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![Page 1: Dynamical Fluctuations & Entropy Production Principles Karel Netočný Institute of Physics AS CR Seminar, 6 March 2007.](https://reader035.fdocuments.us/reader035/viewer/2022070412/5697bf741a28abf838c7fa0e/html5/thumbnails/1.jpg)
Dynamical Fluctuations & Entropy Production Principles
Karel Netočný Institute of Physics AS CR
Seminar, 6 March 2007
![Page 2: Dynamical Fluctuations & Entropy Production Principles Karel Netočný Institute of Physics AS CR Seminar, 6 March 2007.](https://reader035.fdocuments.us/reader035/viewer/2022070412/5697bf741a28abf838c7fa0e/html5/thumbnails/2.jpg)
To be discussed
Min- and Max-entropy production principles: various examples From variational principles to fluctuation laws: equilibrium case Static versus dynamical fluctuations Onsager-Machlup macroscopic fluctuation theory Stochastic models of nonequilibrium Conclusions, open problems, outlook,...
(In collaboration with C. Maes, K. U. Leuven)
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Motivation: Modeling Earth climate[Ozawa et al, Rev. Geoph. 41(4), 1018 (2003)]
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Linear electrical networks explaining MinEP/MaxEP principles
U22
Kirchhoff’s loop law:
Entropy production rate:
MinEP principle:
Stationary values of voltages minimize the entropy production rate
Not valid under inhomogeneous temperature!
X
k
Uj k =X
k
E j k
¾(U) = ¯Q(U) = ¯X
j ;k
U2j k
R j k
![Page 5: Dynamical Fluctuations & Entropy Production Principles Karel Netočný Institute of Physics AS CR Seminar, 6 March 2007.](https://reader035.fdocuments.us/reader035/viewer/2022070412/5697bf741a28abf838c7fa0e/html5/thumbnails/5.jpg)
Linear electrical networks explaining MinEP/MaxEP principles
U22
Kirchhoff’s current law:
Entropy production rate:
Work done by sources:
(Constrained) MaxEP principle:
Stationary values of currents maximize the entropy production under constraint
X
j
I j k =0
¾(I ) = ¯Q(I ) = ¯X
j ;k
R j k I 2j k
Q(I ) =W(I )
W(I ) =X
j k
E j kI j k
![Page 6: Dynamical Fluctuations & Entropy Production Principles Karel Netočný Institute of Physics AS CR Seminar, 6 March 2007.](https://reader035.fdocuments.us/reader035/viewer/2022070412/5697bf741a28abf838c7fa0e/html5/thumbnails/6.jpg)
Linear electrical networks summary of MinEP/MaxEP principles
Current law+
Loop law
MaxEP principle+
Current law
Loop law+
MinEP principleGeneralized
variational principle
I
U
U, I
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From principles to fluctuation laws Questions and ideas
How to go beyond approximate and ad hoc thermodynamical principles?
Inspiration from thermostatics:
Equilibrium variational principles are intimately related to structure of equilibrium fluctuations
Is there a nonequilibrium analogy of thermodynamical fluctuation theory?
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From principles to fluctuation laws Equilibrium fluctuations
H(x) = Ne
M (x) = Nmeq(e)
H (x) = Ne
Typical value
P (M (x) = Nm) = eN [s(e;m)¡ seq(e)]
Probability of fluctuation
H h(x) = H(x) ¡ hM (x) = N[e¡ hm]
The fluctuation made typical!s(e;m) = sheq(e¡ hm)
add
field
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From principles to fluctuation laws Equilibrium fluctuations
Fluctuationfunctional
Variational
functional
Thermodynamic
potentialEntropy (Generalized)
free energy
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From principles to fluctuation laws Static versus dynamical fluctuations
Empirical ergodic average:
Ergodic theorem:
Dynamical fluctuations:
Interpolating between static and dynamical fluctuations:
H(x) = Ne
P ( ¹mT =m) = e¡ T I (m)
P¡1N
P Nk=1
m(x¿k) =m¢= e¡ N I ( ¿ ) (m)
Static: ¿ ! 1I (1 )(m) =s(e) ¡ s(e;m)
Dynamic: ¿ ! 0
¹mT ! meq(e); T ! 1
¹mT = 1T
RT0m(xt) dt
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Effective model of macrofluctuationsOnsager-Machlup theory
Dynamics:
Equilibrium:
Path distribution:
R dmtdt = ¡ smt +
q2RN wt
P (m1 =m) / e¡ 12N sm2
S(m) ¡ S(0)
P (! ) = exp£¡ N
4
RT0
R2
¡dmtdt + s
Rmt¢2¤
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Effective model of macrofluctuationsOnsager-Machlup theory
Dynamics: Path distribution:
Dynamical fluctuations:
(Typical immediate) entropy production rate:
P (! ) = exp£¡ N
4
RT0
R2
¡dmtdt + s
Rmt¢2¤
¾(m) = dS(mt )dt = N s2
2R m2
I (m) = 14¾(m)
