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      New definitions of thermodynamic temperature and entropy not based on the concepts of heat and thermal reservoir

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          Abstract

          From a new rigorous formulation of the general axiomatic foundations of thermodynamics we derive an operational definition of entropy that responds to the emergent need in many technological frameworks to understand and deploy thermodynamic entropy well beyond the traditional realm of equilibrium states of macroscopic systems. The new treatment starts from a previously developed set of carefully worded operational definitions for all the necessary basic concepts, and is not based on the traditional ones of "heat" and of "thermal reservoir." It is achieved in three steps. First, a new definition of thermodynamic temperature is stated, for any stable equilibrium state. Then, by employing this definition, a measurement procedure is developed which defines uniquely the property entropy in a broad domain of states, which could include \textit{in principle}, even some non-equilibrium states of few-particle systems, provided they are separable and uncorrelated. Finally, the domain of validity of the definition is extended, possibly to every state of every system, by a different procedure, based on the preceding one, which associates a range of entropy values to any state not included in the previous domain. The principle of entropy non-decrease and the additivity of entropy are proved in both the domains considered.

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          Most cited references18

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          The second laws of quantum thermodynamics

          The second law of thermodynamics places constraints on state transformations. It applies to systems composed of many particles, however, we are seeing that one can formulate laws of thermodynamics when only a small number of particles are interacting with a heat bath. Is there a second law of thermodynamics in this regime? Here, we find that for processes which are approximately cyclic, the second law for microscopic systems takes on a different form compared to the macroscopic scale, imposing not just one constraint on state transformations, but an entire family of constraints. We find a family of free energies which generalize the traditional one, and show that they can never increase. The ordinary second law relates to one of these, with the remainder imposing additional constraints on thermodynamic transitions. We find three regimes which determine which family of second laws govern state transitions, depending on how cyclic the process is. In one regime one can cause an apparent violation of the usual second law, through a process of embezzling work from a large system which remains arbitrarily close to its original state. These second laws are relevant for small systems, and also apply to individual macroscopic systems interacting via long-range interactions. By making precise the definition of thermal operations, the laws of thermodynamics are unified in this framework, with the first law defining the class of operations, the zeroth law emerging as an equivalence relation between thermal states, and the remaining laws being monotonicity of our generalized free energies.
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            Nonlinear quantum evolution equations to model irreversible adiabatic relaxation with maximal entropy production and other nonunitary processes

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              A unified quantum theory of mechanics and thermodynamics. Part IIa. Available energy

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                Author and article information

                Journal
                18 November 2019
                Article
                10.1478/AAPP.97S1A1
                1911.08576
                3c956b37-eb70-4277-bf77-efa720257e2e

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
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                AAPP, Vol. 97(S1), A1, 1-28 (2019)
                23 pages. Presented at Thermocon'16, International Conference and Summer School on Thermal Theories of Continua: Survey and Developments, Messina, Italy, April 19-22, 2016. Published in AAPP: Atti della Accademia Peloritana dei Pericolanti. http://dx.doi.org/10.1478/AAPP.97S1A1. arXiv admin note: substantial text overlap with arXiv:1411.5395
                quant-ph

                Quantum physics & Field theory
                Quantum physics & Field theory

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