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."'' | |||
| :[[Max Karl Ernst Ludwig Planck | Max Planck]] "The Genesis and Present State of Development of the Quantum Theory" [http://nobelprize.org/nobel_prizes/physics/laureates/1918/planck-lecture.html 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"  | |||
| {{columns-list|3| | |||
| ==B== | |||
| *[[Boyle's law]] | *[[Boyle's law]] | ||
| *[[Boyle temperature]] | *[[Boyle temperature]] | ||
| *[[Bridgman thermodynamic formulas]] | |||
| ==C== | |||
| *[[Capillary waves]] | |||
| *[[Carnot cycle]] | *[[Carnot cycle]] | ||
| *[[Charles's law]] | *[[Charles's law]] | ||
| *[[Chemical potential]] | *[[Chemical potential]] | ||
| *[[Clausius-Clapeyron relation]] | |||
| *[[Clausius theorem]] | |||
| *[[Compressibility]] | *[[Compressibility]] | ||
| *[[Compressibility factor]] | *[[Compressibility factor]] | ||
| *[[Critical points]] | *[[Critical points]] | ||
| ==D== | |||
| *[[Dalton's law]] | |||
| *[[Duhem-Margules equation]] | |||
| ==E== | |||
| *[[Energy equation]] | *[[Energy equation]] | ||
| *[[Enthalpy]] | *[[Enthalpy]] | ||
| *[[Entropy]] | |||
| *[[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]] | ||
| *[[Gibbs phase rule]] | |||
| *[[Griffiths phase rule]] | |||
| ==H== | |||
| *[[Heat]] | |||
| *[[Heat capacity]] | *[[Heat capacity]] | ||
| *[[Helmholtz energy function]] | *[[Helmholtz energy function]] | ||
| *[[Henry's law]] | |||
| ==I== | |||
| *[[Intensive properties]] | |||
| *[[Internal energy]] | *[[Internal energy]] | ||
| ==J== | |||
| *[[Joule-Thomson effect]] | |||
| ==L== | |||
| *[[Latent heat]] | |||
| *[[Law of corresponding states]] | |||
| *[[Le Chatelier's principle]] | |||
| ==M== | |||
| *[[Maxwell's relations]] | *[[Maxwell's relations]] | ||
| *[[ | *[[Melting curve]] | ||
| *[[Mpemba effect]] | |||
| ==P== | |||
| *[[Pressure]] | *[[Pressure]] | ||
| ==R== | |||
| *[[Rankine cycle]] | |||
| *[[Raoult's law]] | |||
| ==S== | |||
| *[[Second law of thermodynamics]] | *[[Second law of thermodynamics]] | ||
| *[[Speed of sound]] | |||
| *[[Stirling cycle]] | |||
| ==T== | |||
| *[[Temperature]] | *[[Temperature]] | ||
| *[[Thermal conductivity]] | |||
| *[[Thermal expansion coefficient]] | *[[Thermal expansion coefficient]] | ||
| *[[Thermodynamic integration]] | *[[Thermodynamic integration]] | ||
| *[[Thermodynamic potential]] | |||
| *[[Thermodynamic relations]] | *[[Thermodynamic relations]] | ||
| *[[Third law of thermodynamics]] | |||
| *[[Triple point]] | |||
| ==V== | |||
| *[[Vapour pressure]] | |||
| ==W== | |||
| *[[Work]] | *[[Work]] | ||
| ==Z== | |||
| *[[Zeno line]] | |||
| *[[Zeroth law of thermodynamics]] | *[[Zeroth law of thermodynamics]] | ||
| }} | |||
| [[category: Classical thermodynamics]] | |||
| __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