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In Big Bang cosmology, the observable universe is the region of space bounded by a sphere, centered on the observer, that is small enough that we might observe objects in it, i.e. there has been sufficient time for a signal emitted from the object at any time after the Big Bang, and moving at the speed of light, to have reached the observer by the present time. Every position has its own observable universe which may or may not overlap with the one centered around the Earth.

The word observable used in this sense has nothing to do with whether modern technology actually permits us to detect radiation from an object in this region. It simply means that it is possible in principle for light or other radiation from the object to reach an observer on Earth. In practice, we can only observe objects as far as the surface of last scattering, before which the universe was opaque to photons. However, it may be possible to infer information from before this time through the detection of gravitational waves which also move at the speed of light.

It is also possible that the universe is smaller than the observable universe. In this case, what we take to be very distant galaxies may actually be duplicate images of nearby galaxies, formed by light that has circumnavigated the universe. It is difficult to test this hypothesis experimentally because different images of a galaxy would show different eras in its history, and consequently might appear quite different. A 2004 paper claims to establish a lower bound of 24 gigaparsecs (78 billion light-years) on the diameter of the whole universe, making it, at most, only slightly smaller than the observable universe. This value is based on matching-circle analysis of the WMAP data.

$frac\{4\}\{3\}\; times\; pi\; times\; mathrm\{R\}^3\; =\; 4\; times\; 10^\{32\}text\{\; ly\}^3$

or about 3×10^{80} cubic meters.

The figures quoted above are distances now (in cosmological time), not distances at the time the light was emitted. For example, the cosmic microwave background radiation that we see right now was emitted at the time of recombination, 379,000 years after the Big Bang, which occurred around 13.7 billion years ago. This radiation was emitted by matter that has, in the intervening time, mostly condensed into galaxies, and those galaxies are now calculated to be about 46 billion light-years from us. To estimate the distance to that matter at the time the light was emitted, a mathematical model of the expansion must be chosen and the scale factor, a(t), calculated for the selected time since the Big Bang, t. For the observationally-favoured Lambda-CDM model, using data from the WMAP satellite, Embedded_LambdaCDM_geometry.png#Mathematical_details yields a scale factor change of approximately 1292. This means the universe has expanded to 1292 times the size it was when the CMBR photons were released. Hence, the most distant matter that is observable at present, 46 billion light-years away, was only 36 million light-years away from the matter that would eventually become Earth when the microwaves we are currently receiving were emitted.

- 13.7 billion light-years. The age of the universe is about 13.7 billion years. While it is commonly understood that nothing travels faster than light, it is a common misconception that the radius of the observable universe must therefore amount to only 13.7 billion light-years. This reasoning only makes sense if the universe is the flat spacetime of special relativity; in the real universe, spacetime is highly curved on cosmological scales, which means that 3-space (which is roughly flat) is expanding, as evidenced by Hubble's law. Distances obtained as the speed of light multiplied by a cosmological time interval have no direct physical significance.
- 15.8 billion light-years. This is obtained in the same way as the 13.7 billion light year figure, but starting from an incorrect age of the universe which was reported in the popular press in mid-2006 . For an analysis of this claim and the paper that prompted it, see .
- 27 billion light-years. This is a diameter obtained from the (incorrect) radius of 13.7 billion light-years.
- 78 billion light-years. This is a lower bound for the size of the whole universe, based on the estimated current distance between points that we can see on opposite sides of the cosmic microwave background radiation, so this figure represents the diameter of the sphere formed by the CMBR. If the whole universe is smaller than this sphere, then light has had time to circumnavigate it since the big bang, producing multiple images of distant points in the CMBR, which would show up as patterns of repeating circles. Cornish et al looked for such an effect at scales of up to 24 gigaparsecs (78 billion light years) and failed to find it, and suggested that if they could extend their search to all possible orientations, they would then "be able to exclude the possibility that we live in a universe smaller than 24 Gpc in diameter". The authors also estimated that with "lower noise and higher resolution CMB maps (from WMAP's extended mission and from Planck), we will be able to search for smaller circles and extend the limit to ~28 Gpc." This estimate of the maximum diameter of the CMBR sphere that will be visible in planned experiments corresponds to a radius of 14 gigaparsecs, the same number given in the previous section.
- 156 billion light-years. This figure was obtained by doubling 78 billion light-years on the assumption that it is a radius. Since 78 billion light-years is already a diameter, the doubled figure is incorrect. This figure was very widely reported.
- 180 billion light-years. This estimate accompanied the age estimate of 15.8 billion years in some sources; it was obtained by incorrectly adding 15 percent to the incorrect figure of 156 billion light years.

