2007 APS March Meeting
Volume 52, Number 1
Monday–Friday, March 5–9, 2007;
Denver, Colorado
Session Y7: Nonequilibrium Thermodynamics
11:15 AM–2:15 PM,
Friday, March 9, 2007
Colorado Convention Center
Room: Korbel 4A-4B
Sponsoring
Unit:
DBP
Chair: Felix Ritort, Universitat de Barcelona
Abstract ID: BAPS.2007.MAR.Y7.4
Abstract: Y7.00004 : Stochastic Thermodynamics: Theory and Experiments
1:03 PM–1:39 PM
Preview Abstract
Abstract
Author:
Udo Seifert
(Universitaet Stuttgart)
Stochastic thermodynamics provides a framework for describing
small systems
embedded in a heat bath and externally driven to non-equilibrium.
Examples
are colloidal particles in time-dependent optical traps, single
biomolecules
manipulated by optical tweezers or AFM tips, and motor proteins
driven by
ATP excess. A first-law like energy balance allows to identify
applied
work and dissipated heat on the level of a single stochastic
trajectory.
Total entropy production includes not only this heat but also
changes in
entropy associated with the state of the small system. Within such a
framework, exact results like an integral fluctuation theorem for
total
entropy production valid for any initial state, any
time-dependent driving
and any length of trajectories can be proven [1]. These results
hold both for
mechanically driven systems modelled by over-damped Langevin
equations and
chemically driven (biochemical) reaction networks [2]. These
theoretical
predictions have been illustrated and tested with experiments on
a colloidal
particle pushed by a periodically modulated laser towards a
surface [3].
Key elements of this framework like a stochastic entropy can also
be applied
to athermal systems as experiments on an optically driven defect
center in
diamond show [4,5]. For mechanically driven non-equilibrium
steady states,
the violation of the fluctuation-dissipation theorem can be
quantified as an
additive term directly related to broken detailed balance (rather
than a
multiplicative effective temperature) [6]. Integrated over time, a
generalized Einstein relation appears. If velocities are measured
with
respect to the local mean velocity, the usual form of the FDT
holds even in
non-equilibrium.
[1] U. Seifert, Phys. Rev. Lett. 95: 040602/1-4, 2005.
[2] T. Schmiedl and U. Seifert, cond-mat/0605080.
[3] V. Blickle, T. Speck, L. Helden, U. Seifert, and C. Bechinger,
Phys. Rev. Lett. 96: 070603/1-4, 2006.
[4] S. Schuler, T. Speck, C. Tietz, J. Wrachtrup, and U. Seifert,
Phys. Rev. Lett. 94: 180602/1-4, 2005.
[5] C. Tietz, S. Schuler, T. Speck, U. Seifert, and J. Wrachtrup,
Phys. Rev. Lett. 97: 050602/1-4, 2006.
[6] T. Speck and U. Seifert, Europhys. Lett. 74: 391-396, 2006.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2007.MAR.Y7.4