The fourth law of thermodynamics: steepest entropy ascent
arXiv:1908.05768 · doi:10.1098/rsta.2019.0168
Abstract
When thermodynamics is understood as the science (or art) of constructing effective models of natural phenomena by choosing a minimal level of description capable of capturing the essential features of the physical reality of interest, the scientific community has identified a set of general rules that the model must incorporate if it aspires to be consistent with the body of known experimental evidence. Some of these rules are believed to be so general that we think of them as laws of Nature, such as the great conservation principles, whose "greatness" derives from their generality, as masterfully explained by Feynman in one of his legendary lectures. The second law of thermodynamics is universally contemplated among the great laws of Nature. In this paper we show that, in the past four decades, an enormous body of scientific research devoted to modeling the essential features of nonequilibrium natural phenomena has converged from many different directions and frameworks towards the general recognition (albeit still expressed in different but equivalent forms and language) that another rule is also indispensable and reveals another great law of Nature that we propose to call the \caporali{fourth law of thermodynamics}. We state it as follows: every nonequilibrium state of a system or local subsystem for which entropy is well-defined must be equipped with a metric in state space with respect to which the irreversible component of its time evolution is in the direction of steepest entropy ascent compatible with the conservation constraints. To illustrate the power of the fourth law, we derive (nonlinear) extensions of Onsager reciprocity and fluctuation-dissipation relations to the far-nonequilibrium realm within the framework of the rate-controlled constrained-equilibrium (RCCE) approximation (also known as the quasi-equilibrium approximation).
arXiv comment15 pages, 5 figures, to appear in a special issue of PTRSA. Presented at the JETC2019 in Barcelona on May 22, 2019
References in corpus (36)
- The second laws of quantum thermodynamics
- The Resource Theory of Quantum States Out of Thermal Equilibrium
- The Physics and Mathematics of the Second Law of Thermodynamics
- Entropy production as correlation between system and reservoir
- Work extraction and thermodynamics for individual quantum systems
- Quantum Refrigerator and the III-law of Thermodynamics
- Entropy of isolated quantum systems after a quench
- Microcanonical and resource-theoretic derivations of the thermal state of a quantum system with noncommuting charges
- On the nature of heat in strongly coupled open quantum systems
- On the relation between gradient flows and the large-deviation principle, with applications to Markov chains and diffusion
- Quantum thermodynamics of general quantum processes
- Exact master equation for a spin interacting with a spin bath: Non-Markovianity and negative entropy production rate
- A nonlinear model dynamics for closed-system, constrained, maximal-entropy-generation relaxation by energy redistribution
- Beyond heat baths: Generalized resource theories for small-scale thermodynamics
- Local effective dynamics of quantum systems: A generalized approach to work and heat
- Entropy and Temperature of a Quantum Carnot Engine
- Steepest Entropy Ascent Model for Far-Non-Equilibrium Thermodynamics. Unified Implementation of the Maximum Entropy Production Principle
- Nonlinear Quantum Evolution Equations to Model Irreversible Adiabatic Relaxation with Maximal Entropy Production and Other Nonunitary Processes
- A Resource Theory for Work and Heat
- Weakly nonlocal irreversible thermodynamics - the Guyer-Krumhansl and the Cahn-Hilliard equations
- Axiomatic relation between thermodynamic and information-theoretic entropies
- GENERIC formalism of a Vlasov-Fokker-Planck equation and connection to large-deviation principles
- Thermal equilibrium of a macroscopic quantum system in a pure state
- The entropy concept for non-equilibrium states
- Nonlinear quantum evolution with maximal entropy production
- Essential equivalence of the GENERIC and Steepest Entropy Ascent models of dissipation for non-equilibrium thermodynamics
- Addendum to "Nonlinear quantum evolution with maximal entropy production"
- Recent Progress in the Definition of Thermodynamic Entropy
- Minimal Curvature Trajectories: Riemannian Geometry Concepts for Model Reduction in Chemical Kinetics
- Nonlinear extensions of Schrödinger-von Neumann quantum dynamics: a list of conditions for compatibility with thermodynamics
- Change, time and information geometry
- Entropy production and the geometry of dissipative evolution equations
- Computing diffusivities from particle models out of equilibrium
- Entropy Meters and the Entropy of Non-extensive Systems
- Model Dynamics for Quantum Computing
- Time-Energy and Time-Entropy Uncertainty Relations in Nonequilibrium Quantum Thermodynamics under Steepest-Entropy-Ascent Nonlinear Master Equations
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