Matches in SemOpenAlex for { <https://semopenalex.org/work/W2470826598> ?p ?o ?g. }
- W2470826598 endingPage "63" @default.
- W2470826598 startingPage "39" @default.
- W2470826598 abstract "Abstract Downward two-phase flow is observed in light water reactor accident scenarios such as loss of coolant accident (LOCA) and loss of heat sink accident (LOHS) due to loss of feed water or a secondary pipe break. Hence, a comprehensive literature review has been performed for the co-current downward two-phase flow with information on the flow regime transitions and flow characteristics for each regime in the downward flow. The review compares the experimental data of the flow regime map and the current available transition models. Objectivity of the data varies on the method utilized as a certain degree of subjectivity is still present in the most objective method. Nevertheless, experimental data through subjective methods such as direct visualization or analysis of a wire mesh sensor (WMS) data were still studied in this review. Despite the wide range of flow regime data for numerous pipe sizes, a consensus was not reached for the effect of pipe sizes on flow regime transition. However, it is known that a larger pipe results in greater degree of coalescence at lower gas flow rates ( Hibiki et al., 2004 ). The introduction of a flow straightener at the inlet led to less coring and fluid rotation and inevitably, reduced bubble coalescence. This also resulted in the disappearance of the kinematic shock wave phenomenon, contrary to an inlet without a flow straightener. The effect of flow inlet, flow location, pipe diameter and bubble interfacial forces on the radial distribution as well as bubble coalescence and breakup rate are studied. Moreover, the interfacial area concentration and the bubble coalescence and breakup mechanisms are shown to vary in the axial direction as well as with flow rate, flow area and pressure drop. The liquid velocity field, bubble shape and shear stress are studied for a stationary slug bubble with downward liquid flow. Furthermore, the relationship between the plug and foam flow shape profiles, relative velocity, void fraction and gas slug velocity at an elevated pressure of 0.2 MPa studied by Sekoguchi et al. (1996) are also analyzed, together with the five plug flow sub-regime groups located in the low slip and high slip velocity regions. For the annular flow, the relationship between liquid film thickness, entrainment mechanisms, film velocity and shear stress are studied as well. Alike to plug flow, five sub-regimes in the annular flow are also examined along with the bubble and droplet entrainment mechanisms. The paper also discusses the pressure drop for bubbly, slug, foam, falling film and annular flow regimes, with a particular focus on the most accurate interfacial friction factor correlation for annular flow and its applicability for a wide range of pipe diameters. The flow instability of a system such as static and dynamic instability in the presence of a downcomer, for both single and parallel heated channels are examined too. Finally, the most accurate and versatile drift-flux correlation applicable to all downward flow regimes is highlighted and compared to drift-flux type correlations as it will be a stepping stone to attain a more accurate co-current downward flow transition model. Further experimental effort is essential to achieve a strong foothold in the understanding of co-current downward two-phase flow, as it is vital for nuclear engineering applications." @default.
- W2470826598 created "2016-07-22" @default.
- W2470826598 creator A5057017873 @default.
- W2470826598 creator A5077024745 @default.
- W2470826598 date "2016-10-01" @default.
- W2470826598 modified "2023-10-12" @default.
- W2470826598 title "Flow regime, void fraction and interfacial area transport and characteristics of co-current downward two-phase flow" @default.
- W2470826598 cites W1858722304 @default.
- W2470826598 cites W1862022608 @default.
- W2470826598 cites W1963637555 @default.
- W2470826598 cites W1964710610 @default.
- W2470826598 cites W1965027421 @default.
- W2470826598 cites W1968940095 @default.
- W2470826598 cites W1969484292 @default.
- W2470826598 cites W1972290899 @default.
- W2470826598 cites W1979748216 @default.
- W2470826598 cites W1980506155 @default.
- W2470826598 cites W1982354491 @default.
- W2470826598 cites W1982487125 @default.
- W2470826598 cites W1985373593 @default.
- W2470826598 cites W1987448193 @default.
- W2470826598 cites W1993393590 @default.
