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This Special Issue concerns the development of a theory for energy conversion on the nanoscale, namely, nanothermodynamics. The theory has been applied to porous media, small surfaces, clusters or fluids under confinement. The number of unsolved issues in these contexts is numerous and the present efforts are only painting part of the broader picture. We attempt to answer the following: How far down in scale does the Gibbs equation apply? Which theory can replace it beyond the thermodynamic limit? It is well known that confinement changes the equation of state of a fluid, but how does confinement change the equilibrium conditions themselves? This Special Issue explores some of the roads that were opened up for us by Hill with the idea of nanothermodynamics. The experimental progress in nanotechnology is advancing rapidly. It is our ambition with this book to inspire an increased effort in the development of suitable theoretical tools and methods to help further progress in nanoscience. All ten contributions to this Special Issue can be seen as efforts to support, enhance and validate the theoretical foundation of Hill.
Technology: general issues --- nanothermodynamics --- porous systems --- molecular simulation --- differential pressure --- integral pressure --- pressure --- confinement --- equilibrium --- thermodynamic --- small-system --- hills-thermodynamics --- pore --- nanopore --- interface --- Kirkwood-Buff integrals --- surface effects --- molecular dynamics --- activated carbon --- high-pressure methane adsorption --- thermodynamics of adsorption systems --- small system method --- thermodynamics of small systems --- hydration shell thermodynamics --- finite size correction --- adsorption --- thin film --- size-dependent --- thermodynamics --- spreading pressure --- entropy of adsorption --- polymers --- single-molecule stretching --- thermodynamics at strong coupling --- temperature-dependent energy levels --- Hill’s thermodynamics of small systems --- porous media --- statistical mechanics --- ideal gas --- nanoparticles --- n/a --- Hill's thermodynamics of small systems
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This Special Issue concerns the development of a theory for energy conversion on the nanoscale, namely, nanothermodynamics. The theory has been applied to porous media, small surfaces, clusters or fluids under confinement. The number of unsolved issues in these contexts is numerous and the present efforts are only painting part of the broader picture. We attempt to answer the following: How far down in scale does the Gibbs equation apply? Which theory can replace it beyond the thermodynamic limit? It is well known that confinement changes the equation of state of a fluid, but how does confinement change the equilibrium conditions themselves? This Special Issue explores some of the roads that were opened up for us by Hill with the idea of nanothermodynamics. The experimental progress in nanotechnology is advancing rapidly. It is our ambition with this book to inspire an increased effort in the development of suitable theoretical tools and methods to help further progress in nanoscience. All ten contributions to this Special Issue can be seen as efforts to support, enhance and validate the theoretical foundation of Hill.
nanothermodynamics --- porous systems --- molecular simulation --- differential pressure --- integral pressure --- pressure --- confinement --- equilibrium --- thermodynamic --- small-system --- hills-thermodynamics --- pore --- nanopore --- interface --- Kirkwood-Buff integrals --- surface effects --- molecular dynamics --- activated carbon --- high-pressure methane adsorption --- thermodynamics of adsorption systems --- small system method --- thermodynamics of small systems --- hydration shell thermodynamics --- finite size correction --- adsorption --- thin film --- size-dependent --- thermodynamics --- spreading pressure --- entropy of adsorption --- polymers --- single-molecule stretching --- thermodynamics at strong coupling --- temperature-dependent energy levels --- Hill’s thermodynamics of small systems --- porous media --- statistical mechanics --- ideal gas --- nanoparticles --- n/a --- Hill's thermodynamics of small systems
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This Special Issue concerns the development of a theory for energy conversion on the nanoscale, namely, nanothermodynamics. The theory has been applied to porous media, small surfaces, clusters or fluids under confinement. The number of unsolved issues in these contexts is numerous and the present efforts are only painting part of the broader picture. We attempt to answer the following: How far down in scale does the Gibbs equation apply? Which theory can replace it beyond the thermodynamic limit? It is well known that confinement changes the equation of state of a fluid, but how does confinement change the equilibrium conditions themselves? This Special Issue explores some of the roads that were opened up for us by Hill with the idea of nanothermodynamics. The experimental progress in nanotechnology is advancing rapidly. It is our ambition with this book to inspire an increased effort in the development of suitable theoretical tools and methods to help further progress in nanoscience. All ten contributions to this Special Issue can be seen as efforts to support, enhance and validate the theoretical foundation of Hill.
