Interdisciplinary Applied Mathematics

Скачать в pdf «Interdisciplinary Applied Mathematics»


f = exp(a + b • v + cbv2),


which is known as the Maxwellian distribution and represents an equilibrium state for number density n0 and temperature T0. It can be rewritten in the familiar form


fo = n 3/2noPi exp(—e2v2),    (15.8)


where we have defined



во



m


with kB = 1.38 05 x 10 23 J/K the Boltzmann constant, and m the molecular mass.


All the macroscopic quantities are defined in terms of the distribution function: for example,


Density


p(x,t) = m / f (x, v,t)dv


Bulk velocity


pu(x,t)



m



vf (x, v, t)dv


Temperature


T{x,t) =    J c2 f (x, v, t)dv,


where c = v u is the peculiar velocity.


The boundary conditions take into account the wall type via the nonnegative scattering kernel, representing a probability density


R(v‘ ^ v; x; t)


that molecules hitting the wall with velocity between v and v + dv at location x at time instance t will be reflected with velocity between v and v + dv. If R is known, then we can obtain the boundary condition for the distribution function as


f (x, v,t) Vn



H (—V‘n )v‘nR(v



v; x, t)f (x, v’, t)dv’,



(15.9)


where H(x) is the Heaviside step function, and vn = v • n is the velocity normal to the surface. If there is no adsorption on the wall surface, then

Скачать в pdf «Interdisciplinary Applied Mathematics»

Метки