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Concentration field of particles ejected into a nonhomogeneous atmosphere by a moving source
Authors:V P Kabashnikov
Affiliation:(1) Institute of Physics, Academy of Sciences of the Belorussian SSR, Minsk
Abstract:We obtain and analyze analytical expressions describing the space-time evolution of the density of solid particles ejected into the atmosphere.Nomenclature f velocity distribution function of particles (depends on position and time) - t time - x position vector referenced to an earth-fixed coordinate system - x1 and x2 horizontal plane with xbottom perpendicular to the trajectory plane - x3 vertical coordinate - xs position vector of the aircraft (source of particles) - v particle velocity - a particle acceleration due to braking in the atmosphere - g acceleration due to gravity - gamma reciprocal of the velocity relaxation time - H scale height of the atmosphere - F(v) initial velocity distribution function - B(t) defined by (8) - Q(t) mass flow rate of particles - rgr(t, x) density of particles created by a continuous source - rgro(t, xding780, x0) density of particles created by an instantaneous point source at the point xu - agr angle of the trajectory to the horizontal - Vs velocity of the aircraft - Va velocity of the exhaust gases at the nozzle exit plane - Fbottom initial distribution function for the transverse components of the velocity - R transverse dimension of the exhaust trail - t* time up to which one can neglect the effect of gravity - v 3 * characteristic value of the vertical velocity - vbottom characteristic value of the initial transverse velocity - Gamma determined by (17) - L determined by (43) Translated from Inzhenerno-Fizicheskii Zhurnal,58, No. 4, pp. 561–566, April, 1990.
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