2009
DOI: 10.1016/j.jcp.2009.05.032
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Accuracy and stability in incompressible SPH (ISPH) based on the projection method and a new approach

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Cited by 551 publications
(417 citation statements)
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References 25 publications
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“…However, this method generally performs quite well for the solitary wave condition due to its ordered motion of the fluid particles during the single wave event. For the periodic waves, however, other types of models or more advanced source term treatments should be considered, such as documented by Hu and Adams (2007), Xu et al (2009) and Khayyer and Gotoh (2011).…”
Section: Solution Proceduresmentioning
confidence: 99%
“…However, this method generally performs quite well for the solitary wave condition due to its ordered motion of the fluid particles during the single wave event. For the periodic waves, however, other types of models or more advanced source term treatments should be considered, such as documented by Hu and Adams (2007), Xu et al (2009) and Khayyer and Gotoh (2011).…”
Section: Solution Proceduresmentioning
confidence: 99%
“…We additionally use the particle shifting technique (ISPH_DFS) from Xu et al (2009). The shifting was implemented at the end of the time step to overcome tensile instabilities which could for instance occur from a homogeneous Cartesian initial particle distribution or the change in interfacial area.…”
Section: Incompressibility Treatment and Time Integrationmentioning
confidence: 99%
“…The shifting was implemented at the end of the time step to overcome tensile instabilities which could for instance occur from a homogeneous Cartesian initial particle distribution or the change in interfacial area. The integration scheme can be found in the work of Xu et al (2009). …”
Section: Incompressibility Treatment and Time Integrationmentioning
confidence: 99%
“…(26) After fl uid fl ow determination, the mass transport equation (concentration) is solved as follows: (27) The time step ( ) is calculated as (28) where β t is a constant coeffi cient between 0 and 1, δ min is the minimum distance between two neighbouring particles, and V max is the maximum velocity magnitude of the particles. The boundary conditions that dominate the wall boundaries are the no slip condition for velocity and Neumann boundary conditions for mass diffusion.…”
Section: Solution Algorithmmentioning
confidence: 99%
“…Defects, tensile instability, and particle clustering are complications in SPH simulations. To avoid these unfavourable phenomena, a shifting algorithm similar to the particle shifting approach of Xu et al 27 was applied in the present study.…”
Section: Solution Algorithmmentioning
confidence: 99%