Morphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity
The accurate morphology identification of gas hydrate-bearing sediments (GHBS) has great significance in practical exploitation and subsequent resource evaluation. Previous studies have disclosed two main morphologies for gas hydrate in sediments: pore- and fracture-filling. However, the existing id...
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oai:doaj.org-article:2d8c4106dd76459397416a40bc0081792021-11-28T04:33:50ZMorphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity2352-484710.1016/j.egyr.2021.06.091https://doaj.org/article/2d8c4106dd76459397416a40bc0081792021-11-01T00:00:00Zhttp://www.sciencedirect.com/science/article/pii/S235248472100456Xhttps://doaj.org/toc/2352-4847The accurate morphology identification of gas hydrate-bearing sediments (GHBS) has great significance in practical exploitation and subsequent resource evaluation. Previous studies have disclosed two main morphologies for gas hydrate in sediments: pore- and fracture-filling. However, the existing identification methods of gas hydrate’s morphology rarely consider their intrinsic differences in distribution characteristics. In this paper, a new method is proposed to identify the morphology of hydrate according to the scattered distribution of fracture dips for fracture-filling GHBS. Firstly, numerical simulations are performed to study the relationships between the morphology of hydrate and the sonic velocities. Considering the dip variation is within a certain range for fracture-filling hydrate, the theoretical curves show that the resulting mutation degrees between P- and S-wave velocities are inconsistent in fracture-filling GHBS, which is different from pore-filling GHBS. Then the modified estimation method for pointwise Lipschitz exponent α is introduced to capture their differences. The cross plots of Lipschitz exponent for P-wave velocity, α(Vp), and Lipschitz exponent for S-wave velocity, α(Vs), indicate that most of the dots representing pore-filling GHBS are evenly distributed near the line α(Vp)=α(Vs), while the dots representing fracture-filling GHBS are scattered outside the line α(Vp)=α(Vs). Based on these characteristics, a ratio method is put forward to differentiate the two types of hydrate. These hypotheses and methods are verified using the measured P- and S-wave velocities log data at different sites in Leg 204, Ocean Drilling Program (ODP), in the United States. Finally, the results of this new method agree closely with core data.Xiangyu ZhuXuewei LiuElsevierarticleGas hydrateMorphologyP-wave velocityS-wave velocityLipschitz exponentElectrical engineering. Electronics. Nuclear engineeringTK1-9971ENEnergy Reports, Vol 7, Iss , Pp 8062-8074 (2021) |
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Gas hydrate Morphology P-wave velocity S-wave velocity Lipschitz exponent Electrical engineering. Electronics. Nuclear engineering TK1-9971 |
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Gas hydrate Morphology P-wave velocity S-wave velocity Lipschitz exponent Electrical engineering. Electronics. Nuclear engineering TK1-9971 Xiangyu Zhu Xuewei Liu Morphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity |
description |
The accurate morphology identification of gas hydrate-bearing sediments (GHBS) has great significance in practical exploitation and subsequent resource evaluation. Previous studies have disclosed two main morphologies for gas hydrate in sediments: pore- and fracture-filling. However, the existing identification methods of gas hydrate’s morphology rarely consider their intrinsic differences in distribution characteristics. In this paper, a new method is proposed to identify the morphology of hydrate according to the scattered distribution of fracture dips for fracture-filling GHBS. Firstly, numerical simulations are performed to study the relationships between the morphology of hydrate and the sonic velocities. Considering the dip variation is within a certain range for fracture-filling hydrate, the theoretical curves show that the resulting mutation degrees between P- and S-wave velocities are inconsistent in fracture-filling GHBS, which is different from pore-filling GHBS. Then the modified estimation method for pointwise Lipschitz exponent α is introduced to capture their differences. The cross plots of Lipschitz exponent for P-wave velocity, α(Vp), and Lipschitz exponent for S-wave velocity, α(Vs), indicate that most of the dots representing pore-filling GHBS are evenly distributed near the line α(Vp)=α(Vs), while the dots representing fracture-filling GHBS are scattered outside the line α(Vp)=α(Vs). Based on these characteristics, a ratio method is put forward to differentiate the two types of hydrate. These hypotheses and methods are verified using the measured P- and S-wave velocities log data at different sites in Leg 204, Ocean Drilling Program (ODP), in the United States. Finally, the results of this new method agree closely with core data. |
format |
article |
author |
Xiangyu Zhu Xuewei Liu |
author_facet |
Xiangyu Zhu Xuewei Liu |
author_sort |
Xiangyu Zhu |
title |
Morphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity |
title_short |
Morphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity |
title_full |
Morphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity |
title_fullStr |
Morphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity |
title_full_unstemmed |
Morphology identification of gas hydrate from pointwise Lipschitz regularity for P- and S-wave velocity |
title_sort |
morphology identification of gas hydrate from pointwise lipschitz regularity for p- and s-wave velocity |
publisher |
Elsevier |
publishDate |
2021 |
url |
https://doaj.org/article/2d8c4106dd76459397416a40bc008179 |
work_keys_str_mv |
AT xiangyuzhu morphologyidentificationofgashydratefrompointwiselipschitzregularityforpandswavevelocity AT xueweiliu morphologyidentificationofgashydratefrompointwiselipschitzregularityforpandswavevelocity |
_version_ |
1718408308236222464 |