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Postseismic Afterslip, Viscoelastic Mantle Flow, and the Earthquake Cycle at the Nankai Trough Subduction Zone

机译:南海海槽俯冲带的地震后滑,粘弹性地幔流动和地震周期

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摘要

Historical leveling data and recent GPS measurements in the Shikoku region of southwestern Japan record 120 years of vertical crustal motions spanning the 1944 and 1946 M8+ earthquakes. We develop 2D boundary element models of the earthquake cycle at the Nankai Trough that incorporate a subducting elastic slab with a Maxwell viscoelastic mantle wedge and subducting mantle lithosphere. We impose repeated earthquakes on the shallow subduction interface and model rate-strengthening creep at greater depths. The model parameters are systematically modified using known coseismic rupture zones and thermal models as geometric constraints to numerically fit vertical deformation profiles to the vertical data in the co-, inter-, and post-seismic periods. Previous models neglecting mantle flow (elastic half-space models with rate-strengthening creep) or neglecting the subducting elastic slab (elastic plate models) fit vertical displacement data near the coastline reasonably well for most time periods throughout the earthquake cycle but are unable to account for the observed inland subsidence during the postseismic and mid-interseismic periods. We show that models including both rate-strengthening creep, viscoelastic mantle flow with viscosities of order 1019 Pa s (mantle relaxation times of 10--25 years) capture the observed vertical deformation profile spanning the entire earthquake cycle in central Shikoku and along the west coast of the Kii peninsula. These results indicate that both afterslip and mantle flow contribute significantly to the postseismic and mid inter-seismic periods. However, recognition that our mantle flow model requires a higher viscosity to fit data later in the earthquake cycle suggests the simplified single Maxwell viscosity is not sufficient to explain deformation at all time periods. 3D models with multiple mantle viscosities or nonlinear, stress-dependent viscosity are a likely needed to explain data for all time periods.
机译:日本西南部四国地区的历史水准数据和最近的GPS测量结果记录了1944年和1946年M8 +地震的120年垂直地壳运动。我们开发了南开海槽地震周期的二维边界元模型,该模型结合了具有麦克斯韦粘弹性地幔楔和俯冲地幔岩石圈的俯冲弹性板。我们在浅层俯冲界面上施加了多次地震,并在更大深度模拟了速率增强蠕变。使用已知的同震破裂带和热模型作为几何约束条件,可以对模型参数进行系统地修改,以便在同震,震中和震后周期中将垂直变形剖面数值拟合到垂直数据中。以前忽略地幔流的模型(具有速率强化蠕变的弹性半空间模型)或忽略俯冲弹性板的模型(弹性板模型)在整个地震周期的大部分时间段内都很好地拟合了海岸线附近的垂直位移数据,但无法解释在地震后和中间地震期间观测到的内陆沉降。我们表明,模型包括速率强化蠕变,粘弹性地幔流(粘度为1019 Pa s s)(地幔弛豫时间为10--25年),都捕获了横跨四国中部和西部整个地震周期的垂直变形剖面基伊半岛的海岸。这些结果表明,后滑流和地幔流都对地震后和中期地震间有重要贡献。但是,认识到我们的地幔流动模型需要更高的粘度才能在地震周期的后期拟合数据,这表明简化的单一麦克斯韦粘度不足以解释所有时间段的变形。要解释所有时间段的数据,可能需要具有多种地幔粘度或非线性的,与应力有关的粘度的3D模型。

著录项

  • 作者

    Tebo, Douglas Wayne.;

  • 作者单位

    Indiana University.;

  • 授予单位 Indiana University.;
  • 学科 Geophysics.
  • 学位 M.S.
  • 年度 2018
  • 页码 61 p.
  • 总页数 61
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-17 11:53:06

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