Math 2.0

Astronomy and astrophysics Large-scale structure and physical cosmology Problem

Olbers' paradox

Builds on Physical cosmologyCosmological redshift

Problem

Assume the universe is infinite, static and Euclidean. Assume it is uniformly filled, on average, with stars of the same mean luminosity that have shone forever. Then every line of sight from the observer ends on the surface of a star. So the whole night sky should be about as bright as the surface of a typical star. Why is the night sky dark?

Remarks

The argument: let nn be the number density of stars and LL their mean luminosity. A thin shell of radius rr and thickness drdr around the observer contains 4πr2n dr4 \pi r^2 n \, dr stars, each of which sends a flux L/(4πr2)L / (4 \pi r^2). So each shell contributes the same flux nL drn L \, dr, and the sum over all shells diverges. Since near stars hide far ones, the sky instead reaches the surface brightness of a star.

Status: resolved within physical cosmology. The universe has a finite age, so light reaches us only from a finite region, and stars have finite lifetimes. These facts alone make the sky dark. The mean distance along a line of sight to a stellar surface is far larger than the distance light has travelled since stars formed. The expansion of the universe adds a further dimming through the cosmological redshift of distant light.

The question is named after Olbers, who wrote about it in 1823; it had been raised earlier, for example by Kepler in 1610 and by de Chéseaux in 1744.

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To understand this page from the ground up, read these 3 pages in order. The foundations come first.

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  1. Cosmological redshift concept
  2. Physical cosmology concept
  3. Olbers' paradox problem

Further reading

  1. Web https://en.wikipedia.org/wiki/Olbers%27_paradox
About this page
TagYGQEBK5X7R
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Kindproblem
WritingW0 stub
MSC85A40
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AboutPhysical cosmology
UsesPhysical cosmology, Cosmological redshift
Changed3 November 2026

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