Technology: general issues --- nanothermodynamics --- porous systems --- molecular simulation --- differential pressure --- integral pressure --- pressure --- confinement --- equilibrium --- thermodynamic --- small-system --- hills-thermodynamics --- pore --- nanopore --- interface --- Kirkwood-Buff integrals --- surface effects --- molecular dynamics --- activated carbon --- high-pressure methane adsorption --- thermodynamics of adsorption systems --- small system method --- thermodynamics of small systems --- hydration shell thermodynamics --- finite size correction --- adsorption --- thin film --- size-dependent --- thermodynamics --- spreading pressure --- entropy of adsorption --- polymers --- single-molecule stretching --- thermodynamics at strong coupling --- temperature-dependent energy levels --- Hill's thermodynamics of small systems --- porous media --- statistical mechanics --- ideal gas --- nanoparticles --- nanothermodynamics --- porous systems --- molecular simulation --- differential pressure --- integral pressure --- pressure --- confinement --- equilibrium --- thermodynamic --- small-system --- hills-thermodynamics --- pore --- nanopore --- interface --- Kirkwood-Buff integrals --- surface effects --- molecular dynamics --- activated carbon --- high-pressure methane adsorption --- thermodynamics of adsorption systems --- small system method --- thermodynamics of small systems --- hydration shell thermodynamics --- finite size correction --- adsorption --- thin film --- size-dependent --- thermodynamics --- spreading pressure --- entropy of adsorption --- polymers --- single-molecule stretching --- thermodynamics at strong coupling --- temperature-dependent energy levels --- Hill's thermodynamics of small systems --- porous media --- statistical mechanics --- ideal gas --- nanoparticles
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The purpose of this book is to encourage the use of non-equilibrium thermodynamics to describe transport in complex, heterogeneous media. With large coupling effects between the transport of heat, mass, charge and chemical reactions at surfaces, it is important to know how one should properly integrate across systems where different phases are in contact. No other book gives a prescription of how to set up flux equations for transports across heterogeneous systems. The authors apply the thermodynamic description in terms of excess densities, developed by Gibbs for equilibrium, to non-equilib
Nonequilibrium thermodynamics. --- Thermodynamics. --- Chemistry, Physical and theoretical --- Dynamics --- Mechanics --- Physics --- Heat --- Heat-engines --- Quantum theory --- Irreversible thermodynamics --- Non-equilibrium thermodynamics --- Thermodynamics of the steady state --- Irreversible processes --- Thermodynamics --- Thermodynamique irréversible
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This volume contains the collected works of the eminent chemist and physicist Lars Onsager, one of the most influential scientists of the 20th Century.The volume includes Onsager's previously unpublished PhD thesis, a biography by H C Longuet-Higgins and M E Fisher, an autobiographical commentary, selected photographs, and a list of Onsager discussion remarks in print.Onsager's scientific achievements were characterized by deep insights into the natural sciences. His two best-known accomplishments are his reciprocal relations for irreversible processes, for which he received the 1968 Nobel Pri
Chemistry, Physical and theoretical. --- Physics. --- Natural philosophy --- Philosophy, Natural --- Physical sciences --- Dynamics --- Chemistry, Theoretical --- Physical chemistry --- Theoretical chemistry --- Chemistry
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The physics of porous media is, when taking a broad view, the physics of multinary mixtures of immiscible solid and fluid constituents. Its relevance to society echoes in numerous engineering disciplines such as chemical engineering, soil mechanics, petroleum engineering, groundwater engineering, geothermics, fuel cell technology… It is also at the core of many scientific disciplines ranging from hydrogeology to pulmonology. Perhaps one may affix a starting point for the study of porous media as the year 1794 when Reinhard Woltman introduced the concept of volume fractions when trying to understand mud. In 1856, Henry Darcy published his findings on the flow of water through sand packed columns and the first constitutive relation was born. Wyckoff and Botset proposed in 1936 a generalization of the Darcy approach to deal with several immiscible fluids flowing simultaneously in a rigid matrix. This effective medium theory assigns to each fluid a relative permeability, i.e. a constitutive law for each fluid species. It remains to this day the standard framework for handling the motion of two or more immiscible fluids in a rigid porous matrix even though there have been many attempts at moving beyond it. When the solid constituent is not rigid, forces in the fluids and the solid phase influence each other. von Terzaghi realized the importance of capillary forces in such systems in the thirties. An effective medium theory of poroelasticity was subsequently developend by Biot in the mid fifties. Biot theory remains to date state of the art for handling matrix-fluid interactions when the deformations of the solid phase remain small. For large deformations, e.g. when the solid phase is unconsolidated, no effective medium theory exists.
