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{{Short description|Thought experiment of 1867}}
'''Maxwell's Demon''' is the name of a creature thought up in [[1867]] by the likely heterosexual[[Scotland|Scottish]] [[physicist]] '''[[James Clerk Maxwell]]''' as part of a [[thought experiment]] meant to illustrate the [[Second law of thermodynamics|Second law]] of [[Thermodynamics]]. This law forbids (among other things) that two bodies of equal [[temperature]] brought in contact with each other and isolated from the rest of the Universe, evolve to a state in which one of the two has a significantly higher temperature than the other. The second law is also expressed as the claim that [[entropy]] never decreases.


[[File:Maxwell's demon.svg|right|340px|thumb|Schematic figure of Maxwell's demon thought experiment]]
In Maxwell's thought experiment, two containers, ''A'' and ''B'', filled with the same [[gas]] at equal temperatures are placed next to each other. A little 'demon' guards a trapdoor between the two containers, observing the [[molecule|molecules]] on both sides. Whenever a faster-than-average molecule from ''A'' flies towards the trapdoor, he opens it, and the molecule will move from ''A'' to ''B''. Then he waits until a slower-than-average molecule from ''B'' comes flying towards the trapdoor, which he opens again, letting the molecule through to ''A''. Thus, the average [[speed]] of the molecules in ''B'' increases and that in ''A'' decreases. But since average molecular speed corresponds to temperature, this means that the temperature in ''B'' increases and that in ''A'' decreases, which is a violation of the second law of thermodynamics.


'''Maxwell's demon''' is a [[thought experiment]] that appears to disprove the [[second law of thermodynamics]]. It was proposed by the physicist [[James Clerk Maxwell]] in 1867.<ref name="WPVsI">{{cite book|author=Cargill Gilston Knott|title=Life and Scientific Work of Peter Guthrie Tait|publisher=[[Cambridge University Press]]|year=1911|pages=213–215|chapter=Quote from undated letter from Maxwell to Tait|chapter-url=https://archive.org/stream/lifescientificwo00knotuoft#page/212/mode/2up}}</ref> In his first letter, Maxwell referred to the entity as a "finite being" or a "being who can play a game of skill with the molecules". [[Lord Kelvin]] would later call it a "''[[Demon (thought experiment)|demon]]''".<ref name="Aiv9S"/>


In the thought experiment, a demon controls a door between two chambers containing gas. As individual gas molecules (or atoms) approach the door, the demon quickly opens and closes the door to allow only fast-moving molecules to pass through in one direction, and only slow-moving molecules to pass through in the other. Because the [[kinetic temperature]] of a gas depends on the velocities of its constituent molecules, the demon's actions cause one chamber to warm up and the other to cool down. This would decrease the total [[entropy]] of the [[Thermodynamic system|system]], seemingly without applying any [[work (thermodynamics)|work]], thereby violating the second law of thermodynamics.
== A short history of Maxwell's Demon ==


The concept of Maxwell's demon has provoked substantial debate in the [[philosophy of science]] and [[theoretical physics]], which continues to the present day. It stimulated work on the relationship between [[thermodynamics]] and [[information theory]]. Most scientists argue that, on theoretical grounds, no practical device can violate the second law in this way. Other researchers have implemented forms of Maxwell's demon in experiments, though they all differ from the thought experiment to some extent and none has been shown to violate the second law.
In 1867, in a letter to his friend P.G. Tate, Maxwell introduced a 'finite being' with the power to exploit the differences in molecular speed which exist in any gas. By opening and closing a frictionless trapdoor between two containers of gas, depending on the speed of approaching molecules, this being could create a temperature difference and break the second law of thermodynamics. Maxwell concluded:


== Origin and history of the idea ==
:Or in short if the heat is the motion of finite portions of matter and if we can apply tools to such portions of matter so as to deal with them separately, then we can take advantage of the different motion of different proportions to restore a uniform hot system to unequal temperatures or to motions of large masses.
The [[thought experiment]] first appeared in a letter [[James Clerk Maxwell|Maxwell]] wrote to [[Peter Guthrie Tait]] on 11 December 1867. It appeared again in a letter to [[John William Strutt]] in 1871, before it was presented to the public in Maxwell's 1872 book on thermodynamics titled ''Theory of Heat''.<ref name="Leff">[[#Leff Rex 02|Leff & Rex (2002)]], p. 370.</ref>


In his letters and books, Maxwell described the agent opening the door between the chambers as a "finite being". Being a deeply religious man, he never used the word "demon". Instead, [[William Thomson, 1st Baron Kelvin|William Thomson (Lord Kelvin)]] was the first to use it for Maxwell's concept, in the journal ''[[Nature (journal)|Nature]]'' in 1874, and implied that he intended the [[Greek mythology]] interpretation of a [[Daimon|daemon]], a supernatural being working in the background, rather than a malevolent being.<ref name="Aiv9S">{{cite journal|first=William|last=Thomson|date=9 April 1874|title=Kinetic theory of the dissipation of energy|journal=[[Nature (journal)|Nature]]|volume=9|issue=232|pages=441–444|doi=10.1038/009441c0|bibcode=1874Natur...9..441T|author-link=William Thomson, 1st Baron Kelvin|doi-access=free}}</ref><ref name="Tqxmq">{{cite journal|year=1879|title=The sorting demon of Maxwell|journal=Nature|volume=20|issue=501|pages=126|bibcode=1879Natur..20Q.126.|doi=10.1038/020126a0|doi-access=free}}</ref><ref name="Weber">{{cite book|first=Alan S.|last=Weber|year=2000|title=Nineteenth Century Science: a Selection of Original Texts|publisher=[[Broadview Press]]|page=300}}</ref>
This finite being, which [[William Thomson 1st Baron Kelvin|William Thomson (Baron Kelvin)]] later dubbed 'demon', was supposed to elucidate the second law of thermodynamics by showing it had only 'statistical certainty'.


== Original thought experiment ==
The twentieth century turned out to be an eventful epoch for Maxwell’s Demon. Started as a helpful thought experiment, before long it was perceived as a threat to a beloved bulwark of physical truth. The second law had to be protected against the malicious attempts of the infernal rascal to violate it; the lofty foundations of thermodynamics had to be secured once and for all by providing a definite and unassailable proof of the demon’s non-existence. Thus began the exorcist tradition.
The second law of thermodynamics ensures (through statistical probability) that two bodies of different [[temperature]], when brought into contact with each other and isolated from the rest of the Universe, will evolve to a thermodynamic equilibrium in which both bodies have approximately the same temperature.<ref name="Bennett87">{{cite journal|last = Bennett|first = Charles H.|title = Demons, Engines, and the Second Law|journal = Scientific American|volume = 257|issue = 5|pages = 108–116|date = November 1987|url = https://ecee.colorado.edu/~ecen5555/SourceMaterial/DemonsEnginesAndSecondLaw87.pdf|doi = 10.1038/scientificamerican1187-108|access-date = November 13, 2014|bibcode = 1987SciAm.257e.108B|archive-date = December 3, 2020|archive-url = https://web.archive.org/web/20201203173214/https://ecee.colorado.edu/~ecen5555/SourceMaterial/DemonsEnginesAndSecondLaw87.pdf|url-status = dead }}</ref> The second law is also expressed as the assertion that in an [[isolated system]], [[entropy]] never decreases.<ref name="Bennett87" />


Maxwell conceived a thought experiment as a way of furthering the understanding of the second law. His description of the experiment is as follows:<ref name="Bennett87" /><ref name="DdgTn">Maxwell (1871), reprinted in [[#Leff Rex 90|Leff & Rex (1990)]] on p. 4.</ref>
The history of exorcism can be divided into three main phases, in which thermal fluctuations, measurement and erasure of information were the consecutive notions thought to contain the key to any successful exorcism. The protagonist exorcists of every phase naturally saw the earlier attempts as well-meant but insufficient, and their own pet idea as the final piece of the puzzle, which at last made everything fit together and had the power to banish the demon for all eternity. Because the erasure-type exorcism is nowadays the predominant position among Maxwell’s Demon scholars, the tale which displays the history of exorcism as one of gradual improvement has become somewhat of an orthodoxy. But the debate rages on, and the past fifteen years have seen a veritable host of scholarly publications on the demon.


