LEADER 00000cam a2200769Ia 4500 001 ocn812174468 003 OCoLC 005 20190405014038.1 006 m o d 007 cr cnu---unuuu 008 121008s2012 enka ob 001 0 eng d 010 2012012613 019 813396635|a817820354|a819631750|a848651384|a1030319719 |a1030742849|a1061046569|a1081292863 020 9781139095167|q(electronic book) 020 1139095161|q(electronic book) 020 9781139569118|q(electronic book) 020 1139569112|q(electronic book) 020 9781139572675|q(electronic book) 020 1139572679|q(electronic book) 020 |z9781107019683 020 |z1107019680 020 |z9781107019638 020 |z110701963X 020 |z6613951137 020 |z9786613951137 020 |z1283638673 020 |z9781283638678 035 (OCoLC)812174468|z(OCoLC)813396635|z(OCoLC)817820354 |z(OCoLC)819631750|z(OCoLC)848651384|z(OCoLC)1030319719 |z(OCoLC)1030742849|z(OCoLC)1061046569|z(OCoLC)1081292863 040 N$T|beng|epn|cN$T|dYDXCP|dIDEBK|dUIU|dCAMBR|dE7B|dUMC|dMYG |dNLGGC|dOCLCF|dOCLCQ|dOTZ|dOCLCQ|dBUF|dUAB|dYDX|dOCLCQ |dOCLCO|dCEF|dCOCUF|dSTF|dLOA|dVT2|dOCLCQ|dOCLCO|dTKN 049 RIDW 050 4 QC318.M35|bH46 2012eb 072 7 SCI|x065000|2bisacsh 072 7 PDA|2bicssc 082 04 536/.71|223 090 QC318.M35|bH46 2012eb 100 1 Hemmo, Meir.|0https://id.loc.gov/authorities/names/ n2012029897 245 14 The Road to Maxwell's demon /|cMeir Hemmo, Orly Shenker. 264 1 Cambridge, U.K. ;|aNew York :|bCambridge University Press, |c2012. 300 1 online resource (xii, 327 pages) :|billustrations 336 text|btxt|2rdacontent 337 computer|bc|2rdamedia 338 online resource|bcr|2rdacarrier 340 |gpolychrome|2rdacc 347 text file|2rdaft 504 Includes bibliographical references and index. 505 0 1. Introduction -- 2. Thermodynamics -- 2.1. The experience of asymmetry in time -- 2.2. The Law of Conservation of Energy -- 2.3. The Law of Approach to Equilibrium -- 2.4. The Second Law of Thermodynamics -- 2.5. The status of the laws of thermodynamics -- 3. Classical mechanics -- 3.1. The fundamental theory of the world -- 3.2. Introducing classical mechanics -- 3.3. Mechanical states -- 3.4. Time evolution of mechanical states -- 3.5. Thermodynamic magnitudes -- 3.6. A mechanical no-go theorem -- 3.7. The ergodic approach -- 3.8. Conclusion -- 4. Time -- 4.1. Introduction: why mechanics cannot underwrite thermodynamics -- 4.2. Classical kinematics -- 4.3. The direction of time and the direction of velocity in time -- 4.4. The description of mechanical states -- 4.5. Velocity reversal -- 4.6. Retrodiction -- 4.7. Time reversal and time-reversal invariance -- 4.8. Why the time-reversal invariance of classical mechanics matters -- 5. Macrostates -- 5.1. The physical nature of macrostates -- 5.2. How do macrostates come about? -- 5.3. Explaining thermodynamics with macrostates -- 5.4. The dynamics of macrostates -- 5.5. The physical origin of thermodynamic macrostates -- 5.6. Boltzmann's macrostates -- 5.7. Maxwell-Boltzmann distribution -- 5.8. The observer in statistical mechanics -- 5.9. Counterfactual observers -- 6. Probability -- 6.1. Introduction -- 6.2. Probability in statistical mechanics -- 6.3. Choice of measure in statistical mechanics -- 6.4. Measure of a macrostate and its probability -- 6.5. Transition probabilities without blobs -- 6.6. Dependence on observed history? -- 6.7. The spin echo experiments -- 6.8. Robustness of transition probabilities -- 6.9. No probability over initial conditions -- 7. Entropy -- 7.1. Introduction -- 7.2. Entropy -- 7.3. The distinction between entropy and probability -- 7.4. Equilibrium in statistical mechanics -- 7.5. Law of Approach to Equilibrium -- 7.6. Second Law of Thermodynamics -- 7.7. Boltzmann's H-theorem -- 7.8. Loschmidt's reversibility objection -- 7.9. Poincare's recurrence theorem -- 7.10. Boltzmann's combinatorial argument -- 7.11. Back to Boltzmann's equation: Lanford's theorem -- 7.12. Conclusion -- 8. Typicality -- 8.1. Introduction -- 8.2. The explanatory arrow in statistical mechanics -- 8.3. Typicality -- 8.4. Are there natural measures? -- 8.5. Typical initial conditions -- 8.6. Measure-1 theorems and typicality -- 8.7. Conclusion -- 9. Measurement -- 9.1. Introduction -- 9.2. What is measurement