日本地球惑星科学連合2016年大会

講演情報

インターナショナルセッション(ポスター発表)

セッション記号 S (固体地球科学) » S-IT 地球内部科学・地球惑星テクトニクス

[S-IT12] Tectonic processes on the incoming plate seaward of the trench: Inputs to subduction zones

2016年5月23日(月) 17:15 〜 18:30 ポスター会場 (国際展示場 6ホール)

コンビーナ:*山野 誠(東京大学地震研究所)、森下 知晃(金沢大学理工研究域自然システム学系)、藤江 剛(海洋研究開発機構)、Straub Susanne(コロンビア大学ラモント地球科学研究所)

17:15 〜 18:30

[SIT12-P05] 人工電流源電磁探査による、沈み込み直前の太平洋プレート地殻比抵抗構造調査

*後藤 忠徳1笠谷 貴史2川田 佳史3市原 寛4山野 誠5 (1.京都大学大学院工学研究科、2.海洋研究開発機構、3.東北大学災害科学国際研究所、4.神戸大学大学院海事科学研究科、5.東京大学地震研究所)

キーワード:比抵抗、人工電流源電磁探査、太平洋プレート

In the Japan Trench subduction zone, an old oceanic plate with an age of over 100 m.y., the Pacific plate, is subducting beneath the northeast Japan arc. However, recent heat flow surveys have revealed that the Pacific plate just before subduction may not be uniformly cold contrary to its old age. Localized high heat flow anomalies suggest that thermal structure of the Pacific plate in this area is not a typical one for old oceanic lithosphere, at least at shallow depths. To evaluate the factors controlling the temperature structure (e.g., fractures, fluid etc., together with heat sources), we conducted dense heat flow surveys and electromagnetic soundings on the seaward slope of the Japan Trench. In this presentation, we focus on the preliminary result obtained by the electromagnetic soundings.
The offshore experiment was done on July, 2014 at the KY14-10 cruise (R/V Kaiyo, JAMSTEC). The water depth in the target area (on the Pacific plate, far off Tohoku region, Japan) is about 5300-5600 m. We used a newly-developed controlled-source electromagnetic (CSEM) survey system for this research. It can be applied to exploration of seafloor resistivity, originally designed for AUV but available with a deep-tow system (DT). The power for transmitter is supplied from the DT. Three pressure cases (transmitter, controller and power converter) are mounted on the DT frame, and a long cable with length of 350m is towed behind the DT. Two source electrodes attached at the both end of cable are used for transmitting the artificial electric current into the seawater. The pulse width for artificial current was 2 seconds, and the amplitude of current was approximately 20-30 A. Two CSEM profiles were conducted in this cruise. The altitude of DT (and the source dipole) was about 50-100m with towing speed of about 1 knot or less.
The preliminary results indicate the low resistivity of shallow layers of the oceanic crust of Pacific plate. The amplitude of received electric field recorded by an OBEM was about 0.04 nV/(Am^2) when the source-receiver separation was about 1km. The received signal can be clearly recognized within the source-receiver separations of about 4km. All of the amplitude of electric field is smaller than the predicted ones from a numerical simulation, with assuming the uniform sub-seafloor structure with 1 Ohm-m (and a sea water layer of 0.3 Ohm-m). This implies that the shallow part of oceanic crust (possibly less than 1km) have very low resistivity than 1 Ohm-m. The anomalous feature may be related to the buried fractures in the top of oceanic crust, and could be related to the fluid circulations, a candidate of factors to explain the high heat flow.