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An Introduction to the Boltzmann Equation and Transport by Gilberto M. Kremer

By Gilberto M. Kremer

This e-book offers with the classical kinetic concept of gases. Its target is to offer the elemental rules of this concept inside of an uncomplicated framework and from a extra rigorous method in accordance with the Boltzmann equation. the topics are offered in a self-contained demeanour such that the readers can comprehend and study a few tools utilized in the kinetic concept of gases so one can examine the Boltzmann equation.

It is predicted that this e-book will be necessary as a textbook for college students and researchers who're attracted to the foundations of the Boltzmann equation and within the tools utilized in the kinetic conception of gases.

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Extra info for An Introduction to the Boltzmann Equation and Transport Processes in Gases

Example text

2 Molecular Structure of a Gas 19 15 k λ ≈ . 48) follows from a more elaborated kinetic theory based on the Boltzmann equation. The diffusion is a process which follows from the thermal motion of the molecules of a gas mixture, when mass transfer from one region to another occurs due to the existence of density gradients of its constituents. The self-diffusion happens in mixtures where the molecules of the constituents have practically the same characteristics, like the isotopes of some element. Consider a situation where a gas is confined between two fixed parallel plates which are at same temperature, and suppose that the plate at x3 = 0 has a particle number density smaller than the one at x3 = L.

Furthermore, suppose two molecules of a rarefied gas with asymptotic precollisional velocities denoted by (c, c1 ), while (c , c1 ) refer to their asymptotic post-collisional velocities. The subindex 1 was introduced only to differ the two molecules which participate in the binary encounter. The relative preand post-collisional velocities are defined, respectively, by g = c1 − c and g = c1 − c . 72) yields m¨ ri1 + m¨ ri2 = 0. 75) mc + mc1 = mc + mc1 . 4 Dynamics of a Binary Collision 27 ∂Φ r , ∂r r where μ = m/2 represents the reduced mass.

FN (x1 , . . , x˙ N , t) dx1 . . dx˙ N = 1. 33) Moreover, due to the fact that the molecules of the gas are undistinguishable, FN is considered a symmetric function of all pairs (xα , x˙ α ) and for all α = 1, 2, · · · , N . From the distribution function FN , one can define another distribution function Fn such that Fn (x1 , . . , x˙ n , t) dx1 . . dx˙ n = FN (x1 , . . , x˙ N , t) dxn+1 . . dx˙ N dx1 . . 34) gives the probability to find, at time t, n molecules with position vectors within the range xα and xα + dxα and with velocity vectors within the range x˙ α and x˙ α + dx˙ α , (α = 1, 2, .

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