{{quote|... if we conceive of a being whose faculties are so sharpened that he can follow every molecule in its course, such a being, whose attributes are as essentially finite as our own, would be able to do what is impossible to us. For we have seen that molecules in a vessel full of air at uniform temperature are moving with velocities by no means uniform, though the mean velocity of any great number of them, arbitrarily selected, is almost exactly uniform. Now let us suppose that such a vessel is divided into two portions, ''A'' and ''B'', by a division in which there is a small hole, and that a being, who can see the individual molecules, opens and closes this hole, so as to allow only the swifter molecules to pass from ''A'' to ''B'', and only the slower molecules to pass from ''B'' to ''A''. He will thus, without expenditure of work, raise the temperature of ''B'' and lower that of ''A'', in contradiction to the second law of thermodynamics.}}In other words, Maxwell imagines one container divided into two parts, ''A'' and ''B''.<ref name="Bennett87" /><ref name="Sagawa">{{cite book|last1 = Sagawa|first1 = Takahiro|title = Thermodynamics of Information Processing in Small Systems|publisher = Springer Science and Business Media|date = 2012|pages = 9–14|url = https://books.google.com/books?id=oKWi-J6LOsEC&pg=PA13|isbn = 978-4431541677}}</ref> Both parts are filled with the same [[gas]] at equal temperatures and placed next to each other. Observing the [[molecule]]s on both sides, an imaginary [[Demon (thought experiment)|demon]] guards a trapdoor between the two parts. When a faster-than-average molecule from ''A'' flies towards the trapdoor, the demon opens it, and the molecule will fly from ''A'' to ''B''. Likewise, when a slower-than-average molecule from ''B'' flies towards the trapdoor, the demon will let it pass from ''B'' to ''A''. The average [[speed]] of the molecules in ''B'' will have increased while in ''A'' they will have slowed down on average. Since average molecular speed corresponds to temperature, the temperature decreases in ''A'' and increases in ''B'', contrary to the second law of thermodynamics. A [[heat engine]] operating between the thermal reservoirs ''A'' and ''B'' could extract useful [[work (physics)|work]] from this temperature difference.
== The original demon ==


The demon must allow molecules to pass in both directions in order to produce only a temperature difference; one-way passage only of faster-than-average molecules from ''A'' to ''B'' will cause higher temperature and pressure to develop on the ''B'' side.
(The rest of this extensive rewrite will follow very soon. For now, the old article is appended below. Because of vast differences in organisation between old and new text, I have deemed it unprofitable to keep up the appearance of unity. References named in the text will be added to the list of references in due time. Please bear with me for a couple of days.)


== Criticism and development ==
=== Two versions of the second law ===
Several physicists have presented calculations that show that the [[second law of thermodynamics]] will not actually be violated, if a more complete analysis is made of the whole system including the demon.<ref name="Bennett87" /><ref name="Sagawa" /><ref name="BennettSchumacher">{{cite journal|last1 = Bennett|first1 = Charles H.|last2 = Schumacher|first2 = Benjamin|title = Maxwell's demons appear in the lab|journal = Nikkei Science|pages = 3–6|date = August 2011|url = http://www.nikkei-science.com/wp-content/uploads/2011/08/201108_032.pdf|access-date = November 13, 2014}}</ref> The essence of the physical argument is to show, by calculation, that any demon must "generate" more entropy segregating the molecules than it could ever eliminate by the method described. That is, it would take more thermodynamic work to gauge the speed of the molecules and selectively allow them to pass through the opening between ''A'' and ''B'' than the amount of [[energy]] gained by the difference of temperature caused by doing so.


One of the most famous responses to this question was suggested in 1929 by [[Leó Szilárd]],<ref name="Szilard">{{cite journal|last = Szilard|first = Leo|title = Über die Entropieverminderung in einem thermodynamischen System bei Eingriffen intelligenter Wesen (On the reduction of entropy in a thermodynamic system by the intervention of intelligent beings)|journal = Zeitschrift für Physik|volume = 53|issue = 11–12|pages = 840–856|date = 1929|doi = 10.1007/bf01341281|bibcode = 1929ZPhy...53..840S|s2cid = 122038206}} cited in Bennett 1987. English translation available as [http://aurellem.org/jaynes/sources/Szilard.pdf NASA document TT F-16723] published 1976</ref> and later by [[Léon Brillouin]].<ref name="Bennett87" /><ref name="Sagawa" /> Szilárd pointed out that a real-life Maxwell's demon would need to have some means of measuring molecular speed, and that the act of acquiring information would require an expenditure of energy. Since the demon and the gas are interacting, we must consider the total entropy of the gas and the demon combined. The expenditure of energy by the demon will cause an increase in the entropy of the demon, which will be larger than the lowering of the entropy of the gas.
[About the thermodynamical and the statistical-mechanical version of the second law.]


In 1960, [[Rolf Landauer]] raised an exception to this argument.<ref name="Bennett87" /><ref name="Sagawa" /><ref name="Landauer">{{cite journal|last = Landauer|first = R.|title = Irreversibility and heat generation in the computing process|journal = IBM Journal of Research and Development|volume = 5|issue = 3|pages = 183–191|date = 1961|url = http://www.pitt.edu/~jdnorton/lectures/Rotman_Summer_School_2013/thermo_computing_docs/Landauer_1961.pdf|doi = 10.1147/rd.53.0183|access-date = November 13, 2014}} reprinted in [http://domino.research.ibm.com/tchjr/journalindex.nsf/c469af92ea9eceac85256bd50048567c/8a9d4b4e96887b8385256bfa0067fba2?OpenDocument Vol. 44, No. 1, January 2000, p. 261] {{Webarchive|url=https://web.archive.org/web/20160303181021/http://domino.research.ibm.com/tchjr/journalindex.nsf/c469af92ea9eceac85256bd50048567c/8a9d4b4e96887b8385256bfa0067fba2?OpenDocument |date=2016-03-03 }}</ref> He realized that some measuring processes need not increase thermodynamic entropy as long as they were [[Reversible process (thermodynamics)|thermodynamically reversible]]. He suggested these "reversible" measurements could be used to sort the molecules, violating the Second Law. However, due to the connection between [[entropy in thermodynamics and information theory]], this also meant that the recorded measurement must not be erased. In other words, to determine whether to let a molecule through, the demon must acquire information about the state of the molecule and either discard it or store it. Discarding it leads to immediate increase in entropy, but the demon cannot store it indefinitely. In 1982, [[Charles H. Bennett (computer scientist)|Charles Bennett]] showed that, however well prepared, eventually the demon will run out of information storage space and must begin to erase the information it has previously gathered.<ref name="Sagawa" /><ref name="Bennett82">{{Cite journal|last1 = Bennett|first1 = C. H.|title = The thermodynamics of computation—a review|doi = 10.1007/BF02084158|journal = International Journal of Theoretical Physics|volume = 21|issue = 12|pages = 905–940|year = 1982|bibcode = 1982IJTP...21..905B|url = http://hexagon.physics.wisc.edu/teaching/2014f+ph805+quantum+information/papers/bennett+thermodynamics+of+computation+ijtp+1982.pdf|type = Submitted manuscript|citeseerx = 10.1.1.655.5610|s2cid = 17471991|access-date = 2017-12-10|archive-url = https://web.archive.org/web/20141014151011/http://hexagon.physics.wisc.edu/teaching/2014f%20ph805%20quantum%20information/papers/bennett%20thermodynamics%20of%20computation%20ijtp%201982.pdf|archive-date = 2014-10-14|url-status = dead}}</ref> Erasing information is a thermodynamically irreversible process that increases the entropy of a system. Although Bennett had reached the same conclusion as Szilard's 1929 paper, that a Maxwellian demon could not violate the second law because entropy would be created, he had reached it for different reasons. Regarding [[Landauer's principle]], the minimum energy dissipated by deleting information was experimentally measured by Eric Lutz ''et al.'' in 2012. Furthermore, Lutz ''et al.'' confirmed that in order to approach the Landauer's limit, the system must asymptotically approach zero processing speed.<ref name="yFOHN">{{cite journal|doi=10.1038/nature.2012.10186|title=The unavoidable cost of computation revealed|journal=Nature|year=2012|last1=Ball|first1=Philip|s2cid=2092541}}</ref>
=== Maxwell's thought experiment ===
Recently, [[Landauer's principle]] has also been invoked to resolve an apparently unrelated paradox of statistical physics, [[Loschmidt’s paradox]]. <ref>{{cite journal|title=The reversibility paradox: Role of the velocity reversal step|author-last=Binder|author-first=P.M.|author-link=P.M. Binder|journal=[[International Journal of Theoretical Physics]]|date=2023|volume=62|issue=9 | page=200|doi=10.1007/s10773-023-05458-x |bibcode=2023IJTP...62..200B |url= https://rdcu.be/dmmuZ |doi-access=free}}</ref>


