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Non-equilibrium Thermodynamics and Statistical Mechanics: Foundations and Applications PDF

479 Pages·2012·3.848 MB·English
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Non-Equilibrium Thermodynamics and Statistical Mechanics This page intentionally left blank Non-Equilibrium Thermodynamics and Statistical Mechanics Foundations and Applications Phil Attard 1 3 GreatClarendonStreet,Oxford,OX26DP, UnitedKingdom OxfordUniversityPressisadepartmentoftheUniversityofOxford. IffurtherstheUniversity’sobjectiveofexcellenceinresearch,scholarship, andeducationbypublishingworldwide.Oxfordisaregisteredtrademarkof OxfordUniversityPressintheUKandincertainothercountries (cid:2)c PhilAttard2012 Themoralrightsoftheauthorhavebeenasserted FirstEditionpublishedin2012 Impression:1 Allrightsreserved.Nopartofthispublicationmaybereproduced,storedin aretrievalsystem,ortransmitted,inanyformorbyanymeans,withoutthe priorpermissioninwritingofOxfordUniversityPress,orasexpresslypermitted bylaw,bylicenceorundertermsagreedwiththeappropriatereprographics rightsorganization.Enquiriesconcerningreproductionoutsidethescopeofthe aboveshouldbesenttotheRightsDepartment,OxfordUniversityPress,atthe addressabove Youmustnotcirculatethisworkinanyotherform andyoumustimposethissameconditiononanyacquirer BritishLibraryCataloguinginPublicationData Dataavailable LibraryofCongressCataloginginPublicationData Dataavailable ISBN 978–0–19–966276–0 PrintedandboundinGreatBritainby CPIGroup(UK)Ltd,Croydon,CR04YY LinkstothirdpartywebsitesareprovidedbyOxfordingoodfaithand forinformationonly.Oxforddisclaimsanyresponsibilityforthematerials containedinanythirdpartywebsitereferencedinthiswork. Preface Fate, Time, Occasion, Chance, and Change, To these all things are subject P. B. Shelley, ‘Prometheus Unbound’ (1820) All things change in time Motionandchangearethenatureoftheworld. Thescaleofmotionrangesfrom the orbit of galaxies and planets, to the winds, ocean currents, and river flows, and even to the sub-microscopic, with the ceaseless movement of atoms and molecules. Inthelivingworldthereisthelocomotionofanimals,themovement of limbs and muscles, and the flows of blood, sap, and other vital fluids. There is also human made motion in the form of transport by planes, trains, and automobiles,the mechanicalmovement ofmotorisedtools, and controlledflows such as those of electricity, heat, and fluids. There are as well other forms of change. Birth, growth, and death is a familiar trajectory for any individual living organism. But these also describe the evolution of a species as a whole, as well as that of the universe, planets, eco-systems, and even social structures. One can also include other physical phenomena that are the subject of more traditional scientific study such as the progress of chemical reactions, the development of heat and current fluxes, the formation of patterns by aerodynamic and hydrodynamic flows, the processes of self-assembly and physical organisation, and the dynamic deformation and response of materials. These of course occur in nature, industry, technology, and under controlled laboratory conditions. The roˆleofchanceinourworldshouldnotbeunderestimated. Whenthings occur, their exact trajectory, and their ultimate fate are not perfectly pre- dictable. In general the complexity of systems, unknown initial conditions, and the influence of uncontrolled external forces all contribute a degree of ran- domness that leads to an uncertain future unconstrained by a strict fatalism. Chancemeansthatchangesintimeoccurnotwithpuredeterminismbutrather with statistical probability. v vi Preface Time changes everything The point belabouredaboveis that time dependent phenomena areubiquitous. Thetechnicalwordfortheseis‘non-equilibrium’. Itisareflectionofthechrono- logical development of science that this, the most common class of systems, is described in the negative. Initially,thermodynamicsandstatisticalmechanicsweredevelopedforequi- librium systems, which do not change macroscopically with time. Thermody- namicsisthescienceofmacroscopicsystems,anditprovidesuniversallawsand relationships that all equilibrium systems must obey. Statistical mechanics en- ablestheprobabilisticdescriptionofequilibriumsystemsatthemolecularlevel. It gives the mathematical basis for the empirical laws of thermodynamics and it provides quantitative values for measured thermodynamic parameters. It is one of the great ironies of science that the word ‘dynamics’ in ‘ther- modynamics’, and the word ‘mechanics’ in ‘statistical mechanics’, both imply motion, when in fact both disciplines have been strictly formulated for static or equilibrium systems. Of course as an approximation they are often applied to time dependent systems, either instantaneously or else over time intervals small enough that any change is negligible, or they can be combined with an empirical theory such as hydrodynamics. But in terms of an exact treatment, thermodynamicsandstatisticalmechanicsarerestrictedtoequilibriumsystems. Thisraisesthequestion: Howdoestimechangethermodynamicsandstatistical mechanics? This book Thisbookseekstoanswerthatdisarminglysimple question. Acoherentformu- lationofnon-equilibriumthermodynamicsisgiven. Theapproachisbasedupon aparticularformofentropy,andithastheadvantagethatalmostallofthecon- cepts ofequilibriumthermodynamicscarryoverto the non-equilibriumfield. It also enables a consistent derivation of most of the known