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== Abstract == | == Abstract == | ||
− | + | Non-Newtonian fluids and granular flows may be simulated as continuums with large time steps in the meshless Lagrangian context, using the novel method. -Coupling of non-Newtonian meshless Lagrangian Differencing Dynamics (LDD) flow solver and Finite Element Method (FEM) solver. -The flow solver is volume–conservative, second–order accurate, and works directly on triangulated geometry. | |
== Video == | == Video == | ||
{{#evt:service=cloudfront|id=276725|alignment=center|filename=1054.mp4}} | {{#evt:service=cloudfront|id=276725|alignment=center|filename=1054.mp4}} | ||
− | == | + | == Abstract == |
+ | <pdf>Media:Basic_et_al_2022a_3820_1054_abstract.pdf</pdf> | ||
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+ | == Full paper == | ||
<pdf>Media:Draft_Content_4327579381054_paper.pdf</pdf> | <pdf>Media:Draft_Content_4327579381054_paper.pdf</pdf> |
Non-Newtonian fluids and granular flows may be simulated as continuums with large time steps in the meshless Lagrangian context, using the novel method. -Coupling of non-Newtonian meshless Lagrangian Differencing Dynamics (LDD) flow solver and Finite Element Method (FEM) solver. -The flow solver is volume–conservative, second–order accurate, and works directly on triangulated geometry.
Published on 15/02/22
Accepted on 15/02/22
Submitted on 15/02/22
Volume IS17 - Particle Methods for Fluid-Structure Interactions, 2022
DOI: 10.23967/particles.2021.025
Licence: CC BY-NC-SA license
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