Homework

Physics 328

Spring Quarter 2009

Last Update 01 June 2009

General Instructions

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.

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General Instructions

1.  Week 1:  Multiplicity; Statistical definitions of entropy, temperature.  Intro to Partition Function.
    DUE Thursday April 9.  5 pm.

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2.  Partition Function and Equipartition.  DUE Thursday, April 16, 5 pm.

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3.   Free energy and partition function, Ideal Gas introduced.  Due Thursday, April 23.

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).

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4.  Chemical Potential and Grand Partition Function

Comments 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.

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5.   Perfect Gases and Ideal Solutions

Comments 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.

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6.  Chemical Reactions and Fermi Gases

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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.

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7.   Semiconductor Statistics.  Due Thursday, May 21

We 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).

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8.  Black Body Radiation.  Due Thursday, May 28

Comments 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.

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9.  Bose Excitations and Condensates.  Due Thursday, June 4.

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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.

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