Classical thermodynamics: Difference between revisions
Jump to navigation
Jump to search
Cloudnine189 (talk | contribs) No edit summary |
Carl McBride (talk | contribs) m (Added an internal link) |
||
| (One intermediate revision by the same user not shown) | |||
| Line 25: | Line 25: | ||
*[[Energy equation]] | *[[Energy equation]] | ||
*[[Enthalpy]] | *[[Enthalpy]] | ||
*[[Entropy]] | |||
*[[Extensive properties]] | *[[Extensive properties]] | ||
==F== | ==F== | ||
| Line 81: | Line 82: | ||
[[category: Classical thermodynamics]] | [[category: Classical thermodynamics]] | ||
__NOTOC__ | __NOTOC__ | ||
Latest revision as of 14:16, 10 January 2017
- "...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 "The Genesis and Present State of Development of the Quantum Theory" Nobel Lecture, June 2, 1920
- "...the deep impression that classical thermodynamics made upon me. It is the only physical theory of universal content concerning which I am convinced that, within the framework of the applicability of its basic concepts, it will never be overthrown."
- Albert Einstein "Autobiographical Notes"
B
C
- Capillary waves
- Carnot cycle
- Charles's law
- Chemical potential
- Clausius-Clapeyron relation
- Clausius theorem
- Compressibility
- Compressibility factor
- Critical points
D
E
F
G
- Gay-Lussac's law
- Gibbs-Duhem relation
- Gibbs-Helmholtz equations
- Gibbs energy function
- Gibbs phase rule
- Griffiths phase rule
H
I
J
L
M
P
R
S
T
- Temperature
- Thermal conductivity
- Thermal expansion coefficient
- Thermodynamic integration
- Thermodynamic potential
- Thermodynamic relations
- Third law of thermodynamics
- Triple point