PART I GENERAL PRINCIPLES OF CLASSICAL THERMODYNAMICS |
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1 | (472) |
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Introduction The Nature of Themodynamics and the Basis of Thermostatistics |
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2 | (3) |
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The Problem and the Postulates |
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5 | (30) |
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The Temporal Nature of Macroscopic Measurements |
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5 | (1) |
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The Spatial Nature of Macrosscopic Measurements |
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6 | (3) |
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The Composition of Thermodynamic Systems |
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9 | (2) |
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11 | (2) |
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Thermodynamic Equilibrium |
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13 | (2) |
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15 | (1) |
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Measurability of the Energy |
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16 | (2) |
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Quantitative Definition of Heat---Units |
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18 | (7) |
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The Basic Problem of Thermodynamics |
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25 | (2) |
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The Entropy Maximum Postulates |
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27 | (8) |
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The Conditions of Equilibrium |
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35 | (24) |
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35 | (2) |
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37 | (3) |
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Entropic Intensive Parameters |
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40 | (3) |
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Thermal Equilibrium---Temperature |
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43 | (2) |
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Agreement with Intuitive Concept of Temperature |
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45 | (1) |
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46 | (3) |
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49 | (5) |
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Equilibrium with Respect to Matter Flow |
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54 | (2) |
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56 | (3) |
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Some Formal Relationships, and Sample Systems |
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59 | (32) |
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59 | (1) |
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The Gibbs--Duhem Relation |
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60 | (3) |
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Summary of Formal Structure |
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63 | (3) |
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The Simple Ideal Gas and Multicomponent Simple Ideal Gases |
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66 | (8) |
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The ``Ideal van der Waals Fluid'' |
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74 | (4) |
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Electromagnetic Radiation |
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78 | (2) |
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80 | (1) |
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Unconstrainable Variables; Magnetic Systems |
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81 | (3) |
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Molar Heat Capacity and Other Derivatives |
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84 | (7) |
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Reversible Processes and the Maximum Work Theorem |
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91 | (40) |
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Possible and Impossible Processes |
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91 | (4) |
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Quasi-Static and Reversible Processes |
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95 | (4) |
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Relaxation Times and Irreversibility |
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99 | (2) |
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Heat Flow: Coupled Systems and Reversal of Processes |
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101 | (2) |
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103 | (10) |
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Coefficients of Engine, Refrigerator, and Heat Pump Performance |
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113 | (5) |
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118 | (5) |
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Measurability of the Temperature and of the Entropy |
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123 | (2) |
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Other Criteria of Engine Performance; Power Output and ``Endoreversible Engines'' |
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125 | (3) |
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128 | (3) |
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Alternative Formulations and Legendre Transformations |
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131 | (22) |
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The Energy Minimum Principle |
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131 | (6) |
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137 | (9) |
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146 | (5) |
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Generalized Massieu Functions |
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151 | (2) |
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The Extremum Principle in the Legendre Transformed Representations |
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153 | (28) |
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The Minimum Principles for the Potentials |
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153 | (4) |
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157 | (3) |
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The Enthalpy; The Joule--Thomson or ``Throttling'' Process |
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160 | (7) |
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The Gibbs Potential; Chemical Reactions |
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167 | (5) |
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172 | (1) |
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Compilations of Empirical Data; The Enthalpy of Formation |
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173 | (6) |
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The Maximum Principles for the Massieu Functions |
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179 | (2) |
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181 | (22) |
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181 | (2) |
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A Thermodynamic Mnemonic Diagram |
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183 | (3) |
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A Procedure for the Reduction of Derivatives in Single-Component Systems |
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186 | (4) |
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190 | (9) |
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Generalizations: Magnetic Systems |
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199 | (4) |
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Stability of Thermodynamic Systems |
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203 | (12) |
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Intrinsic Stability of Thermodynamic Systems |
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203 | (4) |
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Stability Conditions for Thermodynamics Potentials |
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207 | (2) |
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Physical Consequences of Stability |
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209 | (1) |
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Le Chatelier's Principle; The Qualitative Effect of Fluctuations |
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210 | (2) |
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The Le Chatelier-Braun Principle |
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212 | (3) |
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First-Order Phase Transitions |
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215 | (40) |
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First-Order Phase Transitions in Single-Component Systems |
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215 | (7) |
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The Discontinuity in the Entropy-Latent Heat |
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222 | (6) |
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The Slope of Coexistence Curves; the Clapeyron Equation |
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228 | (5) |
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Unstable Isotherms and First-Order Phase Transitions |
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233 | (10) |
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General Attributes of First-Order Phase Transitions |
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243 | (2) |
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First-Order Phase Transitions in Multicoponent Systems---Gibbs Phase Rule |
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245 | (3) |
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Phase Diagrams for Binary Systems |
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248 | (7) |
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255 | (22) |
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Thermodynamics in the Neighborhood of the Critical Point |
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255 | (6) |
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261 | (2) |
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Order Parameters and Critical Exponents |
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263 | (2) |
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Classical Theory in the Critical Region; Landau Theory |
