A higher order Laplacian model for enhancement and stabilization of pressure calculation by the MPS method
By Abbas Khayyer, Hitoshi Gotoh. 2010
268 citations recorded by the source corpus.
Subfields: Computational Mechanics, Materials Chemistry, Mechanics of Materials
View Paper: https://www.semanticscholar.org/paper/6d7b2ccefc903d2dff573ca47d435e22e67f4c59
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In Computational Mechanics
In Materials Chemistry
In Mechanics of Materials
Citations in the corpus
- Meshfree Methods: Progress Made after 20 Years (2017, unknown): “More recently, several stability enhancements have been proposed for this method (Ataie-Ashtiani and Farhadi 2006; Khayyer and Gotoh 2010, 2011; Kondo and Koshizuka 2011).”
- Least squares moving particle semi-implicit method (2014, methodology): “For instance, Khayyer–Gotoh gradient operator anti-symmetrization [42], Khayyer–Gotoh divergence operator correction [43], Khayyer–Gotoh Laplace operator correction [44], Khayyer– Gotoh gradient operator correction [45], and Suzuki gradient operator correction [39,91] are proposed.”
- Enhancement of stability and accuracy of the moving particle semi-implicit method (2011, methodology): “Gotoh [21] provides a concise review on the current state-of-the-art of particle methods and highlights the key issues for enhancements and practical applications of these relatively new computational methods.”
- A review on approaches to solving Poisson’s equation in projection-based meshless methods for modelling strongly nonlinear water waves (2016, methodology): “…have been developed and reported in literature, such as the moving particle semi-implicit method (MPS) (e.g. Koshizuka 1996; Gotoh and Sakai 2006; Khayyer and Gotoh 2010), the smooth particle hydrodynamic method (SPH) (e.g. Monaghan 1994; Shao et al. 2006; Khayyer et al. 2008; Lind et al. 2012),…”
- Current achievements and future perspectives for projection-based particle methods with applications in ocean engineering (2016, methodology): “4) by HS (higher order source; Khayyer and Gotoh 2009a) and HL (higher order Laplacian; Khayyer and Gotoh 2010b, 2012) schemes are conducted as follows: ( Dn Dt )∗ i = ∑ j =i ( ∂wi j ∂ri j ) r i j · u∗i j∣∣r i j ∣∣ (5) 〈 ∇2 pk+1 〉 i = 1 n0 ∑ j =i { ∂pi j ∂ri j ∂wi j ∂ri j + pi j ( ∂2wi j ∂r2i j +…”