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Dissociation of gas hydrates in marine sediments triggered by temperature increase: a theoretical model Lihua Liu, Klaus Wallmann, Tomas Feseker, Tina Treude Leibniz Institute of Marine Sciences (IFM-GEOMAR), Germany lliu@ifm-geomar.de
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Introduction: Global warming (Source: Climate Research Unit, Univ. of East Anglia, UK)
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Introduction: Ocean warming Source: IPCC (2007) 0.1°C World Ocean, 0 – 700 m water depth
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Tishchenko, Hensen, Wallmann & Wong (2005) Introduction: Stability of gas hydrates Hydrate Gas Water
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Introduction: Consequence of ocean warming Bottom waters increase 3ºC, 80% of the vast methane reservoir along the continental margins might be destabilized. (Buffett and Archer 2004). The Arctic region is particularly sensitive to climate change. Arctic ocean is one the most rapidly warming places on Earth and also a large reservoir of methane.
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Introduction: Important biogeochemical processes water column reduced sediment CH 4 Anaerobic oxidation of methane (AOM) Aerobic oxidation of methane atmosphere archaea sulfate- reducing bacteria Boetius et al. 2000
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7 Hydrate dissociation & methane release gas hydrates deep sea continental margin H 2 O + CH 4 free gas rising CH 4 SO 4 2- AO M
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Questions: Effect of seafloor warming on the stability of gas hydrates How will heat be transferred from the water to the sediment column? How fast will the gas hydrates dissociate under realistic environmental conditions? How much methane will be released? How much methane can be dissolved in porewater? How much methane can be consumed by microorganism (eg., AOM)?
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Model parameters Sediment column: 100 m Simulation time: 100 year AOM reaction rate constant: 10 -2 m 3 mol -1 yr -1 Initial conditions no free gas in the sediment column Boundary condition Upper boundary: increase 3°C/100 yr Lower boundary: a constant geothermal gradient Simulation method: 1 D multiphase reactive transport model
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Combination of: - heat transfer from water column to sediment and - mass balance of gas hydrate, methane (gas and dissolved), water, and sulfate. Multiphase mass transfer and transport, coupled with diffusion and biogeochemical reaction. (gas hydrate, dissolved methane, free gas, consumed by AOM) - Heat transfer in each phase - Gas transports in the sediment and into the water column, where gas bubbles rise and dissolve in water synchronously.
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Simulation results: Temperature profile in the sediment column °C°C
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Simulation Results: Gas hydrate volume fraction profile in the sediment column V gas Hydrage V sediment
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Simulation results: gas volume fraction profile in the sediment column V gas V sediment
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Simulation results: AOM rate profile in the sediment column mol m 3.yr
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Simulation results 0 20 40 60 80 100 0. 4 1.0 2.0 3.0 0 10 20 30 40 50 0.01 0.02 0.03 0 1.0 2.0 3.0 0.0 1.0 2.0 Temperature °C Gas hydrate volume fraction Free gas volume fraction AOM rate (mol m -3 yr -1 ) t= 0 t=100 yr t=50 yr Depth (m)
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Conclusion: Methane mass distribution Initial gas hydrate inventory Melted gas hydrate Free gas escape Free gas in sediment column Dissolved methane escape Consumed by AOM 20000 mol m - 2
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Conclusions: Answer the questions The dissociation of gas hydrate slows down temperature increases in the seafloor. Under simulation conditions, 10 % of the gas hydrates will melt in 100 yr. Of the released methane: > 30 % rises into water column as gas bubbles > 30 % remains in the sediment column as free gas. ~ 30 % dissolves into the sediment porewater ~ 3 % diffuses into the water column and > 2 % is consumed by AOM.
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Outlook Future work will focus on the Arctic shelf, where gas hydrate destabilization caused by bottom water temperature increases could become a major problem in the near future.
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Acknowledgements Cluster of Excellence “The Future Ocean” funded by the German Research Foundation (DFG) Dr. Giovanni Aloisi All of my colleagues
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