Unit · year 3
CU-303 · Statistical Thermodynamics
Threads energy · quantum24 lectures5 results
Bridging molecular energy levels to bulk thermodynamic properties.
Lectures
| L01 | The Programme: From Molecules to Bulk Properties — |
| L02 | Microstates and Configurations — |
| L03 | The Boltzmann Distribution |
| L04 | Deriving the Boltzmann Distribution |
| L05 | Temperature as a Population Ratio |
| L06 | The Molecular Partition Function |
| L07 | Interpreting q as Accessible States |
| L08 | The Translational Partition Function |
| L09 | The Rotational Partition Function |
| L10 | The Vibrational Partition Function |
| L11 | The Electronic Partition Function |
| L12 | Factorising the Total Partition Function |
| L13 | Internal Energy from q |
| L14 | Heat Capacity from Energy Levels |
| L15 | The Vibrational Contribution to Cv |
| L16 | The Equipartition Theorem |
| L17 | Where Equipartition Fails |
| L18 | The Statistical Definition of Entropy |
| L19 | The Boltzmann Entropy Formula |
| L20 | Residual Entropy |
| L21 | Free Energy from the Partition Function |
| L22 | Equilibrium Constants from Partition Functions |
| L23 | The Statistical Basis of Transition State Theory — |
| L24 | Synthesis: The Bridge from Levels to Thermodynamics |
Results in this unit
T-082
The molecular partition function
The bridge from energy levels to thermodynamics.
T-083
The Boltzmann distribution of populations
How molecules populate available energy levels.
T-084
The equipartition theorem
An average of (1/2)kT per quadratic degree of freedom.
T-085
The statistical definition of entropy
Boltzmann's S = k ln W.
T-086
Heat capacity from energy levels
The Einstein and Debye models of solids.