2006
DOI: 10.1016/j.ijheatmasstransfer.2006.04.010
|View full text |Cite
|
Sign up to set email alerts
|

Confined growth of a vapour bubble in a capillary tube at initially uniform superheat: Experiments and modelling

Abstract: Bubble growth was triggered in a capillary tube closed at one end and vented to the atmosphere at the other and initially filled with uniformly superheated water. Measurements of the rate of axial growth and the varying pressure at the closed end were used to test under these simplified conditions assumptions employed in one-dimensional models for bubble growth applicable to the more complex conditions of confined-bubble flow boiling in microchannels. Issues included the thickness of the liquid films round con… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
31
0

Year Published

2010
2010
2023
2023

Publication Types

Select...
7
2

Relationship

0
9

Authors

Journals

citations
Cited by 54 publications
(31 citation statements)
references
References 28 publications
(52 reference statements)
0
31
0
Order By: Relevance
“…4B). Although growth of confined bubbles in nanochannels has not yet been reported, the growth of confined vapor bubbles reported in larger microchannels typically does not exhibit a constant evaporation rate (13). Instead, the growth rate of confined vapor bubbles in microchannels is typically observed to increase with time, consistent with the momentum-governed bubble growth theory (13).…”
mentioning
confidence: 76%
“…4B). Although growth of confined bubbles in nanochannels has not yet been reported, the growth of confined vapor bubbles reported in larger microchannels typically does not exhibit a constant evaporation rate (13). Instead, the growth rate of confined vapor bubbles in microchannels is typically observed to increase with time, consistent with the momentum-governed bubble growth theory (13).…”
mentioning
confidence: 76%
“…These have been attributed to transient dryout, particularly at low mass flux, and relatively high heat flux. Kenning et al (2006) suggested that there are two different mechanisms of dryout around individual bubbles in microchannels. These are dryout as a result of depletion of the film thickness below a certain minimum by complete evaporation of the liquid film beneath the confined bubble and dryout due to surface tension driven ‗capillary roll-up' on partially-wetted surfaces with finite contact angles.…”
Section: Temperature and Pressure Fluctuationsmentioning
confidence: 99%
“…However, the liquid film thickness was given as a parameter in these models. Meanwhile, Kenning et al (17) proposed the confined growth model. They introduced the surface tension balance to calculate the pressure difference between the liquid and the vapor phase.…”
Section: Introductionmentioning
confidence: 99%