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


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