Classical thermodynamics: Difference between revisions
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Carl McBride (talk | contribs) m (→M) |
Carl McBride (talk | contribs) m (Added Law of corresponding states internal link.) |
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==J== | ==J== | ||
*[[Joule-Thomson effect]] | *[[Joule-Thomson effect]] | ||
==L== | |||
*[[Law of corresponding states]] | |||
==M== | ==M== | ||
*[[Maxwell's relations]] | *[[Maxwell's relations]] | ||
==P== | ==P== | ||
*[[Pressure]] | *[[Pressure]] |
Revision as of 14:22, 7 April 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
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
H
I
J
L
M
P
R
S
T
- Temperature
- Thermal expansion coefficient
- Thermodynamic integration
- Thermodynamic potential
- Thermodynamic relations
- Triple point