首页> 外文期刊>Journal of geophysical research. Solid earth: JGR >Evolution of Subduction Zone Curvature and its Dependence on the Trench Velocity and the Slab to Upper Mantle Viscosity Ratio
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Evolution of Subduction Zone Curvature and its Dependence on the Trench Velocity and the Slab to Upper Mantle Viscosity Ratio

机译:俯冲带曲率的演变及其对海槽速度和板对上地幔粘度比的影响

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Three-dimensional laboratory models of upper mantle subduction are presented investigating the effect of the trench velocity (v_t) and the slab to upper mantle viscosity ratio (η_(SP)/η_(UM)) on trench curvature and slab curvature. One set of experiments varies η_(SP)/η_(UM) from 66 to 1375. Another set of experiments modifies v_t through applying different velocities at the trailing plate. The results show that the radius of trench curvature (R_(TC)) progressively decreases with continuous trench retreat due to quasi-toroidal mantle return flow from the subslab region around the lateral slab edges and toward the mantle wedge region, but starts to increase when trench retreat changes to trench advance due to quasi-toroidal return flow in the opposite direction. Furthermore, RTC increases with increasing η_(SP)/η_(UM) (i.e., progressively stronger slabs are progressively less curved) following a cubic root function. The force required to curve the slab and trench varies with progressive subduction, but is only 0.1-2.5% of the total negative buoyancy force of the slab, while the viscous dissipation rate due to progressive slab curvature is only 0.01-0.60% of the potential energy release rate. Comparison of trench curvature in the models (scaled slab width w = 750 km) with that of the Scotia subduction zone (w ≈ 800 km) indicates that for the Scotia subduction zone the effective ≈ is of the order 1-2 x 10~2. Finally, the elastic sphere indentation model for arc curvature is revisited, demonstrating that four main predictions are not met by observations, implying that the model should be rejected.
机译:提出了上地幔俯冲的三维实验室模型,研究了沟槽速度(v_t)和平板与上地幔的黏度比(η_(SP)/η_(UM))对沟槽曲率和平板曲率的影响。一组实验将η_(SP)/η_(UM)从66更改为1375。另一组实验通过在尾随板上施加不同的速度来修改v_t。结果表明,由于准环形地幔返回流从次平板区域围绕着平板侧缘向着地幔楔区域流动,沟槽曲率半径(R_(TC))随着沟槽的连续退缩而逐渐减小,但当由于准环形回流沿相反的方向,沟槽后退改变为沟槽前进。此外,遵循立方根函数,RTC随着η_(SP)/η_(UM)的增加而增加(即,逐渐变强的平板弯曲度逐渐减小)。弯曲平板和沟槽所需的力随渐进的俯冲而变化,但仅占平板总负浮力的0.1-2.5%,而渐进的平板曲率引起的粘性耗散率仅为电势的0.01-0.60%能量释放率。将模型中的沟槽曲率(标定板宽w = 750 km)与斯科舍俯冲带(w≈800 km)进行比较表明,对于斯科舍俯冲带,有效≈约为1-2 x 10〜2 。最后,重新讨论了用于弧曲率的弹性球体压痕模型,表明观察结果未满足四个主要预测,这意味着应该拒绝该模型。

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