FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2951832891> ?p ?o ?g. }

• W2951832891 endingPage "2433" @default.
• W2951832891 startingPage "2407" @default.
• W2951832891 abstract "Purpose This paper aims to demonstrate the capabilities of a diffuse interface free energy lattice Boltzmann method to perform direct numerical simulations of liquid–liquid dispersions in a well-controlled turbulent environment. The goal of this research study is to develop numerical techniques that can visualize and quantify drop interaction with the turbulent vortices. The obtained information will be used for the development of sub-models of drop breakup for multi-scale simulations. Design/methodology/approach A pure binary liquid system is considered that is subject to fully developed statistically stationary turbulent flow field in a cubic fully periodic box with the edge size of 300 lattice units. Three turbulent flow fields with varying energy input are examined and their coherent structures are visualized using a normalized Q-criterion. The evolution of the liquid–liquid interface is tracked as a function of time. The detailed explanation of the numerical method is provided with a highlight on a choice of the numerical parameters. Findings Drop breakup mechanisms differ depending on energy input. Drops break due to interaction with the vortices. Quantification of turbulent structures shows that the size of vortices increases with the decrease of energy input. Drop interacts simultaneously with multiple vortices of the size comparable to or smaller than the drop size. Vortices of the size smaller than the drop size disturb drop interface and pinch off the satellites. Vortices of the size comparable to the drop size tend to elongate the drop and tear it apart producing daughter drops and satellites. Addition of the second phase enhances turbulent dissipation at the high wavenumbers. To obtain physically realistic two-phase energy spectra, the multiple-relaxation-time collision operator should be used. Originality/value Detailed information of drop breakup in the turbulent flow field is crucial for the development of drop breakup sub-models that are necessary for multi-scale numerical simulations. The improvement of numerical methods that can provide these data and produce reliable results is important. This work made one step towards a better understanding of how drops interact with the turbulent vortices." @default.
• W2951832891 created "2019-06-27" @default.
• W2951832891 creator A5010404545 @default.
• W2951832891 creator A5072145271 @default.
• W2951832891 date "2019-07-01" @default.
• W2951832891 modified "2023-10-12" @default.
• W2951832891 title "Liquid drop breakup in homogeneous isotropic turbulence" @default.
• W2951832891 cites W1621130145 @default.
• W2951832891 cites W1859199609 @default.
• W2951832891 cites W1964314390 @default.
• W2951832891 cites W1970348574 @default.
• W2951832891 cites W1971927938 @default.
• W2951832891 cites W2007540696 @default.
• W2951832891 cites W2007543823 @default.
• W2951832891 cites W2009507541 @default.
• W2951832891 cites W2022650674 @default.
• W2951832891 cites W2026681071 @default.
• W2951832891 cites W2032549864 @default.
• W2951832891 cites W2033315566 @default.
• W2951832891 cites W2038714505 @default.
• W2951832891 cites W2039545822 @default.
• W2951832891 cites W2051029378 @default.
• W2951832891 cites W2058333241 @default.
• W2951832891 cites W2060138396 @default.
• W2951832891 cites W2066060292 @default.
• W2951832891 cites W2083440017 @default.
• W2951832891 cites W2084364634 @default.
• W2951832891 cites W2095283463 @default.
• W2951832891 cites W2100851379 @default.
• W2951832891 cites W2113731998 @default.
• W2951832891 cites W2126217340 @default.
• W2951832891 cites W2133591138 @default.
• W2951832891 cites W2136084179 @default.
• W2951832891 cites W2137332972 @default.
• W2951832891 cites W2137402934 @default.
• W2951832891 cites W2144233319 @default.
• W2951832891 cites W2169141619 @default.
• W2951832891 cites W2291078057 @default.
• W2951832891 cites W2527484971 @default.
• W2951832891 cites W2793739964 @default.
• W2951832891 cites W2809873809 @default.
• W2951832891 doi "https://doi.org/10.1108/hff-09-2018-0490" @default.
• W2951832891 hasPublicationYear "2019" @default.
• W2951832891 type Work @default.
• W2951832891 sameAs 2951832891 @default.
• W2951832891 citedByCount "7" @default.
• W2951832891 countsByYear W29518328912020 @default.
• W2951832891 countsByYear W29518328912021 @default.
• W2951832891 countsByYear W29518328912022 @default.
• W2951832891 crossrefType "journal-article" @default.
• W2951832891 hasAuthorship W2951832891A5010404545 @default.
• W2951832891 hasAuthorship W2951832891A5072145271 @default.
• W2951832891 hasConcept C121332964 @default.
• W2951832891 hasConcept C121864883 @default.
• W2951832891 hasConcept C140820882 @default.
• W2951832891 hasConcept C15476950 @default.
• W2951832891 hasConcept C182748727 @default.
• W2951832891 hasConcept C18533594 @default.
• W2951832891 hasConcept C192562407 @default.
• W2951832891 hasConcept C196558001 @default.
• W2951832891 hasConcept C21821499 @default.
• W2951832891 hasConcept C2777871205 @default.
• W2951832891 hasConcept C2779251355 @default.
• W2951832891 hasConcept C2781345722 @default.
• W2951832891 hasConcept C41008148 @default.
• W2951832891 hasConcept C57879066 @default.
• W2951832891 hasConcept C74650414 @default.
• W2951832891 hasConcept C76155785 @default.
• W2951832891 hasConceptScore W2951832891C121332964 @default.
• W2951832891 hasConceptScore W2951832891C121864883 @default.
• W2951832891 hasConceptScore W2951832891C140820882 @default.
• W2951832891 hasConceptScore W2951832891C15476950 @default.
• W2951832891 hasConceptScore W2951832891C182748727 @default.
• W2951832891 hasConceptScore W2951832891C18533594 @default.
• W2951832891 hasConceptScore W2951832891C192562407 @default.
• W2951832891 hasConceptScore W2951832891C196558001 @default.
• W2951832891 hasConceptScore W2951832891C21821499 @default.
• W2951832891 hasConceptScore W2951832891C2777871205 @default.
• W2951832891 hasConceptScore W2951832891C2779251355 @default.
• W2951832891 hasConceptScore W2951832891C2781345722 @default.
• W2951832891 hasConceptScore W2951832891C41008148 @default.
• W2951832891 hasConceptScore W2951832891C57879066 @default.
• W2951832891 hasConceptScore W2951832891C74650414 @default.
• W2951832891 hasConceptScore W2951832891C76155785 @default.
• W2951832891 hasIssue "7" @default.
• W2951832891 hasLocation W29518328911 @default.
• W2951832891 hasOpenAccess W2951832891 @default.
• W2951832891 hasPrimaryLocation W29518328911 @default.
• W2951832891 hasRelatedWork W1966493176 @default.
• W2951832891 hasRelatedWork W1987035256 @default.
• W2951832891 hasRelatedWork W2006877806 @default.
• W2951832891 hasRelatedWork W2041328019 @default.
• W2951832891 hasRelatedWork W2054644220 @default.
• W2951832891 hasRelatedWork W2062475262 @default.
• W2951832891 hasRelatedWork W2087946601 @default.
• W2951832891 hasRelatedWork W2151554837 @default.
• W2951832891 hasRelatedWork W2809450413 @default.
• W2951832891 hasRelatedWork W2951832891 @default.

• next