2008
DOI: 10.1016/j.jcis.2008.01.031
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Some aspects of hydrate formation and wetting

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Cited by 29 publications
(30 citation statements)
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“…The clathrate is always sI filled with methane, and the simulations are performed at 277 K and 100 bar with a 5.22 nm –2 surface coverage for the pure dodecanol monolayer and 4.43 nm –2 for the mixed aligned monolayer that consist of dodecanol and dodecane. We find that water wets the clathrate–dodecane interface with a contact angle θ = 34 ± 2° (Figure 6a) in agreement with previous assumptions 35,43,99,100 and experiments that report θ = 29° for water at the clathrate–freon interface. 43 We use the Young equation, 101 cos θ = (γ c-o – γ w-c )/γ w-o , and the surface tensions of the clathrate–water interface, γ w-c = 33 ± 4 mJ m –2 , 2,44,45 and the dodecane–water interface, γ w-o = 53 mJ m –2 , 46,47 to determine that the surface free energy of the clathrate–dodecane interface is γ c-o = 76.9 ± 2 mJ m –2 .…”
Section: Results and Discussionsupporting
confidence: 91%
“…The clathrate is always sI filled with methane, and the simulations are performed at 277 K and 100 bar with a 5.22 nm –2 surface coverage for the pure dodecanol monolayer and 4.43 nm –2 for the mixed aligned monolayer that consist of dodecanol and dodecane. We find that water wets the clathrate–dodecane interface with a contact angle θ = 34 ± 2° (Figure 6a) in agreement with previous assumptions 35,43,99,100 and experiments that report θ = 29° for water at the clathrate–freon interface. 43 We use the Young equation, 101 cos θ = (γ c-o – γ w-c )/γ w-o , and the surface tensions of the clathrate–water interface, γ w-c = 33 ± 4 mJ m –2 , 2,44,45 and the dodecane–water interface, γ w-o = 53 mJ m –2 , 46,47 to determine that the surface free energy of the clathrate–dodecane interface is γ c-o = 76.9 ± 2 mJ m –2 .…”
Section: Results and Discussionsupporting
confidence: 91%
“…7, and the immersion depth was observed close to zero in these experiments. The radius of the hydrate particles used in these experiments was 0.003 ± 0.001 m. It was previously suggested by Fotland and Askvik [35] that for hydrate particles nucleating and growing at oil/brine interfaces, their positioning at the interface is largely dominated by the wetting state of the system, as long as the particles have radius smaller than 0.01 m. Capillary force was suggested to dominate for particles with a radius smaller than 0.001 m [35]. In this present work, the hydrate particles are mechanically removed from the oil/water interface, overriding the natural force balance of the system, but the observed differences in immersion depth could be argued to be related to differences in wetting state and capillary forces in the systems.…”
Section: Influence Of Watersupporting
confidence: 56%
“…When no surfactant molecules are adsorbed, the hydrate surface is wetted by water. 22 When the hydrate particles are preferentially wetted by the oil phase, this means that the surfactant molecules are adsorbed head-down, with the headgroup attached to the hydrate surface and the tail of the alkyl chain oriented away from it. If they are wetted by the surfactant solution, the headgroup of the adsorbed surfactant molecules is oriented away from the hydrate surface.…”
Section: Resultsmentioning
confidence: 99%