[[John Earman]] and [[John D. Norton]] have argued that Szilárd and Landauer's explanations of Maxwell's demon begin by assuming that the [[second law of thermodynamics]] cannot be violated by the demon, and derive further properties of the demon from this assumption, including the necessity of consuming energy when erasing information, etc.<ref name="PAQSZ">{{cite journal|first1=John|last1=Earman|first2=John D.|last2=Norton|name-list-style=amp|year=1998|title=Exorcist XIV: The Wrath of Maxwell's Demon. Part I. From Maxwell to Szilard|url=http://www.pitt.edu/~jdnorton/papers/ExorcistXIV/Exorcist1.pdf|journal=Studies in History and Philosophy of Modern Physics|pages=435|volume=29|issue=4|doi=10.1016/s1355-2198(98)00023-9|bibcode=1998SHPMP..29..435E}}</ref><ref name="CyjZT">{{cite journal|first1=John|last1=Earman|first2=John D.|last2=Norton|name-list-style=amp|year=1999|title=Exorcist XIV: The Wrath of Maxwell's Demon. Part II. From Szilard to Landauer and Beyond|url=http://www.pitt.edu/~jdnorton/papers/ExorcistXIV/Exorcist2.pdf|journal=Studies in History and Philosophy of Modern Physics|pages=1|volume=30|issue=1|doi=10.1016/s1355-2198(98)00026-4|bibcode=1999SHPMP..30....1E}}</ref> It would therefore be circular to invoke these derived properties to defend the second law from the demonic argument. Bennett later acknowledged the validity of Earman and Norton's argument, while maintaining that [[Landauer's principle]] explains the mechanism by which real systems do not violate the second law of thermodynamics.<ref name="a5o0j">{{cite journal|first=Charles H.|last=Bennett|year=2002–2003|title=Notes on Landauer's principle, reversible computation, and Maxwell's demon|journal=Studies in History and Philosophy of Modern Physics|volume=34|issue=3|pages=501–510|arxiv=physics/0210005|bibcode = 2003SHPMP..34..501B|doi=10.1016/S1355-2198(03)00039-X|s2cid=9648186}}</ref>
[About the demon, including quotes by Maxwell]


== Recent progress ==
=== The purpose of the demon ===
Although the argument by Landauer and Bennett only answers the consistency between the second law of thermodynamics and the whole cyclic process of the entire system of a [[Entropy in thermodynamics and information theory#Szilard's engine|Szilard engine]] (a composite system of the engine and the demon), a recent approach based on the [[non-equilibrium thermodynamics]] for small fluctuating systems has provided deeper insight on each information process with each subsystem. From this viewpoint, the measurement process is regarded as a process where the correlation ([[mutual information]]) between the engine and the demon increases, decreasing the entropy of the system in an amount given by the mutual information.<ref name=":0">{{Cite journal|last1=Cao|first1=F. J.|last2=Feito|first2=M.|date=2009-04-10|title=Thermodynamics of feedback controlled systems|url=https://link.aps.org/doi/10.1103/PhysRevE.79.041118|journal=Physical Review E|language=en|volume=79|issue=4|page=041118 |doi=10.1103/PhysRevE.79.041118|pmid=19518184 |issn=1539-3755|arxiv=0805.4824|bibcode=2009PhRvE..79d1118C }}</ref> If the correlation changes, thermodynamic relations such as the second law of thermodynamics and the [[fluctuation theorem]] for each subsystem should be modified, and for the case of external control a second-law like inequality<ref name=":0" /><ref>{{Cite journal|last1=Sagawa|first1=Takahiro|last2=Ueda|first2=Masahito|date=2008-02-26|title=Second Law of Thermodynamics with Discrete Quantum Feedback Control|url=https://link.aps.org/doi/10.1103/PhysRevLett.100.080403|journal=Physical Review Letters|volume=100|issue=8|pages=080403|arxiv=0710.0956|bibcode=2008PhRvL.100h0403S|doi=10.1103/PhysRevLett.100.080403|pmid=18352605|s2cid=41799543}}</ref><ref name="HnKlB">{{cite journal|author1=Hugo Touchette|author2=Seth Lloyd|name-list-style=amp|year=2000|title=Information-Theoretic Limits of Control|journal=Physical Review Letters|volume=84|issue=6|pages=1156–1159|doi=10.1103/PhysRevLett.84.1156|bibcode = 2000PhRvL..84.1156T|pmid=11017467|arxiv=chao-dyn/9905039|s2cid=25507688}}</ref> and a generalized fluctuation theorem<ref name="GWNNE">{{cite journal|author1=Takahiro Sagawa|author2=Masahito Ueda|name-list-style=amp|year=2010|title=Generalized Jarzynski Equality under Nonequilibrium Feedback Control|journal=Physical Review Letters|volume=104|issue=9|pages=090602|doi=10.1103/PhysRevLett.104.090602|pmid=20366975|arxiv = 0907.4914|bibcode = 2010PhRvL.104i0602S|s2cid=1549122}}</ref> with mutual information are satisfied. For more general information processes including biological information processing, both inequality<ref name="HKXgx">{{cite journal|author=Armen E Allahverdyan, Dominik Janzing and Guenter Mahler|year=2009|title=Thermodynamic efficiency of information and heat flow|journal=Journal of Statistical Mechanics: Theory and Experiment|volume=2009|issue=9|pages=P09011|doi=10.1088/1742-5468/2009/09/P09011|arxiv = 0907.3320|bibcode = 2009JSMTE..09..011A|s2cid=118440998}}</ref> and equality<ref name="0VCnm">{{cite journal|author1=Naoto Shiraishi|author2=Takahiro Sagawa|name-list-style=amp|year=2015|title=Fluctuation theorem for partially masked nonequilibrium dynamics|journal=Physical Review E|volume=91|issue=1|pages=012130|doi=10.1103/PhysRevE.91.012130|pmid=25679593|arxiv = 1403.4018|bibcode = 2015PhRvE..91a2130S|s2cid=1805888}}</ref> with mutual information hold. When repeated measurements are performed, the entropy reduction of the system is given by the [[Entropy (information theory)#Entropy of a sequence|entropy of the sequence]] of measurements,<ref name=":0" /><ref>{{Cite journal|last1=Jarillo|first1=Javier|last2=Tangarife|first2=Tomás|last3=Cao|first3=Francisco J.|date=2016-01-22|title=Efficiency at maximum power of a discrete feedback ratchet|url=https://link.aps.org/doi/10.1103/PhysRevE.93.012142|journal=Physical Review E|volume=93|issue=1|pages=012142|doi=10.1103/PhysRevE.93.012142|pmid=26871058 |bibcode=2016PhRvE..93a2142J }}</ref><ref>{{Cite journal|last1=Ruiz-Pino|first1=Natalia|last2=Villarrubia-Moreno|first2=Daniel|last3=Prados|first3=Antonio|last4=Cao-García|first4=Francisco J.|date=2023-09-12|title=Information in feedback ratchets|url=https://link.aps.org/doi/10.1103/PhysRevE.108.034112|journal=Physical Review E|volume=108|issue=3|pages=034112|doi=10.1103/PhysRevE.108.034112|pmid=37849167 |arxiv=2303.16804 |bibcode=2023PhRvE.108c4112R }}</ref> which takes into account the reduction of information due to the correlation between the measurements.


== Applications ==
[The demon points to the fact that the second law is only 'statistically certain' (quote Maxwell). What this does and does not mean.]
Real-life versions of Maxwellian demons occur, but all such "real demons" or [[molecular demon]]s have their entropy-lowering effects duly balanced by increase of entropy elsewhere.<ref name="c543N">{{Cite book|title=Physics in mind : a quantum view of the brain|last=Loewenstein|first=Werner R.|isbn=9780465029846|publisher=Basic Books|location=New York|oclc=778420640|date=2013-01-29}}</ref> Molecular-sized mechanisms are no longer found only in biology; they are also the subject of the emerging field of [[nanotechnology]]. Single-atom traps used by particle physicists allow an experimenter to control the state of individual quanta in a way similar to Maxwell's demon.


If hypothetical [[mirror matter]] exists, Zurab Silagadze proposes that demons can be envisaged, "which can act like perpetuum mobiles of the second kind: extract heat energy from only one reservoir, use it to do work and be isolated from the rest of ordinary world. Yet the Second Law is not violated because the demons pay their entropy cost in the hidden (mirror) sector of the world by emitting mirror photons."<ref name="1aEYK">{{Cite journal|arxiv=physics/0608114|title=Maxwell's demon through the looking glass|journal=Acta Physica Polonica B|volume=38|issue=1|pages=101–126|year=2007|last1=Silagadze|first1=Z. K|bibcode=2007AcPPB..38..101S}}</ref>
== Exorcising the demon ==


== Experimental work ==
=== The first stage: fluctuations ===
In 2007, [[David Leigh (scientist)|David Leigh]] announced the creation of a nano-device based on the [[Brownian ratchet]] popularized by [[Richard Feynman]]. Leigh's device is able to drive a chemical system out of [[Chemical equilibrium|equilibrium]], but it must be powered by an external source ([[light]] in this case) and therefore does not violate thermodynamics.<ref name="H6rVx">{{cite journal|doi = 10.1038/nature05452|volume=445|issue=7127|title=A molecular information ratchet|journal=Nature|pages=523–527|pmid=17268466|date=February 2007|last1 = Serreli|first1 = V|last2 = Lee|first2 = CF|last3 = Kay|first3 = ER|last4 = Leigh|first4 = DA|bibcode=2007Natur.445..523S|s2cid=4314051}}</ref>


Previously, researchers including Nobel Prize winner [[Fraser Stoddart]] had created ring-shaped molecules called [[rotaxane]]s which could be placed on an axle connecting two sites, ''A'' and ''B''. Particles from either site would bump into the ring and move it from end to end. If a large collection of these devices were placed in a system, half of the devices had the ring at site ''A'' and half at ''B'', at any given moment in time.<ref name="t78Hu">{{cite journal|last1=Bissell|first1=Richard A|last2=Córdova|first2=Emilio|last3=Kaifer|first3=Angel E.|last4=Stoddart|first4=J. Fraser|title=A chemically and electrochemically switchable molecular shuttle|journal=Nature|date=12 May 1994|volume=369|issue=6476|pages=133–137|doi=10.1038/369133a0|bibcode=1994Natur.369..133B|s2cid=44926804}}</ref>
[Smoluchowksi's exorcism: the trapdoor fluctuates so fast that it doesn't work. Assumptions needed.]


