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Encyclopedia > Boltzmann equation

The Boltzmann equation describes the statistical distribution of particles in a fluid. It is one of the most important equations of non-equilibrium statistical mechanics, the area of statistical mechanics that deals with systems far from thermodynamic equilibrium; for instance, when there is an applied temperature gradient or electric field. The Boltzmann equation is used to study how a fluid transports physical quantities such as heat and current, and thus to derive transport-related properties such as electrical conductivity, Hall conductivity, viscosity, and thermal conductivity.


The Boltzmann equation is

where t denotes time, r position, and p momentum. F(r, t) is the force field acting on the particles in the fluid, and m is the mass of the particles. The term ∂f/∂t|coll on the right hand side describes the effect of collisions between particles, and has to be independently supplied; it is zero if the particles do not collide with one another. Finally, the quantity f(r, p, t), which is known as the distribution function, is defined as follows:

the mean number of particles with center of mass located within a small volume d³r near the point r, and momentum within a range d³p near p, at time t.

The quantity h is customarily inserted to make f a dimensionless quantity. For classical statistical mechanics, this is just a matter of convention, since it does not show up in the final results of calculations. For quantum statistical mechanics, one usually takes h to be Planck's constant, so that f stands for the occupancy of a cell in phase space delineated by the Heisenberg uncertainty principle.


The Boltzmann equation is also often used in the field of dynamics, especially galactic dynamics. A galaxy, under certain assumptions, may be approximated as a continuous fluid; its mass distribution is then represented by f. When the collision term is null, the equation is also named non-collisional Boltzmann equation; in galaxies, physical collisions between the stars are very rare, and the effect gravitational collisions can be neglected for times far longer than the age of the universe.


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Boltzmann






  Results from FactBites:
 
Boltzmann's Work in Statistical Physics (Stanford Encyclopedia of Philosophy) (12986 words)
However, Boltzmann's ideas on the precise relationship between the thermodynamical properties of macroscopic bodies and their microscopic constitution, and the role of probability in this relationship are involved and differed quite remarkably in different periods of his life.
Boltzmann is often portrayed as a staunch defender of the atomic view of matter, at a time when the dominant opinion in the German-speaking physics community, led by influential authors like Mach and Ostwald, disapproved of this view.
Actually, Boltzmann's subsequent work in gas theory in the next decade and a half was predominantly concerned with technical applications of his 1872 Boltzmann equation, in particular to gas diffusion and gas friction.
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