TY - JOUR
T1 - Structural controls on the 1998 volcanic unrest at Iwate volcano
T2 - Relationship between a shallow, electrically resistive body and the possible ascent route of magmatic fluid
AU - Aizawa, Koki
AU - Ogawa, Yasuo
AU - Mishina, Masaaki
AU - Takahashi, Kosuke
AU - Nagaoka, Shintaro
AU - Takagi, Nobumasa
AU - Sakanaka, Shin'ya
AU - Miura, Takuya
N1 - Funding Information:
The geomagnetic data used for remote-reference processing were kindly provided by the Esashi Geomagnetic Observatory, Geographical Survey Institute. We acknowledge S. Tanaka at JAMSTEC for generously providing hypocenter data. The geodetic model was kindly provided by M. Sato at Hakusan Corporation. We acknowledge the New Energy and Industrial Technology Development Organization (NEDO) for permitting the reproduction of well-log data from an open-file report. J. Ito and N. Doi are thanked for providing ongoing advice during the project. M. Utsugi provided light-weight batteries suitable for undertaking field surveys in mountainous areas. Careful reviews and critical comments by Jean-François Lénat and an anonymous reviewer improved an early version of the manuscript. One of the authors (K.A.) acknowledges the support of a JSPS fellowship.
Copyright:
Copyright 2009 Elsevier B.V., All rights reserved.
PY - 2009/10/30
Y1 - 2009/10/30
N2 - Magnetotelluric (MT) measurements were conducted at Iwate volcano, across the entirety of the mountain, in 1997, 1999, 2003, 2006, and 2007. The survey line was 18 km in length and oriented E-W, comprising 38 measurements sites. Following 2D inversion, we obtained the resistivity structure to a depth of 4 km. The surface resistive layer (~ several hundreds of meters thick) is underlain by extensive highly conductive zones. Based on drilling data, the bottom of the highly conductive zone is interpreted to represent the 200 °C isotherm, below which (i.e., at higher temperatures) conductive clay minerals (smectite) are rare. The high conductivity is therefore mainly attributed to the presence of hydrothermally altered clay. The focus of this study is a resistive body beneath the Onigajo (West-Iwate) caldera at depths of 0.5-3 km. This body appears to have impeded magmatic fluid ascent during the 1998 volcanic unrest, as inferred from geodetic data. Both tectonic and low-frequency earthquakes are sparsely distributed throughout this resistive body. We interpret this resistive body as a zone of old, solidified intrusive magma with temperatures in excess of 200 °C. Given that a similar relationship between a resistive body and subsurface volcanic activity has been suggested for Asama volcano, structural controls on subsurface magmatic fluid movement may be a common phenomenon at shallow levels beneath volcanoes.
AB - Magnetotelluric (MT) measurements were conducted at Iwate volcano, across the entirety of the mountain, in 1997, 1999, 2003, 2006, and 2007. The survey line was 18 km in length and oriented E-W, comprising 38 measurements sites. Following 2D inversion, we obtained the resistivity structure to a depth of 4 km. The surface resistive layer (~ several hundreds of meters thick) is underlain by extensive highly conductive zones. Based on drilling data, the bottom of the highly conductive zone is interpreted to represent the 200 °C isotherm, below which (i.e., at higher temperatures) conductive clay minerals (smectite) are rare. The high conductivity is therefore mainly attributed to the presence of hydrothermally altered clay. The focus of this study is a resistive body beneath the Onigajo (West-Iwate) caldera at depths of 0.5-3 km. This body appears to have impeded magmatic fluid ascent during the 1998 volcanic unrest, as inferred from geodetic data. Both tectonic and low-frequency earthquakes are sparsely distributed throughout this resistive body. We interpret this resistive body as a zone of old, solidified intrusive magma with temperatures in excess of 200 °C. Given that a similar relationship between a resistive body and subsurface volcanic activity has been suggested for Asama volcano, structural controls on subsurface magmatic fluid movement may be a common phenomenon at shallow levels beneath volcanoes.
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U2 - 10.1016/j.jvolgeores.2009.08.009
DO - 10.1016/j.jvolgeores.2009.08.009
M3 - Article
AN - SCOPUS:70349783547
SN - 0377-0273
VL - 187
SP - 131
EP - 139
JO - Journal of Volcanology and Geothermal Research
JF - Journal of Volcanology and Geothermal Research
IS - 1-2
ER -