TY - JOUR
T1 - Estimation of Spatial Distribution and Fluid Fraction of a Potential Supercritical Geothermal Reservoir by Magnetotelluric Data
T2 - A Case Study From Yuzawa Geothermal Field, NE Japan
AU - Ishizu, Keiichi
AU - Ogawa, Yasuo
AU - Nunohara, Keishi
AU - Tsuchiya, Noriyoshi
AU - Ichiki, Masahiro
AU - Hase, Hideaki
AU - Kanda, Wataru
AU - Sakanaka, Shinya
AU - Honkura, Yoshimori
AU - Hino, Yuta
AU - Seki, Kaori
AU - Tseng, Kuo Hsuan
AU - Yamaya, Yusuke
AU - Mogi, Toru
N1 - Funding Information:
This work was supported by the Japan Society for the Promotion of Science KAKENHI (20K22326 and 21109003). One of the authors (K. Ishizu) would like to acknowledge the support from the Hiki Foundation, Tokyo Institute of Technology. The authors thank W. Siripunvaraporn for allowing us to use WSINV3DMT, and T. Okada for providing seismic data and velocity models. The authors are grateful to N. Watanabe for helpful discussions on the resistivity of supercritical fluids, Y. Kawada for meaningful discussions on supercritical fluids, R. Yamada for his help with the geological interpretation of the resistivity model and A. Kelbert for her help in archiving our MT data. The authors would like to thank two anonymous reviewers, the associate editor M. Moorkamp and the editor D. Schmitt for their detailed and helpful comments that led to significant improvements in this article.
Publisher Copyright:
© 2022. The Authors.
PY - 2022/2
Y1 - 2022/2
N2 - Fluids within the Earth's crust may exist under supercritical conditions (i.e., >374°C and >22.1 MPa for pure water). Supercritical geothermal reservoirs at depths of 2–10 km below the surface in northeastern (NE) Japan mainly consist of magmatic fluids that exsolved from the melt during the course of fractional crystallization. Supercritical geothermal reservoirs have received attention as next-generation geothermal resources because they can offer significantly more energy than that obtained from conventional geothermal reservoirs found at temperatures <350°C. However, the spatial distribution and fluid fraction of supercritical geothermal reservoirs, which are required for their resource assessment, are poorly understood. Here, the magnetotelluric (MT) method with electrical resistivity imaging is used in the Yuzawa geothermal field, NE Japan, to collect data on the fluid fraction and spatial distribution of a supercritical geothermal reservoir. The collected MT data reveal a potential supercritical geothermal reservoir (>400°C) with dimensions of 3 km (width) × 5 km (length) at a depth of 2.5–6.0 km below the surface. The estimated fluid fraction of the reservoir is 0.1%–4.2% with salinity values of 5–10 wt%. The melt is also imaged below the reservoir, and based on the resistivity model; we develop a mechanism for the evolution of the supercritical geothermal reservoir, wherein upwelling supercritical fluids supplied from the melt are trapped under less permeable silica sealing and accumulate there.
AB - Fluids within the Earth's crust may exist under supercritical conditions (i.e., >374°C and >22.1 MPa for pure water). Supercritical geothermal reservoirs at depths of 2–10 km below the surface in northeastern (NE) Japan mainly consist of magmatic fluids that exsolved from the melt during the course of fractional crystallization. Supercritical geothermal reservoirs have received attention as next-generation geothermal resources because they can offer significantly more energy than that obtained from conventional geothermal reservoirs found at temperatures <350°C. However, the spatial distribution and fluid fraction of supercritical geothermal reservoirs, which are required for their resource assessment, are poorly understood. Here, the magnetotelluric (MT) method with electrical resistivity imaging is used in the Yuzawa geothermal field, NE Japan, to collect data on the fluid fraction and spatial distribution of a supercritical geothermal reservoir. The collected MT data reveal a potential supercritical geothermal reservoir (>400°C) with dimensions of 3 km (width) × 5 km (length) at a depth of 2.5–6.0 km below the surface. The estimated fluid fraction of the reservoir is 0.1%–4.2% with salinity values of 5–10 wt%. The melt is also imaged below the reservoir, and based on the resistivity model; we develop a mechanism for the evolution of the supercritical geothermal reservoir, wherein upwelling supercritical fluids supplied from the melt are trapped under less permeable silica sealing and accumulate there.
KW - fluid
KW - magmatic fluid
KW - melt
KW - northeastern Japan
KW - resistivity
KW - supercritical geothermal reservoir
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U2 - 10.1029/2021JB022911
DO - 10.1029/2021JB022911
M3 - Article
AN - SCOPUS:85125416556
SN - 2169-9313
VL - 127
JO - Journal of Geophysical Research: Solid Earth
JF - Journal of Geophysical Research: Solid Earth
IS - 2
M1 - e2021JB022911
ER -