Leigh made a minor change to the axle so that if a light is shone on the device, the center of the axle will thicken, restricting the motion of the ring. It keeps the ring from moving, however, only if it is at ''A''. Over time, therefore, the rings will be bumped from ''B'' to ''A'' and get stuck there, creating an imbalance in the system. In his experiments, Leigh was able to take a pot of "billions of these devices" from 50:50 equilibrium to a 70:30 imbalance within a few minutes.<ref name="bErhf">{{cite journal|author=Katharine Sanderson|date=31 January 2007|title=A demon of a device|journal=[[Nature (journal)|Nature]]|doi=10.1038/news070129-10|s2cid=121130699}}</ref>
Smoluchowski 1912, one of the early classics of the exorcist literature, contains a very short description of perhaps the simplest example of a mechanical demon: a one-way valve. Take two containers of gas, again called ''A'' and ''B'', at equal temperatures with a little hole between them. Instead of a shutter, as in Maxwell's thought experiment, put a valve on it which opens only one way, say into ''B''. The easiest way to visualise the valve is as a little trapdoor held closed by a very weak spring. Every time a molecule in ''A'' hits the trapdoor, it opens (we assume the spring is very weak) and lets the molecule pass. But whenever a molecule from ''B'' hits the valve, it remains shut, because it is pressed against the container wall. In this way, a pressure difference between ''A'' and ''B'' will build up without any change in the environment or the demon taking place, which qualifies the valve as a Maxwell’s Demon.


In 2009, [[Mark G. Raizen]] developed a laser atomic cooling technique which realizes the process Maxwell envisioned of sorting individual atoms in a gas into different containers based on their energy.<ref name="Bennett87" /><ref name="Raizen2009">{{cite journal|last = Raizen|first = Mark G.|title = Comprehensive Control of Atomic Motion|journal = Science|volume = 324|issue = 5933|pages = 1403–1406|date = June 12, 2009|doi = 10.1126/science.1171506|pmid = 19520950|bibcode = 2009Sci...324.1403R|s2cid = 10235622}}</ref><ref name="Raizen2011">{{cite journal|last = Raizen|first = Mark G.|title = Demons, Entropy, and the Quest for Absolute Zero|journal = Scientific American|volume = 304|issue = 3|pages = 54–59|date = March 2011|url = http://www.scientificamerican.com/article/demons-entropy-and-the-quest/|doi = 10.1038/scientificamerican0311-54|pmid = 21438491|access-date = November 14, 2014|bibcode =2011SciAm.304c..54R}}</ref> The new concept is a one-way wall for atoms or molecules that allows them to move in one direction, but not go back. The operation of the one-way wall relies on an irreversible atomic and molecular process of absorption of a photon at a specific wavelength, followed by spontaneous emission to a different internal state. The irreversible process is coupled to a conservative force created by magnetic fields and/or light. Raizen and collaborators proposed using the one-way wall in order to reduce the entropy of an ensemble of atoms. In parallel, Gonzalo Muga and Andreas Ruschhaupt independently developed a similar concept. Their "atom diode" was not proposed for cooling, but rather for regulating the flow of atoms. The Raizen Group demonstrated significant cooling of atoms with the one-way wall in a series of experiments in 2008. Subsequently, the operation of a one-way wall for atoms was demonstrated by Daniel Steck and collaborators later in 2008. Their experiment was based on the 2005 scheme for the one-way wall, and was not used for cooling. The cooling method realized by the Raizen Group was called "single-photon cooling", because only one photon on average is required in order to bring an atom to near-rest. This is in contrast to other [[laser cooling]] techniques which use the momentum of the photon and require a two-level cycling transition.
Smoluchowski, however, does not accept this prima facie correct reasoning. He points out that the valve will be at the same temperature as the gas. That means it will be subject to thermal fluctuations: its kinetic energy will randomly change by amount of – on average – ''1/2kT''. There are two possible scenario’s, depending on the strength of the spring which holds the trapdoor closed. Either the spring is so strong that the thermal fluctuations can hardly get the valve to move; but in that case, no molecules will be able to pass either. (After all, the kinetic energy of the molecules in any direction is also of the order ''kT''.) Or the spring is so weak that molecules from ''A'' can push aside the trap door and enter ''B'', but then the door will be a constant victim of thermal fluctuations which make it jump one way, then the other, and stop it from functioning as a pressure demon. Thus, the fact that the trapdoor has the same temperature as the gas, and therefore the same average kinetic energy fluctuations, defeats Smoluchowski’s design.


In 2006, Raizen, Muga, and Ruschhaupt showed in a theoretical paper that as each atom crosses the one-way wall, it scatters one photon, and information is provided about the turning point and hence the energy of that particle. The entropy increase of the radiation field scattered from a directional laser into a random direction is exactly balanced by the entropy reduction of the atoms as they are trapped by the one-way wall.
One may wonder whether the trapdoor would not still function as a demon, if somewhat less efficient than originally envisaged. It is open part of the time, in which case it does nothing; but it is closed another part of the time, in which case it does work. Therefore, it would create at least somewhat of a pressure gradient, although not as efficiently as we could have hoped. Bennett 1987 attempts to remove this objection. Indeed the trapdoor will stop some molecules in ''B'' from entering ''A'' (namely when it is closed). But this is compensated for by the fact that every time it bangs shut, any molecule in ''B'' which is in its path will actively be pushed into ''A'', and molecules just passing from ''A'' to ''B'' may be bounced back. An analytical solution of this problem is quite involved, but computer simulations with a similar valve have confirmed Bennet’s result; see Skordos & Zurek 1992.


This technique is widely described as a "Maxwell's demon" because it realizes Maxwell's process of creating a temperature difference by sorting high and low energy atoms into different containers. However, scientists have pointed out that it does not violate the [[second law of thermodynamics]],<ref name="Bennett87" /><ref name="Orzel">{{cite web|last = Orzel|first = Chad|title = Single-Photon Cooling: Making Maxwell's Demon|website = Uncertain Principles|publisher = [[ScienceBlogs]] website|date = January 25, 2010|url = http://scienceblogs.com/principles/2010/01/25/single-photon-cooling-making-m/|access-date = November 14, 2014}}</ref> does not result in a net decrease in entropy,<ref name="Bennett87" /><ref name="Orzel" /> and cannot be used to produce useful energy. This is because the process requires more energy from the laser beams than could be produced by the temperature difference generated. The atoms absorb low entropy photons from the laser beam and emit them in a random direction, thus increasing the entropy of the environment.<ref name="Bennett87" /><ref name="Orzel" />
=== The second stage: measurements ===


