Two nondegenerate levels have energies 0 and ε with exp(−βε)=0.25. Find Z.
Answer and explanation
1.25
Add weights 1+0.25.
Subjects
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1.25
Add weights 1+0.25.
0.2
Divide the excited weight by total weight: 0.25/1.25.
g
There are g microstates at that energy, each contributing a Boltzmann weight.
3.5
Z=2×1+3×0.5.
Mean energy
Differentiating the canonical partition sum produces the weighted energy mean.
Individual weights need not sum to one. Dividing by Z ensures a valid probability distribution across all included microstates.
Credit Z as the normalization sum.
For a system at inverse temperature β=1/(kBT), the canonical probability of a microstate of energy E is exp(−βE)/Z.
Advanced universityFor a system at inverse temperature β=1/(kBT), the canonical probability of a microstate of energy E is exp(−βE)/Z.
Advanced universityGround energy is zero with degeneracy 1; the excited level has degeneracy g. Energies are measured from the ground state.
Advanced universityGround energy is zero with degeneracy 1; the excited level has degeneracy g. Energies are measured from the ground state.
Advanced universityThe probability refers to the whole excited level, including all its degenerate states.
Advanced universityThe probability refers to the whole excited level, including all its degenerate states.
Advanced universityUse the microcanonical equal-a-priori-probability model and a ratio of multiplicities.
Advanced universityUse the microcanonical equal-a-priori-probability model and a ratio of multiplicities.
Advanced universityConnect rotation, oscillations, central forces and continuous wave models.
Work with Gauss laws, electrical field models, thermodynamic laws and electromagnetic waves.
Compare relativistic measurement with quantum states, the Schrödinger equation and uncertainty.
Use Lagrangian and Hamiltonian methods, then interpret canonical ensembles.
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