We consider a dilute gas of hard spheres in dimension d≥2 that upon
collision either annihilate with probability p or undergo an elastic
scattering with probability 1−p. For such a system neither mass, momentum,
nor kinetic energy are conserved quantities. We establish the hydrodynamic
equations from the Boltzmann equation description. Within the Chapman-Enskog
scheme, we determine the transport coefficients up to Navier-Stokes order, and
give the closed set of equations for the hydrodynamic fields chosen for the
above coarse grained description (density, momentum and kinetic temperature).
Linear stability analysis is performed, and the conditions of stability for the
local fields are discussed.Comment: 19 pages, 3 eps figures include