In 2014, [[Jukka Pekola|Pekola]] et al. demonstrated an experimental realization of a Szilárd engine.<ref name="Pekola 1">{{cite journal|last1=Koski|first1=J.V.|last2=Maisi|first2=V.F.|last3=Sagava|first3=T.|last4=Pekola|first4=J.P.|title=Experimental Observation of the Role of Mutual Information in the Nonequilibrium Dynamics of a Maxwell Demon|journal=Physical Review Letters|date=14 July 2014|volume=113|issue=3|page=030601|doi=10.1103/PhysRevLett.113.030601|pmid=25083623|arxiv=1405.1272|bibcode=2014PhRvL.113c0601K|s2cid=119311588|url=https://aaltodoc.aalto.fi/handle/123456789/16122}}</ref><ref name="Pekola 2">{{cite journal|last1=Koski|first1=J.V.|last2=Maisi|first2=V.F.|last3=Pekola|first3=J.P.|last4=Averin|first4=D.V.|title=Experimental realization of a Szilard engine with a single electron|journal=Proceedings of the National Academy of Sciences of the United States of America|date=23 Sep 2014|volume=111|issue=38|pages=13786–9|doi=10.1073/pnas.1406966111|pmid=25201966|pmc=4183300|arxiv=1402.5907|bibcode=2014PNAS..11113786K|doi-access=free}}</ref> Only a year later and based on an earlier theoretical proposal,<ref name="Strasberg et al">{{cite journal|last1=Strasberg|first1=P.|last2=Schaller|first2=G.|last3=Brandes|first3=T.|last4=Esposito|first4=M.|title=Thermodynamics of a Physical Model Implementing a Maxwell Demon|journal=Physical Review Letters|date=24 Jan 2013|volume=110|issue=4|page=040601|doi=10.1103/PhysRevLett.110.040601|pmid=25166147|arxiv=1210.5661|bibcode=2013PhRvL.110d0601S|s2cid=5782312|url=http://orbilu.uni.lu/handle/10993/11416|type=Submitted manuscript}}</ref> the same group presented the first experimental realization of an autonomous Maxwell's demon, which extracts microscopic information from a system and reduces its entropy by applying feedback. The demon is based on two capacitively coupled single-electron devices, both integrated on the same electronic circuit. The operation of the demon is directly observed as a temperature drop in the system, with a simultaneous temperature rise in the demon arising from the thermodynamic cost of generating the mutual information.<ref name="Pekola 3">{{cite journal|last1=Koski|first1=J.V.|last2=Kutvonen|first2=A.|last3=Khaymovich|first3=I.M.|last4=Ala-Nissila|first4=T.|last5=Pekola|first5=J.P.|title=On-Chip Maxwell's Demon as an Information-Powered Refrigerator|journal=Physical Review Letters|year=2015|volume=115|issue=26|page=260602|doi=10.1103/PhysRevLett.115.260602|pmid=26764980|arxiv=1507.00530|bibcode=2015PhRvL.115z0602K|s2cid=3393380}}</ref> In 2016, Pekola et al. demonstrated a proof-of-principle of an autonomous demon in coupled single-electron circuits, showing a way to cool critical elements in a circuit with information as a fuel.<ref name="Pekola 4">{{cite journal|last1=Koski|first1=J.V.|last2=Pekola|first2=J.P.|title=Maxwell's demons realized in electronic circuits|journal=Comptes Rendus Physique|date=16 December 2016|volume=17|issue=10|pages=1130–1138|doi=10.1016/j.crhy.2016.08.011|bibcode=2016CRPhy..17.1130K|doi-access=free}}</ref> Pekola et al. have also proposed that a simple qubit circuit, e.g., made of a superconducting circuit, could provide a basis to study a quantum Szilard's engine.<ref name="Pekola 5">{{cite journal|last1=Pekola|first1=J.P.|last2=Golubev|first2=D.S.|last3=Averin|first3=D.V.|title=Maxwell's demon based on a single qubit|journal=Physical Review B|date=5 Jan 2016|volume=93|issue=2|page=024501|doi=10.1103/PhysRevB.93.024501|arxiv=1508.03803|bibcode=2016PhRvB..93b4501P|s2cid=55523206}}</ref>
[Szilard and Brillouin's exorcism: measuring the molecules costs energy. Assumptions needed.]


== As metaphor ==
=== The third stage: information ===
[[Daemon (computing)|Daemons in computing]], generally processes that run on servers to respond to users, are named for Maxwell's demon.<ref name="OjRq9">{{Cite web|url=http://www.takeourword.com/TOW146/page4.html|author=Fernando J. Corbató|title=Take Our Word for It|date=2002-01-23|access-date=2006-08-20|author-link=Fernando J. Corbató}}</ref>


Historian [[Henry Brooks Adams]], in his manuscript ''[[The Rule of Phase Applied to History]]'', attempted to use Maxwell's demon as a historical [[metaphor]], though he misunderstood and misapplied the original principle.<ref name="lKeHq">[[#Cater|Cater (1947)]], pp. 640–647; see also Daub (1970), reprinted in [[#Leff Rex 90|Leff & Rex (1990)]], pp. 37–51.</ref> Adams interpreted [[history]] as a process moving towards "equilibrium", but he saw [[militarism|militaristic]] nations (he felt [[Germany]] pre-eminent in this class) as tending to reverse this process, a Maxwell's demon of history. Adams made many attempts to respond to the criticism of his formulation from his scientific colleagues, but the work remained incomplete at his death in 1918 and was published posthumously.<ref name="UgW96">[[#Adams|Adams (1919)]], p. 267.</ref>
[Landauer and Bennett's exorcism using information erasure. Controversy, assumptions needed.]
== See also ==
{{div col|colwidth=18em}}
* [[Brownian ratchet]]
* [[Catalysis]]
* ''[[Chance and Necessity]]''
* [[Dispersive mass transfer]]
* [[Entropy in thermodynamics and information theory]]
* [[Evaporation]]
* [[Gibbs paradox]]
* [[Hall effect]]
* [[Heisenberg's uncertainty principle]]
* [[Joule–Thomson effect]]
* [[Laplace's demon]]
* [[Laws of thermodynamics]]
* [[Mass spectrometry]]
* [[Photoelectric effect]]
* [[Quantum tunnelling]]
* [[Schrödinger's cat]]
* [[Second law of thermodynamics]]
* [[Thermionic emission]]
* [[Vortex tube]]
{{div col end}}


== Notes ==
== Is Maxwell's Demon still alive? ==
{{reflist|colwidth=30em}}


== References ==
[Recent anti-exorcist voices; specifically Norton and Earman. NPOV conclusion: there is no consensus.]
{{refbegin}}
* {{cite book|editor=Cater, H. D.|title=Henry Adams and his Friends|publisher=Boston|year=1947|ref=Cater}}
* {{cite journal|author=Daub, E. E.|year=1967|title=Atomism and Thermodynamics|journal=[[Isis (journal)|Isis]]|volume=58|issue=3|pages=293–303|doi=10.1086/350264|s2cid=143459461|ref=Daub}}
* {{cite book|editor=Leff, Harvey S. & Andrew F. Rex|year=1990|title=Maxwell's Demon: Entropy, Information, Computing|location=Bristol|publisher=Adam-Hilger|isbn=978-0-7503-0057-5|ref=Leff_Rex_90}}
* {{cite book|editor=Leff, Harvey S. & Andrew F. Rex|year=2002|title=Maxwell's Demon 2: Entropy, Classical and Quantum Information, Computing|publisher=[[CRC Press]]|isbn=978-0-7503-0759-8|ref=Leff_Rex_02}}
* {{cite book|author=Adams, H.|title=The Degradation of the Democratic Dogma|location=New York|publisher=Kessinger|year=1919|isbn=978-1-4179-1598-9|ref=Adams}}
{{refend}}


