Department of Geology and Geophysics, Yale University, New Haven, Connecticut 06520-8109, USA.
Laboratoire de Géologie de Lyon, Université de Lyon 1, CNRS, ENS-Lyon, 69622 Villeurbanne Cedex, France.
Nature. 2014 Apr 24;508(7497):513-6. doi: 10.1038/nature13072. Epub 2014 Apr 6.
The initiation of plate tectonics on Earth is a critical event in our planet's history. The time lag between the first proto-subduction (about 4 billion years ago) and global tectonics (approximately 3 billion years ago) suggests that plates and plate boundaries became widespread over a period of 1 billion years. The reason for this time lag is unknown but fundamental to understanding the origin of plate tectonics. Here we suggest that when sufficient lithospheric damage (which promotes shear localization and long-lived weak zones) combines with transient mantle flow and migrating proto-subduction, it leads to the accumulation of weak plate boundaries and eventually to fully formed tectonic plates driven by subduction alone. We simulate this process using a grain evolution and damage mechanism with a composite rheology (which is compatible with field and laboratory observations of polycrystalline rocks), coupled to an idealized model of pressure-driven lithospheric flow in which a low-pressure zone is equivalent to the suction of convective downwellings. In the simplest case, for Earth-like conditions, a few successive rotations of the driving pressure field yield relic damaged weak zones that are inherited by the lithospheric flow to form a nearly perfect plate, with passive spreading and strike-slip margins that persist and localize further, even though flow is driven only by subduction. But for hotter surface conditions, such as those on Venus, accumulation and inheritance of damage is negligible; hence only subduction zones survive and plate tectonics does not spread, which corresponds to observations. After plates have developed, continued changes in driving forces, combined with inherited damage and weak zones, promote increased tectonic complexity, such as oblique subduction, strike-slip boundaries that are subparallel to plate motion, and spalling of minor plates.
地球板块构造的启动是我们星球历史上的一个关键事件。最初的原俯冲(约 40 亿年前)和全球构造(约 30 亿年前)之间的时间滞后表明,板块和板块边界在 10 亿年的时间内广泛分布。造成这种时间滞后的原因尚不清楚,但对于理解板块构造的起源至关重要。在这里,我们提出,当足够的岩石圈损伤(促进剪切局部化和长期存在的弱区)与瞬态地幔流和迁移的原俯冲相结合时,它会导致弱板块边界的积累,并最终导致由俯冲单独驱动的完全形成的构造板块。我们使用具有复合流变学的晶粒演化和损伤机制(与多晶岩石的野外和实验室观测兼容)来模拟这个过程,该机制与压力驱动的岩石圈流动的理想化模型相结合,其中低压区相当于对流下降的抽吸。在最简单的情况下,对于类地条件,几个连续的驱动力场旋转会产生遗留的损伤弱区,这些弱区被岩石圈流动继承,形成一个几乎完美的板块,具有被动扩张和走滑边界,即使只有俯冲驱动,这些边界也会持续存在并进一步局部化。但对于更热的表面条件,如金星上的条件,损伤的积累和继承可以忽略不计;因此,只有俯冲带幸存下来,板块构造不会扩散,这与观测结果一致。在板块形成后,驱动力的持续变化,加上继承的损伤和弱区,会促进构造复杂性的增加,如斜向俯冲、与板块运动平行的走滑边界,以及小板块的剥落。