Two back-of-the-envelope calculations give the number of atoms in the observable universe to be around 10^{80}.

- Observations of the cosmic microwave background from the Wilkinson Microwave Anisotropy Probe suggest that the spatial curvature of the universe is very close to zero, which in current cosmological models implies that the value of the density parameter must be very close to a certain critical value. This works out to 9.9×10
^{−27}kilograms/meter^{3}, which would be equal to about 5.9 hydrogen atoms per cubic meter. Analysis of the WMAP results suggests that only about 4.6% of the critical density is in the form of normal atoms, while 23% is thought to be made of cold dark matter and 72% is thought to be dark energy, so this leaves 0.27 hydrogen atoms/m^{3}. Multiplying this by the volume of the visible universe, you get about 8×10^{79}hydrogen atoms. - A typical star has a mass of about 2×10
^{30}kg, which is about 1×10^{57}atoms of hydrogen per star. A typical galaxy has about 400 billion stars so that means each galaxy has 1×10^{57}× 4×10^{11}= 4×10^{68}hydrogen atoms. There are possibly 80 billion galaxies in the Universe, so that means that there are about 4×10^{68}× 8×10^{10}= 3×10^{79}hydrogen atoms in the observable Universe. But this is definitely a lower limit calculation, and it ignores many possible atom sources.

$frac\{4\}\{3\}\; pi\; \{S\_textrm\{horizon\}\}^3\; =\; 9\; times\; 10^\{30\}\; textrm\{ly\}^3$

and a stellar density calculated from observations by the Hubble Space Telescope

$frac\{5\; times\; 10^\{21\}\; textrm\{stars\}\}\{4\; times\; 10^\{30\}\; textrm\{light-years\}^3\}\; =\; 10^\{-9\}\; textrm\{stars\}/textrm\{ly\}^3$

yielding an estimate of the number of stars in the observable universe of 9 × 10^{21} stars (9 billion trillion stars).

Taking the mass of Sol (2 × 10^{30} kg) as the mean solar mass (on the basis that the large population of dwarf stars balances out the population of stars whose mass is greater than Sol) and rounding the estimate of the number of stars up to 10^{22} yields a total mass for all the stars in the observable universe of 2 × 10^{52} kg. However, as noted in the "matter content" section, the WMAP results in combination with the Lambda-CDM model predict that less than 5% of the total mass of the observable universe is made up of visible matter such as stars, the rest being made up of dark matter and dark energy.

Sir Fred Hoyle calculated the mass of an observable steady-state universe using the formula

$frac\{4\}\{3\}cdot\; pi\; cdot\; rho\; cdot\; (frac\{c\}\{H\})^3$

which can also be stated as

$frac\{c^3\}\{2GH\}$.

- Particle horizon
- Event horizon of the universe
- Causality (physics)
- Hubble volume
- Large-scale structure of the cosmos
- Observation
- Multiverse
- Open multiverse
- Nine Million Bicycles (a physicist challenges the scientific accuracy of some song lyrics)
- Universe

- Cosmology FAQ
- Hubble, VLT and Spitzer Capture Galaxy Formation in the Early Universe
- Star Survey reaches 70 sextillion
- Inflation and the Cosmic Microwave Background, Lineweaver 2003
- Animation of the cosmic light horizon
- Logarithmic Maps of the Universe

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Last updated on Thursday October 09, 2008 at 22:17:44 PDT (GMT -0700)

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This article is licensed under the GNU Free Documentation License.

Last updated on Thursday October 09, 2008 at 22:17:44 PDT (GMT -0700)

View this article at Wikipedia.org - Edit this article at Wikipedia.org - Donate to the Wikimedia Foundation

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