Sengan Geothermal Area, Northeast Japan


  • Topographic Map of the Sengan Geothermal Area

Topographic map of the Sengan Geothermal Area

Fig.1 Topographic map of the Sengan Geothermal Area, Northeast Japan (Okuma, 1998)
Contour interval is 100 m. The small and large boxes bounded by black solid lines show the close-up and the detail study area of Akita-Yakeyama volcano, respectively. The box bounded by blue solid lines show the detailed study area of Iwate-san volcano.


  • Simplified Geologic Map of the Sengan Geothermal Area

Geologic Map of the Sengan Geothermal Area

Fig.2 Geological map of the Sengan Geothermal Area modified from Research group for the geologic map of Sengan Geothermal Area (1985) and Suto (1992) (Okuma, 1998)
Younger Volcanic Rocks 1: Matsukawa Andesite, Younger Volcanic Rocks 2: Otsuki-yama volcanics, Younger Volcanic Rocks 3: Hachimantai volcanics and Kayo-dake volcanics, Younger Volcanic Rocks 4: Nanashigure-yama volcanics, Takakura-yama volcanics, Moriyoshi-yama volcanics, Akita-Yakeyama volcanics, Iwate-san volcanics and Akita-Komagatake volcanics.


Recently, detailed geologic maps have been compiled for the Sengan Geothermal Area (Research group for the geological map of Sengan Geothermal Area, 1985) and for Akita-Yakeyama volcano and its surrounding areas (Suto, 1992), respectively. These maps show that the geothermal area is covered widely by Quaternary volcanic rocks with outcrops of Pleistocene ones (Fig. 2). Drilling showed that the surface volcanic rocks are underlain by Neogene volcanic and sedimentary rocks in the Sengan Geothermal Area. The absence of pre-Neogene rocks inside the geothermal area and the presence of Paleozoic sedimentary rocks and Cretaceous granitic rocks outside the area suggest the existence of a large tectonic subsidence beneath the surface volcanic rocks.


  • Aeromagnetic Anomaly Map of the Sengan Geothermal Area

Aeromagnetic anomaly map of the Sengan Geothermal Area

Fig.3 Total intensity aeromagnetic anomaly (IGRF residuals) map of the Sengan Geothermal Area (Okuma, 1998).
Contour interval is 25 nT. The altitude of datum plane is 1,800 m above sea level. See also Fig.1.


Magnetic features

In conjunction with various geophysical surveys, an aeromagnetic survey for geothermal exploration was conducted in the Sengan Geothermal Area (MITI, 1978). Okuma and Suto (1986) recompiled aeromagnetic anomaly maps from the original anomaly data. The observed magnetic anomalies (Fig. 3) are influenced strongly by the effect of topographic relief. The volcanic rocks which compose the terrain have their magnetic properties, strong enough to cause intensive magnetic anomalies. Magnetic highs and lows lie in the southern and northern flanks of many volcanoes: Iwate-san volcano, Takakura-yama volcano, Akita-Komagatake volcano, Maemori-yama volcano, Nanashigure-yama volcano and Moriyoshi-yama volcano, etc. On the contrary, such simple relationship between the topography and magnetic anomalies has not been observed for Akita-Yakeyama volcano, Hachimantai volcano, Kayo-dake volcano, etc.


Magnetization Intensity Mapping

To remove the effects of magnetic terrain, an apparent magnetization intensity mapping method (Okuma et al., 1994; Nakatsuka, 1995) was adopted to the magnetic anomalies of the Sengan Geothermal Area. These methods were useful for revealing concealed old volcanic edifices on Izu-Oshima Island (Okuma et al., 1994) and the quadratic distribution pattern of magnetization intensity along the Tanna fault, presumably caused by movements of the strike-slip fault (Nakatsuka, 1995).

Magnetic model for a magnetization intensity mapping

Fig. 4 Magnetic model employed for an apparent magnetization intensity mapping

Mij: Magnetization of a prism at ij-th point, Tij: Synthetic magnetic anomaly at ij-th point
ZijU: Top depth of a prism at ij-th point, ZijL: Bottom depth of a prism at ij-th point


A magnetic model composed of finite rectangle prisms that corresponds to the volcanic terrain (Fig. 4) was assumed. Each prism is magnetized uniformly in a direction of the present Earth's magnetic field. Magnetization intensities vary only laterally among the prisms. The top depth of the model corresponds to the ground surface, while the bottom depth corresponds to a flat surface, though it can be assumed to be of any shape. A flat surface of 5 km below sea level was used for the bottom depth of the magnetic model, taking account of a local shallow Curie depth (< 8 km) (Okubo et al., 1989). A magnetization intensity of a prism at ij-th point can be inverted from the observed magnetic anomaly by employing the conjugate gradient method (Nakatsuka, 1995) instead of solving simultaneous linear equations directly.


  • Apparent Magnetization Intensity Map of the Sengan Geothermal Area

Magnetization intensity map of the Sengan Geothermal Area

Fig.5 Magnetization intensity map of the Sengan Geothermal Area with a topographic shading (Okuma, 1998).
Contour interval is 0.2 A/m. The areas bounded by solid lines indicate hydrothermal altered areas. Solid and open circles locate volcanic rocks which are normally and reversely magnetized, respectively. Paleomagnetic data (Suto, 1985; Suto, 1987; Suto and Mukoyama, 1987; Suto, 1992) which have stable magnetization intensities (
³1.0 A/m ) with magnetic pole latitudes (³ |±50°|) were plotted. See also Fig. 1.


Characteristics of the distribution of magnetization intensities

(1) Magnetization highs lie obviously on Quaternary volcanoes such as Maemori-yama volcano, Iwate-san volcano, Obuka-dake volcano, Takakura-yama volcano and Akita-Komagatake volcano (Fig. 5). This result clearly shows that each edifice is roughly magnetized in a direction of the present earthÕs magnetic field.

(2) On the other hand, obvious magnetization lows lie on Kurasawa-yama and Kayo-dake volcano. Paleomagnetic dada indicate that normally magnetized volcanic rocks are distributed in high magnetization areas, whereas reversely magnetized rocks are in low magnetization areas. This relationship is much clearer than that of Okuma and Suto (1987).

(3) Magnetization lows with small amplitudes, or rather to say weak magnetization areas, correspond to hydrothermally altered areas mapped by Research group for the geological map of Sengan Geothermal Area (1985); weak magnetizations lie on and around the summit of Akita-Yakeyama volcano, between Sumikawa and Onuma, in Matsukawa and Kakkonda, between Takakura-yama and Akita-Komagatake volcanoes, etc. It is implied that hydrothermal alterations caused a loss of a large amount of magnetic minerals in volcanic rocks. Recently, young granitic intrusions have been found in Kakkonda area, one of weak magnetization areas, by drilling. A temperature of the bodies exceeded 600
¡C at the bottom of a drill hole close to the Kakkonda geothermal power plant. On the basis of the results, the apparent magnetization intensity method is useful to estimate the location of hydrothermal areas in Quaternary volcanic areas.

More Detailed Information

[Iwate-san volcano]

[Akita-Yakeyama volcano]





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