FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2904103069> ?p ?o ?g. }

• W2904103069 endingPage "440" @default.
• W2904103069 startingPage "419" @default.
• W2904103069 abstract "Previous direct numerical simulations (DNS) of mass transfer across the air–water interface have been limited to low-intensity turbulent flow with turbulent Reynolds numbers of $R_{T}leqslant 500$ . This paper presents the first DNS of low-diffusivity interfacial mass transfer across a clean surface driven by high-intensity ( $1440leqslant R_{T}leqslant 1856$ ) isotropic turbulent flow diffusing from below. The detailed results, presented here for Schmidt numbers $Sc=20$ and $500$ , support the validity of theoretical scaling laws and existing experimental data obtained at high $R_{T}$ . In the DNS, to properly resolve the turbulent flow and the scalar transport at $Sc=20$ , up to $524times 10^{6}$ grid points were needed, while $65.5times 10^{9}$ grid points were required to resolve the scalar transport at $Sc=500$ , which is typical for oxygen in water. Compared to the low- $R_{T}$ simulations, where turbulent mass flux is dominated by large eddies, in the present high- $R_{T}$ simulation the contribution of small eddies to the turbulent mass flux was confirmed to increase significantly. Consequently, the normalised mass transfer velocity was found to agree with the $R_{T}^{-1/4}$ scaling, as opposed to the $R_{T}^{-1/2}$ scaling that is typical for low- $R_{T}$ simulations. At constant $R_{T}$ , the present results show that the mass transfer velocity $K_{L}$ scales with $Sc^{-1/2}$ , which is identical to the scaling found in the large-eddy regime for $R_{T}leqslant 500$ . As previously found for a no-slip interface, also for a shear-free interface the critical $R_{T}$ separating the large- from the small-eddy regime was confirmed to be approximately $R_{T}=500$ ." @default.
• W2904103069 created "2018-12-22" @default.
• W2904103069 creator A5037121668 @default.
• W2904103069 creator A5081905613 @default.
• W2904103069 date "2018-12-07" @default.
• W2904103069 modified "2023-09-26" @default.
• W2904103069 title "Simulation of air–water interfacial mass transfer driven by high-intensity isotropic turbulence" @default.
• W2904103069 cites W1973504909 @default.
• W2904103069 cites W1979176272 @default.
• W2904103069 cites W1997961774 @default.
• W2904103069 cites W2004791468 @default.
• W2904103069 cites W2008926704 @default.
• W2904103069 cites W2010871141 @default.
• W2904103069 cites W2010957824 @default.
• W2904103069 cites W2010971513 @default.
• W2904103069 cites W2012073402 @default.
• W2904103069 cites W2031914890 @default.
• W2904103069 cites W2045849310 @default.
• W2904103069 cites W2046110872 @default.
• W2904103069 cites W2046445604 @default.
• W2904103069 cites W2047284939 @default.
• W2904103069 cites W2047579283 @default.
• W2904103069 cites W2051713476 @default.
• W2904103069 cites W2052966285 @default.
• W2904103069 cites W2055960739 @default.
• W2904103069 cites W2058934915 @default.
• W2904103069 cites W2075215700 @default.
• W2904103069 cites W2077036659 @default.
• W2904103069 cites W2082544677 @default.
• W2904103069 cites W2096128105 @default.
• W2904103069 cites W2102288689 @default.
• W2904103069 cites W2103898010 @default.
• W2904103069 cites W2112251633 @default.
• W2904103069 cites W2113780917 @default.
• W2904103069 cites W2114736234 @default.
• W2904103069 cites W2140482043 @default.
• W2904103069 cites W2141412152 @default.
• W2904103069 cites W2142970957 @default.
• W2904103069 cites W2152179664 @default.
• W2904103069 cites W2157705273 @default.
• W2904103069 cites W2161603983 @default.
• W2904103069 cites W2165819524 @default.
• W2904103069 cites W2208633697 @default.
• W2904103069 cites W2295518379 @default.
• W2904103069 cites W2398270552 @default.
• W2904103069 cites W250663856 @default.
• W2904103069 cites W2580829089 @default.
• W2904103069 cites W2590281816 @default.
• W2904103069 cites W2606373084 @default.
• W2904103069 cites W2618271069 @default.
• W2904103069 cites W2750579866 @default.
• W2904103069 cites W306458078 @default.
• W2904103069 doi "https://doi.org/10.1017/jfm.2018.884" @default.
• W2904103069 hasPublicationYear "2018" @default.
• W2904103069 type Work @default.
• W2904103069 sameAs 2904103069 @default.
• W2904103069 citedByCount "9" @default.
• W2904103069 countsByYear W29041030692020 @default.
• W2904103069 countsByYear W29041030692021 @default.
• W2904103069 countsByYear W29041030692022 @default.
• W2904103069 countsByYear W29041030692023 @default.
• W2904103069 crossrefType "journal-article" @default.
• W2904103069 hasAuthorship W2904103069A5037121668 @default.
• W2904103069 hasAuthorship W2904103069A5081905613 @default.
• W2904103069 hasBestOaLocation W29041030692 @default.
• W2904103069 hasConcept C120665830 @default.
• W2904103069 hasConcept C121332964 @default.
• W2904103069 hasConcept C155231867 @default.
• W2904103069 hasConcept C179065325 @default.
• W2904103069 hasConcept C182748727 @default.
• W2904103069 hasConcept C184050105 @default.
• W2904103069 hasConcept C18533594 @default.
• W2904103069 hasConcept C196558001 @default.
• W2904103069 hasConcept C2524010 @default.
• W2904103069 hasConcept C33923547 @default.
• W2904103069 hasConcept C51038369 @default.
• W2904103069 hasConcept C57691317 @default.
• W2904103069 hasConcept C57879066 @default.
• W2904103069 hasConcept C91738503 @default.
• W2904103069 hasConcept C93038891 @default.
• W2904103069 hasConcept C97355855 @default.
• W2904103069 hasConcept C99844830 @default.
• W2904103069 hasConceptScore W2904103069C120665830 @default.
• W2904103069 hasConceptScore W2904103069C121332964 @default.
• W2904103069 hasConceptScore W2904103069C155231867 @default.
• W2904103069 hasConceptScore W2904103069C179065325 @default.
• W2904103069 hasConceptScore W2904103069C182748727 @default.
• W2904103069 hasConceptScore W2904103069C184050105 @default.
• W2904103069 hasConceptScore W2904103069C18533594 @default.
• W2904103069 hasConceptScore W2904103069C196558001 @default.
• W2904103069 hasConceptScore W2904103069C2524010 @default.
• W2904103069 hasConceptScore W2904103069C33923547 @default.
• W2904103069 hasConceptScore W2904103069C51038369 @default.
• W2904103069 hasConceptScore W2904103069C57691317 @default.
• W2904103069 hasConceptScore W2904103069C57879066 @default.
• W2904103069 hasConceptScore W2904103069C91738503 @default.
• W2904103069 hasConceptScore W2904103069C93038891 @default.
• W2904103069 hasConceptScore W2904103069C97355855 @default.

• next