Classical thermodynamics: Difference between revisions
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Carl McBride (talk | contribs) m (Added a nice quote from Max Planck) |
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:''"...all the signs suggest that the main principles of thermodynamics from the classical theory will not only rule unchallenged but will more probably become correspondingly extended. "'' | |||
:Max Planck on quantum theory, [http://nobelprize.org/nobel_prizes/physics/laureates/1918/planck-lecture.html Nobel Lecture, June 2, 1920] | |||
*[[Boyle's law]] | *[[Boyle's law]] | ||
*[[Boyle temperature]] | *[[Boyle temperature]] | ||
Revision as of 16:51, 14 February 2008
- "...all the signs suggest that the main principles of thermodynamics from the classical theory will not only rule unchallenged but will more probably become correspondingly extended. "
- Max Planck on quantum theory, Nobel Lecture, June 2, 1920
- Boyle's law
- Boyle temperature
- Capillary waves
- Carnot cycle
- Charles's law
- Chemical potential
- Clausius-Clapeyron relation
- Clausius theorem
- Compressibility
- Compressibility factor
- Critical points
- Dalton's law
- Energy equation
- Enthalpy
- First law of thermodynamics
- Gay-Lussac's law
- Gibbs-Duhem relation
- Gibbs-Helmholtz equations
- Gibbs energy function
- Heat
- Heat capacity
- Helmholtz energy function
- Henry's law
- Internal energy
- Joule-Thomson effect
- Maxwell's relations
- Maxwell's equal area construction
- Pressure
- Raoult's law
- Second law of thermodynamics
- Stirling cycle
- Temperature
- Thermal expansion coefficient
- Thermodynamic integration
- Thermodynamic potential
- Thermodynamic relations
- Triple point
- Work
- Zeroth law of thermodynamics