== External links ==
{{wikiquote}}
* [https://quantamagazine.org/how-maxwells-demon-continues-to-startle-scientists-20210422 How Maxwell's Demon Continues to Startle Scientists]
* Bennett, C. H. (1987) "Demons, Engines and the Second Law", ''[[Scientific American]]'', November, ''pp''108-116
* {{cite journal|author=Binder, P.-M.|year=2008|pages= 1334–1335|issue=5906|title=Reflections on a Wall of Light|volume=322|journal=Science|doi=10.1126/science.1166681|pmid=19039125|s2cid=42821883}}
* {{cite journal|author1=Earman, J. |author2=Norton, J. |name-list-style=amp|year=1998|title=Exorcist XIV: The Wrath of Maxwell's Demon. Part I. From Maxwell to Szilard|journal=Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics|volume=29|issue=4|pages=435–471|doi=10.1016/S1355-2198(98)00023-9|url=http://www.pitt.edu/~jdnorton/papers/ExorcistXIV/Exorcist1.pdf|bibcode=1998SHPMP..29..435E}}
* {{cite journal|author1=Earman, J. |author2=Norton, J. |name-list-style=amp|year=1999|title=Exorcist XIV: The Wrath of Maxwell's Demon. Part II. From Szilard to Landauer and Beyond|journal=Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics|volume=30|issue=1|pages=1–40|doi= 10.1016/s1355-2198(98)00026-4|bibcode=1999SHPMP..30....1E|url=http://www.pitt.edu/~jdnorton/papers/ExorcistXIV/Exorcist2.pdf }}
* {{cite book|author=Feynman, R. P.|title=Feynman Lectures on Computation|url=https://archive.org/details/feynmanlectureso0000feyn|url-access=registration|publisher=Addison-Wesley|year=1996|isbn=978-0-14-028451-5|pages=[https://archive.org/details/feynmanlectureso0000feyn/page/148 148–150]|display-authors=etal}}
* {{cite book|author=Jordy, W. H.|title=Henry Adams: Scientific Historian|publisher=New Haven|year=1952|isbn=978-0-685-26683-0 }}
* {{cite web|url=https://khanexercises.appspot.com/video?v=aKRDvSZ-igA|archive-url=https://web.archive.org/web/20100317034202/http://khanexercises.appspot.com/video?v=aKRDvSZ-igA|url-status=dead|archive-date=2010-03-17|title=Maxwell's Demon|author=Khan, Salman }}
* Maroney, O. J. E. (2009) "[http://plato.stanford.edu/entries/information-entropy/ "Information Processing and Thermodynamic Entropy]" The Stanford Encyclopedia of Philosophy (Autumn 2009 Edition)
* {{cite book|author=Maxwell, J. C.|title=Theory of Heat|url=https://archive.org/details/theoryofheat00maxwrich|publisher= London, New York [etc.] Longmans, Green|year=1871 }}, reprinted (2001) New York: Dover, {{ISBN|0-486-41735-2}}
* {{cite journal|author=Norton, J.|year=2005|title=Eaters of the lotus: Landauer's principle and the return of Maxwell's demon|journal=Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics|volume=36|issue=2|pages=375–411|doi=10.1016/j.shpsb.2004.12.002|url=http://philsci-archive.pitt.edu/archive/00001729/02/Norton.pdf|archive-url=https://web.archive.org/web/20060901211014/http://philsci-archive.pitt.edu/archive/00001729/02/Norton.pdf|archive-date=2006-09-01|url-status=live|bibcode=2005SHPMP..36..375N|citeseerx=10.1.1.468.3017|s2cid=21104635 }}
* Raizen, Mark G. (2011) "Demons, Entropy, and the Quest for Absolute Zero", ''[[Scientific American]], ''March, ''pp''54-59
* Reaney, Patricia. [http://www.iol.co.za/index.php?set_id=1&click_id=116&art_id=qw1170340561317B216 "Scientists build nanomachine"], ''Reuters'', February 1, 2007
* Rubi, J Miguel, "[http://www.sciam.com/article.cfm?id=how-nature-breaks-the-second-law&sc=SA_20081020 Does Nature Break the Second Law of Thermodynamics?]"; Scientific American, October 2008 :
* Splasho (2008) – [http://splasho.com/blog/essays/maxwell-thermodynamics-meets-the-demon/ Historical development of Maxwell's demon]
* Weiss, Peter. [https://web.archive.org/web/20070621222301/http://www.sciencenews.org/articles/20001007/bob9.asp "Breaking the Law – Can quantum mechanics + thermodynamics = perpetual motion?"], ''Science News'', October 7, 2000


[[Category:1867 introductions]]

[[Category:Fictional demons]]
== Temporary repository of old article ==
[[Category:James Clerk Maxwell]]

[[Category:Nanotechnology]]
The demon is an excellent demonstration of [[entropy]], how it is related to
[[Category:Perpetual motion]]
:(a) the fraction of energy that is not available to do useful work, and
[[Category:Philosophy of thermal and statistical physics]]
:(b) the amount of information we lack about the detailed state of the system.
[[Category:Thought experiments in physics]]
In Maxwell's thought experiment, the demon manages to decrease the entropy. In other words, it increases the amount of energy available by increasing its knowledge about the motion of all the molecules.

The [[Second law of thermodynamics|Second law]] of [[Thermodynamics]] says this is impossible: you can only increase entropy (or rather, you can decrease it at one place as long as that is balanced by at least as big an increase somewhere else).

So, why wouldn't a setup like Maxwell's demon work? The question was first answered in [[1929]] by [[Leó Szilárd]].
Any real "demon" that does this would not be a disembodied spirit receiving its information telepathically; to acquire information about the world you must be in physical interaction with it. In determining what side of the gate a molecule must be on, the demon must store information about the state of the molecule. Eventually, the demon will run out of information storage space and must begin to erase the information that has been previously gathered. Erasing information is a thermodynamically irreversible process that increases the entropy of a system. Maxwell's demon therefore reveals a deep connection between [[thermodynamics]] and [[information theory]].

Real-life versions of Maxwellian demons (with their entropy lowering effects of course duly balanced by increase of entropy elsewhere) actually occur in living systems, such as the [[ion channel]]s and [[transmembrane ATPase|pumps]] that make our [[nervous system]]s work, including our brains.
Molecular-sized mechanisms are no longer found only in biology; they are also the subject of the emerging field of [[nanotechnology]].

Maxwell's demon plays a significant role in the book ''[[The Crying of Lot 49]]'' by noted author [[Thomas Pynchon]].


==External links and references==

* [[Richard Feynman|Feynman, Richard P.]], ''Feynman Lectures on Computation'' (Perseus: 1996). ISBN 0201489910.
* Grayce, Christopher J., "''[http://www.chem.uci.edu/education/undergrad_pgm/applets/bounce/demon.htm Maxwell's Demon]''". Educational Applets. University of California, Irvine, Irvine, CA.
* [http://www.ipmt-hpm.ac.ru/SecondLaw/index.en.html First International Conference on Quantum Limits to the Second Law of Thermodynamics], San Diego, CA, July 2002
* Vlatko Vedral's [http://www.qubit.org/people/vlatko/Papers/maxwell2.pdf Lengthy discussion of Maxwell's Demon] ([[Portable Document Format|PDF]])
* Xin Yong Fu and Zi Tao Fu, "''[http://arxiv.org/abs/physics/0311104 Realization of Maxwell's Hypothesis : An Experiment Against the Second Law of Thermodynamics]''". Shanghai Jiao Tong University, Shanghai, P.R. China ([[arXiv.org]] is a site for pre-prints of scientific papers; but this paper is not endorsed or sponsored under arXiv's procedures by any known scientist including the authors.)
* Charles H. Bennet, "Demons, Engines and the Second Law", Scientific American , pp.108-116 (November, 1987).


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[[Category:Thermodynamics]]

Latest revision as of 04:23, 22 November 2024

Schematic figure of Maxwell's demon thought experiment

Maxwell's demon is a thought experiment that appears to disprove the second law of thermodynamics. It was proposed by the physicist James Clerk Maxwell in 1867.[1] In his first letter, Maxwell referred to the entity as a "finite being" or a "being who can play a game of skill with the molecules". Lord Kelvin would later call it a "demon".[2]

In the thought experiment, a demon controls a door between two chambers containing gas. As individual gas molecules (or atoms) approach the door, the demon quickly opens and closes the door to allow only fast-moving molecules to pass through in one direction, and only slow-moving molecules to pass through in the other. Because the kinetic temperature of a gas depends on the velocities of its constituent molecules, the demon's actions cause one chamber to warm up and the other to cool down. This would decrease the total entropy of the system, seemingly without applying any work, thereby violating the second law of thermodynamics.

The concept of Maxwell's demon has provoked substantial debate in the philosophy of science and theoretical physics, which continues to the present day. It stimulated work on the relationship between thermodynamics and information theory. Most scientists argue that, on theoretical grounds, no practical device can violate the second law in this way. Other researchers have implemented forms of Maxwell's demon in experiments, though they all differ from the thought experiment to some extent and none has been shown to violate the second law.

Origin and history of the idea

[edit]

The thought experiment first appeared in a letter Maxwell wrote to Peter Guthrie Tait on 11 December 1867. It appeared again in a letter to John William Strutt in 1871, before it was presented to the public in Maxwell's 1872 book on thermodynamics titled Theory of Heat.[3]

In his letters and books, Maxwell described the agent opening the door between the chambers as a "finite being". Being a deeply religious man, he never used the word "demon". Instead, William Thomson (Lord Kelvin) was the first to use it for Maxwell's concept, in the journal Nature in 1874, and implied that he intended the Greek mythology interpretation of a daemon, a supernatural being working in the background, rather than a malevolent being.[2][4][5]

Original thought experiment

[edit]

The second law of thermodynamics ensures (through statistical probability) that two bodies of different temperature, when brought into contact with each other and isolated from the rest of the Universe, will evolve to a thermodynamic equilibrium in which both bodies have approximately the same temperature.[6] The second law is also expressed as the assertion that in an isolated system, entropy never decreases.[6]

Maxwell conceived a thought experiment as a way of furthering the understanding of the second law. His description of the experiment is as follows:[6][7]

... if we conceive of a being whose faculties are so sharpened that he can follow every molecule in its course, such a being, whose attributes are as essentially finite as our own, would be able to do what is impossible to us. For we have seen that molecules in a vessel full of air at uniform temperature are moving with velocities by no means uniform, though the mean velocity of any great number of them, arbitrarily selected, is almost exactly uniform. Now let us suppose that such a vessel is divided into two portions, A and B, by a division in which there is a small hole, and that a being, who can see the individual molecules, opens and closes this hole, so as to allow only the swifter molecules to pass from A to B, and only the slower molecules to pass from B to A. He will thus, without expenditure of work, raise the temperature of B and lower that of A, in contradiction to the second law of thermodynamics.

