1992
DOI: 10.1016/0196-8904(92)90072-5
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Density change of water due to dissolution of carbon dioxide and near-field behavior of CO2 from a source on deep-sea floor

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Cited by 64 publications
(53 citation statements)
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“…5 The density change was calculated using ρ/ DIC = 0.0120 g m −3 /(µmol kg −1 ) (Song et al, 2005). Since Bradshaw (1973) found 0.0110 g m −3 /(µmol kg −1 ) and Ohsumi et al (1992) found 0.0128 g m −3 /(µmol kg −1 ), the uncertainty in ρ/ DIC may be 20 %. density measurement, which is always less than 30 min.…”
Section: Air Saturationmentioning
confidence: 99%
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“…5 The density change was calculated using ρ/ DIC = 0.0120 g m −3 /(µmol kg −1 ) (Song et al, 2005). Since Bradshaw (1973) found 0.0110 g m −3 /(µmol kg −1 ) and Ohsumi et al (1992) found 0.0128 g m −3 /(µmol kg −1 ), the uncertainty in ρ/ DIC may be 20 %. density measurement, which is always less than 30 min.…”
Section: Air Saturationmentioning
confidence: 99%
“…(A2) given in Appendix A. Isotopic composition variations in the water of the pedosphere are even more significant. The D and 18 O isotopic abundances δ D and δ 18 in the natural seawater that was used as the raw material for the diluted seawater preparation at the area of sampling were measured in 1972 and made available by Ostlund et al (1987). The water which is deionized and used for dilution of the natural seawater (N. Higgs, personal communication, 2011) is tap water from Havant, UK, where the supplier of the IAPSO SSW is located.…”
Section: Isotopic Compositionmentioning
confidence: 99%
“…Furthermore, dissolution of CO 2 increases the density of water, and it was suggested by Drange et al (1993) that a gravity current could be achieved toward the deep ocean if sufficiently dense CO 2 -enriched water (Haugan and Drange 1992) were released on a sloping bottom. Disposal of liquid CO 2 at depths where it is denser than seawater (Ͼ3,000 m) is expected to fill topographic depressions and, in turn, accumulate as a large lake of CO 2 (Ohsumi 1993) over which a thin hydrate layer forms and retards the dissolution. The hydrate films are not perfect insulators against the interliquid-phase CO 2 transfer, and they are continuously ''metabolized'' through decomposition of aged crystals and formation of new crystals (Mori 1998).…”
Section: Acknowledgmentsmentioning
confidence: 99%
“…The values of the parameters , p, n, r c , , and given above are retained for all cases in which hydrate is present. Following Ohsumi et al (1992), the thickness of the BBL for cases 1-3 is taken as h ϭ 100 m, which is about 14 times the Ekman layer thickness, ␦ E , obtained from Eq. 1 for f ϭ O(10 Ϫ4 ) s…”
Section: The Modelmentioning
confidence: 99%
“…A possibility of cyclic gas bursts from lakes which are charged by a gas influx from the lake bottoms was also pointed out by Tietze (1992). He argued that dissolution of CO 2(aq) will inevitably create a stratification of the lake because the density of CO 2 -containing water is higher than that of pure water, due to a small partial volume of dissolved CO 2(aq) in water (Ohsumi et al, 1992), and that the stratification will limit upward gas transport, leading to an accumulation of the gas below the stratified layers. If limnic eruptions take place repetitively on a timescale of ~100 years, evidence of past eruptions might be found in geological records and local documents.…”
Section: -3 Repetitive Nature Of a Limnic Eruptionmentioning
confidence: 99%