Science: general issues --- Physics --- flow in porous media --- two-phase flow in porous media --- non-Newtonian fluids --- reactive fluids --- electrohydrodynamics (EHD) --- capillary fiber bundle model --- soil mechanics --- thermodynamics of small systems
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The physics of porous media is, when taking a broad view, the physics of multinary mixtures of immiscible solid and fluid constituents. Its relevance to society echoes in numerous engineering disciplines such as chemical engineering, soil mechanics, petroleum engineering, groundwater engineering, geothermics, fuel cell technology… It is also at the core of many scientific disciplines ranging from hydrogeology to pulmonology. Perhaps one may affix a starting point for the study of porous media as the year 1794 when Reinhard Woltman introduced the concept of volume fractions when trying to understand mud. In 1856, Henry Darcy published his findings on the flow of water through sand packed columns and the first constitutive relation was born. Wyckoff and Botset proposed in 1936 a generalization of the Darcy approach to deal with several immiscible fluids flowing simultaneously in a rigid matrix. This effective medium theory assigns to each fluid a relative permeability, i.e. a constitutive law for each fluid species. It remains to this day the standard framework for handling the motion of two or more immiscible fluids in a rigid porous matrix even though there have been many attempts at moving beyond it. When the solid constituent is not rigid, forces in the fluids and the solid phase influence each other. von Terzaghi realized the importance of capillary forces in such systems in the thirties. An effective medium theory of poroelasticity was subsequently developend by Biot in the mid fifties. Biot theory remains to date state of the art for handling matrix-fluid interactions when the deformations of the solid phase remain small. For large deformations, e.g. when the solid phase is unconsolidated, no effective medium theory exists.
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The physics of porous media is, when taking a broad view, the physics of multinary mixtures of immiscible solid and fluid constituents. Its relevance to society echoes in numerous engineering disciplines such as chemical engineering, soil mechanics, petroleum engineering, groundwater engineering, geothermics, fuel cell technology… It is also at the core of many scientific disciplines ranging from hydrogeology to pulmonology. Perhaps one may affix a starting point for the study of porous media as the year 1794 when Reinhard Woltman introduced the concept of volume fractions when trying to understand mud. In 1856, Henry Darcy published his findings on the flow of water through sand packed columns and the first constitutive relation was born. Wyckoff and Botset proposed in 1936 a generalization of the Darcy approach to deal with several immiscible fluids flowing simultaneously in a rigid matrix. This effective medium theory assigns to each fluid a relative permeability, i.e. a constitutive law for each fluid species. It remains to this day the standard framework for handling the motion of two or more immiscible fluids in a rigid porous matrix even though there have been many attempts at moving beyond it. When the solid constituent is not rigid, forces in the fluids and the solid phase influence each other. von Terzaghi realized the importance of capillary forces in such systems in the thirties. An effective medium theory of poroelasticity was subsequently developend by Biot in the mid fifties. Biot theory remains to date state of the art for handling matrix-fluid interactions when the deformations of the solid phase remain small. For large deformations, e.g. when the solid phase is unconsolidated, no effective medium theory exists.
Science: general issues --- Physics --- flow in porous media --- two-phase flow in porous media --- non-Newtonian fluids --- reactive fluids --- electrohydrodynamics (EHD) --- capillary fiber bundle model --- soil mechanics --- thermodynamics of small systems --- flow in porous media --- two-phase flow in porous media --- non-Newtonian fluids --- reactive fluids --- electrohydrodynamics (EHD) --- capillary fiber bundle model --- soil mechanics --- thermodynamics of small systems
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