Heat death of the universe
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The heat death of the universe is a plausible ultimate fate of the universe in which the universe has diminished to a state of no thermodynamic free energy and therefore can no longer sustain processes that increase entropy. Heat death does not imply any particular absolute temperature; it only requires that temperature differences or other processes may no longer be exploited to perform work. In the language of physics, this is when the universe reaches thermodynamic equilibrium (maximum entropy).
If the topology of the universe is open or flat, or if dark energy is a positive cosmological constant (both of which are consistent with current data), the universe will continue expanding forever and a heat death is expected to occur,^{[1]} with the universe cooling to approach equilibrium at a very low temperature after a very long time period.
The hypothesis of heat death stems from the ideas of William Thomson, 1st Baron Kelvin, who in the 1850s took the theory of heat as mechanical energy loss in nature (as embodied in the first two laws of thermodynamics) and extrapolated it to larger processes on a universal scale.
Contents
Origins of the idea
The idea of heat death stems from the second law of thermodynamics, of which one version states that entropy tends to increase in an isolated system. From this, the hypothesis infers that if the universe lasts for a sufficient time, it will asymptotically approach a state where all energy is evenly distributed. In other words, according to this hypothesis, in nature there is a tendency to the dissipation (energy transformation) of mechanical energy (motion) into thermal energy; hence, by extrapolation, there exists the view that the mechanical movement of the universe will run down, as work is converted to heat, in time because of the second law.
The conjecture that all bodies in the universe cool off, eventually becoming too cold to support life, seems to have been first put forward by the French astronomer JeanSylvain Bailly in 1777 in his writings on the history of astronomy and in the ensuing correspondence with Voltaire. In Bailly's view, all planets have an internal heat and are now at some particular stage of cooling. Jupiter, for instance, is still too hot for life to arise there for thousands of years, while the Moon is already too cold. The final state, in this view, is described as one of "equilibrium" in which all motion ceases.^{[2]}
The idea of heat death as a consequence of the laws of thermodynamics, however, was first proposed in loose terms beginning in 1851 by William Thomson, 1st Baron Kelvin, who theorized further on the mechanical energy loss views of Sadi Carnot (1824), James Joule (1843), and Rudolf Clausius (1850). Thomson’s views were then elaborated on more definitively over the next decade by Hermann von Helmholtz and William Rankine.^{[citation needed]}
History
The idea of heat death of the universe derives from discussion of the application of the first two laws of thermodynamics to universal processes. Specifically, in 1851 William Thomson (Lord Kelvin) outlined the view, as based on recent experiments on the dynamical theory of heat, that "heat is not a substance, but a dynamical form of mechanical effect, we perceive that there must be an equivalence between mechanical work and heat, as between cause and effect."^{[3]}
In 1852, Thomson published On a Universal Tendency in Nature to the Dissipation of Mechanical Energy in which he outlined the rudiments of the second law of thermodynamics summarized by the view that mechanical motion and the energy used to create that motion will tend to dissipate or run down, naturally.^{[4]} The ideas in this paper, in relation to their application to the age of the sun and the dynamics of the universal operation, attracted the likes of William Rankine and Hermann von Helmholtz. The three of them were said to have exchanged ideas on this subject.^{[5]} In 1862, Thomson published "On the age of the Sun’s heat", an article in which he reiterated his fundamental beliefs in the indestructibility of energy (the first law) and the universal dissipation of energy (the second law), leading to diffusion of heat, cessation of useful motion (work), and exhaustion of potential energy through the material universe while clarifying his view of the consequences for the universe as a whole. In a key paragraph, Thomson wrote:
The result would inevitably be a state of universal rest and death, if the universe were finite and left to obey existing laws. But it is impossible to conceive a limit to the extent of matter in the universe; and therefore science points rather to an endless progress, through an endless space, of action involving the transformation of potential energy into palpable motion and hence into heat, than to a single finite mechanism, running down like a clock, and stopping for ever.^{[6]}
In the years to follow both Thomson’s 1852 and the 1865 papers, Helmholtz and Rankine both credited Thomson with the idea, but read further into his papers by publishing views stating that Thomson argued that the universe will end in a "heat death" (Helmholtz) which will be the "end of all physical phenomena" (Rankine).^{[5]}^{[7]}
Current status
