law

Boltzmann distribution

The Boltzmann distribution is a statistical law describing the probability distribution of particle energies in a system at thermal equilibrium.
15 related articles · 6 formulas · 2 who worked here

Description

Imagine a crowd of people on an escalator in the subway: there are always fewer people at the top because it’s harder to get there. In the world of atoms and molecules, a similar principle applies: the greater the energy of a state, the fewer molecules “climb” to that “energy floor.” The Boltzmann distribution is a mathematical rule that says the chance of finding a particle in a state with a given energy drops exponentially as the energy increases. It’s like having a mountain, and with height, the number of tourists would decrease according to a strict exponential law, determined by the steepness of the slope (the temperature).

History

L. Boltzmann began his research by extending Maxwell's (James Clerk Maxwell) distribution for an ideal gas to systems with an external field. In 1871, he formulated the general principle: if a system can be in discrete states, then its equilibrium distribution is determined only by energy and temperature. In 1877, he linked entropy to the logarithm of the number of microstates (the famous Boltzmann formula), which led to a deep understanding of the statistical nature of the second law of thermodynamics. In the 20th century, quantum mechanics expanded the application of the distribution, and Erwin Schrödinger in his lectures 'What is Life?' used it to explain order and disorder in biological systems.

How it works

The Boltzmann distribution works for classical and quantum systems in thermal equilibrium, when quantum exchange effects can be neglected (i.e., for 'distinguishable' particles in the classical limit). It describes the populations of energy levels of atoms and molecules in spectroscopy, impurity distributions in semiconductors, thermal ionization, diffusion. Limits of applicability: the distribution fails when Fermi–Dirac statistics (for fermions, e.g., electrons in metals at low temperatures) or Bose–Einstein statistics (for bosons, like photons) are important, where the Pauli principle or Bose condensation must be accounted for. It is also valid only in equilibrium; in non-equilibrium systems, populations may be different.

Fun fact

It is precisely because of the Boltzmann distribution that water evaporates at room temperature: the fastest molecules at the surface, having energy above average, can overcome the attraction and fly away. Moreover, this law explains why it’s hard to breathe at high altitudes: the density of air (the number of molecules at a given height in the gravitational field) drops exponentially with height — exactly according to Boltzmann, where the role of energy is played by gravitational potential energy.

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Formulas

$$f(x) \propto x^{-k}$$
A probability distribution following a power law.
What is in the formula
fvariableprobability density function — probability density function
xvariablerandom variable — random variable
kvariablepower law exponent — power law exponent
f(v)\proptov^{-5} · 2601.03344v2
$$\frac{N_i}{N} = \frac{g_i e^{-E_i/kT}}{Q}$$
Probability of a state in thermal equilibrium.
What is in the formula
N_ivariableNumber of particles in state i — particle number
NvariableTotal number of particles — particle number
g_ivariableDegeneracy of state i — degeneracy
E_ivariableEnergy of state i — energy joule
TvariableAbsolute temperature — temperature kelvin
kconstantRelates energy to temperature at the particle level — boltzmann constant = 1.380649e-23 joule per kelvin
e^{-E_i/kT}operatorExponential of the negative energy over kT — exponential function
\frac{n_u}{n_{{tot}}}=\frac{g_u}{q}e^{-e_u/kt} · 2606.03313v1
p(s)=\frac{1}{z(β)}\exp(-βe) · 2607.10285
$$BC(p,q) = \int \sqrt{p(x)q(x)} \, dx$$
Measures the overlap between two probability distributions.
What is in the formula
p(x)variableProbability density of distribution p — probability density
q(x)variableProbability density of distribution q — probability density
xvariableIntegration variable (sample space)
∫operatorIntegration over the sample space — integral operator
bc(p,q)=\int\sqrt{p(m)q(m)}dm · 2607.01121
$$P(v) = \sqrt{\frac{2}{\pi}} \frac{v^2}{\sigma^3} \exp\left(-\frac{v^2}{2\sigma^2}\right)$$
Probability distribution of speeds in an ideal gas.
What is in the formula
P(v)variableProbability density of speed v — probability density second per metre
vvariableSpeed of a particle — speed metre per second
σvariableScale parameter related to temperature — speed scale metre per second
expoperatorExponential function — exponential function
√operatorSquare root — square root
p(v_{{kick}})=\sqrt{\frac{2}{π}}\frac{v_{{kick}}^2}{σ_{{kick}}^3}\exp(-\frac{v_{{kick}}^2}{2σ_{{kick}}^2}) · 2607.02653v1
f(v)=\frac{1}{n}\exp(-\frac{v^2}{2σ_v^2})\theta(v_{\rmesc}-v) · 2607.20620v1
$$\langle n \rangle = \frac{1}{e^{\hbar\omega / k_B T} - 1}$$
Average occupation number for bosonic energy states.
What is in the formula
\langle n \ranglevariableAverage occupation number — occupation number
\omegavariableAngular frequency of the bosonic mode — angular frequency radian per second
TvariableAbsolute temperature — temperature kelvin
\hbarconstantReduced Planck constant, relating energy to angular frequency. — reduced planck constant = 1.054571817e-34 joule second
k_BconstantBoltzmann constant, relating temperature to energy. — boltzmann constant = 1.380649e-23 joule per kelvin
\bar{n}=\frac{1}{e^{ħω/k_bt}-1} · 2606.25834
$$S = k_B \ln W$$
Entropy is proportional to logarithm of states.
What is in the formula
SvariableEntropy of the system — entropy joule per kelvin
WvariableNumber of microstates — number of microstates
k_BconstantRelates energy to temperature at the particle level — boltzmann constant = 1.380649e-23 joule per kelvin
lnoperatorNatural logarithm — natural logarithm
δs=k_b\logd · 2607.02188

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