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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Spohn, T.
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Topics
Publications (7/7 displayed)
- 2019The Thermal, Mechanical, Structural, and Dielectric Properties of Cometary Nuclei After Rosettacitations
- 2014Internal state of Lutetia as a function of the macroporosity
- 2014Core and crust formation on Vesta: Controlling factors
- 2014Modeling of planetesimal compaction by hot pressing
- 2014Controls on the differentiation of Vesta
- 2012Numerical modelling of accretion, sintering and differentiation of asteroid 4 Vesta
- 2012Differentiation and core formation in accreting planetesimalscitations
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document
Controls on the differentiation of Vesta
Abstract
Recent observations by Dawn confirmed Vesta as a differentiated body with an iron-rich core, a silicate mantle, and a basaltic crust. Its core radius is estimated to be 105-126 km [1] and its crust to be at least 30-45 km thick [2]. Vesta is the only known intact differentiated asteroid and is widely held as the parent body of the HED meteorites. The origin of the HEDs is closely related to the differentiation history. The chronological records of HEDs seem to indicate that the core-mantle differentiation likely precedes the mantle-crust differentiation [3]. However, the formation scenarios of the eucrites and diogenites are contradictory, either assuming the solidification of the early partial melt of the silicate phase [4] or magma fractionation in a magma ocean or magma chambers [5,6]. <P />Here, we investigate the differentiation of Vesta by porous flow, evaluating thereby the influence of several parameters on the timing of core, mantle, and crust formation, as well as on the possibility of the formation of a magma ocean. We use our thermal evolution model from previous studies [7,8], which considers thermal and structural evolution of ordinary chondritic planetesimals including differentiation. In these studies, it has been recognised that, in particular, the velocity of the melt relative to the solid matrix determines the timing of the differentiation events and the existence of a whole-mantle magma ocean. <P />The melt velocity, v, is computed from the Darcy law: v = K ∆ ρ g / ϕ η with the permeability K=b^{2} ϕ^{n} / τ, the grain size b, the volume fraction of the melt ϕ, the Darcy coefficient τ, the Darcy exponent n, the density contrast ∆ ρ, the gravity g, and the viscosity of the melt η. We investigate the influence of the following factors on the process of melt segregation in a partially molten system. (1) Grain size b and Ostwald ripening: Metal-melt segregation can occur prior to silicate melting for large grains (e.g., 10^{-2} m), or is negligible prior to the melting of the silicate phase for small grains (≈ 10^{-4} m). Ostwald ripening can cause a rapid increase of the grain size and, thus, of the permeability. It is, in particular, important for the formation of the basaltic crust due to the ascending silicate melt, taken a strong cooling in the shallow depths. (2) Composition and corresponding solidus and liquidus temperatures of silicates and iron-rich components: Adopted mineral abundances determine the volume fraction of the silicate and metal phases. Thus, after the onset of melting of, e.g., metal, the melt in a composition with more metal (e.g., H chondritic relative to L or LL chondritic ones) will have a higher segregation velocity. Furthermore, the solidus and liquidus temperatures T_{S} and T_{L} of the phases determine the melt fraction at a given temperature and, therefore, the segregation velocity. Note that most numerical studies used a melting window for the metal phase of only 20 K between 1213 K and 1233 K, which results in an unrealistically high metal-melt fraction and in the core formation long before the melting of silicates. (3) Density contrast between the melt and the solid matrix ∆ ρ: Some silicate melts are weakly positively or even negatively buoyant relative to a silicate matrix [9]. Such melts would remain in the mantle and would not contribute to the crust thickness. (4) Partitioning of ^{26}Al into the silicate melt: This process is important for the differentiation in the shallow depths and for the formation of the basaltic crust, due to the accumulation of ^{26}Al in the sub-surface and a possible formation of a shallow magma ocean [8]. (5) Viscosity of the silicate melt η: A large variation by several orders of magnitude makes this the most important parameter for the formation of the basaltic crust. It determines, furthermore, whether a shallow magma ocean or a whole-mantle magma ocean will form. <P />We will discuss the influence of the parameters mentioned above on the differentiation event on Vesta. Based on the constraints like the core size, crustal thickness and that the relative timing of the core-mantle differentiation likely precedes the mantle-crust differentiation, we will show possible evolution scenarios that are consistent with the observations....