4.6 Article

Unusual Chemistry of the C-H-N-O System under Pressure and Implications for Giant Planets

Journal

JOURNAL OF PHYSICAL CHEMISTRY A
Volume 125, Issue 18, Pages 3936-3942

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.jpca.1c00591

Keywords

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Funding

  1. Russian Science Foundation [19-72-30043]
  2. Russian Foundation for Basic Research [19-02-00394]
  3. Russian Ministry of Science and Higher Education [2711.2020.2]
  4. Russian Science Foundation [19-72-30043] Funding Source: Russian Science Foundation

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The C-H-N-O system is crucial in organic chemistry, biochemistry, and planetary science, with new stable phases predicted under high pressure and temperature conditions. Detailed phase diagrams of CH4-NH3-H2O at high pressures were provided, revealing deficiencies in current ice giant models and proposing new insights into the internal structure of Uranus and Neptune.
C-H-N-O system is central for organic chemistry and biochemistry and plays a major role in planetary science (dominating the composition of ice giants Uranus and Neptune). The inexhaustible chemical diversity of this system at normal conditions explains its role as the basis of all known life, but the chemistry of this system at high pressures and temperatures of planetary interiors is poorly known. Using ab initio evolutionary algorithm USPEX, we performed an extensive study of the phase diagram of the C-H-N-O system at pressures of 50, 200, and 400 GPa and temperatures up to 3000 K. Seven novel thermodynamically stable phases were predicted, including quaternary polymeric crystal C2H2N2O2 and several new N-O and H-N-O compounds. We describe the main patterns of changes in the chemistry of the C-H-N-O system under pressure and confirm that diamond should be formed at conditions of the middle-ice layers of Uranus and Neptune. We also provide the detailed CH4-NH3-H2O phase diagrams at high pressures, which are important for further improvement of the models of ice giants, and point out that current models are clearly deficient. In particular, in the existing models, Uranus and Neptune are assumed to have identical composition, nearly identical pressure-temperature profiles, and a single convecting middle layer (mantle) made of a mixture of H2O/CH4/NH3 in the ratio of 56.5:32.5:11. Here, we provide new insights, shedding light into the difference of heat flows from Uranus and Neptune, which require them to have different compositions, pressure-temperature conditions, and a more complex internal structure.

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