1. HW1. Due Thursday, April 9.
Ch. 2,3. Multiplicity; Statistical definitions of entropy,
temperature.
2. HW2. Due Thursday, April 16.
Ch 6. Partition function and Equipartition.
3. HW3 Due Thursday, April 23. Ch
6. Partition function and free energy.
4. HW4 Due Thursday, April
30. notes + Ch 7.1. Chemical potential and grand partition
function
5. HW5
Due Thursday, May 7. Perfect Gases and Ideal Solutions
6. HW6. Due Thursday, May 14.
Degenerate Fermi Gases
7. HW7 Due Thursday, May
21. Semiconductor Statistics
8. HW8 Due Thursday, May
28. Black Body Radiation
9. HW9 Due Thursday, June 4.
Phonons, Bose Condensates.
Back to Physics 328 Home Page.
Comments on Reading
- Read chapters 2 and 3, with emphasis on 2.1 through 2.4 and 3.1 to 3.4. We will do a slightly more mathematical description in class, as many of you saw this in Physics 224. Spend the time you need to learn/review this basic underpinning of statistical physics. In class, we also will review the laws of thermodynamics and relate them to the statistical definitions of temperature and entropy.
- For week 2, read chapter 6.1-2-3. Section 6.1 is the core of statistical mechanics. As you read section 6.2, think about the differences between statistical probabilities and averages vs. quantum mechanical probabilities and expectation values. For section 6.3, equipartition, we will derive the general formula in class.
Assignment
Comments on Reading
- In week 3, we will cover most of the rest of chapter 6 -- Maxwell Boltzmann statistics; connection between partition function and Helmholtz free energy, and then apply the partition function to a multiparticle system, heading into developing the partition function for an ideal gas (which we'll finish up in week 4). We'll also spend a little time reviewing the four energy functions -- U, H, F, G. Since Free Energy is inherently a property of many particles, I may invert the order of sections 6.5 and 6.6 to cover composite partition functions first, and then make the connection to free energy. We'll then use these concepts for particle-in-a-box states and after about 1.5 lectures we'll have derived the ideal gas law from first principles.
Assignment
Comments on Reading: Schroeder assumes you already are familiar with chemical potential as he introduces the Gibbs factor and grand partition function. We'll take time in class to show how chemical potential arises from diffusive equilibrium in the same way that temperature arises from thermal equilibrium. You might want to read parts of chapter 5 for macroscopic applications of chemical potential. The midterm is on Friday, April 24, and covers through the first three HW sets (The parts of Chapters 1-5 that we covered in class, plus chapter 6 and any extra material covered in lecture notes through Monday April 20).
back to topAssignment
- 6.42. Entropy of simple harmonic oscillator. ALSO: take the limits of your expression at high and low temperature (compared to hf/k), and discuss them.
- 6.48 a. Entropy of air. Skip part b -- we'll come back to that in another week once we have discussed chemical potential.
- 6.52 Relativistic gas partition function. Use the same particle in a box states in wavevector as for the non-relativistic case, but the relativistic relationship between momentum (wavelength) and energy.
- Extra Problem 3.A. Rayleigh Scattering HERE in a pdf file.
- Extra Problem 3.B Adiabatic Demagnetization. HERE in a pdf file.
back to topComments on Reading: Schroeder treats the full electrochemical potential or gravichemical potential as what he calls the chemical potential. Other books will treat the two separately. It is the full electrochemical potential that is constant in equilibrium, so what Schroeder is doing is better, but you should be warned that others treat it differently. We will take a different approach to the Gibbs Factor derivation than the text -- you should remember whichever one makes more sense to you. We will then move on to the perfect gas for the next couple of weeks, which is a remarkably good approximation to a huge number of real-life situations.
Assignment
- Short this week due to midterm -- we'll have more Grand Partition Function practice next week.
- 7.2: Hemoglobin oxygen adsorption. Remember that each distinct energy level and number is a state to count in the Grand partition function.
- 7.6 Particle number averages and fluctuations. This is similar to the derivatives of the partition function for energy.
- extra 4: Tree sap in a gravichemical potential. Here in a pdf file. This is simpler than many students think at first glance.
back to topComments on Reading.
