2006
DOI: 10.1016/j.jcp.2005.06.016
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A shock-capturing SPH scheme based on adaptive kernel estimation

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Cited by 52 publications
(33 citation statements)
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“…Neither hydrodynamic nor particle based simulations can operate with point-like energy depositions and have therefore to choose a finite size injection region. For hydrodynamic codes it has been shown that the size and shape of this region can impact the density, velocity, and pressure evolution of the shock front [93,94]. The vanishingly small number densities at the center of the simulation space can be a challenge for codes operating with a finite number of particles as densities cannot become arbitrarily small [95].…”
Section: Sedov-taylor Testmentioning
confidence: 99%
“…Neither hydrodynamic nor particle based simulations can operate with point-like energy depositions and have therefore to choose a finite size injection region. For hydrodynamic codes it has been shown that the size and shape of this region can impact the density, velocity, and pressure evolution of the shock front [93,94]. The vanishingly small number densities at the center of the simulation space can be a challenge for codes operating with a finite number of particles as densities cannot become arbitrarily small [95].…”
Section: Sedov-taylor Testmentioning
confidence: 99%
“…The derivation of these symmetrizations are explained in [36]. In calculations of compressible flows involving the formation and propagation of shocks, an artificial viscosity term, P ij , must be added to the SPH equations to dissipate postshock oscillations in the solution and avoid particle interpenetration in high Mach number collisions.…”
Section: The Sph Equationsmentioning
confidence: 99%
“…It has also been incorporated into a standard Smoothed Particle Hydrodynamics (SPH) method to simulate conventional fluid dynamics yielding a substantial improvement on the stability of the calculations. In recent work [15], we have reported a variant of SPH method that allows for the simulation of compressible fluid with strong shocks and rarefaction waves in one and two dimensions. The known instabilities of the conventional scheme (the wall heating phenomena) virtually dissapear when adaptive kernels, as presented here, are implemented.…”
Section: Discussionmentioning
confidence: 99%