2004
DOI: 10.1029/2004gl021151
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Air bubble to clathrate hydrate transformation in polar ice sheets: A reconsideration based on the new data from Dome Fuji ice core

Abstract: [1] Mapping the spatial distribution of air bubbles and clathrate hydrates in thick sections of Antarctic ice from Dome Fuji station reveals a considerable redistribution of the inclusions in terms of number and volume in the bubbleto-hydrate transition zone. Analysis of the data indicated that more than 10% of the hydrates nucleated outside the preceding bubbles and more than 30% of the bubbles completely expired due to the gas outflow toward the coexisting hydrates. These features of the gas-hydrate-ice none… Show more

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Cited by 18 publications
(84 citation statements)
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References 13 publications
(19 reference statements)
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“…At low subcoolings this can have a very low probability since the critical radius can be appreciable. In the case of hydrate formation from air inclusions in ice cores, nucleation can take thousands of years (Ohno et al, 2004;Salamantin et al, 1998Salamantin et al, , 2001Shimanda and Hondoh, 2004). At higher subcoolings, the difference in free energy between the parent and daughter phase increases, this shifts the critical nucleus to lower radii.…”
Section: Introductionmentioning
confidence: 99%
“…At low subcoolings this can have a very low probability since the critical radius can be appreciable. In the case of hydrate formation from air inclusions in ice cores, nucleation can take thousands of years (Ohno et al, 2004;Salamantin et al, 1998Salamantin et al, , 2001Shimanda and Hondoh, 2004). At higher subcoolings, the difference in free energy between the parent and daughter phase increases, this shifts the critical nucleus to lower radii.…”
Section: Introductionmentioning
confidence: 99%
“…4, a) along the edges of ice crystals similar in shape to equilibrium polyhedrons that fill the whole space, like tetrakaidecahedrons of Lord Kelvin and Robert Williams [Maeno and Ebinuma, 1983]. Pores in fi rn close off and the air remaining in the pore volume becomes 1 -δD (‰) according to diff erent estimates: [Jouzel et al, 2007] (a), [Watanabe et al, 2003] (b), [Petit et al, 1999] (c) (δD scales are inverse); 2 -number of air bubbles per unit mass (N, g -1 ), according to diff erent estimates: this study (a), [Ohno et al, 2004] (b), [Lipenkov and Salamatin, 2014] (c). Horizontal dash lines are average N in LGM ice deposited in Holocene climate.…”
Section: Correlation Of Sizes and Numbers Of Air Bubbles With Ice Micmentioning
confidence: 89%
“…1.08 60 [Ohno et al, 2004] 22 Dome A 80°22′ S, 77°22′ E -58.5 2.32 0.41 2933 1.50 75 This study N o t e. T is snow temperature at the depth where it becomes seasonally invariable (10-15 m); b is snow accumulation rate; d s is relative density of snow on ice sheet surface; τ c * and τ c are, respectively, ages of ice at the fi rn/ice transition, measured and calculated using equation 11; A c is calculated ice grain size at the fi rn/ice transition; 〈r c 〉 and s are, respectively, mean radius of air bubbles at the fi rn/ice transition and its variance; N is measured number of air bubbles per unit mass, with two-sigma error. N and A c values for LGM ice are additionally quoted for Vostok, Concordia and Dome Fuji cores (Fig.…”
Section: Present Ice Formation Conditions and Parameters Of Air Bubblmentioning
confidence: 99%
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