P ( ¹mT =m) = P (mt =m; 0 · t · T) = exp£¡ T
Ns2
8Rm2
¤
R dmtdt = ¡ smt +
q2RN »t
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Towards general theory
Equilibrium Nonequilibrium
ClosedHamiltonian dynamics
OpenStochastic dynamics
MesoscopicMacroscopic
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Linear electrical networks revisitedDynamical fluctuations
Fluctuating dynamics:
Johnson-Nyquist noise:
Empirical ergodic average:
Dynamical fluctuation law:
R1 R2
E
C
E f1 E f
2
E f =q
2R¯ »
white noise
U
total dissipated heat
E = U +R2I +E f2
I = C _U +U ¡ E f
1
R1
¹UT = 1T
RT0Ut dt
¡ 1TlogP ( ¹UT =U) = 1
4¯ 1¯ 2 (R 1+R 2 )¯ 1R 1+¯ 2R 2
hU 2
R 1+ (E ¡ U )2
R 2¡ E 2
R 1+R 2
i
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Stochastic models of nonequilibriumjump Markov processes
Local detailed balance:
Global detailed balance generally broken:
Markov dynamics:
log k(x;y)k(y;x) = ¢ s(x;y) = ¡ ¢ s(y;x)
entropy changein the
environment
breaking term¢ s(x;y) = s(y) ¡ s(x) + ²(x;y)
x y
k(x;y)
k(y;x)
d½t(x)dt =
X
y
£½t(y)k(y;x) ¡ ½t(x)k(x;y)
¤
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Stochastic models of nonequilibriumjump Markov processes
Entropy of the system:
Entropy fluxes:
Mean entropy production rate:
S(½) = ¡P
x ½(x) log½(x)
Warning:Only for time-reversal invariant observables!
x y
k(x;y)
k(y;x)
¾(½) =dS(½t)dt
+12
X
(x;y)
j½(x;y)¢ s(x;y)
=X
x;y
½(x)k(x;y)½(x)k(x;y)½(y)k(y;x)
j½(x;y) =½(x)k(x;y) ¡ ½(y)k(y;x)| {z }
zero at detailed balance
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Stochastic models of nonequilibriumjump Markov processes
(“Microscopic”) MinEP principle:
Can we again recognize entropy production as a fluctuation functional?
x y
k(x;y)
k(y;x)
In the first order in the expansionof the breaking term:
¾(½) =min , ½=½s
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Stochastic models of nonequilibriumjump Markov processes
Empirical occupation times:
Ergodic theorem:
Fluctuation law for occupation times?
Note:
¹pT (x) ! ½s(x); T ! 1
P (¹pT =½) = e¡ T I (½)
¹pT (x) = 1T
RT0Â(! t = x)dt
x y
k(x;y)
k(y;x)
I (½s) = 0 Natural variational functional
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Stochastic models of nonequilibriumjump Markov processes
Idea: Make the empirical distribution typical by modifying dynamics:
The “field” a(x) is such that p(x) is stationary distribution for the modified dynamics:
Comparing both processes yields the fluctuation law:
Py6=x
£p(x)ka(y;x) ¡ p(y)ka(x;y)
¤= 0
k(x;y) ¡ ! ka(x;y) = k(x;y) ea(y)¡ a(x)
I (p) =P
y6=x
£k(x;y) ¡ ka(x;y)
¤
difference of escape rates
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Stochastic models of nonequilibriumfluctuations versus MinEP principle
General observation:
In the first order approximation around detailed balance
The variational functional is recognized as an approximate fluctuation functional
A consequence: A natural way how to go beyond MinEP principle is to study various fluctuation laws
I (½) = 14
£¾(½) ¡ ¾(½s)
¤+o(²2)
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General conclusionsopen problems
Similarly, MaxEP principle is obtained from the fluctuation law of empirical current
Is there a natural computational scheme for the fluctuation functional far from equilibrium (e.g. for ratchets)?
Natural mathematical formalism: the large deviation and Donsker-Varadhan theory
Might the dynamical fluctuation theory provide a natural nonequilibrium thermodynamical formalism far from equilibrium?
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Outlook from fluctuations to nonequilibrium thermodynamics?
Fluctuationfunctional
Variational
functional
Nonequilibriumpotential
“Corrected”entropy production
??
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References C. Maes, K. N. (2006). math-ph/0612063. S. Bruers, C. Maes, K. N. (2007). cond-mat/0701035. C. Maes, K. N. (2006). cond-mat/0612525.
M. D. Donsker and S. R. Varadhan. Comm. Pure Appl. Math., 28:1–47 (1975).
M. J. Klein and P. H. E. Meijer. Phys. Rev., 96:250-255 (1954). I. Prigogine. Introduction to Non-Equilibrium Thermodynamics. Wiley-
Interscience, New York (1962). G. Eyink, J. L. Lebowitz, and H. Spohn. In: Chaos, Soviet-American Perspectives in Nonlinear Science, Ed. D. Campbell, p. 367–391 (1990). E. T. Jaynes. Ann. Rev. Phys. Chem., 31:579–601 (1980). R. Landauer. Phys. Rev. A, 12:636–638 (1975)