1964
DOI: 10.1063/1.1711368
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Shock Structure in a Simple Discrete Velocity Gas

Abstract: The structure of a shock wave in a simple discrete velocity gas—a gas in which the molecules move with a finite set of velocities—is discussed. The Boltzmann equation becomes, for this gas, a set of coupled differential equations which, in the present example, can be solved exactly. The solution describes an infinite Mach number shock in a gas consisting of hard elastic spheres. Although only six molecular velocities are considered, and the solution is easy to obtain, it compares remarkably well with those of … Show more

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Cited by 341 publications
(124 citation statements)
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“…The classical example to which these methods are applied and tested is the Broadwell model. 9 We will demonstrate that the GOL two-fluid model and resistive MHD are example systems that can be accurately solved using these methods. The significant benefits of this approach for the GOL case are as follows: the current density can be accurately solved on grids much larger than the elec-tron inertial length; the Hall term is locally implicit without the need for large linear system solves; the resistive term is also locally implicit; the treatment of the plasma-vacuum interface is physical and automatic; and the time step is usually limited by the cell transit time for waves moving at a reduced numerical speed of light.…”
Section: Introductionmentioning
confidence: 99%
“…The classical example to which these methods are applied and tested is the Broadwell model. 9 We will demonstrate that the GOL two-fluid model and resistive MHD are example systems that can be accurately solved using these methods. The significant benefits of this approach for the GOL case are as follows: the current density can be accurately solved on grids much larger than the elec-tron inertial length; the Hall term is locally implicit without the need for large linear system solves; the resistive term is also locally implicit; the treatment of the plasma-vacuum interface is physical and automatic; and the time step is usually limited by the cell transit time for waves moving at a reduced numerical speed of light.…”
Section: Introductionmentioning
confidence: 99%
“…We now consider the case when the vapor, gas A, is modeled by a six-velocity model with velocities (±1, 0) and (±1, ±1), and the non-condensable gas B is modelled by the classical Broadwell model [8] …”
Section: Exact Solution For a Reduced Six+four-velocity Modelmentioning
confidence: 99%
“…The Hardy-Pomeau model, a lattice version of a discrete velocity gas, 9,10 consists of indistinguishable articles moving on a two-dimensional lattice with four fixed velocities. Particles move and collide according to the following rules.…”
Section: Problem Formulationmentioning
confidence: 99%