Proposals about the final state of the universe depend on the assumptions made about its ultimate fate, and these assumptions have varied considerably over the late 20th century and early 21st century. In a hypothesized "open" or "flat" universe that continues expanding indefinitely, either a heat death or a Big Rip is expected to eventually occur.^{[1]} If the cosmological constant is zero, the universe will approach absolute zero temperature over a very long timescale. However, if the cosmological constant is positive, as appears to be the case in recent observations, the temperature will asymptote to a nonzero, positive value and the universe will approach a state of maximum entropy.^{[8]}
If Big Rip doesn't happen long before that then the "heat death" situation could be avoided if there is a method or mechanism to regenerate hydrogen atoms from radiation, dark matter, dark energy, zeropoint energy, or other sources so that star formation and heat transfer can continue to avoid a gradual running down of the universe due to the conversion of matter into energy and heavier elements in stellar processes and the absorption of matter by black holes and their subsequent evaporation as Hawking radiation.^{[9]}^{[10]}
Time frame for heat death
From the Big Bang through the present day, matter and dark matter in the universe are thought to have been concentrated in stars, galaxies, and galaxy clusters, and are presumed to continue to be so well into the future. Therefore, the universe is not in thermodynamic equilibrium and objects can do physical work.^{[11]}^{, §VID.} The decay time for a supermassive black hole of roughly 1 galaxymass (10^{11} solar masses) due to Hawking radiation is on the order of 10^{100} years,^{[12]} so entropy can be produced until at least that time. Some monster black holes in the universe are predicted to continue to grow up to perhaps 10^{14} M_{☉} during the collapse of superclusters of galaxies. Even these would evaporate over a timescale of up to 10^{106} years^{[13]}. After that time, the universe enters the socalled Dark Era, and is expected to consist chiefly of a dilute gas of photons and leptons.^{[11]}^{§VIA} With only very diffuse matter remaining, activity in the universe will have tailed off dramatically, with extremely low energy levels and extremely long time scales. Speculatively, it is possible that the universe may enter a second inflationary epoch, or, assuming that the current vacuum state is a false vacuum, the vacuum may decay into a lowerenergy state.^{[11]}^{, §VE.} It is also possible that entropy production will cease and the universe will reach heat death.^{[11]}^{, §VID.} Another universe could possibly be created by random quantum fluctuations or quantum tunneling in roughly years.^{[14]} Over an infinite time, there would be a spontaneous entropy decrease via the Poincaré recurrence theorem^{[citation needed]}, thermal fluctuations,^{[15]}^{[16]}^{[17]} and Fluctuation theorem.^{[18]}^{[19]} Such a scenario, however, has been described as "highly speculative, probably wrong [and] completely untestable".^{[20]} Sean M. Carroll, originally an advocate of this idea, no longer supports it.^{[21]}^{[22]}
Controversies
Max Planck wrote that the phrase "entropy of the universe" has no meaning because it admits of no accurate definition.^{[23]}^{[24]} More recently, Grandy writes: "It is rather presumptuous to speak of the entropy of a universe about which we still understand so little, and we wonder how one might define thermodynamic entropy for a universe and its major constituents that have never been in equilibrium in their entire existence."^{[25]} According to Tisza: "If an isolated system is not in equilibrium, we cannot associate an entropy with it."^{[26]} Buchdahl writes of "the entirely unjustifiable assumption that the universe can be treated as a closed thermodynamic system".^{[27]} According to Gallavotti: "... there is no universally accepted notion of entropy for systems out of equilibrium, even when in a stationary state."^{[28]} Discussing the question of entropy for nonequilibrium states in general, Lieb and Yngvason express their opinion as follows: "Despite the fact that most physicists believe in such a nonequilibrium entropy, it has so far proved impossible to define it in a clearly satisfactory way."^{[29]} In Landsberg's opinion, "The third misconception is that thermodynamics, and in particular, the concept of entropy, can without further enquiry be applied to the whole universe. ... These questions have a certain fascination, but the answers are speculations, and lie beyond the scope of this book."^{[30]}
A recent analysis of entropy states that "The entropy of a general gravitational field is still not known," and that "gravitational entropy is difficult to quantify." The analysis considers several possible assumptions that would be needed for estimates, and suggests that the visible universe has more entropy than previously thought. This is because the analysis concludes that supermassive black holes are the largest contributor.^{[31]} Another writer goes further; "It has long been known that gravity is important for keeping the universe out of thermal equilibrium. Gravitationally bound systems have negative specific heat—that is, the velocities of their components increase when energy is removed. ... Such a system does not evolve toward a homogeneous equilibrium state. Instead it becomes increasingly structured and heterogeneous as it fragments into subsystems."^{[32]}
See also
References
 ^ ^{a} ^{b} Plait, Philip Death From the Skies!, Viking Penguin, NY, ISBN 9780670019977, p. 259
 ^ Brush, Stephen G. (1996). A History of Modern Planetary Physics: Nebulous Earth. Cambridge University Press. p. 77. ISBN 9780521441711.
