FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W1764872018> ?p ?o ?g. }

• W1764872018 endingPage "407" @default.
• W1764872018 startingPage "391" @default.
• W1764872018 abstract "In our recent work (Zhang et al., 2015), a Particulate Immersed Boundary Method (PIBM) for simulating fluid-particle multiphase flow was proposed and assessed in both two- and three-dimensional applications. In this study, the PIBM was extended to solve thermal interaction problems between spherical particles and fluid. The Lattice Boltzmann Method (LBM) was adopted to solve the fluid flow and temperature fields, the PIBM was responsible for the no-slip velocity and temperature boundary conditions at the particle surface, and the kinematics and trajectory of the solid particles were evaluated by the Discrete Element Method (DEM). Four case studies were implemented to demonstrate the capability of the current coupling scheme. Firstly, numerical simulation of natural convection in a two-dimensional square cavity with an isothermal concentric annulus was carried out for verification purpose. The current results were found to have good agreement with previous references. Then, sedimentation of two-and three-dimensional isothermal particles in fluid was numerically studied, respectively. The instantaneous temperature distribution in the cavity was captured. The effect of the thermal buoyancy on particle behaviors was discussed. Finally, sedimentation of three-dimensional thermosensitive particles in fluid was numerically investigated. Our results revealed that the LBM–PIBM–DEM is a promising scheme for the solution of complex fluid–particle interaction problems with heat transfer." @default.
• W1764872018 created "2016-06-24" @default.
• W1764872018 creator A5033171768 @default.
• W1764872018 creator A5039741784 @default.
• W1764872018 creator A5046909351 @default.
• W1764872018 creator A5047486115 @default.
• W1764872018 creator A5049341927 @default.
• W1764872018 creator A5091808332 @default.
• W1764872018 date "2016-01-01" @default.
• W1764872018 modified "2023-10-14" @default.
• W1764872018 title "Particulate Immersed Boundary Method for complex fluid–particle interaction problems with heat transfer" @default.
• W1764872018 cites W1060040552 @default.
• W1764872018 cites W1753933271 @default.
• W1764872018 cites W1964024479 @default.
• W1764872018 cites W1971387704 @default.
• W1764872018 cites W1972478448 @default.
• W1764872018 cites W1978300980 @default.
• W1764872018 cites W1992773065 @default.
• W1764872018 cites W1997987658 @default.
• W1764872018 cites W2016807555 @default.
• W1764872018 cites W2019667677 @default.
• W1764872018 cites W2022180204 @default.
• W1764872018 cites W2029177009 @default.
• W1764872018 cites W2030325934 @default.
• W1764872018 cites W2031257337 @default.
• W1764872018 cites W2041548211 @default.
• W1764872018 cites W2049842481 @default.
• W1764872018 cites W2059428790 @default.
• W1764872018 cites W2064320404 @default.
• W1764872018 cites W2066432247 @default.
• W1764872018 cites W2067647683 @default.
• W1764872018 cites W2069396006 @default.
• W1764872018 cites W2077488657 @default.
• W1764872018 cites W2081104114 @default.
• W1764872018 cites W2085612763 @default.
• W1764872018 cites W2088732779 @default.
• W1764872018 cites W2092701343 @default.
• W1764872018 cites W2095006601 @default.
• W1764872018 cites W2100992688 @default.
• W1764872018 cites W2119133219 @default.
• W1764872018 cites W2143475401 @default.
• W1764872018 cites W2154894521 @default.
• W1764872018 cites W2166950647 @default.
• W1764872018 cites W2180496922 @default.
• W1764872018 cites W2333413506 @default.
• W1764872018 cites W2504044668 @default.
• W1764872018 cites W4246155273 @default.
• W1764872018 doi "https://doi.org/10.1016/j.camwa.2015.12.003" @default.
• W1764872018 hasPublicationYear "2016" @default.
• W1764872018 type Work @default.
• W1764872018 sameAs 1764872018 @default.
• W1764872018 citedByCount "16" @default.
• W1764872018 countsByYear W17648720182017 @default.
• W1764872018 countsByYear W17648720182018 @default.
• W1764872018 countsByYear W17648720182019 @default.
• W1764872018 countsByYear W17648720182020 @default.
• W1764872018 countsByYear W17648720182021 @default.
• W1764872018 countsByYear W17648720182022 @default.
• W1764872018 crossrefType "journal-article" @default.
• W1764872018 hasAuthorship W1764872018A5033171768 @default.
• W1764872018 hasAuthorship W1764872018A5039741784 @default.
• W1764872018 hasAuthorship W1764872018A5046909351 @default.
• W1764872018 hasAuthorship W1764872018A5047486115 @default.
• W1764872018 hasAuthorship W1764872018A5049341927 @default.
• W1764872018 hasAuthorship W1764872018A5091808332 @default.
• W1764872018 hasBestOaLocation W17648720181 @default.
• W1764872018 hasConcept C111368507 @default.
• W1764872018 hasConcept C121332964 @default.
• W1764872018 hasConcept C121704545 @default.
• W1764872018 hasConcept C127313418 @default.
• W1764872018 hasConcept C134306372 @default.
• W1764872018 hasConcept C178790620 @default.
• W1764872018 hasConcept C185592680 @default.
• W1764872018 hasConcept C24245907 @default.
• W1764872018 hasConcept C2778517922 @default.
• W1764872018 hasConcept C33923547 @default.
• W1764872018 hasConcept C50517652 @default.
• W1764872018 hasConcept C57879066 @default.
• W1764872018 hasConcept C62354387 @default.
• W1764872018 hasConceptScore W1764872018C111368507 @default.
• W1764872018 hasConceptScore W1764872018C121332964 @default.
• W1764872018 hasConceptScore W1764872018C121704545 @default.
• W1764872018 hasConceptScore W1764872018C127313418 @default.
• W1764872018 hasConceptScore W1764872018C134306372 @default.
• W1764872018 hasConceptScore W1764872018C178790620 @default.
• W1764872018 hasConceptScore W1764872018C185592680 @default.
• W1764872018 hasConceptScore W1764872018C24245907 @default.
• W1764872018 hasConceptScore W1764872018C2778517922 @default.
• W1764872018 hasConceptScore W1764872018C33923547 @default.
• W1764872018 hasConceptScore W1764872018C50517652 @default.
• W1764872018 hasConceptScore W1764872018C57879066 @default.
• W1764872018 hasConceptScore W1764872018C62354387 @default.
• W1764872018 hasFunder F4320321001 @default.
• W1764872018 hasFunder F4320322930 @default.
• W1764872018 hasFunder F4320335473 @default.
• W1764872018 hasIssue "1" @default.
• W1764872018 hasLocation W17648720181 @default.
• W1764872018 hasLocation W17648720182 @default.

• next