In other words, Maxwell imagines one container divided into two parts, A and B.[6][8] Both parts are filled with the same gas at equal temperatures and placed next to each other. Observing the molecules on both sides, an imaginary demon guards a trapdoor between the two parts. When a faster-than-average molecule from A flies towards the trapdoor, the demon opens it, and the molecule will fly from A to B. Likewise, when a slower-than-average molecule from B flies towards the trapdoor, the demon will let it pass from B to A. The average speed of the molecules in B will have increased while in A they will have slowed down on average. Since average molecular speed corresponds to temperature, the temperature decreases in A and increases in B, contrary to the second law of thermodynamics. A heat engine operating between the thermal reservoirs A and B could extract useful work from this temperature difference.

The demon must allow molecules to pass in both directions in order to produce only a temperature difference; one-way passage only of faster-than-average molecules from A to B will cause higher temperature and pressure to develop on the B side.

Criticism and development

[edit]

Several physicists have presented calculations that show that the second law of thermodynamics will not actually be violated, if a more complete analysis is made of the whole system including the demon.[6][8][9] The essence of the physical argument is to show, by calculation, that any demon must "generate" more entropy segregating the molecules than it could ever eliminate by the method described. That is, it would take more thermodynamic work to gauge the speed of the molecules and selectively allow them to pass through the opening between A and B than the amount of energy gained by the difference of temperature caused by doing so.

One of the most famous responses to this question was suggested in 1929 by Leó Szilárd,[10] and later by Léon Brillouin.[6][8] Szilárd pointed out that a real-life Maxwell's demon would need to have some means of measuring molecular speed, and that the act of acquiring information would require an expenditure of energy. Since the demon and the gas are interacting, we must consider the total entropy of the gas and the demon combined. The expenditure of energy by the demon will cause an increase in the entropy of the demon, which will be larger than the lowering of the entropy of the gas.

In 1960, Rolf Landauer raised an exception to this argument.[6][8][11] He realized that some measuring processes need not increase thermodynamic entropy as long as they were thermodynamically reversible. He suggested these "reversible" measurements could be used to sort the molecules, violating the Second Law. However, due to the connection between entropy in thermodynamics and information theory, this also meant that the recorded measurement must not be erased. In other words, to determine whether to let a molecule through, the demon must acquire information about the state of the molecule and either discard it or store it. Discarding it leads to immediate increase in entropy, but the demon cannot store it indefinitely. In 1982, Charles Bennett showed that, however well prepared, eventually the demon will run out of information storage space and must begin to erase the information it has previously gathered.[8][12] Erasing information is a thermodynamically irreversible process that increases the entropy of a system. Although Bennett had reached the same conclusion as Szilard's 1929 paper, that a Maxwellian demon could not violate the second law because entropy would be created, he had reached it for different reasons. Regarding Landauer's principle, the minimum energy dissipated by deleting information was experimentally measured by Eric Lutz et al. in 2012. Furthermore, Lutz et al. confirmed that in order to approach the Landauer's limit, the system must asymptotically approach zero processing speed.[13] Recently, Landauer's principle has also been invoked to resolve an apparently unrelated paradox of statistical physics, Loschmidt’s paradox. [14]

John Earman and John D. Norton have argued that Szilárd and Landauer's explanations of Maxwell's demon begin by assuming that the second law of thermodynamics cannot be violated by the demon, and derive further properties of the demon from this assumption, including the necessity of consuming energy when erasing information, etc.[15][16] It would therefore be circular to invoke these derived properties to defend the second law from the demonic argument. Bennett later acknowledged the validity of Earman and Norton's argument, while maintaining that Landauer's principle explains the mechanism by which real systems do not violate the second law of thermodynamics.[17]

Recent progress

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Although the argument by Landauer and Bennett only answers the consistency between the second law of thermodynamics and the whole cyclic process of the entire system of a Szilard engine (a composite system of the engine and the demon), a recent approach based on the non-equilibrium thermodynamics for small fluctuating systems has provided deeper insight on each information process with each subsystem. From this viewpoint, the measurement process is regarded as a process where the correlation (mutual information) between the engine and the demon increases, decreasing the entropy of the system in an amount given by the mutual information.[18] If the correlation changes, thermodynamic relations such as the second law of thermodynamics and the fluctuation theorem for each subsystem should be modified, and for the case of external control a second-law like inequality[18][19][20] and a generalized fluctuation theorem[21] with mutual information are satisfied. For more general information processes including biological information processing, both inequality[22] and equality[23] with mutual information hold. When repeated measurements are performed, the entropy reduction of the system is given by the entropy of the sequence of measurements,[18][24][25] which takes into account the reduction of information due to the correlation between the measurements.

Applications

[edit]

Real-life versions of Maxwellian demons occur, but all such "real demons" or molecular demons have their entropy-lowering effects duly balanced by increase of entropy elsewhere.[26] Molecular-sized mechanisms are no longer found only in biology; they are also the subject of the emerging field of nanotechnology. Single-atom traps used by particle physicists allow an experimenter to control the state of individual quanta in a way similar to Maxwell's demon.

If hypothetical mirror matter exists, Zurab Silagadze proposes that demons can be envisaged, "which can act like perpetuum mobiles of the second kind: extract heat energy from only one reservoir, use it to do work and be isolated from the rest of ordinary world. Yet the Second Law is not violated because the demons pay their entropy cost in the hidden (mirror) sector of the world by emitting mirror photons."[27]

Experimental work

[edit]

In 2007, David Leigh announced the creation of a nano-device based on the Brownian ratchet popularized by Richard Feynman. Leigh's device is able to drive a chemical system out of equilibrium, but it must be powered by an external source (light in this case) and therefore does not violate thermodynamics.[28]

Previously, researchers including Nobel Prize winner Fraser Stoddart had created ring-shaped molecules called rotaxanes which could be placed on an axle connecting two sites, A and B. Particles from either site would bump into the ring and move it from end to end. If a large collection of these devices were placed in a system, half of the devices had the ring at site A and half at B, at any given moment in time.[29]

Leigh made a minor change to the axle so that if a light is shone on the device, the center of the axle will thicken, restricting the motion of the ring. It keeps the ring from moving, however, only if it is at A. Over time, therefore, the rings will be bumped from B to A and get stuck there, creating an imbalance in the system. In his experiments, Leigh was able to take a pot of "billions of these devices" from 50:50 equilibrium to a 70:30 imbalance within a few minutes.[30]

In 2009, Mark G. Raizen developed a laser atomic cooling technique which realizes the process Maxwell envisioned of sorting individual atoms in a gas into different containers based on their energy.[6][31][32] The new concept is a one-way wall for atoms or molecules that allows them to move in one direction, but not go back. The operation of the one-way wall relies on an irreversible atomic and molecular process of absorption of a photon at a specific wavelength, followed by spontaneous emission to a different internal state. The irreversible process is coupled to a conservative force created by magnetic fields and/or light. Raizen and collaborators proposed using the one-way wall in order to reduce the entropy of an ensemble of atoms. In parallel, Gonzalo Muga and Andreas Ruschhaupt independently developed a similar concept. Their "atom diode" was not proposed for cooling, but rather for regulating the flow of atoms. The Raizen Group demonstrated significant cooling of atoms with the one-way wall in a series of experiments in 2008. Subsequently, the operation of a one-way wall for atoms was demonstrated by Daniel Steck and collaborators later in 2008. Their experiment was based on the 2005 scheme for the one-way wall, and was not used for cooling. The cooling method realized by the Raizen Group was called "single-photon cooling", because only one photon on average is required in order to bring an atom to near-rest. This is in contrast to other laser cooling techniques which use the momentum of the photon and require a two-level cycling transition.

In 2006, Raizen, Muga, and Ruschhaupt showed in a theoretical paper that as each atom crosses the one-way wall, it scatters one photon, and information is provided about the turning point and hence the energy of that particle. The entropy increase of the radiation field scattered from a directional laser into a random direction is exactly balanced by the entropy reduction of the atoms as they are trapped by the one-way wall.

