Moving particle semi-implicit method: Difference between revisions

Revision as of 19:26, 26 December 2016

Revision as of 19:30, 26 December 2016

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==Improvements==

Improved versions of MPS method have been proposed for enhancement of numerical stability (e.g. [http://www3.interscience.wiley.com/journal/2910/abstract Koshizuka et al., 1998]; [http://dx.doi.org/10.1002/fld.1106 Zhang et al., 2005]; [http://dx.doi.org/10.1016/j.fluiddyn.2005.12.002 Ataie-Ashtiani and Farhadi, 2006];[http://dx.doi.org/10.1002/fld.2132 Shakibaeina and Jin, 2009] ), momentum conservation (e.g. Hamiltonian MPS by [http://dx.doi.org/10.1016/j.cma.2006.12.006 Suzuki et al., 2007]; Corrected MPS by [http://dx.doi.org/10.1142/S0578563408001788 Khayyer and Gotoh, 2008]), mechanical energy conservation (e.g. Hamiltonian MPS by [http://dx.doi.org/10.1016/j.cma.2006.12.006 Suzuki et al., 2007]) and, pressure calculation (e.g. [http://dx.doi.org/10.1016/j.coastaleng.2008.10.004 Khayyer and Gotoh, 2009], [http://dx.doi.org/10.1002/fld.2207 Kondo and Koshizuka, 2010], [http://dx.doi.org/10.1016/j.apor.2010.01.001 Khayyer and Gotoh, 2010]), and for simulation of multiphase and granular flows ([http://ascelibrary.org/doi/10.1061/%28ASCE%29HY.1943-7900.0001275 Nabian and Farhadi 2016]).

== References ==