Matches in SemOpenAlex for { <https://semopenalex.org/work/W2060565566> ?p ?o ?g. }
Showing items 1 to 95 of
95
with 100 items per page.
- W2060565566 endingPage "163" @default.
- W2060565566 startingPage "154" @default.
- W2060565566 abstract "In nuclear safety, some severe accident scenarios lead to the presence of fission products in aerosol form in the closed containment atmosphere. It is important to understand the particle depletion process to estimate the risk of a release of radioactivity to the environment should a containment break occur. As a model for the containment, we use the three-dimensional differentially heated cavity problem. The differentially heated cavity is a cubical box with a hot wall and a cold wall on vertical opposite sides. On the other walls of the cube we have adiabatic boundary conditions. For the velocity field the no-slip boundary condition is applied. The flow of the air in the cavity is described by the Boussinesq equations. The method used to simulate the turbulent flow is the large eddy simulation (LES) where the dynamics of the large eddies is resolved by the computational grid and the small eddies are modelled by the introduction of subgrid scale quantities using a filter function. Particle trajectories are computed using the Lagrangian particle tracking method, including the relevant forces (drag, gravity, thermophoresis). Four different sets with each set containing one million particles and diameters of 10 μm, 15 μm, 25 μm and 35 μm are simulated. Simulation results for the flow field and particle sizes from 15 μm to 35 μm are compared to previous results from direct numerical simulation (DNS). The integration time of the LES is three times longer and the smallest particles have been simulated only in the LES. Particle statistics in the LES and the DNS were similar and the settling rates were practically identical. It was found that for this type of flow no model was necessary for the influence of the unresolved flow scales on the particle motions. This can be explained by the dominant nature of gravity settling compared to turbophoresis which is negligible for the particle sizes of the present study." @default.
- W2060565566 created "2016-06-24" @default.
- W2060565566 creator A5017981929 @default.
- W2060565566 creator A5035899744 @default.
- W2060565566 creator A5059513669 @default.
- W2060565566 creator A5063055552 @default.
- W2060565566 creator A5086906586 @default.
- W2060565566 date "2014-02-01" @default.
- W2060565566 modified "2023-09-27" @default.
- W2060565566 title "Large eddy simulation of particulate flow inside a differentially heated cavity" @default.
- W2060565566 cites W1600383739 @default.
- W2060565566 cites W1977322360 @default.
- W2060565566 cites W1983876043 @default.
- W2060565566 cites W1990794270 @default.
- W2060565566 cites W2002076392 @default.
- W2060565566 cites W2003408966 @default.
- W2060565566 cites W2005058545 @default.
- W2060565566 cites W2011808401 @default.
- W2060565566 cites W2018127490 @default.
- W2060565566 cites W2021132569 @default.
- W2060565566 cites W2029401646 @default.
- W2060565566 cites W2042943462 @default.
- W2060565566 cites W2044665398 @default.
- W2060565566 cites W2053996479 @default.
- W2060565566 cites W2054946417 @default.
- W2060565566 cites W2056651346 @default.
- W2060565566 cites W2062712788 @default.
- W2060565566 cites W2066641324 @default.
- W2060565566 cites W2070147180 @default.
- W2060565566 cites W2086209713 @default.
- W2060565566 cites W2089442232 @default.
- W2060565566 cites W2090421213 @default.
- W2060565566 cites W2111162544 @default.
- W2060565566 cites W2116365626 @default.
- W2060565566 cites W2145617321 @default.
- W2060565566 cites W2154570448 @default.
- W2060565566 cites W2155532339 @default.
- W2060565566 cites W2178382472 @default.
- W2060565566 doi "https://doi.org/10.1016/j.nucengdes.2013.12.035" @default.
- W2060565566 hasPublicationYear "2014" @default.
- W2060565566 type Work @default.
- W2060565566 sameAs 2060565566 @default.
- W2060565566 citedByCount "9" @default.
- W2060565566 countsByYear W20605655662015 @default.
- W2060565566 countsByYear W20605655662016 @default.
- W2060565566 countsByYear W20605655662017 @default.
- W2060565566 countsByYear W20605655662018 @default.
- W2060565566 countsByYear W20605655662021 @default.
- W2060565566 countsByYear W20605655662022 @default.
- W2060565566 crossrefType "journal-article" @default.
- W2060565566 hasAuthorship W2060565566A5017981929 @default.
- W2060565566 hasAuthorship W2060565566A5035899744 @default.
- W2060565566 hasAuthorship W2060565566A5059513669 @default.
- W2060565566 hasAuthorship W2060565566A5063055552 @default.
- W2060565566 hasAuthorship W2060565566A5086906586 @default.
- W2060565566 hasConcept C121332964 @default.
- W2060565566 hasConcept C121448008 @default.
- W2060565566 hasConcept C18903297 @default.
- W2060565566 hasConcept C192562407 @default.
- W2060565566 hasConcept C196558001 @default.
- W2060565566 hasConcept C24245907 @default.
- W2060565566 hasConcept C38349280 @default.
- W2060565566 hasConcept C57879066 @default.
- W2060565566 hasConcept C86803240 @default.
- W2060565566 hasConceptScore W2060565566C121332964 @default.
- W2060565566 hasConceptScore W2060565566C121448008 @default.
- W2060565566 hasConceptScore W2060565566C18903297 @default.
- W2060565566 hasConceptScore W2060565566C192562407 @default.
- W2060565566 hasConceptScore W2060565566C196558001 @default.
- W2060565566 hasConceptScore W2060565566C24245907 @default.
- W2060565566 hasConceptScore W2060565566C38349280 @default.
- W2060565566 hasConceptScore W2060565566C57879066 @default.
- W2060565566 hasConceptScore W2060565566C86803240 @default.
- W2060565566 hasLocation W20605655661 @default.
- W2060565566 hasLocation W20605655662 @default.
- W2060565566 hasLocation W20605655663 @default.
- W2060565566 hasOpenAccess W2060565566 @default.
- W2060565566 hasPrimaryLocation W20605655661 @default.
- W2060565566 hasRelatedWork W140364542 @default.
- W2060565566 hasRelatedWork W2008830759 @default.
- W2060565566 hasRelatedWork W2075826007 @default.
- W2060565566 hasRelatedWork W2077895587 @default.
- W2060565566 hasRelatedWork W2379432499 @default.
- W2060565566 hasRelatedWork W2918007473 @default.
- W2060565566 hasRelatedWork W2971066193 @default.
- W2060565566 hasRelatedWork W3082698993 @default.
- W2060565566 hasRelatedWork W4206459880 @default.
- W2060565566 hasRelatedWork W176200520 @default.
- W2060565566 hasVolume "267" @default.
- W2060565566 isParatext "false" @default.
- W2060565566 isRetracted "false" @default.
- W2060565566 magId "2060565566" @default.
- W2060565566 workType "article" @default.