The Lucky Engine: Probabilistic Emergence and Persistence of Near-Maximum Dissipation States

A paradigm, wherein a nonequilibrium system has multiple modes of transport that can act in combination, permits the resolution of several difficulties with the notion of maximum entropy production (MaxEP or MEP). First, physical constraints, such as the density of the atmosphere or the planetary rotation rate, merely define the portfolio of modes that can be engaged by the system: physically impossible states cannot be selected. Second, with minimal sensitivity to how the system evolves, it is seen that there are simply more numerous quasi-steady microstates (combinations of modes) that are near the maximum of work output (or dissipation rate or EP) than there are far from it, and so it is more probable that the system will be observed to be near that maximum. Third, this paradigm naturally permits exploration of the system behavior when subjected to non-steady forcing. Finally, it provides a framework to explain when a system has 'enough' degrees of freedom to attain a maximum dissipation state, as opposed to the minimum dissipation state expected for certain constrained systems.

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Publication Details

Journal
Entropy
Published
2025-06-27
DOI
https://doi.org/10.3390/e27070687
Primary Topic
Advanced Thermodynamics and Statistical Mechanics
Type
article
Field-Weighted Citation Impact
0.00
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article

The Lucky Engine: Probabilistic Emergence and Persistence of Near-Maximum Dissipation States

R. D. Lorenz
Entropy
Advanced Thermodynamics and Statistical Mechanics
article

The Lucky Engine: Probabilistic Emergence and Persistence of Near-Maximum Dissipation States

R. D. Lorenz
article en

Abstract

A paradigm, wherein a nonequilibrium system has multiple modes of transport that can act in combination, permits the resolution of several difficulties with the notion of maximum entropy production (MaxEP or MEP). First, physical constraints, such as the density of the atmosphere or the planetary rotation rate, merely define the portfolio of modes that can be engaged by the system: physically impossible states cannot be selected. Second, with minimal sensitivity to how the system evolves, it is seen that there are simply more numerous quasi-steady microstates (combinations of modes) that are near the maximum of work output (or dissipation rate or EP) than there are far from it, and so it is more probable that the system will be observed to be near that maximum. Third, this paradigm naturally permits exploration of the system behavior when subjected to non-steady forcing. Finally, it provides a framework to explain when a system has 'enough' degrees of freedom to attain a maximum dissipation state, as opposed to the minimum dissipation state expected for certain constrained systems.

EntropyVol. 27(7)
Johns Hopkins University Applied Physics Laboratory (US)
Openalex Percentile: Top 88%
Advanced Thermodynamics and Statistical Mechanics
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