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265 | (5) |
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Roots of the Critical Point Problem |
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270 | (2) |
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272 | (5) |
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277 | (6) |
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Nernst's Postulate, and the Principle of Tomsen and Bertholot |
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277 | (3) |
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Heat Capacities and Other Derivatives at Low Temperatures |
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280 | (1) |
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The ``Unattainability'' of Zero Temperature |
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281 | (2) |
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Summary of Principles for General Systems |
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283 | (6) |
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283 | (1) |
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283 | (1) |
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284 | (1) |
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285 | (1) |
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285 | (1) |
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Stability and Phase Transitions |
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286 | (1) |
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287 | (1) |
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Properties at Zero Temperature |
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287 | (2) |
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289 | (18) |
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289 | (3) |
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Chemical Reactions in Ideal Gases |
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292 | (5) |
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Small Deviations from ``Ideality''---The Virial Expansion |
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297 | (2) |
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The ``Law of Corresponding States'' for Gases |
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299 | (3) |
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Dilute Solutions: Osmotic Pressure and Vapor Pressure |
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302 | (3) |
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305 | (2) |
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Irreversible Thermodynamics |
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307 | (22) |
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307 | (1) |
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308 | (4) |
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Purely-Resistive and Linear Systems |
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312 | (2) |
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The Theoretical Basis of the Onsager Reciprocity |
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314 | (2) |
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316 | (3) |
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319 | (1) |
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the Seebeck Effect and the Thermoelectric Power |
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320 | (3) |
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323 | (1) |
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324 | (5) |
PART II STATISTICAL MECHANICS |
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Statistical Mechanics in the Entropy Representation: The Microcanonical Formalism |
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329 | (20) |
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Physical Significance of the Entropy for Closed Systems |
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329 | (4) |
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The Einstein Model of a Crystalline Solid |
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333 | (4) |
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337 | (2) |
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A Polymer Model---The Rubber Band Revisited |
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339 | (4) |
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Counting Techniques and their Circumvention; High Dimensionality |
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343 | (6) |
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The Canonical Formalism; Statistical Mechanics in Helmholtz Representation |
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349 | (30) |
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The Probability Distribution |
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349 | (4) |
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Additive Energies and Factorizability of the Partition Sum |
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353 | (2) |
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355 | (3) |
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Probabilities in Factorizable Systems |
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358 | (2) |
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Statistical Mechanics of Small Systems: Ensembles |
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360 | (2) |
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Density of States and Density-of-Orbital States |
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362 | (2) |
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The Debye Model of Non-metallic Crystals |
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364 | (4) |
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Electromagnetic Radiation |
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368 | (2) |
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The Classical Density of States |
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370 | (2) |
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372 | (3) |
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High Temperature Properties---The Equipartition Theorem |
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375 | (4) |
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Entropy and Disorder; Generalized Canonical Formulations |
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379 | (14) |
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Entropy as a Measure of Disorder |
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379 | (3) |
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Distributions of Maximal Disorder |
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382 | (3) |
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The Grand Canonical Formalism |
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385 | (8) |
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393 | (30) |
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Quantum Particles; A ``Fermion Pre-Gas Model'' |
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393 | (6) |
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399 | (3) |
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The Classical Limit and the Quantum Criteria |
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402 | (3) |
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The Strong Quantum Regime; Electrons in a Metal |
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405 | (5) |
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410 | (2) |
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Non-Conserved Ideal Bose Fluids; Electromagnetic Radiation Revisited |
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412 | (1) |
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413 | (10) |
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423 | (10) |
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The Probability Distribution of Fluctuations |
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423 | (1) |
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Moments and The Energy Fluctuations |
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424 | (2) |
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General Moments and Correlation Moments |
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426 | (7) |
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Variational Properties, Perturbation Expansions, and Mean Field Theory |
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433 | (22) |
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The Bogoliubov Variational Theorem |
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433 | (1) |
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433 | (16) |
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Mean Field Theory in Generalized Representation; the Binary Alloy |
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449 | (6) |
PART III FOUNDATIONS |
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Postlude: Symmetry and the Conceptual Foundations of Thermostatistics |
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455 | (18) |
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455 | (3) |
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458 | (2) |
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460 | (1) |
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Energy, Momentum and Angular Momentum; the Generalized ``First Law'' of Thermodynamics |
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461 | (1) |
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Broken Symmetry and Goldstone's Theorem |
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462 | (3) |
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Other Broken Symmetry Coordinates---Electric and Magnetic Moments |
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465 | (1) |
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Mole Numbers and Gauge Sysmmetry |
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466 | (1) |
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Time Reversal, the Equal Probability of Microstates, and the Entropy Principle |
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467 | (2) |
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Symmetry and Completeness |
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469 | (4) |
APPENDIX A SOME RELATIONS INVOLVING PARTIAL DERIVATIVES |
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473 | (6) |
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473 | (1) |
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474 | (1) |
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475 | (1) |
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475 | (1) |
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476 | (3) |
APPENDIX B MAGNETIC SYSTEMS |
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479 | (6) |
General References |
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485 | (2) |
Index |
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487 | |