Abstract

The position of the critical point determines the top of the liquid-vapor coexistence dome, and it is a physical parameter of fundamental importance in the study of high-energy shocks, including those associated with large planetary impacts. For most major planetary materials, such as oxides and silicates, the estimated position of the critical point is below $1\phantom{\rule{4pt}{0ex}}\mathrm{g}/{\mathrm{cm}}^{3}$ at temperatures above 5000 K. Here we compute the position of the critical point of one of the most ubiquitous materials: MgO. For this we perform first-principles molecular dynamics simulations. We find the critical density to be in the 0.45--$0.6\phantom{\rule{4pt}{0ex}}\mathrm{g}/{\mathrm{cm}}^{3}$ range and the critical temperature in the 6500--7000 K range. We investigate in detail the behavior of MgO in the subcritical and supercritical regimes, and we provide insight into the structure and chemical speciation. We see a change in Mg-O speciation toward lower degrees of coordination as the temperature is increased from 4000 to 10 000 K. This change in speciation is less pronounced at higher densities. We observe the liquid-gas separation in nucleating nanobubbles at densities below the liquid spinodal. The majority of the chemical species forming the incipient gas phase consists of isolated Mg and O atoms and some MgO and ${\mathrm{O}}_{2}$ molecules. We find that the ionization state of the atoms in the liquid phase is close to the nominal charge, but it almost vanishes close to the liquid-gas boundary and in the gas phase, which is consequently largely atomic.

Highlights

  • Giant impacts are a characteristic of the early stages of the evolution of planets, when chaotic trajectories of planets and planetesimals oftentimes intersect

  • The position of the critical point determines the top of the liquid-vapor coexistence dome, and it is a physical parameter of fundamental importance in the study of high-energy shocks, including those associated with large planetary impacts

  • We find that the ionization state of the atoms in the liquid phase is close to the nominal charge, but it almost vanishes close to the liquid-gas boundary and in the gas phase, which is largely atomic

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Summary

Introduction

Giant impacts are a characteristic of the early stages of the evolution of planets, when chaotic trajectories of planets and planetesimals oftentimes intersect. The impact processes can be so energetic that they can produce partial or even total melting and/or vaporization of the bodies involved. The resulting ejecta gather to form a disk. If the temperatures reached during the peak of the impacts exceed the conditions of the critical point (CP), the constituting materials of those celestial bodies become supercritical. Upon cooling of a supercritical disk, or in case the supercritical conditions are not reached in the disk during the impact, the system evolves toward a biphase system along the liquid-vapor equilibrium curve. As the maximum of the liquid-vapor equilibrium is fixed by the CP, the position of the CP itself is of fundamental importance in understanding large and giant planetary impacts. Even though giant impacts may be considered rare events, they can be responsible for the creation of planets and moons, or sometimes for their destruction

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