in years).
So we can look at anytime at the center of the Universe and see the first bigbang light.
The problem is:
- Universe is not expanding at light speed, right ?
- Universe does not have a center, right ? Then could the first big bang light be observed anywhere or nowhere ? Really, how far/back in time could we see if we were not limited by the instruments ?
while I usually do not tend to discuss with nameless people, cyber robots or shell scripts
, here are nevertheless a couple of issues to consider for your question:
1) You may have overlooked, that one of the most spectacular recent experiments in this area was the quantitative recording of the cosmic microwave background radiation ( CMB) from BOOMERANG, WMAP,... This is a /direct/ testimony of the BigBang or very close to it: the universe was then merely 300000 years old! It's size was only about 1 degree in the sky as seen from here. Of course one cannot see any light earlier than that, since the hot and dense plasma of the early universe was NOT transparent to light. The CMB signal is just from the time threshold where the decoupling of photons from the plasma took place...
2) Of course you MUST apply
general relativity to your considerations, otherwise you sure get nonsense.
Based on the assumption that the universe is
homogeneous and isotropic on large scales, the framework for modern cosmology rests on Einstein's
general theory of relativity, leading to the successful hot Big Bang or
Friedmann- Robertson-Walker cosmological model. The dynamics of the expanding universe are described by the Friedmann equation, relating the expansion rate to the
density and
curvature of the universe.
Today's expansion rate of the Universe is given by the
Hubble constant, that can be directly measured with various methods.
The expansion rate would only equal the speed of light in /empty space/ with the gravitational force neglected! While the speed of light is always the same, the high initial density of mass induced a strong /curvature/ of space-time along with many other important effects.
You must also take into account that gravity was a strong force at the very short distances corresponding to right after the big bang. Only at the huge distances involved in today's cosmology, gravity acts extremely weakly.
Bye Fridger