Duration of the lunar overturn during magma ocean crystallization

1Line Colin, 1Stéphane Labrosse, 1Chloé Michaut, 2Adrien Morison
Earth and Planetary Science Letters 690, 120164 Open Access Link to Article [https://doi.org/10.1016/j.epsl.2026.120164]
1Laboratoire de Géologie de Lyon: Terre, Planète, Environnement, Ecole Normale Supérieure de Lyon, Université de Lyon, Université Claude Bernard Lyon 1, Lyon,France
2Research Software Engineering, MVLS SRF, University of Glasgow, Glasgow,United Kingdom
Copyright Elsevier

The Moon presents a striking asymmetry between the nearside, which concentrates the lunar mare and shows a thin crust, and the farside, composed of thick anorthosite terranes. One proposed explanation for this asymmetry is a mantle overturn, driven by the instability of a dense, ilmenite-rich layer at the top of cumulates near the end of lunar magma ocean solidification. However, thermal instabilities may arise before the crystallization of this dense layer. In particular, material exchange by melting and crystallization at the magma ocean-cumulates boundary facilitates flow through the boundary and hence the onset of convection in the cumulates. Accounting for this flow-through interface, we investigate the onset and duration of a thermal overturn using linear stability analysis and direct numerical simulations. Our results show that a thermal overturn can initiate well before the end of magma ocean solidification, lasting from ten thousand years to tens of millions of years. The dominant convective mode corresponds to a spherical harmonic of degree one and could affect crustal growth and stabilization if the top interface is sufficiently flow-through and the Rayleigh number not too large. Taking into account the thermal evolution of the core, this early overturn could generate an early lunar dynamo.

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