1997
DOI: 10.1016/s0360-5442(96)00112-0
|View full text |Cite
|
Sign up to set email alerts
|

Measurements of mechanical properties of the liquid CO2-water-CO2-hydrate system

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

2
33
1

Year Published

2000
2000
2018
2018

Publication Types

Select...
7
1

Relationship

0
8

Authors

Journals

citations
Cited by 42 publications
(36 citation statements)
references
References 8 publications
2
33
1
Order By: Relevance
“…Figure 4 shows that the heat release into the guest‐fluid phase almost vanishes within one minute and that the further film growth is exclusively sustained by the heat transfer into the film. These predictions are not in good agreement with existing experimental results indicating a hydrate‐film thickness of the order of 10 μm 7,8. This inconsistency between the predictions and the experimental results indicates that some mechanism, other than the heat removal, dominates the rate of hydrate formation.…”
Section: Resultscontrasting
confidence: 76%
“…Figure 4 shows that the heat release into the guest‐fluid phase almost vanishes within one minute and that the further film growth is exclusively sustained by the heat transfer into the film. These predictions are not in good agreement with existing experimental results indicating a hydrate‐film thickness of the order of 10 μm 7,8. This inconsistency between the predictions and the experimental results indicates that some mechanism, other than the heat removal, dominates the rate of hydrate formation.…”
Section: Resultscontrasting
confidence: 76%
“…The change in the hydrate thickness on a CO2 droplet results from hydrate growth and dissolution, which are controlled by mass transfer from liquid CO2 into water depending on the saturation state of CO2 in water (20,31,34). For the case in which a liquid CO2 droplet is surrounded by water, a mass transfer model has shown that the hydrate shell greatly reduces the mass transfer of CO2 into water (19,28,35). The rate of change of the hydrate shell is limited by mass transfer, expressed as dr/dt ) k*, where r is the radius of the drop and k* is the overall mass transfer coefficient (19).…”
Section: Resultsmentioning
confidence: 99%
“…Accordingly, k* is the overall mass transfer coefficient across the hydrate film. Combining eqs 4-6, one derives or The latter expression (eq 9) is obtained because the thickness of the hydrate shell, ∆r, is normally on the order of 1-10 µm (31,34,35), making ∆r/r 0 < 1/20.…”
Section: Resultsmentioning
confidence: 99%
“…29 The SMD/D SM correlated well with the Weber number for each mixer; the SMD decreased with increasing Weber number, or equivalently the water flow velocity. It is known that the SMD/D SM of the drops formed in Kenics static mixers from liquid-liquid flows are well correlated with the Weber number.…”
mentioning
confidence: 80%