Ehrenfest Model
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The Ehrenfest model (or dog–flea model) of
diffusion Diffusion is the net movement of anything (for example, atoms, ions, molecules, energy) generally from a region of higher concentration to a region of lower concentration. Diffusion is driven by a gradient in Gibbs free energy or chemical p ...
was proposed by
Tatiana Tatiana (or Tatianna, also romanized as Tatyana, Tatjana, Tatijana, etc.) is a female name of Sabine-Roman origin that became widespread in Eastern Europe. Origin Tatiana is a feminine, diminutive derivative of the Sabine—and later Latinâ ...
and
Paul Ehrenfest Paul Ehrenfest (; 18 January 1880 – 25 September 1933) was an Austrian Theoretical physics, theoretical physicist who made major contributions to statistical mechanics and its relation to quantum physics, quantum mechanics, including the theory ...
to explain the
second law of thermodynamics The second law of thermodynamics is a physical law based on Universal (metaphysics), universal empirical observation concerning heat and Energy transformation, energy interconversions. A simple statement of the law is that heat always flows spont ...
. The model considers ''N'' particles in two containers. Particles independently change container at a rate ''λ''. If ''X''(''t'') = ''i'' is defined to be the number of particles in one container at time ''t'', then it is a
birth–death process The birth–death process (or birth-and-death process) is a special case of continuous-time Markov process where the state transitions are of only two types: "births", which increase the state variable by one and "deaths", which decrease the stat ...
with transition rates * q_ = i\, \lambda for ''i'' = 1, 2, ..., ''N'' * q_ = (N-i\,) \lambda for ''i'' = 0, 1, ..., ''N'' – 1 and equilibrium distribution \pi_i = 2^ \tbinom Ni.
Mark Kac Mark Kac ( ; Polish: ''Marek Kac''; August 3, 1914 – October 26, 1984) was a Polish-American mathematician. His main interest was probability theory. His question, " Can one hear the shape of a drum?" set off research into spectral theory, th ...
proved in 1947 that if the initial system state is not equilibrium, then the
entropy Entropy is a scientific concept, most commonly associated with states of disorder, randomness, or uncertainty. The term and the concept are used in diverse fields, from classical thermodynamics, where it was first recognized, to the micros ...
, given by :H(t) = -\sum_ P(X(t)=i) \log \left( \frac\right), is monotonically increasing (
H-theorem In classical statistical mechanics, the ''H''-theorem, introduced by Ludwig Boltzmann in 1872, describes the tendency of the quantity ''H'' (defined below) to decrease in a nearly-ideal gas of molecules.L. Boltzmann,Weitere Studien über das Wär ...
). This is a consequence of the convergence to the equilibrium distribution.


Interpretation of results

Consider that at the beginning all the particles are in one of the containers. It is expected that over time the number of particles in this container will approach N/2 and stabilize near that state (containers will have approximately the same number of particles). However from mathematical point of view, going back to the initial state is possible (even almost sure). From mean recurrence theorem follows that even the expected time to going back to the initial state is finite, and it is 2^N. Using
Stirling's approximation In mathematics, Stirling's approximation (or Stirling's formula) is an asymptotic approximation for factorials. It is a good approximation, leading to accurate results even for small values of n. It is named after James Stirling, though a related ...
one finds that if we start at equilibrium (equal number of particles in the containers), the expected time to return to equilibrium is asymptotically equal to \textstyle\sqrt. If we assume that particles change containers at rate one in a second, in the particular case of N=100 particles, starting at equilibrium the return to equilibrium is expected to occur in 13 seconds, while starting at configuration 100 in one of the containers, 0 at the other, the return to that state is expected to take 4\cdot 10^ years. This supposes that while theoretically sure, recurrence to the initial highly disproportionate state is unlikely to be observed.


Bibliography

* Paul and Tatjana Ehrenfest: Über zwei bekannte Einwände gegen das Boltzmannsche H-Theorem. ''
Physikalische Zeitschrift ''Physikalische Zeitschrift'' (English: ''Physical Journal'') was a German scientific journal of physics published from 1899 to 1945 by S. Hirzel Verlag. In 1924, it merged with ''Jahrbuch der Radioaktivität und Elektronik''. From 1944 onwards, t ...
, vol. 8 (1907)'', pp. 311–314. * F.P. Kelly: ''The Ehrenfest model'', in ''Reversibility and Stochastic Networks''. Wiley, Chichester, 1979. pp. 17–20. * David O. Siegmund: ''Ehrenfest model of diffusion (mathematics)''.
Encyclopædia Britannica The is a general knowledge, general-knowledge English-language encyclopaedia. It has been published by Encyclopædia Britannica, Inc. since 1768, although the company has changed ownership seven times. The 2010 version of the 15th edition, ...
.


See also

*
Kac ring In statistical mechanics, the Kac ring is a toy model introduced by Mark Kac in 1956 to explain how the second law of thermodynamics emerges from T-symmetry, time-symmetric interactions between molecules (see reversibility paradox). Although artif ...
*
Ornstein–Uhlenbeck process In mathematics, the Ornstein–Uhlenbeck process is a stochastic process with applications in financial mathematics and the physical sciences. Its original application in physics was as a model for the velocity of a massive Brownian particle ...


References

{{Reflist Queueing theory Diffusion Stochastic models