Gibbs sum for a two level system

• Gibbs sum Microstate Thermal average energy
• face Chemical potential and Gibbs distribution

  face Lecture

  120 min.

  Chemical potential and Gibbs distribution

  Thermal and Statistical Physics 2020

  chemical potential Gibbs distribution grand canonical ensemble statistical mechanics

  These notes from the fifth week of Thermal and Statistical Physics cover the grand canonical ensemble. They include several small group activities.
• face Review of Thermal Physics

  face Lecture

  30 min.

  Review of Thermal Physics

  Thermal and Statistical Physics 2020

  thermodynamics statistical mechanics

  These are notes, essentially the equation sheet, from the final review session for Thermal and Statistical Physics.
• face Gibbs entropy approach

  face Lecture

  120 min.

  Gibbs entropy approach

  Thermal and Statistical Physics 2020

  Gibbs entropy information theory probability statistical mechanics

  These lecture notes for the first week of Thermal and Statistical Physics include a couple of small group activities in which students work with the Gibbs formulation of the entropy.
• assignment Boltzmann probabilities

  assignment Homework

  Boltzmann probabilities

  Energy Entropy Boltzmann probabilities Thermal and Statistical Physics 2020 (3 years) Consider a three-state system with energies \((-\epsilon,0,\epsilon)\).

  1. At infinite temperature, what are the probabilities of the three states being occupied? What is the internal energy \(U\)? What is the entropy \(S\)?
  2. At very low temperature, what are the three probabilities?
  3. What are the three probabilities at zero temperature? What is the internal energy \(U\)? What is the entropy \(S\)?
  4. What happens to the probabilities if you allow the temperature to be negative?
• group Hydrogen emission

  group Small Group Activity

  30 min.

  Hydrogen emission

  Contemporary Challenges 2021 (5 years)

  hydrogen atom photon energy

  In this activity students work out energy level transitions in hydrogen that lead to visible light.
• assignment Ideal gas calculations

  assignment Homework

  Ideal gas calculations

  Ideal gas Entropy Sackur-Tetrode Thermal and Statistical Physics 2020

  Consider one mole of an ideal monatomic gas at 300K and 1 atm. First, let the gas expand isothermally and reversibly to twice the initial volume; second, let this be followed by an isentropic expansion from twice to four times the original volume.

  1. How much heat (in joules) is added to the gas in each of these two processes?

  2. What is the temperature at the end of the second process?

  3. Suppose the first process is replaced by an irreversible expansion into a vacuum, to a total volume twice the initial volume. What is the increase of entropy in the irreversible expansion, in J/K?

• assignment Fluctuations in a Fermi gas

  assignment Homework

  Fluctuations in a Fermi gas

  Fermi gas grand canonical ensemble statistical mechanics Thermal and Statistical Physics 2020 (K&K 7.11) Show for a single orbital of a fermion system that \begin{align} \left<(\Delta N)^2\right> = \left<N\right>(1+\left<N\right>) \end{align} if \(\left<N\right>\) is the average number of fermions in that orbital. Notice that the fluctuation vanishes for orbitals with energies far enough from the chemical potential \(\mu\) so that \(\left<N\right>=1\) or \(\left<N\right>=0\).
• assignment Pressure and entropy of a degenerate Fermi gas

  assignment Homework

  Pressure and entropy of a degenerate Fermi gas

  Fermi gas Pressure Entropy Thermal and Statistical Physics 2020

  1. Show that a Fermi electron gas in the ground state exerts a pressure \begin{align} p = \frac{\left(3\pi^2\right)^{\frac23}}{5} \frac{\hbar^2}{m}\left(\frac{N}{V}\right)^{\frac53} \end{align} In a uniform decrease of the volume of a cube every orbital has its energy raised: The energy of each orbital is proportional to \(\frac1{L^2}\) or to \(\frac1{V^{\frac23}}\).

  2. Find an expression for the entropy of a Fermi electron gas in the region \(kT\ll \varepsilon_F\). Notice that \(S\rightarrow 0\) as \(T\rightarrow 0\).

• assignment Extensive Internal Energy

  assignment Homework

  Extensive Internal Energy

  Energy and Entropy 2021 (2 years)

  Consider a system which has an internal energy \(U\) defined by: \begin{align} U &= \gamma V^\alpha S^\beta \end{align} where \(\alpha\), \(\beta\) and \(\gamma\) are constants. The internal energy is an extensive quantity. What constraint does this place on the values \(\alpha\) and \(\beta\) may have?

• assignment Mass Density

  assignment Homework

  Mass Density

  Static Fields 2023 (4 years) Consider a rod of length \(L\) lying on the \(z\)-axis. Find an algebraic expression for the mass density of the rod if the mass density at \(z=0\) is \(\lambda_0\) and at \(z=L\) is \(7\lambda_0\) and you know that the mass density increases

  • linearly;
  • like the square of the distance along the rod;
  • exponentially.
• Thermal and Statistical Physics 2020

  1. Consider a system that may be unoccupied with energy zero, or occupied by one particle in either of two states, one of energy zero and one of energy \(\varepsilon\). Find the Gibbs sum for this system is in terms of the activity \(\lambda\equiv e^{\beta\mu}\). Note that the system can hold a maximum of one particle.

  2. Solve for the thermal average occupancy of the system in terms of \(\lambda\).

  3. Show that the thermal average occupancy of the state at energy \(\varepsilon\) is \begin{align} \langle N(\varepsilon)\rangle = \frac{\lambda e^{-\frac{\varepsilon}{kT}}}{\mathcal{Z}} \end{align}

  4. Find an expression for the thermal average energy of the system.

  5. Allow the possibility that the orbitals at \(0\) and at \(\varepsilon\) may each be occupied each by one particle at the same time; Show that \begin{align} \mathcal{Z} &= 1 + \lambda + \lambda e^{-\frac{\varepsilon}{kT}} + \lambda^2 e^{-\frac{\varepsilon}{kT}} \\ &= (1+\lambda)\left(1+e^{-\frac{\varepsilon}{kT}}\right) \end{align} Because \(\mathcal{Z}\) can be factored as shown, we have in effect two independent systems.