Classical thermodynamics: Difference between revisions
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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."'' | :''"...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] | :Max Planck on quantum theory, [http://nobelprize.org/nobel_prizes/physics/laureates/1918/planck-lecture.html Nobel Lecture, June 2, 1920] | ||
==B== | |||
*[[Boyle's law]] | *[[Boyle's law]] | ||
*[[Boyle temperature]] | *[[Boyle temperature]] | ||
==C== | |||
*[[Capillary waves]] | *[[Capillary waves]] | ||
*[[Carnot cycle]] | *[[Carnot cycle]] | ||
| Line 12: | Line 14: | ||
*[[Compressibility factor]] | *[[Compressibility factor]] | ||
*[[Critical points]] | *[[Critical points]] | ||
==D== | |||
*[[Dalton's law]] | *[[Dalton's law]] | ||
==E== | |||
*[[Energy equation]] | *[[Energy equation]] | ||
*[[Enthalpy]] | *[[Enthalpy]] | ||
*[[Extensive properties]] | |||
==F== | |||
*[[First law of thermodynamics]] | *[[First law of thermodynamics]] | ||
==G== | |||
*[[Gay-Lussac's law]] | *[[Gay-Lussac's law]] | ||
*[[Gibbs-Duhem relation]] | *[[Gibbs-Duhem relation]] | ||
*[[Gibbs-Helmholtz equations]] | *[[Gibbs-Helmholtz equations]] | ||
*[[Gibbs energy function]] | *[[Gibbs energy function]] | ||
==H== | |||
*[[Heat]] | *[[Heat]] | ||
*[[Heat capacity]] | *[[Heat capacity]] | ||
*[[Helmholtz energy function]] | *[[Helmholtz energy function]] | ||
*[[Henry's law]] | *[[Henry's law]] | ||
==I== | |||
*[[Intensive properties]] | |||
*[[Internal energy]] | *[[Internal energy]] | ||
==J== | |||
*[[Joule-Thomson effect]] | *[[Joule-Thomson effect]] | ||
==M== | |||
*[[Maxwell's relations]] | *[[Maxwell's relations]] | ||
*[[Maxwell's equal area construction]] | *[[Maxwell's equal area construction]] | ||
==P== | |||
*[[Pressure]] | *[[Pressure]] | ||
==R== | |||
*[[Raoult's law]] | *[[Raoult's law]] | ||
==S== | |||
*[[Second law of thermodynamics]] | *[[Second law of thermodynamics]] | ||
*[[Stirling cycle]] | *[[Stirling cycle]] | ||
==T== | |||
*[[Temperature]] | *[[Temperature]] | ||
*[[Thermal expansion coefficient]] | *[[Thermal expansion coefficient]] | ||
| Line 38: | Line 54: | ||
*[[Thermodynamic relations]] | *[[Thermodynamic relations]] | ||
*[[Triple point]] | *[[Triple point]] | ||
==W== | |||
*[[Work]] | *[[Work]] | ||
==Z== | |||
*[[Zeroth law of thermodynamics]] | *[[Zeroth law of thermodynamics]] | ||
==General reading== | ==General reading== | ||
*[http://store.doverpublications.com/048666371x.html Max Planck "Treatise on Thermodynamics", Dover Publications ISBN: 048666371X] | *[http://store.doverpublications.com/048666371x.html Max Planck "Treatise on Thermodynamics", Dover Publications ISBN: 048666371X] | ||
[[category: Classical thermodynamics]] | [[category: Classical thermodynamics]] | ||
__NOTOC__ | |||
Revision as of 17:57, 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
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
M
P
R
S
T
- Temperature
- Thermal expansion coefficient
- Thermodynamic integration
- Thermodynamic potential
- Thermodynamic relations
- Triple point