non-equilibrium the- orems and results, which exhibits their inter-relationships and places them in the context of a bigger picture. Thenon-equilibriumprobabilitydistributionisalsodeveloped,andthispro- vides a basis for the field of non-equilibrium statistical mechanics. Again, this enables a unified derivation of known and previously unknown theorems. Im- portantly, it also enables the development of computer simulation algorithms for non-equilibrium systems, which are used to test quantitatively the results and to illustrate them at the molecular level. Because of the significance of time dependent phenomena, there are many books and scientific papers concerned with the formulation of non-equilibrium thermodynamics and non-equilibrium statistical mechanics, and with their ap- plication to specific systems. The selection of topics, underlying approach,and method ofpresentationvary enormously,althoughcertainnon-equilibriumthe- orems and results for which there is broad consensus commonly recur. Others results lie at the cutting edge of current research,and for these detailed justifi- Preface vii cation and explanation are required. As mentioned above, this book proceeds from the very fundamental prin- ciples that determine the optimum non-equilibrium thermodynamic state, and also from the equations of motion and probability distributions appropriate for non-equilibriumstatisticalmechanics. The strategy employedhere is to set out thephysicalbasisoftheaxioms,thecloseanalogybetweennon-equilibriumand equilibriumprinciples,and,mostimportantly,thetheoremsanddetailedresults that follow as a consequence. In general an attempt is made to provide quanti- tative tests, experimental or computational, and detailed comparisons between different approaches, and alternative, independent derivations of the same re- sult. Itishopedthatsuchconcreteevidenceandtheconsistencyoftheapproach will give some confidence in the fundamental principles that the book is based upon. In the present book, most of the traditional topics in the non-equilibrium field are covered, and some new ones besides. What is perhaps unique here is that a single underlying approach suffices to derive and to describe all these results. Thefieldsofnon-equilibriumthermodynamicsandnon-equilibriumsta- tisticalmechanicsarehereregardedasacontinuumthatrangesfromthemacro- scopic to the sub-microscopic, with Brownian motion and stochastic processes lying in the boundary region where they merge. In a sense, this book is one long argument for non-equilibrium thermody- namicsandstatisticalmechanics. Thereareseveralreasonswhythereadermay find the present approach useful and may have confidence in the results. First, is the simplicity of the concepts, examples, and equations. Stripping away all that is unnecessary removes the possibility of confusion masquerading as com- plexity, and displays the results in a clear and unambiguous light. Second, is the physical basis of the approach. Thermodynamics and statistical mechanics are derived from, and designed for the real world, and here is emphasised the physical basis and interpretation of all the terms that occur in each equation. This removes the likelihood of inadvertent non-physical behaviour due to arti- ficial assumptions, it gives an intuitive feel to the equations and results, and it enablesthecommonsensetesttobereadilyapplied. Third,isthecoherenceand self-consistencyoftheapproach. Thosetheoremsandresultsinnon-equilibrium thermodynamics and statistical mechanics that are widely accepted are all de- rivedherefromasingleapproachbasedonentropy. This consiliencegivessome confidence in both the approach itself and the new results also generated by it. Fourth, the results of a number of computer simulations are given in the text, both to illustrate the procedures and to test quantitatively the results. In addition, certain experimental measurements are used, again quantitatively, to test predictions of the theory. Such tests should prove convincing, both of the individual results and of the formulation as a whole. The fields of thermodynamics and statistical mechanics have grown over the years. This book is part of that evolution; it is intended to be timely rather than timeless. The principles for non-equilibrium thermodynamics and statistical mechanics set out herein consolidate the present state of knowledge and provide a basis for future growth and new applications. This page intentionally left blank Contents 1 Prologue ..............................................................1 2 Fluctuation Theory ..................................................33 3 Brownian Motion ....................................................61 4 Heat Conduction ....................................................97 5 Second Entropy for Fluctuating Hydrodynamics ....................121 6 Heat Convection and Non-Equilibrium Phase Transitions ...........145 7 Equilibrium Statistical Mechanics ..................................173 8 Non-Equilibrium Statistical Mechanics ..............................233 9 Statistical Mechanics of Steady Flow: Heat and Shear ..............295 10 Generalised Langevin Equation .....................................329 11 Non-Equilibrium Computer Simulation Algorithms .................389 References ..........................................................451 Index ...............................................................455 ix

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