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
1 - Introducing thermodynamics
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
The atomistic nature of matter as conceptualized by the Greeks had, by the 19th century, been raised by scientists to a high probability. But it was Planck's law of radiation that yielded the first exact determination of the absolute size of atoms. More than that, he convincingly showed that in addition to the atomistic structure of matter there is a kind of atomistic structure to energy, governed by the universal constant h.
This discovery has almost completely dominated the development of physics in the 20th century. Without this discovery a workable theory of molecules and atoms and the energy processes that govern their transformations would not have been possible. It has, moreover, shaken the whole framework of classical mechanics and electrodynamics and set science the fresh task of finding a new conceptual basis for all of physics. Despite partial success, the problem is still far from solved.
Albert Einstein, “Max Planck memorial service” (1948). Original image, Einstein Archives Online, Jerusalem (trans. A. Wasserman)The beginning
Thermodynamics has exceeded the scope and applicability of its utile origins in the industrial revolution to a far greater extent than other subjects of physics' classical era, such as mechanics and electromagnetism. Unquestionably this results from over a century of synergistic development with quantum mechanics, to which it has given and from which it has gained clarification, enhancement and relevance, earning for it a vital role in the modern development of physics as well as chemistry, biology, engineering, and even aspects of philosophy.
- Type
- Chapter
- Information
- Thermal PhysicsConcepts and Practice, pp. 1 - 11Publisher: Cambridge University PressPrint publication year: 2011