Abstract

Abstract A three-dimensional non-uniform magnetic modeling is proposed to obtain information about a magnetization of a seamount, which was divided into many blocks modeled by layered and rectangular prisms, and parameters were assigned to each block describing magnetic three components. Our data were the magnetic total force on the sea. A set of linear observation equations was formulated in terms of three components of magnetization for each block. The solution was obtained by using the conjugate gradients method because of its fast and accurate advantages of calculation. In this inversion, a common set of three components was defined for several blocks to decrease the number of unknown parameters. A computer program has been tested with artificial data and applied to data of Daiichi Kashima Seamount observed during the first phase of the Kaiko project carried out with the R/V Jean Charcot in 1984. In the real application, the crustal structure was divided into three layers (top depth to 5 km depth, 5–6.5 km depth and 6.5–8 km depth). The result of the inversion shows that the top portion and the submerged western half of this seamount are covered with the low magnetization layers, and in the middle layer (5–6.5 km depth) of eastern half side, declinations, inclinations and intensities are almost northward, 15° and 3–5 A/m, respectively. In the third layer (6.5–8 km depth), the reverse magnetizations are revealed in the southeastern and northern sides of Daiichi Kashima Seamount and around Katori Seamount. These reverse magnetizations may reflect part of the magnetic lineations of the Pacific plate.

Highlights

  • Seamount paleomagnetism is of particular interest and importance in the study of paleomagnetic field and oceanic plate motions, because it is extremely difficult to obtain fully-oriented samples from the oceans for laboratory paleomagnetic studies

  • With reference to the result by Ueda (1985), the crustal structure was divided into three layers, which were from minimum depth of studied area to 5 km depth, 5 km to 6.5 km depth and 6.5 km to 8 km depth as shown in Fig. 7, to evaluate differences among the top portion of the eastern half part of Daiichi Kashima Seamount (Layer 1), the lower part and the submerged western half part of the seamount (Layer 2), and the upper oceanic crust (Layer 3)

  • Discussions and Conclusions Ueda (1985) indicated that the magnetization vector defined by declination and inclination of the lower part of Daiichi Kashima Seamount (5.25–7 km depth in the eastern part and 6.5–8 km in the western part) were −12◦ and 20.1◦, respectively, and the intensity 10.7 A/m

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Summary

Introduction

Seamount paleomagnetism is of particular interest and importance in the study of paleomagnetic field and oceanic plate motions, because it is extremely difficult to obtain fully-oriented samples from the oceans for laboratory paleomagnetic studies. We shall apply our method to data of Daiichi Kashima Seamount observed during the first phase of the Kaiko project carried out with the R/V Jean Charcot in 1984 (Kaiko I Research Group, 1986).

Results
Conclusion
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