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Dynamic multiphase flow model of hydrate formation in marine sediments

291

Citations

53

References

2007

Year

TLDR

Hydrate formation in marine sediments is driven by free gas from depth, which depletes water, raises salinity, and reduces permeability, leading to upward increases in salinity and hydrate concentration and topographic variation of the hydrate stability zone. The authors developed a multicomponent, multiphase fluid and heat flow model that captures dynamic effects of hydrate formation on salinity, temperature, pressure, and hydraulic properties, and shows that gas chimneys couple the free gas zone to the seafloor through high‑salinity conduits maintained at the three‑phase boundary by gas flow. The model predicts that gas pressure buildup drives gas through the hydrate stability zone, trapping gas and allowing significant amounts of methane to bypass the zone, resulting in a smaller hydrate reservoir and a highly economical methane deposit with concentrations above 70 % located near the seafloor at the three‑phase boundary.

Abstract

We developed a multicomponent, multiphase, fluid and heat flow model to describe hydrate formation in marine sediments; the one‐ and two‐dimensional model accounts for the dynamic effects of hydrate formation on salinity, temperature, pressure, and hydraulic properties. Free gas supplied from depth forms hydrate, depletes water, and elevates salinity until pore water is too saline for further hydrate formation: Salinity and hydrate concentration increase upward from the base of the regional hydrate stability zone (RHSZ) to the seafloor, and the base of the hydrate stability zone has significant topography. In fine‐grained sediments, hydrate formation leads to rapid permeability reduction and capillary sealing to free gas. This traps gas and causes gas pressure to build up until it exceeds the overburden stress and drives gas through the RHSZ. Gas chimneys couple the free gas zone to the seafloor through high‐salinity conduits that are maintained at the three‐phase boundary by gas flow. As a result, significant amounts of gaseous methane can bypass the RHSZ, which implies a significantly smaller hydrate reservoir than previously envisioned. Hydrate within gas chimneys lies at the three‐phase boundary, and thus small increases in temperature or decreases in pressure can immediately transport methane into the ocean. This type of hydrate deposit may be the most economical for producing energy because it has very high methane concentrations ( S h > 70%), located near the seafloor, which lie on the three‐phase boundary.

References

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