2001
DOI: 10.1016/s0169-5983(01)00005-3
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Similarity solution for laser-driven shock waves in a particle-laden gas

Abstract: A similarity solution has been obtained for a laser-driven strong shock wave propagating in a mixture of gas and small solid particles. It is assumed that the equilibrium-ow condition is maintained and the variable laser energy is completely absorbed at the shock front according to a time-dependent power law. The similarity solution is valid for adiabatic ow as long as the e ect of the counter pressure is neglected. The e ects of a parameter characterising the various energy input of the blast wave on the simi… Show more

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Cited by 7 publications
(11 citation statements)
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“…This behaviour remains unaltered with the value of K > 0.349. (8) We conclude that with the non-idealness parameters and with the introduction of artificial viscosity (K = 0.00349, 0.0349 and 0.349) the excitation of oscillations in the molecules dampen and the smoothness in the profiles increases.…”
Section: Discussionmentioning
confidence: 79%
See 1 more Smart Citation
“…This behaviour remains unaltered with the value of K > 0.349. (8) We conclude that with the non-idealness parameters and with the introduction of artificial viscosity (K = 0.00349, 0.0349 and 0.349) the excitation of oscillations in the molecules dampen and the smoothness in the profiles increases.…”
Section: Discussionmentioning
confidence: 79%
“…The viscosity term suggested by is included into the hydrodynamic equations for spherically symmetric flow in magnetogasdynamics regime, can be written in Eulerian form [8,14,20,25,26,27] where r and t are independent space and time coordinates ρ, u, p, q and e are density, velocity, pressure, artificial viscosity and internal energy per unit mass respectively and h = µH 2 2 is the magnetic pressure, H and µ being magnetic field strength and the magnetic permeability respectively. The shock position is given by R s (t) and its velocity D = dR s (t)…”
Section: Formulation Of the Problemmentioning
confidence: 99%
“…Results are obtained for a spherical variable-energy wave over the complete physical range of possibilities for the energy-input parameter, from ÿ = 0 to an upper limit. Some of these results are compared with the adiabatic solutions presented in our previous paper (Gretler and Regenfelder, 2001).…”
Section: Introductionmentioning
confidence: 92%
“…Narasimhulu Naidu et al (1985) Laumbach and Probstein (1969). Recently, Gretler and Regenfelder (2001) provided a similarity solution for a laser-driven strong shock wave in a mixture of gas and small solid particles for adiabatic ow. As in the present study, this radiation-driven shock wave can be generated by a number of lasers focused on a common plane, line or point; a sudden breakdown at the centre of the irradiated region then causes an exploding plane, cylindrical or spherical shock wave.…”
Section: Introductionmentioning
confidence: 99%
“…The non-steady one dimensional flow is a function of two independent variables the time t and the space coordinate r. The conservation equations governing the flow can be written as [12,[16][17][18][19][20] @q @t þ u @q @r þ q @u @r þ ðm À 1Þqu r ¼ 0 ð1Þ @u @t þ u @u @r þ q À1 @p @r þ @h @r ¼ 0 ð2Þ @p @t þ u @p @r À a 2 @q @t þ u @q @r ¼ 0 ð3Þ…”
Section: Basic Equations and Boundary Conditionsmentioning
confidence: 99%