Vol 69, No 12 (2024)
- Year: 2024
- Articles: 4
- URL: https://journals.eco-vector.com/0016-7525/issue/view/11467
- DOI: https://doi.org/10.31857/S0016-75256912
Full Issue
Articles
Chemical Composition, Mineralogy and Physical Properties of the Mantle of the Moon: a Review
Abstract
The problem of the internal structure plays a special role in the geochemistry and geophysics of the Moon. The main sources of information about the chemical composition and physical state of the deep interior are seismic experiments of the Apollo expeditions, gravity data from the GRAIL mission, geochemical and isotopic studies of lunar samples. Despite the high degree of similarity of terrestrial and lunar matter in the isotopic composition of a number of elements, the question of the similarity and/or difference in the composition of the silicate shells of the Earth and its satellite in relation to the main elements remains unresolved. The review article summarizes and critically analyzes information on the composition and structure of the Moon, examines the main contradictions between geochemical and geophysical classes of mantle structure models both within each class and between the classes, related to the estimation of the abundance of the major element oxides Fe, Mg, Si, Al, Ca, and analyzes bulk silicate Moon (BSM) models. The principles of the approach to modeling the internal structure of a planetary body, based on the joint inversion of an integrated set of selenophysical, seismic, and geochemical parameters combined with calculations of phase equilibria and physical properties, are presented. Two new classes of the chemical composition of the Moon, enriched in silica (~50% SiO2) and ferrous iron (11-13% FeO, Mg# 79–81) in relation to the bulk composition of the silicate component of the Earth (BSE) are discussed — models E with terrestrial concentrations of CaO and Al2O3 (Earth-like models) and models M with higher refractory oxide content (Moon-like models), which determine the features of the mineralogical and seismic structure of the lunar interior. The probabilistic distribution of geochemical (oxide concentrations) and geophysical (P-, S-wave velocities and density) parameters in the four-layer lunar mantle within the range of permissible selenotherms was obtained. Systematic differences in the content of rock-forming oxides in the silicate shells of the Earth and the Moon have been revealed. Calculations of the mineral composition, P-, S-wave velocities, and density of the E/M models and two classes of conceptual geochemical models LPUM (Lunar Primitive Upper Mantle) and TWM (Taylor Whole Moon) with Earth’s silica content (~45 wt.% SiO2) and different FeO and Al2O3 contents were carried out. The justification of the SiO2-FeO-enriched (olivine-pyroxenite) lunar mantle, which has no genetic similarity with Earth’s pyrolitic mantle, is provided as a geochemical consequence of the inversion of geophysical parameters and determined by cosmochemical conditions and the Moon’s formation mechanism. The major mineral of the lunar upper mantle is high-magnesium orthopyroxene with low calcium content rather than olivine, as confirmed by Apollo seismic data and supported by spacecraft analysis of spectral data from a number of impact basin rocks. In contrast, the P- and S-wave velocities of the TWM and LPUM geochemical models, in which olivine is the major mineral of the lunar mantle, do not match the Apollo seismic data. The geochemical constraints in the scenarios for the formation of the Moon are considered. The simultaneous enrichment of the Moon in SiO2 and FeO relative to pyrolitic mantle of the Earth is incompatible with the formation of the Moon as a result of a giant impact from terrestrial matter or an impact body (bodies) of chondritic composition and becomes the same obstacle in modern scenarios of the formation of the Moon as the similarity in the isotopic compositions of lunar and terrestrial samples. The problem of how to fit these different geochemical factors into the Procrustean bed of cosmogonic models for the Earth-Moon system formation is discussed.



The Formation of K-Cymrite in Subduction Zones and its Potential in the Transport of Potassium, Water and Nitrogen into the Mantle
Abstract
The conditions for the formation of K-cymrite in volatile-rich pelite and partially devolatilized quartz–muscovite–chlorite schist were experimentally investigated at pressures of 5.5, 6.3, and 7.8 GPa and temperatures ranging from 900 to 1090°C. The experimental samples at these P-T conditions formed an eclogite-like assemblage of solid phases (Grt + Coe + Phe + Cpx + Ky, with accessory Po + Ru + Zrn ± Mnz) and water-enriched supercritical fluid-melt. Analysis of the obtained data indicates that the stability of phengite and its potential replacement by K-cymrite in the eclogite-like residue depends on the P-T conditions and the amount of volatiles in the metasediment. In samples of volatile-rich pelite and schist at 5.5 GPa and 900°C, as well as at 6.3 GPa and 1000°C, phengite remains stable in equilibrium with the fluid-melt (3–13 wt%). For the first time, phase assemblage with phengite and K-cymrite (± kokchetavite) was identified using Raman mapping in samples of pelite and schist obtained at 7.8 GPa and 1070°C. It was concluded that the most effective transport of volatiles (primarily water) in the metasediment to depths exceeding 240 km may occur during its partial and early (before the formation of supercritical fluid-melt) devolatilization. In this case, almost all phengite may reach depths of 240 km during subduction of the metasediment and then transform into water-bearing K-cymrite. Furthermore, in the presence of nitrogen in the metasediment, nitrogen-bearing K-cymrite can facilitate the further transport of LILE (large-ion lithophile elements), water, and nitrogen. However, the formation of a significant portion of supercritical fluid-melt leads to the complete dissolution of phengite with increasing P-T parameters, making further transport of LILE, water, and nitrogen impossible. During deep multi-stage devolatilization, phengite remains stable up to depths of 240 km; however, during further subduction, it likely transforms into an anhydrous mineral such as K-hollandite.



Shaka Ridge (South Atlantic): a Remnant of Continental Crust?
Abstract
As a result of a study of igneous rocks of the basalt — andesite series, dredged on the Shaka Ridge in the South Atlantic, it was found that they differ from the basalts of mid-ocean ridges and ocean islands, and have an age of 183–186 Ma, corresponding to the time of manifestation of the Karoo-Mod mantle plume in central Gondwana. The input of ice-rafted debris into the study area due to ice transportion is considered unlikely. Geochemical and isotopic features of the studied igneous rocks show their similarity with the Jurassic mafic complexes of the Ferrar province in Antarctica and the Falkland Islands, formed during the intrusion of the Karoo Maud plume and paleo-Pacific subduction. Based on the all data obtained, it was concluded that the Shaka Ridge is a continental block that was moved during the opening of the South Atlantic in the Early Cretaceous-Early Miocene from the continental margin of Africa along an extended transform fault into the present Bouvet triple junction area.



Kinetics of Individual С1–С5 Hydrocarbons Formation of Domanik Shale in Hydrothermal Experiments
Abstract
Twelve hydrothermal experiments were conducted with Domanik oil shale from the Ukhta region (Chut River) at temperatures of 250–375 °C and periods of 24 hours (6 experiments), 72 hours (5 experiments), and 48 hours (1 experiment). The composition of hydrocarbon gases C1–C5 was studied for each experiment and quantitative data on their yields were obtained. Based on these data, the kinetic spectra of individual gases C1–C5 were established under hydrothermal experiment conditions. The character of the kinetic spectra of individual alkanes C2–C5 is virtually identical; their main narrow maximum corresponds to Ea 55 kcal/mol with an Arrhenius factor of 1×1014 s-1. The distribution of the methane generation potential by activation energies is distinguished by the fact that a significant part of its generation potential falls within the region of activation energies of 60–70 kcal/mol and by the uncertainty of the distribution character in this region.


