The feasibility of csem monitoring in gas hydrate production of the range of porosity and saturation

Conference Paper (2022)
Author(s)

Y. Li (Student TU Delft, Beijing University of Technology)

H Lu (Beijing University of Technology, Peking University)

L Wang (Beihang University)

M.F.M.I. Eltayieb (TU Delft - Applied Geophysics and Petrophysics)

Evert Slob (TU Delft - Applied Geophysics and Petrophysics)

Research Group
Applied Geophysics and Petrophysics
Copyright
© 2022 Y. Li, H. Lu, L. Wang, M.F.M.I. Eltayieb, E.C. Slob
DOI related publication
https://doi.org/10.3997/2214-4609.202210625
More Info
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Publication Year
2022
Language
English
Copyright
© 2022 Y. Li, H. Lu, L. Wang, M.F.M.I. Eltayieb, E.C. Slob
Research Group
Applied Geophysics and Petrophysics
Pages (from-to)
2349-2353
ISBN (electronic)
978-171385931-4
Reuse Rights

Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons.

Abstract

Natural gas hydrates production tests over the last two decades has sown that production is not without risks. Indirect effects in the sedimentary rocks of phase changes are changes in porosity, permeability, and saturation. From a field production test site, porosity changes in the range of 15% to 19% and saturation from 5% to 60% were reported. Monitoring is in principle possible using an electromagnetic survey with a downhole vertical electric source and a horizontal electric field receiver on the seafloor. Computed model responses over a wide frequency range and for many depth locations of an electric current source show that both changes can be detected. Best detectability occurs when the current source is below the reservoir layer in case of changes differences can be detected above, inside and below the reservoir layer at frequencyies below 10 Hz. At a source operating frequency of 0.1 Hz maximum response difference between the two values in saturation occur when the source is 20 m above the top of the reservoir layer unil 100 m below the bottom. Only below the top of the reservoir there is almost no difference in the electric field amplitude between the two saturation levels below 10 Hz.

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