Book contents
- Frontmatter
- Contents
- Preface
- 1 Introducing thermodynamics
- 2 A road to thermodynamics
- 3 Work, heat and the First Law
- 4 A mathematical digression
- 5 Thermodynamic potentials
- 6 Knowing the “unknowable”
- 7 The ideal gas
- 8 The two-level system
- 9 Lattice heat capacity
- 10 Elastomers: entropy springs
- 11 Magnetic thermodynamics
- 12 Open systems
- 13 The amazing chemical potential
- 14 Thermodynamics of radiation
- 15 Ideal Fermi gas
- 16 Ideal Bose–Einstein system
- 17 Thermodynamics and the cosmic microwave background
- Appendix A How pure is pure? An inequality
- Appendix B Bias and the thermal Lagrangian
- Appendix C Euler's homogeneous function theorem
- Appendix D Occupation numbers and the partition function
- Appendix E Density of states
- Appendix F A lab experiment in elasticity
- Appendix G Magnetic and electric fields in matter
- Appendix H Maxwell's equations and electromagnetic fields
- Appendix I Fermi–Dirac integrals
- Appendix J Bose–Einstein integrals
- Index
Preface
Published online by Cambridge University Press: 05 June 2012
- Frontmatter
- Contents
- Preface
- 1 Introducing thermodynamics
- 2 A road to thermodynamics
- 3 Work, heat and the First Law
- 4 A mathematical digression
- 5 Thermodynamic potentials
- 6 Knowing the “unknowable”
- 7 The ideal gas
- 8 The two-level system
- 9 Lattice heat capacity
- 10 Elastomers: entropy springs
- 11 Magnetic thermodynamics
- 12 Open systems
- 13 The amazing chemical potential
- 14 Thermodynamics of radiation
- 15 Ideal Fermi gas
- 16 Ideal Bose–Einstein system
- 17 Thermodynamics and the cosmic microwave background
- Appendix A How pure is pure? An inequality
- Appendix B Bias and the thermal Lagrangian
- Appendix C Euler's homogeneous function theorem
- Appendix D Occupation numbers and the partition function
- Appendix E Density of states
- Appendix F A lab experiment in elasticity
- Appendix G Magnetic and electric fields in matter
- Appendix H Maxwell's equations and electromagnetic fields
- Appendix I Fermi–Dirac integrals
- Appendix J Bose–Einstein integrals
- Index
Summary
In the preface to his book Statistical Mechanics Made Simple Professor Daniel Mattis writes:
My own experience in thermodynamics and statistical mechanics, a half century ago at M.I.T., consisted of a single semester of Sears, skillfully taught by the man himself. But it was a subject that seemed as distant from “real” physics as did poetry or French literature.
This frank but discouraging admission suggests that thermodynamics may not be a course eagerly anticipated by many students – not even physics, chemistry or engineering majors – and at completion I would suppose that few are likely to claim it was an especially inspiring experience. With such open aversion, the often disappointing performance on GRE questions covering the subject should not be a surprise. As a teacher of the subject I have often conjectured on reasons for this lack of enthusiasm.
Apart from its subtlety and perceived difficulty, which are probably immutable, I venture to guess that one problem might be that most curricula resemble the thermodynamics of nearly a century ago.
Another might be that, unlike other areas of physics with their epigrammatic equations – Newton's, Maxwell's or Schrödinger's, which provide accessibility and direction – thermal physics seems to lack a comparable unifying principle. Students may therefore fail to see conceptual or methodological coherence and experience confusion instead.
With those assumptions I propose in this book alternatives which try to address the disappointing experience of Professor Mattis and undoubtedly others.
Thermodynamics, the set of rules and constraints governing interconversion and dissipation of energy in macroscopic systems, can be regarded as having begun with Carnot's (1824) pioneering paper on heat-engine efficiency.
- Type
- Chapter
- Information
- Thermal PhysicsConcepts and Practice, pp. xi - xivPublisher: Cambridge University PressPrint publication year: 2011