Matches in SemOpenAlex for { <https://semopenalex.org/work/W2890618571> ?p ?o ?g. }
- W2890618571 endingPage "71" @default.
- W2890618571 startingPage "61" @default.
- W2890618571 abstract "Abstract The use of traditional Re number turbulence indicator can be extended for a variety of non-pipe flow channel geometries by the use of appropriately defined equivalent diameters. A modified equivalent diameter can be defined also for open channel flow, however, it fails when condensation is present at the open channel interface. This is shown by experimental measurements performed at the LEI (Lithuanian Energy Institute) two–phase test facility for condensing separated flows. It was observed that for such conditions the liquid region can become fully turbulent even when Ref" @default.
- W2890618571 created "2018-09-27" @default.
- W2890618571 creator A5010034546 @default.
- W2890618571 creator A5063623941 @default.
- W2890618571 creator A5078484921 @default.
- W2890618571 date "2019-01-01" @default.
- W2890618571 modified "2023-09-26" @default.
- W2890618571 title "Turbulence predicting criterion based on shear forces at the boundaries in a two-phase flow" @default.
- W2890618571 cites W1812431571 @default.
- W2890618571 cites W1974957184 @default.
- W2890618571 cites W1984710104 @default.
- W2890618571 cites W2005181573 @default.
- W2890618571 cites W2016174669 @default.
- W2890618571 cites W2021231050 @default.
- W2890618571 cites W2027789274 @default.
- W2890618571 cites W2035065456 @default.
- W2890618571 cites W2048401566 @default.
- W2890618571 cites W2053155959 @default.
- W2890618571 cites W2059694256 @default.
- W2890618571 cites W2061644490 @default.
- W2890618571 cites W2080798380 @default.
- W2890618571 cites W2080811537 @default.
- W2890618571 cites W2097696163 @default.
- W2890618571 cites W2109898176 @default.
- W2890618571 cites W2115804172 @default.
- W2890618571 cites W2116866488 @default.
- W2890618571 cites W2135912504 @default.
- W2890618571 cites W2233101635 @default.
- W2890618571 cites W2276418792 @default.
- W2890618571 cites W2337222895 @default.
- W2890618571 cites W2401526628 @default.
- W2890618571 cites W2402599464 @default.
- W2890618571 cites W2494687576 @default.
- W2890618571 cites W2517995215 @default.
- W2890618571 cites W2536105634 @default.
- W2890618571 cites W2584212915 @default.
- W2890618571 cites W2604722650 @default.
- W2890618571 cites W2606079548 @default.
- W2890618571 cites W2612097386 @default.
- W2890618571 cites W2733508969 @default.
- W2890618571 cites W2735509657 @default.
- W2890618571 cites W2746081606 @default.
- W2890618571 cites W2779350999 @default.
- W2890618571 cites W2790671977 @default.
- W2890618571 cites W4211110691 @default.
- W2890618571 doi "https://doi.org/10.1016/j.ijthermalsci.2018.08.011" @default.
- W2890618571 hasPublicationYear "2019" @default.
- W2890618571 type Work @default.
- W2890618571 sameAs 2890618571 @default.
- W2890618571 citedByCount "5" @default.
- W2890618571 countsByYear W28906185712020 @default.
- W2890618571 countsByYear W28906185712022 @default.
- W2890618571 countsByYear W28906185712023 @default.
- W2890618571 crossrefType "journal-article" @default.
- W2890618571 hasAuthorship W2890618571A5010034546 @default.
- W2890618571 hasAuthorship W2890618571A5063623941 @default.
- W2890618571 hasAuthorship W2890618571A5078484921 @default.
- W2890618571 hasConcept C121332964 @default.
- W2890618571 hasConcept C144308804 @default.
- W2890618571 hasConcept C150711758 @default.
- W2890618571 hasConcept C15476950 @default.
- W2890618571 hasConcept C159985019 @default.
- W2890618571 hasConcept C180925781 @default.
- W2890618571 hasConcept C192562407 @default.
- W2890618571 hasConcept C196558001 @default.
- W2890618571 hasConcept C204561356 @default.
- W2890618571 hasConcept C204573209 @default.
- W2890618571 hasConcept C2776310255 @default.
- W2890618571 hasConcept C38349280 @default.
- W2890618571 hasConcept C57879066 @default.
- W2890618571 hasConcept C96035792 @default.
- W2890618571 hasConceptScore W2890618571C121332964 @default.
- W2890618571 hasConceptScore W2890618571C144308804 @default.
- W2890618571 hasConceptScore W2890618571C150711758 @default.
- W2890618571 hasConceptScore W2890618571C15476950 @default.
- W2890618571 hasConceptScore W2890618571C159985019 @default.
- W2890618571 hasConceptScore W2890618571C180925781 @default.
- W2890618571 hasConceptScore W2890618571C192562407 @default.
- W2890618571 hasConceptScore W2890618571C196558001 @default.
- W2890618571 hasConceptScore W2890618571C204561356 @default.
- W2890618571 hasConceptScore W2890618571C204573209 @default.
- W2890618571 hasConceptScore W2890618571C2776310255 @default.
- W2890618571 hasConceptScore W2890618571C38349280 @default.
- W2890618571 hasConceptScore W2890618571C57879066 @default.
- W2890618571 hasConceptScore W2890618571C96035792 @default.
- W2890618571 hasLocation W28906185711 @default.
- W2890618571 hasOpenAccess W2890618571 @default.
- W2890618571 hasPrimaryLocation W28906185711 @default.
- W2890618571 hasRelatedWork W1916722776 @default.
- W2890618571 hasRelatedWork W1965398802 @default.
- W2890618571 hasRelatedWork W1967782048 @default.
- W2890618571 hasRelatedWork W1987164077 @default.
- W2890618571 hasRelatedWork W2151728674 @default.
- W2890618571 hasRelatedWork W2281507024 @default.
- W2890618571 hasRelatedWork W2319357844 @default.
- W2890618571 hasRelatedWork W2621183777 @default.
- W2890618571 hasRelatedWork W2726373787 @default.
- W2890618571 hasRelatedWork W4362649909 @default.