equipartition theorem
E57415
The equipartition theorem is a principle in classical statistical mechanics stating that, at thermal equilibrium, each independent quadratic degree of freedom of a system contributes an average energy of (1/2)kT.
Statements (51)
| Predicate | Object |
|---|---|
| instanceOf |
physical law
→
result in classical thermodynamics → theorem in statistical mechanics → |
| appliesTo |
classical systems
→
harmonic oscillator → ideal gas → molecules in a gas → solids in the classical limit → systems in thermal equilibrium → |
| assumes |
classical limit
→
continuous energy spectrum → thermal equilibrium → validity of classical mechanics → |
| concerns |
average energy
→
distribution of energy among degrees of freedom → thermal equilibrium properties → |
| contrastsWith |
quantum statistics
→
|
| energyPerDegreeOfFreedom |
(1/2)kT
→
|
| field |
classical mechanics
→
statistical mechanics → thermodynamics → |
| hasLimitation |
does not hold when energy levels are quantized and not thermally accessible
→
fails at low temperatures due to quantum effects → overestimates heat capacities of diatomic gases at room temperature → overestimates heat capacity of solids at low temperature → |
| historicallyAttributedTo |
James Clerk Maxwell
→
Ludwig Boltzmann → |
| implies |
Dulong–Petit law for molar heat capacity of many solids at high temperature
→
average translational kinetic energy per particle is (3/2)kT in three dimensions → each quadratic term in the Hamiltonian contributes (1/2)kT to the mean energy → heat capacity of a monatomic ideal gas is (3/2)Nk → internal energy of a monatomic ideal gas is (3/2)NkT → |
| mathematicallyBasedOn |
canonical ensemble average
→
classical Hamiltonian mechanics → phase space integrals → |
| relatedTo |
Boltzmann distribution
→
Dulong–Petit law → Maxwell–Boltzmann statistics → canonical ensemble → kinetic theory of gases → partition function → specific heat of gases → |
| statedAs |
each independent quadratic degree of freedom contributes an average energy of (1/2)kT
→
|
| usedFor |
approximating high-temperature behavior of solids
→
deriving ideal gas internal energy → estimating heat capacities → understanding molecular motion → |
| usesQuantity |
Boltzmann constant
→
absolute temperature → degree of freedom → |
| validWhen |
kT is large compared to energy level spacings
→
|
Referenced by (4)
| Subject (surface form when different) | Predicate |
|---|---|
|
Boltzmann constant
→
|
appearsIn |
|
Rayleigh–Jeans law at low frequencies
→
|
derivedFrom |
|
k_B
→
|
playsRoleIn |
|
Maxwell–Boltzmann statistics
→
|
relatedTo |