 ^ Thomson, William. (1851). "On the Dynamical Theory of Heat, with numerical results deduced from Mr Joule’s equivalent of a Thermal Unit, and M. Regnault’s Observations on Steam." Excerpts. [§§1–14 & §§99–100], Transactions of the Royal Society of Edinburgh, March, 1851; and Philosophical Magazine IV. 1852. [from Mathematical and Physical Papers, vol. i, art. XLVIII, pp. 174]
 ^ Thomson, William (1852). "On a Universal Tendency in Nature to the Dissipation of Mechanical Energy" Proceedings of the Royal Society of Edinburgh for April 19, 1852, also Philosophical Magazine, Oct. 1852. [This version from Mathematical and Physical Papers, vol. i, art. 59, pp. 511.]
 ^ ^{a} ^{b} Smith, Crosbie & Wise, Matthew Norton. (1989). Energy and Empire: A Biographical Study of Lord Kelvin. (pg. 500). Cambridge University Press.
 ^ Thomson, William. (1862). "On the age of the sun’s heat", Macmillan’s Mag., 5, 288–93; PL, 1, 394–68.
 ^ Physics Timeline (Helmholtz and Heat Death, 1854)
 ^ Lisa Dyson, Matthew Kleban, Leonard Susskind: "Disturbing Implications of a Cosmological Constant"
 ^ MacMillan, W.D. (1918). "On stellar evolution". Astrophys. J. 48: 35–49. Bibcode:1918ApJ....48...35M. doi:10.1086/142412.
 ^ Macmillan, William D. (1925). "Some Mathematical Aspects of Cosmology". Science. 62 (1596): 96–9. Bibcode:1925Sci....62..121M. doi:10.1126/science.62.1596.96. PMID 17752724.
 ^ ^{a} ^{b} ^{c} ^{d} Fred C. Adams and Gregory Laughlin (1997). "A dying universe: the longterm fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astroph/9701131 . Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337..
 ^ See in particular equation (27) in Page, Don N. (15 January 1976). "Particle emission rates from a black hole: Massless particles from an uncharged, nonrotating hole". Physical Review D. 13 (2): 198–206. Bibcode:1976PhRvD..13..198P. doi:10.1103/PhysRevD.13.198..

^ Frautschi, S., 1982. Entropy in an expanding universe. Science, 217(4560), pp.593599. See page 596: table 1 and section "black hole decay" and previous sentence on that page
"Since we have assumed a maximum scale of gravitational binding  for instance, superclusters of galaxies  black hole formation eventually comes to an end in our model, with masses of up to 10^{14}M_{☉} ... the timescale for black holes to radiate away all their energy ranges ... to 10^{106} years for black holes of up to 10^{14}M_{☉}"
 ^ Carroll, Sean M. and Chen, Jennifer (2004). Carroll, Sean M.; Chen, Jennifer (2004). "Spontaneous Inflation and Origin of the Arrow of Time". arXiv:hepth/0410270 .
