1. 2/26/2014PHY 770 Spring 2014 -- Lecture 131 PHY 770 -- Statistical Mechanics 12:00 * -1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course Webpage: http://www.wfu.edu/~natalie/s14phy770http://www.wfu.edu/~natalie/s14phy770 Lecture 13 Chap. 5 – Canonical esemble  Partition function  Ising model in 1d and mean field approximation Chap. 6 – Grand canonical ensemble  Grand partition function  Classical and quantum ideal gases * Partial make-up lecture -- early start time

2. 2/26/2014PHY 770 Spring 2014 -- Lecture 132

3. 2/26/2014PHY 770 Spring 2014 -- Lecture 133 Summary of results for the canonical ensemble

4. 2/26/2014PHY 770 Spring 2014 -- Lecture 134 1-dimensional Ising system of N spins (s i =-1,+1) with periodic boundary conditions (s N+1 =s 1 )

5. 2/26/2014PHY 770 Spring 2014 -- Lecture 135 1-dimensional Ising system of N spins with periodic boundary conditions (s N+1 =s 1 ) (continued)

6. 2/26/2014PHY 770 Spring 2014 -- Lecture 136 1-dimensional Ising system of N spins with periodic boundary conditions (s N+1 =s 1 ) (continued)

7. 2/26/2014PHY 770 Spring 2014 -- Lecture 137 1-dimensional Ising system of N spins with periodic boundary conditions (s N+1 =s 1 ) (continued)

8. 2/26/2014PHY 770 Spring 2014 -- Lecture 138 1-dimensional Ising system of N spins with periodic boundary conditions (s N+1 =s 1 ) (continued)       B 

9. 2/26/2014PHY 770 Spring 2014 -- Lecture 139 1-dimensional Ising system of N spins with periodic boundary conditions (s N+1 =s 1 ) (continued)

10. 2/26/2014PHY 770 Spring 2014 -- Lecture 1310  B   =0  =1 

11. 2/26/2014PHY 770 Spring 2014 -- Lecture 1311 Mean field approximation for 1-dimensional Ising model

12. 2/26/2014PHY 770 Spring 2014 -- Lecture 1312 Mean field partition function and Free energy:

13. 2/26/2014PHY 770 Spring 2014 -- Lecture 1313 s

14. 2/26/2014PHY 770 Spring 2014 -- Lecture 1314  =1  =1 BB One dimensional Ising model with periodic boundary conditions:

15. 2/26/2014PHY 770 Spring 2014 -- Lecture 1315 Extension of mean field analysis to more complicated geometries

16. 2/26/2014PHY 770 Spring 2014 -- Lecture 1316 Extension of mean field analysis to more complicated geometries -- continued Mean field partition function and Free energy:

17. 2/26/2014PHY 770 Spring 2014 -- Lecture 1317 Extension of mean field analysis to more complicated geometries -- continued

18. 2/26/2014PHY 770 Spring 2014 -- Lecture 1318 Extension of mean field analysis to more complicated geometries -- continued

19. 2/26/2014PHY 770 Spring 2014 -- Lecture 1319 Extension of mean field analysis to more complicated geometries -- continued

20. 2/26/2014PHY 770 Spring 2014 -- Lecture 1320 Extension of mean field analysis to more complicated geometries -- continued

21. 2/26/2014PHY 770 Spring 2014 -- Lecture 1321 Extension of mean field analysis to more complicated geometries -- continued CNCN T TcTc

22. 2/26/2014PHY 770 Spring 2014 -- Lecture 1322 Comment on mean field heat capacity

23. 2/26/2014PHY 770 Spring 2014 -- Lecture 1323 Comment about 1-dimensional case One can show (rigorously) that for one dimensional systems, there can be no phase transitions! (Mean field results are qualitative correct for 2 and 3 dimensions.)

24. 2/26/2014PHY 770 Spring 2014 -- Lecture 1324 Canonical ensemble – derivation from optimization Find form of probability density which optimizes S with constraints

25. 2/26/2014PHY 770 Spring 2014 -- Lecture 1325 Generalization: Grand canonical ensemble – derivation from optimization Find form of probability density which optimizes S with constraints

26. 2/26/2014PHY 770 Spring 2014 -- Lecture 1326 Grand partition function -- continued

27. 2/26/2014PHY 770 Spring 2014 -- Lecture 1327 Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions

28. 2/26/2014PHY 770 Spring 2014 -- Lecture 1328 Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Fermi-Dirac case In the absence of a magnetic field, the particle spin does not effect the energy spectrum, and only effects the enumeration of possible states

29. 2/26/2014PHY 770 Spring 2014 -- Lecture 1329 Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Fermi-Dirac case -- continued

30. 2/26/2014PHY 770 Spring 2014 -- Lecture 1330 Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Fermi-Dirac case -- continued

31. 2/26/2014PHY 770 Spring 2014 -- Lecture 1331 Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Fermi-Dirac case -- continued

32. 2/26/2014PHY 770 Spring 2014 -- Lecture 1332 Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Fermi-Dirac case -- continued

33. 2/26/2014PHY 770 Spring 2014 -- Lecture 1333 Examples of grand canonical ensembles – ideal (non-interacting) quantum particles in a cube of length L with periodic boundary conditions -- Fermi-Dirac case -- continued