Abstract

Trench-parallel subduction of mid-ocean ridges occurs frequently in plate motion history, such as along the western boundary of the Pacific plate in the early Cenozoic and along the eastern boundary of the Pacific plate at present. Such subduction may strongly alter the surface topography, volcanic activity and slab morphology in the mantle, whereas few studies have been conducted to investigate its evolutionary process. Here, we construct a 2-D viscoelastoplastic numerical model to study the modes and key parameters controlling trench-parallel subduction of mid-ocean ridges. Our model results show that the subduction modes of mid-ocean ridges can be primarily categorized into three types: the fast spreading mode, the slow spreading mode, and the extinction mode. The key factor controlling these subduction modes is the relative motion between the foregoing and the following oceanic plates, which are separated by the mid-ocean ridge. Different subduction modes exert different surface geological expressions, which may explain specific evolutionary processes related to mid-ocean ridge subduction, such as topographic deformation and the eruption gap of volcanic rocks in East Asia within 55–45 Ma and in the western North American plate during the late Cenozoic.

Highlights

  • A mid-ocean ridge (MOR) is a divergent boundary of plate tectonics where new plates are continuously generated (Turcotte and Schubert, 2002)

  • Based on our model results, we find that Δv is a key factor influencing the mode of trench-parallel subduction of the MOR

  • We construct a 2-D viscoelastoplastic model to study the modes and key parameters controlling the trench-parallel subduction of the mid-ocean ridge

Read more

Summary

Introduction

A mid-ocean ridge (MOR) is a divergent boundary of plate tectonics where new plates are continuously generated (Turcotte and Schubert, 2002). MORs are generally located at the centers of ocean basins, such as the present mid-Atlantic ridge, they may subduct into the deep mantle when tectonic environments cause MORs to move to ocean trenches (Georgieva et al, 2019). Typical examples include the subducted MOR between the Izanagi plate and the Pacific plate, which subducted at 55–45 Ma (Müller et al, 2016) and the subducted MOR between the Farallon plate and the Pacific plate, which subducted at 30–0 Ma (Ferrari et al, 2018). According to the contact angle between the MOR and the trench, MOR subduction can be divided into high-angle (trench-vertical) subduction and low-angle (trench-parallel) subduction (Wu and Wu, 2019)

Methods
Results
Discussion
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call