This technique is widely described as a "Maxwell's demon" because it realizes Maxwell's process of creating a temperature difference by sorting high and low energy atoms into different containers. However, scientists have pointed out that it does not violate the second law of thermodynamics,[6][33] does not result in a net decrease in entropy,[6][33] and cannot be used to produce useful energy. This is because the process requires more energy from the laser beams than could be produced by the temperature difference generated. The atoms absorb low entropy photons from the laser beam and emit them in a random direction, thus increasing the entropy of the environment.[6][33]

In 2014, Pekola et al. demonstrated an experimental realization of a Szilárd engine.[34][35] Only a year later and based on an earlier theoretical proposal,[36] the same group presented the first experimental realization of an autonomous Maxwell's demon, which extracts microscopic information from a system and reduces its entropy by applying feedback. The demon is based on two capacitively coupled single-electron devices, both integrated on the same electronic circuit. The operation of the demon is directly observed as a temperature drop in the system, with a simultaneous temperature rise in the demon arising from the thermodynamic cost of generating the mutual information.[37] In 2016, Pekola et al. demonstrated a proof-of-principle of an autonomous demon in coupled single-electron circuits, showing a way to cool critical elements in a circuit with information as a fuel.[38] Pekola et al. have also proposed that a simple qubit circuit, e.g., made of a superconducting circuit, could provide a basis to study a quantum Szilard's engine.[39]

As metaphor

[edit]

Daemons in computing, generally processes that run on servers to respond to users, are named for Maxwell's demon.[40]

Historian Henry Brooks Adams, in his manuscript The Rule of Phase Applied to History, attempted to use Maxwell's demon as a historical metaphor, though he misunderstood and misapplied the original principle.[41] Adams interpreted history as a process moving towards "equilibrium", but he saw militaristic nations (he felt Germany pre-eminent in this class) as tending to reverse this process, a Maxwell's demon of history. Adams made many attempts to respond to the criticism of his formulation from his scientific colleagues, but the work remained incomplete at his death in 1918 and was published posthumously.[42]

See also

[edit]

Notes

[edit]
  1. ^ Cargill Gilston Knott (1911). "Quote from undated letter from Maxwell to Tait". Life and Scientific Work of Peter Guthrie Tait. Cambridge University Press. pp. 213–215.
  2. ^ a b Thomson, William (9 April 1874). "Kinetic theory of the dissipation of energy". Nature. 9 (232): 441–444. Bibcode:1874Natur...9..441T. doi:10.1038/009441c0.
  3. ^ Leff & Rex (2002), p. 370.
  4. ^ "The sorting demon of Maxwell". Nature. 20 (501): 126. 1879. Bibcode:1879Natur..20Q.126.. doi:10.1038/020126a0.
  5. ^ Weber, Alan S. (2000). Nineteenth Century Science: a Selection of Original Texts. Broadview Press. p. 300.
  6. ^ a b c d e f g h i j k Bennett, Charles H. (November 1987). "Demons, Engines, and the Second Law" (PDF). Scientific American. 257 (5): 108–116. Bibcode:1987SciAm.257e.108B. doi:10.1038/scientificamerican1187-108. Archived from the original (PDF) on December 3, 2020. Retrieved November 13, 2014.
  7. ^ Maxwell (1871), reprinted in Leff & Rex (1990) on p. 4.
  8. ^ a b c d e Sagawa, Takahiro (2012). Thermodynamics of Information Processing in Small Systems. Springer Science and Business Media. pp. 9–14. ISBN 978-4431541677.
  9. ^ Bennett, Charles H.; Schumacher, Benjamin (August 2011). "Maxwell's demons appear in the lab" (PDF). Nikkei Science: 3–6. Retrieved November 13, 2014.
  10. ^ Szilard, Leo (1929). "Über die Entropieverminderung in einem thermodynamischen System bei Eingriffen intelligenter Wesen (On the reduction of entropy in a thermodynamic system by the intervention of intelligent beings)". Zeitschrift für Physik. 53 (11–12): 840–856. Bibcode:1929ZPhy...53..840S. doi:10.1007/bf01341281. S2CID 122038206. cited in Bennett 1987. English translation available as NASA document TT F-16723 published 1976
  11. ^ Landauer, R. (1961). "Irreversibility and heat generation in the computing process" (PDF). IBM Journal of Research and Development. 5 (3): 183–191. doi:10.1147/rd.53.0183. Retrieved November 13, 2014. reprinted in Vol. 44, No. 1, January 2000, p. 261 Archived 2016-03-03 at the Wayback Machine
  12. ^ Bennett, C. H. (1982). "The thermodynamics of computation—a review" (PDF). International Journal of Theoretical Physics (Submitted manuscript). 21 (12): 905–940. Bibcode:1982IJTP...21..905B. CiteSeerX 10.1.1.655.5610. doi:10.1007/BF02084158. S2CID 17471991. Archived from the original (PDF) on 2014-10-14. Retrieved 2017-12-10.
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  21. ^ Takahiro Sagawa & Masahito Ueda (2010). "Generalized Jarzynski Equality under Nonequilibrium Feedback Control". Physical Review Letters. 104 (9): 090602. arXiv:0907.4914. Bibcode:2010PhRvL.104i0602S. doi:10.1103/PhysRevLett.104.090602. PMID 20366975. S2CID 1549122.
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  23. ^ Naoto Shiraishi & Takahiro Sagawa (2015). "Fluctuation theorem for partially masked nonequilibrium dynamics". Physical Review E. 91 (1): 012130. arXiv:1403.4018. Bibcode:2015PhRvE..91a2130S. doi:10.1103/PhysRevE.91.012130. PMID 25679593. S2CID 1805888.
  24. ^ Jarillo, Javier; Tangarife, Tomás; Cao, Francisco J. (2016-01-22). "Efficiency at maximum power of a discrete feedback ratchet". Physical Review E. 93 (1): 012142. Bibcode:2016PhRvE..93a2142J. doi:10.1103/PhysRevE.93.012142. PMID 26871058.
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  32. ^ Raizen, Mark G. (March 2011). "Demons, Entropy, and the Quest for Absolute Zero". Scientific American. 304 (3): 54–59. Bibcode:2011SciAm.304c..54R. doi:10.1038/scientificamerican0311-54. PMID 21438491. Retrieved November 14, 2014.
  33. ^ a b c Orzel, Chad (January 25, 2010). "Single-Photon Cooling: Making Maxwell's Demon". Uncertain Principles. ScienceBlogs website. Retrieved November 14, 2014.
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  35. ^ Koski, J.V.; Maisi, V.F.; Pekola, J.P.; Averin, D.V. (23 Sep 2014). "Experimental realization of a Szilard engine with a single electron". Proceedings of the National Academy of Sciences of the United States of America. 111 (38): 13786–9. arXiv:1402.5907. Bibcode:2014PNAS..11113786K. doi:10.1073/pnas.1406966111. PMC 4183300. PMID 25201966.
  36. ^ Strasberg, P.; Schaller, G.; Brandes, T.; Esposito, M. (24 Jan 2013). "Thermodynamics of a Physical Model Implementing a Maxwell Demon". Physical Review Letters (Submitted manuscript). 110 (4): 040601. arXiv:1210.5661. Bibcode:2013PhRvL.110d0601S. doi:10.1103/PhysRevLett.110.040601. PMID 25166147. S2CID 5782312.
  37. ^ Koski, J.V.; Kutvonen, A.; Khaymovich, I.M.; Ala-Nissila, T.; Pekola, J.P. (2015). "On-Chip Maxwell's Demon as an Information-Powered Refrigerator". Physical Review Letters. 115 (26): 260602. arXiv:1507.00530. Bibcode:2015PhRvL.115z0602K. doi:10.1103/PhysRevLett.115.260602. PMID 26764980. S2CID 3393380.
  38. ^ Koski, J.V.; Pekola, J.P. (16 December 2016). "Maxwell's demons realized in electronic circuits". Comptes Rendus Physique. 17 (10): 1130–1138. Bibcode:2016CRPhy..17.1130K. doi:10.1016/j.crhy.2016.08.011.
  39. ^ Pekola, J.P.; Golubev, D.S.; Averin, D.V. (5 Jan 2016). "Maxwell's demon based on a single qubit". Physical Review B. 93 (2): 024501. arXiv:1508.03803. Bibcode:2016PhRvB..93b4501P. doi:10.1103/PhysRevB.93.024501. S2CID 55523206.
  40. ^ Fernando J. Corbató (2002-01-23). "Take Our Word for It". Retrieved 2006-08-20.
  41. ^ Cater (1947), pp. 640–647; see also Daub (1970), reprinted in Leff & Rex (1990), pp. 37–51.
  42. ^ Adams (1919), p. 267.

References

[edit]
  • Cater, H. D., ed. (1947). Henry Adams and his Friends. Boston.
  • Daub, E. E. (1967). "Atomism and Thermodynamics". Isis. 58 (3): 293–303. doi:10.1086/350264. S2CID 143459461.
  • Leff, Harvey S. & Andrew F. Rex, ed. (1990). Maxwell's Demon: Entropy, Information, Computing. Bristol: Adam-Hilger. ISBN 978-0-7503-0057-5.
  • Leff, Harvey S. & Andrew F. Rex, ed. (2002). Maxwell's Demon 2: Entropy, Classical and Quantum Information, Computing. CRC Press. ISBN 978-0-7503-0759-8.
  • Adams, H. (1919). The Degradation of the Democratic Dogma. New York: Kessinger. ISBN 978-1-4179-1598-9.
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