首页> 外文期刊>Journal of geophysical research. Solid earth: JGR >Subduction Initiation During Collision-Induced Subduction Transference: Numerical Modeling and Implications for the Tethyan Evolution
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Subduction Initiation During Collision-Induced Subduction Transference: Numerical Modeling and Implications for the Tethyan Evolution

机译:碰撞诱导的俯冲转移期间的俯冲开始:Tethyan演化的数值建模和影响

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The collision-induced subduction transference is a composite dynamic process including both the terrane collision/accretion and the subduction initiation (SI) at the neighboring passive margin. This process occurred repeatedly during the evolution of Tethyan systems, with multiple ribbon-like continents or microcontinents drifting from Gondwana in the southern hemisphere and accreting to the Eurasian continent since Paleozoic. In the previous numerical studies, the dynamics of terrane collision and induced SI are investigated individually, which however need to be integrated to study the controlling factors and time scales of collision-induced subduction transference. Systematic numerical models are conducted with variable properties of converging plates and different boundary conditions. The model results indicate that the forced convergence, rather than pure free subduction, is required to trigger and sustain the SI at the neighboring passive margin after terrane collision. In addition, a weak passive margin can significantly promote the occurrence of SI, by decreasing the required boundary force to reasonable value of plate tectonics. The lengths of subducted oceanic slab and accreting terrane play secondary roles in the occurrence of SI after collision. Under the favorable conditions of collision-induced subduction transference, the time required for SI after collision is generally short within 10 Myr, which is consistent with the general geological records of Cimmerian collision and the following Neo-Tethyan SI. In contrast, the stable Indian passive margin and absence of SI in the present Indian Ocean may he due to the low convergent force and/or the lack of proper weak zones, which remains an open question.
机译:碰撞诱导的俯冲转移是一种复合动态过程,包括邻近被动裕度的地落碰撞/增生和俯冲开始(SI)。该过程在Tethyan Systems的演变期间反复发生,其中多种带状的大陆或微直流素从南半球漂流到南半球的Gondwana,因为古生代以来对欧亚大陆的影响。在先前的数值研究中,单独研究了地落碰撞和诱导的Si的动态,但是需要集成,以研究碰撞诱导的俯冲转移的控制因素和时间尺度。系统数值模型采用融合板的可变性能和不同的边界条件进行。模型结果表明,强制收敛,而不是纯粹的自由俯冲,需要在地际碰撞之后触发和维持邻近被动边缘的SI。此外,通过将所需的边界力降低到平板构造的合理值,通过将所需的边界力降低,弱无源裕度可以显着促进Si的发生。碰撞后Si发生的底层海洋板和凸台的长度在Si发生中发挥次要作用。在碰撞诱导的郊区转移的有利条件下,碰撞后Si所需的时间通常在10中略微短暂,这与Cimmerian碰撞的总体地质记录一致,并且以下Neo-Tethyan Si一致。相比之下,目前印度洋中稳定的印度被动率和缺乏Si可能是由于较低的收敛力和/或缺乏适当的弱区,这仍然是一个开放的问题。

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