- W2470826598 cites W1999355910 @default.
- W2470826598 cites W2001455326 @default.
- W2470826598 cites W2002925529 @default.
- W2470826598 cites W2004992590 @default.
- W2470826598 cites W2006605824 @default.
- W2470826598 cites W2009419740 @default.
- W2470826598 cites W2013966666 @default.
- W2470826598 cites W2014350219 @default.
- W2470826598 cites W2017358914 @default.
- W2470826598 cites W2030398153 @default.
- W2470826598 cites W2031751828 @default.
- W2470826598 cites W2034828276 @default.
- W2470826598 cites W2037587405 @default.
- W2470826598 cites W2037645662 @default.
- W2470826598 cites W2043636449 @default.
- W2470826598 cites W2044762986 @default.
- W2470826598 cites W2045132934 @default.
- W2470826598 cites W2051586483 @default.
- W2470826598 cites W2053005571 @default.
- W2470826598 cites W2055675230 @default.
- W2470826598 cites W2057724648 @default.
- W2470826598 cites W2058924105 @default.
- W2470826598 cites W2060527237 @default.
- W2470826598 cites W2061182160 @default.
- W2470826598 cites W2066777787 @default.
- W2470826598 cites W2068423497 @default.
- W2470826598 cites W2069048604 @default.
- W2470826598 cites W2069644672 @default.
- W2470826598 cites W2070441547 @default.
- W2470826598 cites W2072710157 @default.
- W2470826598 cites W2074563397 @default.
- W2470826598 cites W2081440156 @default.
- W2470826598 cites W2085102802 @default.
- W2470826598 cites W2088581397 @default.
- W2470826598 cites W2090064343 @default.
- W2470826598 cites W2090556488 @default.
- W2470826598 cites W2103210945 @default.
- W2470826598 cites W2130859504 @default.
- W2470826598 cites W2132145594 @default.
- W2470826598 cites W2134020148 @default.
- W2470826598 cites W2170221086 @default.
- W2470826598 cites W2209848126 @default.
- W2470826598 cites W4231809816 @default.
- W2470826598 cites W4234055473 @default.
- W2470826598 cites W4254075243 @default.
- W2470826598 doi "https://doi.org/10.1016/j.nucengdes.2016.05.042" @default.
- W2470826598 hasPublicationYear "2016" @default.
- W2470826598 type Work @default.
- W2470826598 sameAs 2470826598 @default.
- W2470826598 citedByCount "21" @default.
- W2470826598 countsByYear W24708265982018 @default.
- W2470826598 countsByYear W24708265982019 @default.
- W2470826598 countsByYear W24708265982020 @default.
- W2470826598 countsByYear W24708265982022 @default.
- W2470826598 countsByYear W24708265982023 @default.
- W2470826598 crossrefType "journal-article" @default.
- W2470826598 hasAuthorship W2470826598A5057017873 @default.
- W2470826598 hasAuthorship W2470826598A5077024745 @default.
- W2470826598 hasConcept C121332964 @default.
- W2470826598 hasConcept C144308804 @default.
- W2470826598 hasConcept C148043351 @default.
- W2470826598 hasConcept C159985019 @default.
- W2470826598 hasConcept C192562407 @default.
- W2470826598 hasConcept C2779772531 @default.
- W2470826598 hasConcept C38349280 @default.
- W2470826598 hasConcept C57879066 @default.
- W2470826598 hasConcept C6648577 @default.
- W2470826598 hasConcept C97355855 @default.
- W2470826598 hasConceptScore W2470826598C121332964 @default.
- W2470826598 hasConceptScore W2470826598C144308804 @default.
- W2470826598 hasConceptScore W2470826598C148043351 @default.
- W2470826598 hasConceptScore W2470826598C159985019 @default.
- W2470826598 hasConceptScore W2470826598C192562407 @default.
- W2470826598 hasConceptScore W2470826598C2779772531 @default.
- W2470826598 hasConceptScore W2470826598C38349280 @default.
- W2470826598 hasConceptScore W2470826598C57879066 @default.