This week we will take a break from Chapter 7 to return to the parts of chapter 5 that weren't covered in 224, namely solutions and osmotic pressure and chemical reactions. We will come at reactions from a different point of view than the text, using the concept of the grand partition function and how it gets modified by internal degrees of freedom.
Assignment
- 7.8 Partition functions and quantum statistics
- 7.12 Symmetry in Fermi-Dirac distribution
- Note we are doing 7.15 in class on Friday, so it is not assigned, but interesting none-the-less.
- 7.16 OR 7.17 Building up the Fermi (7.16) and Bose (7.17) distributions from scratch. Pick either ONE of these (they are both interesting, but it gets tedious after a while).
- 5.75 Comparison of class and book derivation In class on Friday or Monday, we will derive the chemical potential of solution from the free energy of an ideal mixture. The book takes the approach of adding solute molecules to a container of solvent. This problem asks you to think about the range of validity of the two approaches and show they give the same result.
- 5.76 Osmotic pressure and desalination
- extra 5. Partial pressures SORRY this never got linked to. Moved to Next Week's Assignment.
back to topComments on Reading
Degenerate Fermi Gases are present in metals, semiconductors and stars. We will come back to the particle in a box states, and see what happens when will fill them with Fermions at a density much larger than the quantum density. Electrons in a metal are at low enough energies that they are non-relativistic. When a white dwarf collapses to a neutron star, however, the electrons go relativistic. When the neutron star collapses to a black hole, it is the neutron Fermi gas that goes relativistic. The book covers stars only in a HW problem -- we'll spend some time on them in class. We will then move on to systems at finite temperature, and look at heat capacity and Pauli paramagnetism, and then semiconductors. Again, the book contains the bare minimum equations, and puts all the applications into HW problems. We'll spend an extra couple of lectures on semiconductors next week, covering material that isn't in the book.
Assignment
- Extra 6.A Partial Pressures (relevant to last week, but forgot to link to it)
- Extra 6.B Polymer stability. Using the chemical equilibrium equations to look at a real system.
- Extra 6.C Thermal ionization of hydrogen. This extends the example in the text.
- 7.28 Chemical Potential of a 2D electron gas
- 7.22 Relativistic Fermi Gas. You will need this result for 6.D.
- Extra 6.D Neutron Star
- LINK for the non-text problems.
back to topWe will return to the text this week for Bose gases, including photons (black body radiation), phonons (including heat capacity of a solid) and Bose condensates (superfluid He and ultracold gases).
Assignment
- Since semiconductors are not covered well in the text, this weeks problems are all from outside the text.
- Extra 7.A. Semi-insulating GaAs.
- Extra 7.B. Extrinsic vs. Intrinsic contributions to the conductivity.
- Extra 7.C. Degenerate semiconductors.
- Optional 7.D. Fields in a pn-junction. This problem is more E&M than Stat-Mech, and is included for the interested student.
- Link for the non-text problems
back to topComments on Reading
There is no class Monday, May 25 due to the Memorial Day Holiday. The rest of the week we'll look at phonons and Bose Condensates. The book does a reasonable job on both topics, though we'll approach condensation slightly differently in class.
Assignment
- 7.41 Einstein A and B coefficients.
- 7.43 Solar radiation.
- 7.46 Free energy of the photon gas.
- 7.56 Venus as a greenhouse
back to topComments on Reading
The final week of the quarter we will spend Monday on superfluids (see notes) and magnons (covered in problem 7.64). Wednesday we will cover the Ising model (8.2), and then both tie up loose ends and review on Friday in preparation for the final exam on Monday. The problems on magnons and the Ising model are optional, since you don't really have enough time to learn it in time for the HW to be due.
Assignment
- 7.60 Heat capacity of copper [note -- This is a classic problem. There was a Prof. at Berkeley who was famous for always asking in the oral qualifying exam -- "What's the specific heat of a penny?"]
- 7.63 2D Solid
- 7.66 Bose condensation of Rubidium
- Extra 8.A. 2-D Bose Condensate Considerations. Updated on Monday June 1 with a hint on the DOS for the oscillator.
- Extra 8.B. Fountain Effect
- link for extra.