| PART ONE CLASSICAL THEORY |
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Thermoelasticity from the Continuum Viewpoint |
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3 | (46) |
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3 | (1) |
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4 | (5) |
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9 | (6) |
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15 | (9) |
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Various Thermodynamic Potentials |
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24 | (3) |
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Thermoelastic Stress-Strain Relations |
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27 | (3) |
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Thermoelastic Relations for Small Changes from Reference State |
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30 | (4) |
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Related Thermodynamic Functions |
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34 | (4) |
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Elastic Constants in Terms of Displacement Gradients |
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38 | (4) |
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42 | (7) |
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Appendix: Notation of Thurston (1964) |
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47 | (2) |
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Concepts of Classical Statistical Mechanics |
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49 | (36) |
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49 | (1) |
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50 | (4) |
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Use of Statistics in Statistical Mechanics |
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54 | (2) |
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Phase Functions and Time Averages |
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56 | (5) |
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Phase Space Dynamics of Isolated Systems |
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61 | (11) |
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Systems in Weak Interaction |
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72 | (4) |
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76 | (4) |
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Time Averages versus Ensemble Averages |
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80 | (5) |
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Corresponding Concepts in Thermodynamics and Statistical Mechanics |
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85 | (42) |
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85 | (2) |
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87 | (1) |
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88 | (1) |
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Phase Functions for Generalized Forces |
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89 | (1) |
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First Law of Thermodynamics |
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90 | (3) |
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Second Law of Thermodynamics |
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93 | (3) |
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Use of Mechanical Variables as Controllable Parameters |
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96 | (8) |
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104 | (11) |
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Partition Function Relations |
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115 | (1) |
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Continuum Formulations of Nonuniform Processes |
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116 | (2) |
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118 | (2) |
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Entropy from the Information Theory Viewpoint |
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120 | (7) |
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127 | (58) |
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127 | (2) |
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129 | (2) |
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The Atomistic Concept of Stress in a Perfect Crystal |
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131 | (9) |
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Harmonic and Quasi-Harmonic Approximations |
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140 | (3) |
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Thermoelastic Stress--Strain Relations Based on the Harmonic Approximation |
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143 | (7) |
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150 | (6) |
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156 | (4) |
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Linear Chain with Nearest Neighbor Interactions |
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160 | (14) |
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Lattice Dynamics and Crystal Elasticity |
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174 | (11) |
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185 | (26) |
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185 | (1) |
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Relative Roles of Internal Energy and Entropy |
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186 | (2) |
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Atomic Structure of Long-Chain Molecules and Networks |
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188 | (5) |
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One-Dimensional Polymer Model |
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193 | (5) |
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Three-Dimensional Polymer Models |
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198 | (7) |
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Network Theory of Rubber Elasticity |
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205 | (6) |
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211 | (46) |
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211 | (1) |
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212 | (5) |
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217 | (4) |
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221 | (2) |
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Curvilinear Coordinates for Stressed Polymer Chains |
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223 | (5) |
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Rigid and Flexible Polymer Models |
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228 | (6) |
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Use of S = k log p for Stretched Polymers |
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234 | (3) |
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Strain Ensemble for Short Freely Jointed Chains |
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237 | (7) |
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Stress Ensemble for Chain Molecules |
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244 | (3) |
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Statistical Mechanics of Phantom Networks |
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247 | (10) |
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Addendum Atomic View of Stress in Polymer Systems |
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1 | |
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257 | (40) |
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257 | (1) |
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258 | (3) |
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A Simple One-Dimensional Rate Theory |
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261 | (4) |
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265 | (2) |
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267 | (8) |
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Transition-State Assumption |
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275 | (1) |
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276 | (11) |
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287 | (10) |
| PART TWO QUANTUM THEORY |
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Basic Concepts of Quantum Mechanics |
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297 | (50) |
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297 | (1) |
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Structure of Classical Mechanics |
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298 | (1) |
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Structure of Quantum Mechanics |
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299 | (4) |
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Consequences of the Fourier Transform Relation between ψx(x) and ψp(p) |
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303 | (9) |
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Extension to Three-Dimensional Motion and to N Particles |
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312 | (3) |
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Hydrodynamic Analogy to Quantum Mechanics |
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315 | (3) |
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318 | (2) |
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Aspects of the Measurement Process |
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320 | (2) |
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Some Examples of Stationary States |
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322 | (12) |
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Tensor Product of Two Spaces |
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334 | (2) |
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336 | (4) |
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Identical Particles and the Pauli Principle |
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340 | (7) |
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347 | (25) |
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347 | (1) |
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348 | (5) |
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353 | (4) |
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Hellmann--Feynman Theorem |
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357 | (3) |
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Harmonic Elastic Moduli Based on Hellmann-Feynman Theorem |
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360 | (5) |
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Categories of Interatomic Force Laws |
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365 | (7) |
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Quantum Statistical Effects |
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372 | (49) |
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372 | (1) |
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Quantum Statistical Mechanics |
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372 | (14) |
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Quantum Statistical Effects in Crystals |
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386 | (17) |
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Quantum Statistics for Polymer Models |
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403 | (3) |
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Gaussian Wave Packet Dynamics |
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406 | (6) |
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Canonical Ensemble in Terms of Coherent States |
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412 | (4) |
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Quantum Effects on Rate Processes |
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416 | (5) |
| References |
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421 | (10) |
| Index |
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431 | |