Boltzmann equation

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Boltzmann equation

An equation derived by the Austrian physicist Ludwig Boltzmann in the 1870s that shows how the distribution of molecules, atoms, or ions in their various energy levels depends on the temperature of the system; the system is in thermal equilibrium, with excitation balanced by de-excitation. The equation gives the ratio of the number density (number per unit volume) of molecules, atoms, or ions, N 2, in one energy level to the number density, N 1, in another lower energy level as
N 2 /N 1 = (g 2 /g 1 )eE/kT

g 1 and g 2 are the degeneracies of the two levels, i.e. the multiplicity of energy levels with the same energy, E is the energy required to excite the molecule, atom, or ion from the lower to the higher energy level, k is the Boltzmann constant, and T is the thermodynamic temperature. Thus as T increases a greater number of species will become excited.

The Boltzmann equation together with the Saha ionization equation are widely used to interpret the absorption and emission spectra of stars and to determine stellar temperatures and densities.

Boltzmann (Kinetic) Equation


an equation for the distribution function f(v, r, t) of gas molecules in the velocities ν and coordinates r (as functions of time t) that describes nonequilibrium processes in gases of low density. The function f determines the average number of particles having velocities within a small range from ν to ν + Δν and coordinates within a small range from r to r + Δr. If the distribution function depends only on the coordinate x and the velocity component vx, then the Boltzmann (kinetic) equation has the form

where m is the mass of the particle. The rate of change of the distribution function is characterized by the partial derivative ∂f/∂t. The second term in the equation, which is proportional to the partial derivative of the distribution function with respect to the coordinate, takes account of the change in f as a result of the movement of particles in space. The third term determines the change in the distribution function owing to the action of external forces F. The term on the right-hand side of the equation, which characterizes the rate of change of the distribution function owing to collisions between particles, depends on f and the nature of the forces of interaction between particles and is equal to

Here, f, f1, and fʹ, f1ʹ are the distribution functions of the molecules before and after collision, respectively; v, v1 are the velocities of the molecules before collision; and dσ =σdΩ is the differential effective scattering cross section into the solid angle dΩ (in the laboratory coordinate system) dependent on the law of molecular interaction. When molecules are simulated by rigid elastic spheres (of radius R), σ = 4R2 cos θ, where θ is the angle between the relative velocity v1 - v of the colliding molecules and the line connecting its centers. The kinetic equation was derived by L. Boltzmann in 1872.

Various generalizations of the Boltzmann kinetic equation describe the behavior of electron gas in metals, of phonons in crystal lattices, and so forth (however, these equations are often called simply kinetic equations, or transport equations).


References in periodicals archive ?
These glancing collisions turn out to be dominant type of collision for the full Boltzmann equation with long-range interactions.
Physically, since the Boltzmann equation describes the balancing of particle transfer, by solving for all the moments at a spatial node first, this relaxation somewhat enforces a local balancing of particle transfer at each spatial node.
This simplified form of the Boltzmann equation is obtained by assuming the approximate energy separatibility of and taking a truncated Legendre series expansion of [[sigma].
n] discretizations of the Boltzmann equation lead to non-symmetric linear systems that are difficult to solve efficiently, and standard Galerkin [P.
Thus, one obtains a scheme for solving the full multi-group, anisotropic scattering Boltzmann equation by using an outer block Gauss-Seidel iteration over the groups.
To derive the continuity equation of a phase, the Boltzmann equation is multiplied by the characteristic mass of the phase and is integrated over the velocity space.
By weighting the Boltzmann equation of each phase by property parameters and integrating over the velocity space, the continuity and momentum equations are derived.
By multiplying the k-phase Boltzmann equation by appropriate property parameters and integrating over the velocity space, the continuity and momentum equations are obtained.
First, the importance function is unknown; the Schrodinger equation doesn't let you calculate the interaction potential as easily as the Boltzmann equation does.
The begin by describing plasma and its classification, then examine the phenomenological description of the charged vehicle transport, macroscopic plasma characteristics, elementary processes in the gas phase and on surfaces, the Boltzmann equation and transport equations of charged particles, general properties of charges particle transport in gases, modeling of nonequilibrium (low-temperature) plasmas, the numerical procedure of modeling, capacity coupled plasma, inductively coupled plasma, magnetically enhanced plasma and plasma processing and related topics.
Other sections present work on direct numerical solution of the Boltzmann equation, microflows, granular gases, molecular beams, and gas phase molecular collision dynamics.