FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2023353740> ?p ?o ?g. }

• W2023353740 endingPage "17" @default.
• W2023353740 startingPage "6" @default.
• W2023353740 abstract "This article presents an interface-energy-conserving coupling strategy for transient fluid–structure interaction. The solid sub-domain is discretized by finite element method with Newmark time integrator, whereas for the fluid sub-domain we use the mesh-less method SPH-ALE with 2nd order Runge–Kutta scheme. This paper proposes a method to impose a mean interface normal velocity continuity in such a way that the algorithmic interface energy is zero during the whole period of numerical simulation. This coupling method thus ensures that the coupled problem shall be stable in time. Secondly it will converge in time with the rate of convergence of the worst time integrator chosen for each problem. The proposed method is first applied to a mono-dimensional problem by which we investigate the phenomena of propagation of shock waves across the fluid–structure interface. A good agreement is observed between the numerical result and the analytical solution in the 1D shock wave propagation test cases. Finally, a multi-dimensional example is presented and compared to another coupling approach." @default.
• W2023353740 created "2016-06-24" @default.
• W2023353740 creator A5021850914 @default.
• W2023353740 creator A5023826377 @default.
• W2023353740 creator A5029736916 @default.
• W2023353740 creator A5078374631 @default.
• W2023353740 date "2014-11-01" @default.
• W2023353740 modified "2023-09-25" @default.
• W2023353740 title "Coupling of SPH-ALE method and finite element method for transient fluid–structure interaction" @default.
• W2023353740 cites W1968312755 @default.
• W2023353740 cites W1975332389 @default.
• W2023353740 cites W1979475531 @default.
• W2023353740 cites W1980365163 @default.
• W2023353740 cites W1980938760 @default.
• W2023353740 cites W1986772922 @default.
• W2023353740 cites W1990023626 @default.
• W2023353740 cites W2000734244 @default.
• W2023353740 cites W2003372231 @default.
• W2023353740 cites W2003919582 @default.
• W2023353740 cites W2020272655 @default.
• W2023353740 cites W2037319105 @default.
• W2023353740 cites W2054731935 @default.
• W2023353740 cites W2054758926 @default.
• W2023353740 cites W2069017037 @default.
• W2023353740 cites W2071187519 @default.
• W2023353740 cites W2071667005 @default.
• W2023353740 cites W2089245375 @default.
• W2023353740 cites W2100636165 @default.
• W2023353740 cites W2100710937 @default.
• W2023353740 cites W2102155928 @default.
• W2023353740 cites W2106615044 @default.
• W2023353740 cites W2112548197 @default.
• W2023353740 cites W2118786393 @default.
• W2023353740 cites W2121032832 @default.
• W2023353740 cites W2136898588 @default.
• W2023353740 cites W2147803399 @default.
• W2023353740 cites W2157906950 @default.
• W2023353740 cites W2550093246 @default.
• W2023353740 cites W3021622851 @default.
• W2023353740 doi "https://doi.org/10.1016/j.compfluid.2014.06.028" @default.
• W2023353740 hasPublicationYear "2014" @default.
• W2023353740 type Work @default.
• W2023353740 sameAs 2023353740 @default.
• W2023353740 citedByCount "24" @default.
• W2023353740 countsByYear W20233537402014 @default.
• W2023353740 countsByYear W20233537402015 @default.
• W2023353740 countsByYear W20233537402016 @default.
• W2023353740 countsByYear W20233537402017 @default.
• W2023353740 countsByYear W20233537402018 @default.
• W2023353740 countsByYear W20233537402019 @default.
• W2023353740 countsByYear W20233537402020 @default.
• W2023353740 countsByYear W20233537402021 @default.
• W2023353740 countsByYear W20233537402022 @default.
• W2023353740 countsByYear W20233537402023 @default.
• W2023353740 crossrefType "journal-article" @default.
• W2023353740 hasAuthorship W2023353740A5021850914 @default.
• W2023353740 hasAuthorship W2023353740A5023826377 @default.
• W2023353740 hasAuthorship W2023353740A5029736916 @default.
• W2023353740 hasAuthorship W2023353740A5078374631 @default.
• W2023353740 hasConcept C111919701 @default.
• W2023353740 hasConcept C121332964 @default.
• W2023353740 hasConcept C126322002 @default.
• W2023353740 hasConcept C131584629 @default.
• W2023353740 hasConcept C134306372 @default.
• W2023353740 hasConcept C135628077 @default.
• W2023353740 hasConcept C162324750 @default.
• W2023353740 hasConcept C191897082 @default.
• W2023353740 hasConcept C192562407 @default.
• W2023353740 hasConcept C2776257435 @default.
• W2023353740 hasConcept C2777303404 @default.
• W2023353740 hasConcept C2779126057 @default.
• W2023353740 hasConcept C2780799671 @default.
• W2023353740 hasConcept C2781300812 @default.
• W2023353740 hasConcept C28826006 @default.
• W2023353740 hasConcept C31258907 @default.
• W2023353740 hasConcept C33923547 @default.
• W2023353740 hasConcept C41008148 @default.
• W2023353740 hasConcept C50522688 @default.
• W2023353740 hasConcept C57879066 @default.
• W2023353740 hasConcept C70477161 @default.
• W2023353740 hasConcept C71924100 @default.
• W2023353740 hasConcept C73000952 @default.
• W2023353740 hasConcept C79518650 @default.
• W2023353740 hasConcept C97355855 @default.
• W2023353740 hasConceptScore W2023353740C111919701 @default.
• W2023353740 hasConceptScore W2023353740C121332964 @default.
• W2023353740 hasConceptScore W2023353740C126322002 @default.
• W2023353740 hasConceptScore W2023353740C131584629 @default.
• W2023353740 hasConceptScore W2023353740C134306372 @default.
• W2023353740 hasConceptScore W2023353740C135628077 @default.
• W2023353740 hasConceptScore W2023353740C162324750 @default.
• W2023353740 hasConceptScore W2023353740C191897082 @default.
• W2023353740 hasConceptScore W2023353740C192562407 @default.
• W2023353740 hasConceptScore W2023353740C2776257435 @default.
• W2023353740 hasConceptScore W2023353740C2777303404 @default.
• W2023353740 hasConceptScore W2023353740C2779126057 @default.
• W2023353740 hasConceptScore W2023353740C2780799671 @default.
• W2023353740 hasConceptScore W2023353740C2781300812 @default.

• next