2008
DOI: 10.1061/(asce)0733-9429(2008)134:11(1570)
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Dissolution of Direct Ocean Carbon Sequestration Plumes Using an Integral Model Approach

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Cited by 7 publications
(4 citation statements)
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“…The model contains several parameters, each of which are well-understood and should not be used as calibration parameters. The entrainment and detrainment coefficients are taken from Socolofsky et al 9 and Socolofsky and Bhaumik. 10 Correlations for bubble and droplet slip velocity and the heatand mass-transfer coefficients are taken from the appropriate equations by Clift et al 5 Because of the high pressures at depth in the ocean, the Peng−Robinson equation of state is used to compute density and fugacity of seawater and oil and gas mixtures.…”
Section: Energy and Fuelsmentioning
confidence: 99%
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“…The model contains several parameters, each of which are well-understood and should not be used as calibration parameters. The entrainment and detrainment coefficients are taken from Socolofsky et al 9 and Socolofsky and Bhaumik. 10 Correlations for bubble and droplet slip velocity and the heatand mass-transfer coefficients are taken from the appropriate equations by Clift et al 5 Because of the high pressures at depth in the ocean, the Peng−Robinson equation of state is used to compute density and fugacity of seawater and oil and gas mixtures.…”
Section: Energy and Fuelsmentioning
confidence: 99%
“…The primary difference in these models is seen at heights above the peel height of the first intrusion. Because we are limiting our discussion to plume heights below the first intrusion, we will discuss results from the TAMU integral model adapted to oil and gas plumes.…”
Section: Larger Hydrocarbon Flows Above the Mudlinementioning
confidence: 99%
“…This confirms previous findings that gaseous CO 2 is mostly dissolved within a few meters above the emission source, 13,20 resulting in much more localized inputs to the water column compared to hydrocarbon gases 13,23,46,74,76 or CO 2 droplets. 50,99,100 The results in Figure 2, panels b and c, might appear contradictory at first because most of the CO 2 escapes the ascending bubbles (Figure 2c) before a significant decrease of the CO 2 gas-phase mole fraction becomes evident (Figure 2b). This is caused by the larger solubility of CO 2 , by a factor of 25−62, with respect to other major dissolved gases at local conditions.…”
Section: ■ Results and Discussionmentioning
confidence: 97%
“…The pressures at the ocean bottom are large to contain CO 2 in its liquid phase. 2 At this location, it is easier to get stable and stationary pools of carbon-dioxide. The potential capacity of an ocean is very large and can hold more than a thousand billion tons of carbon dioxide.…”
Section: Ocean Storagementioning
confidence: 99%