1980
DOI: 10.1016/0301-9322(80)90042-7
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Condensation-driven fluid motions

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Cited by 25 publications
(6 citation statements)
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“…6). At the same time, the remaining attached vapor was cut off from the nozzle exit due to the shock front generated by bubble implosions [29][30][31], and a new cycle began as another bubble grew from the nozzle. Fig.…”
Section: Bubble Motionsmentioning
confidence: 99%
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“…6). At the same time, the remaining attached vapor was cut off from the nozzle exit due to the shock front generated by bubble implosions [29][30][31], and a new cycle began as another bubble grew from the nozzle. Fig.…”
Section: Bubble Motionsmentioning
confidence: 99%
“…At Stage 2 (1.8-2.452ms), the deviations after the detachment may be caused by the dramatic increase of capillary waves formed on the bubble surface. These waves intensify the roughness of bubble surface, which greatly enhances the shear stress between bubbles moving with translatory velocity and motionless cool bulk [28,29]. Thus, the viscosity near the interface is the dominant factor for the dissipation caused by shear stress.…”
Section: Verification Of Modelmentioning
confidence: 99%
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“…In certain cases there is a collapse of the original bubble after detachment. Detached parts of the bubble are dragged away from the steam injector and continue to condense, generating a trace of smaller steam bubbles in the downstream flow [19]. Figure 4 shows a possible cycle of a bubbling regime of DCC.…”
Section: Bubbling Regimementioning
confidence: 99%
“…This map is a graph describing the appearance of different regimes at specific conditions in terms of their geometric appearances and dynamic features. Various regime maps have been published in literature [6], [7], [9], [19]- [21] which show the occurrence of different regimes, depending on the steam inflow rate and the temperature of water subcooling. These two-dimensional maps were obtained during experiments performed at various environmental conditions.…”
Section: Introductionmentioning
confidence: 99%