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I. Seafloor morphology of the Osbourn Trough and Kermadec Trench and II. Multiscale dynamics of subduction zones

机译:I. Osbourn Trough和Kermadec Trench和II的海底形态。俯冲带的多尺度动力学

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摘要

This thesis aims to demonstrate that integration of detailed observations of deformation at short to long length scales with carefully formulated numerical modeling is an effective method for simulating the complex multiscale nature of mantle-lithosphere dynamics. In Part I, marine geophysical observations are used to determine the origin of the Osbourn Trough, a long linear depression within the Pacific Plate seaward of the Tonga-Kermadec Trench, and to determine the elastic strength of the subducting plate within the Kermadec Trench. Based on the morphology of the seafloor from swath bathymetry mapping and modeling of magnetic data, we conclude that the Osbourn Trough is an extinct spreading center which stopped spreading about 72 million years ago. Swath bathymetry mapping within the Kermadec Trench reveals extensive faulting within the trench on the subducting plate, with oblique grabens aligned perpendicular to the absolute plate motion direction. Using isostatic flexural response methods, we find that the flexural rigidity (1e19-1e20 Nm) is smaller than normally found for old oceanic lithosphere reflecting a local reduction in the strength of the plate.ududIn Part II, regional 3-D dynamic models of the Tonga-Kermadec and Aleutian subduction zones are used to constrain lateral variations in viscosity in the upper mantle. Modeling of the dynamic topography of the overriding plate for the Tonga-Kermadec subduction zone requires a low viscosity and low density (-20 kg/m^3) region within the wedge above the slab to decouple the slab-induced flow from. These efforts lead to a good fit to the observed shallow bathymetry on the overriding plate for a model with a slab density anomaly due to temperature of ~80 kg/m^3. However, the geoid anomaly above the subduction zone is too large by 20-40 m at length scales of 100-1000 km. A reduction of the slab density by a factor of 1.5 is needed to match both the geoid and topography, suggesting the density anomaly of the slab due to temperature is compensated within the upper mantle (~100-300 km). Similar modeling for the Aleutians including a narrower low viscosity region and smaller density anomaly (-10 kg/m^3) in the wedge is able to fit the geoid and topography without reducing the slab density.
机译:本文旨在证明,将短至长尺度的详细变形观测与精心制定的数值模型相结合,是一种模拟地幔-岩石圈动力学复杂的多尺度性质的有效方法。在第一部分中,海洋地球物理观测被用于确定奥斯本海槽的起源,该区域是汤加-克马德克海沟太平洋板块海中的一个长线性凹陷,并确定了克马德克海槽内俯冲板的弹性强度。根据条幅测深法制图的海底形态和磁数据建模,我们得出结论,奥斯本海槽是一个灭绝的传播中心,大约在7200万年前就停止了传播。克马德克海沟内的测深图显示了俯冲板上沟槽内的广泛断层,倾斜,片垂直于板的绝对运动方向排列。使用等静挠曲响应方法,我们发现挠曲刚度(1e19-1e20 Nm)小于正常的旧岩石圈的反射刚度,反映了板块强度的局部降低。 ud ud第二部分,区域3-D动态Tonga-Kermadec和Aleutian俯冲带的模型被用来限制上地幔粘度的横向变化。汤加-克马德克俯冲带上覆板的动态地形建模需要在板坯上方的楔块内形成一个低粘度和低密度(-20 kg / m ^ 3)的区域,以使板坯引起的水流脱离。这些努力导致了由于温度为〜80 kg / m ^ 3而导致板坯密度异常的模型在上覆板上观测到的浅测深很好地拟合。但是,俯冲带上方的大地水准面异常在100-1000 km的长度尺度上太大了20-40 m。为了使大地水准面和地形匹配,需要将板坯密度降低1.5倍,这表明由于温度引起的板坯密度异常在上地幔(约100-300 km)内得到了补偿。对于阿留申群岛而言,在楔形体中包括较窄的低粘度区域和较小的密度异常(-10 kg / m ^ 3)的类似模型能够拟合大地水准面和地形,而不会降低板坯密度。

著录项

  • 作者

    Billen Magali Isabelle;

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  • 年度 2002
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