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   | :[[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]]  | *[[Capillary waves]]  | ||
*[[Carnot cycle]]  | *[[Carnot cycle]]  | ||
| Line 12: | Line 19: | ||
*[[Compressibility factor]]  | *[[Compressibility factor]]  | ||
*[[Critical points]]  | *[[Critical points]]  | ||
==D==  | |||
*[[Dalton's law]]  | *[[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]]  | ||
*[[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]]  | ||
==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]]  | *[[Raoult's law]]  | ||
==S==  | |||
*[[Second law of thermodynamics]]  | *[[Second law of thermodynamics]]  | ||
*[[Speed of sound]]  | |||
*[[Stirling cycle]]  | *[[Stirling cycle]]  | ||
==T==  | |||
*[[Temperature]]  | *[[Temperature]]  | ||
*[[Thermal conductivity]]  | |||
*[[Thermal expansion coefficient]]  | *[[Thermal expansion coefficient]]  | ||
*[[Thermodynamic integration]]  | *[[Thermodynamic integration]]  | ||
*[[Thermodynamic potential]]  | *[[Thermodynamic potential]]  | ||
*[[Thermodynamic relations]]  | *[[Thermodynamic relations]]  | ||
*[[Third law of thermodynamics]]  | |||
*[[Triple point]]  | *[[Triple point]]  | ||
==V==  | |||
*[[Vapour pressure]]  | |||
==W==  | |||
*[[Work]]  | *[[Work]]  | ||
==Z==  | |||
*[[Zeno line]]  | |||
*[[Zeroth law of thermodynamics]]  | *[[Zeroth law of thermodynamics]]  | ||
}}  | |||
[[category: Classical 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