Elsevier

Tectonophysics

Volume 302, Issues 3–4, 28 February 1999, Pages 287-296
Tectonophysics

Restoration of the depression structure at the eastern part of central Kyushu, Japan by means of dislocation modeling

https://doi.org/10.1016/S0040-1951(98)00287-XGet rights and content

Abstract

We have attempted to restore a subsurface structure in the eastern part of central Kyushu, Japan, by combining fault motions which were modeled as dislocation planes embedded in an elastic isotropic half space. The simulated crustal deformation pattern was compared with the subsurface structures estimated from gravity anomalies and/or seismic prospecting. The modeling procedure successfully restored all tectonic basins in the area without any need for motive forces for uplift or subsidence. The results also suggest that two major tectonic events have occurred in this region. Those are (1) the formation of half-graben caused by north–south extension, and (2) the formation of the pull-apart basin caused by east–west compression.

Introduction

Subsurface structure shows the present contemporary static basement form, and is also considered to indicate the accumulated result of crustal deformation in the past. Accordingly, the restoration of a subsurface structure provides us important information on the tectonic history of the region concerned.

There are a number of alternative approaches to basin structure restoration. Katzman et al. (1995), for instance, employed the Boundary Element Method for the study of tectonics in the Dead Sea. However, in our paper, a dislocation model was used to restore the subsurface structures by calculating the extent of static vertical displacement caused by fault motion, which is obtained as a superposition of analytical solutions for dislocation planes embedded in an elastic isotropic half space (Rodgers, 1980). If the subsurface structures are actually formed by fault motions, they should be restored by combining dislocation plane motions.

As Chinnery and Petrak (1968), Katzman et al. (1995)or others have pointed out, the dislocation model has the disadvantage of a so called `edge effect' which causes singularities at the edges of the fault plane. This effect is due to the unrealistic assumption of a constant discontinuity over the fault plane, and causes indeterminate displacement and infinite stress at the edges. In spite of this disadvantage, we employed the dislocation model because it is a simple calculation which represents the essential characteristics of regional tectonic movements and does not require the assumption of a dynamic frictional constant over the fault plane.

The eastern part of central Kyushu is a key area for understanding the tectonic history of Southwest Japan because the region is located at an intersection of tectonic lines and is near an inflection point of the subducting Philippine Sea plate margin (Fig. 1). This region is also characterized by gravity lows which are caused by the tectonic and volcanic depression structures. Although many studies have discussed the formation of the region, a definitive model of the mechanical formation has not been established so far. We therefore propose the following dislocation model as one important aspect of our understanding of the tectonic history of the region.

Section snippets

Location and fundamental geology

The eastern part of central Kyushu, Japan, is the junction between the Honshu-arc and Ryukyu-arc. It is located at the western end of the Median Tectonic Line (MTL) which is the largest right-lateral tectonic line in Southwest Japan. It is also at the eastern end of the Oita–Kumamoto Tectonic Line [OKTL; the buried fault which is estimated from the steep gradient in gravity anomaly and is considered to be the western extension of an older MTL (Kamata, 1992)] and the Kurume–Hiji Line (KHL, Kido,

Model

In the modeling procedure, tectonic lines were modeled as dislocation planes embedded in an elastic isotropic half space. Although the method is almost the same as that used by Rodgers (1980), we employed Okada's dislocation plane (Okada, 1985) for the calculation rather than that of Chinnery (1961), since the former permits easier change of dip angle (Fig. 5). In our modeling, the locations of tectonic lines correspond to the traces at the surface (Fig. 6). The other parameters are assigned as

Discussion

Because the dislocation modeling did not consider the effects of interactions between faults, the results obtained here show some differences in vertical displacement compared with results from 3-D numerical modeling in which the fault interaction is considered implicitly (e.g., Katzman et al., 1995; ten Brink et al., 1996). However, the distribution of the subsidence and uplift is not so different. Thus, we employed the dislocation modeling in this study.

In the modeling of the half-graben, we

Conclusion

In this paper, we employed a dislocation model for restoration of subsurface structures. Although the dislocation model in an elastic medium has an excessive concentration of vertical deformation at the edge of the fault and can not consider the effect of interactions between faults, the model retains simplicity and is of sufficient accuracy to restore the local subsurface structures to first order and to provide a meaningful basis for discussion of the local tectonic history.

We applied the

Acknowledgements

We are thankful to H. Kerr and U.S. ten Brink for their careful reviews of the paper and helpful comments on the manuscript. We also wish to express sincere thanks to J.P. Matthews for critical reading of the manuscript. This work was partly supported by a Grant in Aid for Scientific Research from the Ministry of Education, Science, Sports and Culture of Japan (No. 08454132).

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