in classical mechanics? -- 9.3. Collapse in classical measurement -- 9.4. State preparation -- 9.5. The shadows approach -- 9.6. Entropy -- 9.7. Status of the observer -- 10. The past -- 10.1. Introduction -- 10.2. The problem of retrodiction -- 10.3. The Past Hypothesis: memory and measurement -- 10.4. The Reliability Hypothesis -- 10.5. Past low entropy hypothesis -- 10.6. Remembering the future -- 10.7. Problem of initial improbable state -- 10.8. The dynamics of the Past Hypothesis -- 10.9. Local and global Past Hypotheses -- 10.10. Past Hypothesis and physics of memory -- 10.11. Memory in a time-reversed universe -- 11. Gibbs -- 11.1. Introduction -- 11.2. The Gibbsian method in equilibrium -- 11.3. Gibbsian method in terms of blobs and macrostates -- 11.4. Gibbsian equilibrium probability distributions -- 11.5. The approach to equilibrium -- 12. Erasure -- 12.1. Introduction -- 12.2. Why there is no microscopic erasure -- 12.3. What is a macroscopic erasure? -- 12.4. Necessary and sufficient conditions for erasure -- 12.5. Logic and entropy -- 12.6. Another logically irreversible operation -- 12.7. Logic and entropy: a model -- 12.8. What does erasure erase? -- 12.9. Conclusion -- 13. Maxwell's Demon -- 13.1. Thermodynamic and statistical mechanical demons - - 13.2. Szilard's insight -- 13.3. Entropy reduction: measurement -- 13.4. Efficiency and predictability -- 13.5. Completing the cycle of operation: erasure -- 13.6. The Liberal Stance -- 13.7. Conclusion -- Appendix A Szilard's engine -- Appendix B Quantum mechanics -- B.1. Albert's approach -- B.2. Bohmian mechanics -- B.3. A quantum mechanical Maxwellian Demon. 520 "Time asymmetric phenomena are successfully predicted by statistical mechanics. Yet the foundations of this theory are surprisingly shaky. Its explanation for the ease of mixing milk with coffee is incomplete, and even implies that un-mixing them should be just as easy. In this book the authors develop a new conceptual foundation for statistical mechanics that addresses this difficulty. Explaining the notions of macrostates, probability, measurement, memory, and the arrow of time in statistical mechanics, they reach the startling conclusion that Maxwell's Demon, the famous perpetuum mobile, is consistent with the fundamental physical laws. Mathematical treatments are avoided where possible, and instead the authors use novel diagrams to illustrate the text. This is a fascinating book for graduate students and researchers interested in the foundations and philosophy of physics."--|cProvided by publisher. 588 0 Print version record. 590 eBooks on EBSCOhost|bEBSCO eBook Subscription Academic Collection - North America 600 10 Maxwell, James Clerk,|d1831-1879.|0https://id.loc.gov/ authorities/names/n79089636 600 17 Maxwell, James Clerk,|d1831-1879.|2fast|0https:// id.worldcat.org/fast/40685 650 0 Maxwell's demon.|0https://id.loc.gov/authorities/subjects/ sh90003971 650 0 Second law of thermodynamics.|0https://id.loc.gov/ authorities/subjects/sh2003010100 650 0 Statistical thermodynamics.|0https://id.loc.gov/ authorities/subjects/sh85127576 650 7 Maxwell's demon.|2fast|0https://id.worldcat.org/fast/ 1012679 650 7 Second law of thermodynamics.|2fast|0https:// id.worldcat.org/fast/1110592 650 7 Statistical thermodynamics.|2fast|0https://id.worldcat.org /fast/1132092 655 4 Electronic books. 700 1 Shenker, Orly.|0https://id.loc.gov/authorities/names/ n87874878 776 08 |iPrint version:|aHemmo, Meir.|tRoad to Maxwell's demon. |dCambridge ; New York : Cambridge University Press, 2012 |z9781107019683|w(DLC) 2012012613|w(OCoLC)793169734 856 40 |uhttps://rider.idm.oclc.org/login?url=http:// search.ebscohost.com/login.aspx?direct=true&scope=site& db=nlebk&AN=480294|zOnline eBook via EBSCO. Access restricted to current Rider University students, faculty, and staff. 856 42 |3Instructions for reading/downloading the EBSCO version of this eBook|uhttp://guides.rider.edu/ebooks/ebsco 901 MARCIVE 20231220 948 |d20190507|cEBSCO|tEBSCOebooksacademic NEW 4-5-19 7552 |lridw 994 92|bRID