Thermodynamics and Statistical Mechanics The Third Law of
- Slides: 14
Thermodynamics and Statistical Mechanics The Third Law of Thermodynamics Thermo & Stat Mech Spring 2006 Class 10 1
Statements of Third Law All reactions in a liquid or solid in thermal equilibrium take place with no change of entropy in the neighborhood of absolute zero. (Nernst) The entropy of a true equilibrium state of a system at absolute zero is zero. (Planck) Thermo & Stat Mech - Spring 2006 Class 10 2
Statements of Third Law It is impossible to reduce the temperature of a system to absolute zero using a finite number of processes. (Unattainability statement) Thermo & Stat Mech - Spring 2006 Class 10 3
Entropy Thermo & Stat Mech - Spring 2006 Class 10 4
Nernst Postulate Thermo & Stat Mech - Spring 2006 Class 10 5
Planck Thermo & Stat Mech - Spring 2006 Class 10 6
Equivalence of Statements Assume that the unattainability statement of the third law is valid, and show that it leads to the Nernst statement. DS 0 = S 01 – S 02 = 0 Thermo & Stat Mech - Spring 2006 Class 10 7
Equivalence of Statements Consider adiabatic cooling Thermo & Stat Mech - Spring 2006 Class 10 8
Adiabatic Cooling Plot Thermo & Stat Mech - Spring 2006 Class 10 9
Can Achieve T = 0 Thermo & Stat Mech - Spring 2006 Class 10 10
Real Cooling Thermo & Stat Mech - Spring 2006 Class 10 11
Consequences of Third Law Thermo & Stat Mech - Spring 2006 Class 10 12
Consequences of Third Law Clausius-Clapeyron equation Thermo & Stat Mech - Spring 2006 Class 10 13
Consequences of Third Law Thermo & Stat Mech - Spring 2006 Class 10 14
- Dulong petit law
- Thermodynamics and statistical mechanics
- Newton's first law and second law and third law
- Newton's first law
- Third law of thermodynamics is depend on
- Newtons third law of thermodynamics
- Zeroth law of thermodynamics examples
- Statistical thermodynamics in chemistry
- Statistical thermodynamics
- Microstate and macrostate examples
- Studyja
- Stat
- Statistical mechanics
- Equipartition theorem in statistical mechanics
- Partition function in statistical mechanics