 ^ Tegmark, Max (2003). "Parallel Universes". In J. D. Barrow, P. C. W. Davies, C. L. Harper. Science and Ultimate Reality: from Quantum to Cosmos. Cambridge University Press. arXiv:astroph/0302131 . Bibcode:2003SciAm.288e..40T. doi:10.1038/scientificamerican050340.
 ^ Tegmark, Max (May 2003). "Parallel Universes". Scientific American. 288 (5): 40–51. arXiv:astroph/0302131 . Bibcode:2003SciAm.288e..40T. doi:10.1038/scientificamerican050340.
 ^ Werlang, T.; Ribeiro, G. A. P.; Rigolin, Gustavo (2012). "Interplay between quantum phase transitions and the behavior of quantum correlations at finite temperatures.org". International Journal of Modern Physics B. 27 (1345032): 1345032. arXiv:1205.1046 . Bibcode:2013IJMPB..2745032W. doi:10.1142/S021797921345032X.
 ^ XiuSan Xing (1 November 2007). "Spontaneous entropy decrease and its statistical formula". ResearchGate.
 ^ Linde, Andrei (24 January 2007). "Sinks in the landscape, Boltzmann brains and the cosmological constant problem". Journal of Cosmology and Astroparticle Physics. 2007 (1): 022–022. arXiv:hepth/0611043 . Bibcode:2007JCAP...01..022L. doi:10.1088/14757516/2007/01/022.
 ^ https://theconversation.com/thefateoftheuniverseheatdeathbigriporcosmicconsciousness46157
 ^ Sean Carroll, "Fluctuations in de Sitter Space" FQXi conference 2014 in Vieques
 ^ Boddy, Kimberly K; Carroll, Sean M; Pollack, Jason (2014). "De Sitter Space Without Dynamical Quantum Fluctuations". arXiv:1405.0298 [hepth].
 ^ Uffink, J. (2003). Irreversibility and the Second Law of Thermodynamics, Chapter 7 of Entropy, p. 129 of Greven, A., Keller, G., Warnecke (editors) (2003), Entropy, Princeton University Press, Princeton NJ, ISBN 0691113386. Uffink writes: "The importance of Planck's Vorlesungen über Thermodynamik (Planck 1897) can hardly be [over]estimated. The book has gone through 11 editions, from 1897 until 1964, and still remains the most authoritative exposition of classical thermodynamics."
 ^ Planck, M. (1897/193). Treatise on Thermodynamics, translated by A. Ogg, p. 101.
 ^ Grandy, W.T. (Jr) (2008). Entropy and the Time Evolution of Macroscopic Systems, Oxford University Press, Oxford UK, ISBN 9780199546176, p. 151.
 ^ Tisza, L. (1966). Generalized Thermodynamics, M.I.T Press, Cambridge MA, p. 41.
 ^ Buchdahl, H.A. (1966). The Concepts of Classical Thermodynamics, Cambridge University Press, Cambridge UK, p. 97.
 ^ Gallavotti, G. (1999). Short Treatise of Statistical Mechanics, Springer, Berlin, ISBN 9783540648833, p. 290.
 ^ Lieb, E.H., Yngvason, J. (2003). The entropy of classical thermodynamics, Chapter 8 of Greven, A., Keller, G., Warnecke (editors) (2003). Entropy, Princeton University Press, Princeton NJ, ISBN 0691113386, page 190.
 ^ Landsberg, P.T. (1961). Thermodynamics, with Quantum Statistical Illustrations, Wiley, New York, p. 391.
 ^ Egan, Chas A.; Lineweaver, Charles H. (2009). "A Larger Estimate of the Entropy of the Universe". The Astrophysical Journal. 710 (2): 1825–1834. arXiv:0909.3983 . Bibcode:2010ApJ...710.1825E. doi:10.1088/0004637X/710/2/1825.
 ^ Smolin, L. (2014). "Time, laws, and future of cosmology". Physics Today. 67 (3): 38–43 [42]. Bibcode:2014PhT....67c..38S. doi:10.1063/pt.3.2310.