1 E19 s and more

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To help compare orders of magnitude of different times, this page lists times longer than 10¹⁹ seconds (317 billion years) See also times of other orders of magnitude.

See the article about the ultimate fate of the Universe for more discussion of these issues.

• Shorter times
• 2.0 × 10¹⁰ years – the end of the universe by the Big Rip
• 3.3 × 10¹² years – According to the traditional Vedic time of Hinduism, this is the lifetime of Brahma.
• 7.7 × 10¹⁵ years – half-life of cadmium-113
• 1.4 × 10¹⁷ years – half-life of vanadium-50
• > 1.8 × 10¹⁷ years – half life of chromium-50
• > 6 × 10¹⁸ years – half life of calcium-48
• (1.9 ± 0.2) × 10¹⁹ years – alpha emission half-life of bismuth-209
• 3.1 × 10²² years – estimated half-life of iron-54

The following times all assume that the Universe is "open":

• 10¹⁴ years – the estimated time until low-mass stars cool off. The smallest red dwarf stars are the longest-lived stars, and are believed to have a lifetime of up to 14 trillion years (1.4 x 10¹³ years). Star formation is expected to cease in galaxies in about 10¹³ to 10¹⁴ years as galaxies are depleted of the gas clouds they need to form stars. The longest-lived stars formed from the last gas clouds will therefore cool off after about 2 x 10¹⁴ years.
• 10¹⁵ years – the estimated time until planets detach from stars. Whenever two stars pass close to each other, the orbits of the planets can be disrupted and the planets can be ejected from orbit around their parent star. Planets that orbit closer to their stars take longer to be ejected in this manner on average because a passing star must make a closer pass to the planet's star to eject the planet.
• 10¹⁹ years – the estimated time until stars detach from galaxies. When two stars pass close enough to each other, the stars exchange orbital energy with lower-mass stars tending to gain energy. The lower-mass stars can gain enough energy in this manner through repeated encounters to be ejected from the galaxy. This process can cause the galaxy to eject the majority of its stars.
• 10²⁰ years – the estimated time until orbits decay by gravitational radiation
• 10³⁰ years – the estimated time until galaxies disappear due to black holes
• 10³⁶ years – the estimated half-life for proton decay, if GUT is right
• 10⁴⁰ years – the estimated expiration of all protons in the universe due to proton decay, if GUT is right (probability dictates only less than one proton in the universe will survive its half-life if its true value is close to our theoretical lower bound)
• 10⁶⁴ years – the estimated time until black holes decay by the Hawking process
• 10⁶⁵ years – the estimated timescale at which all matter is liquid at zero temperature due to tunneling effects
• 10¹⁰⁰ years (a googol year) – the estimated time until supermassive black holes decay by the Hawking process
• 10¹⁵⁰⁰ years – the estimated time until all matter decays to iron (if the proton does not decay)

An alternative could be the following also according to Dyson Freeman's "Time without end: physics and biology in an open universe"

• 10^{100,000,000,000,000,000,000,000,000} years () – low estimate for the time until all matter collapses into black holes, assuming no proton decay
• 10^{10,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000} years () – high estimate for the time until all matter collapses into neutron stars or black holes, again assuming no proton decay. Dyson Freeman, Reviews of Modern Physics, Vol. 51, No. 3, July 1979(c) 1979 American Physical Society

This time assumes a statistical model subject to Poincaré recurrence and is likely the longest finite time ever explicitly calculated by a physicist. A much simplified way of thinking about this time is in a model where our universe's history repeats itself arbitrarily many times due to properties of statistical mechanics, this is the time scale when it will first be somewhat similar (for a reasonable choice of "similar") to its current state again.

• years – scale of an estimated Poincaré recurrence time for the quantum state of a hypothetical box containing a black hole with the estimated mass of our entire universe.

[edit] External links

• [1] Dyson Freeman, Reviews of Modern Physics, Vol. 51, No. 3, July 1979(c) 1979 American Physical Society
• [2] Poincaré recurrence and large numbers

Orders of magnitude (time), by powers of seconds
Negative powers	10−44 s | ... | 10−25 s | 10−24 s | 10−23 s | 10−22 s | 10−21 s | 10−20 s | 10−19 s | 10−18 s | 10−17 s | 10−16 s | 10−15 s | 10−14 s | 10−13 s | 10−12 s | 10−11 s | 10−10 s | 10−9 s | 10−8 s | 10−7 s | 10−6 s | 10−5 s | 10−4 s | 10−3 s | 10−2 s | 10−1 s
Positive powers	1 s | 10 s | 102 s | 103 s | 104 s | 105 s | 106 s | 107 s | 108 s | 109 s | 1010 s | 1011 s | 1012 s | 1013 s |1014 s | 1015 s | 1016 s | 1017 s | 1018 s | 1019 s and more