THE EQUATION OF STATE AND HIGH-PRESSURE BEHAVIOR OF MAGNESITE

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dc.contributor.author Ross N.L.
dc.date.accessioned 2020-12-12T05:09:24Z
dc.date.available 2020-12-12T05:09:24Z
dc.date.issued 1997
dc.identifier https://elibrary.ru/item.asp?id=31202822
dc.identifier.citation American Mineralogist, 1997, , 7, 682-688
dc.identifier.issn 0003-004X
dc.identifier.uri https://repository.geologyscience.ru/handle/123456789/20595
dc.description.abstract Unit-cell parameters of magnesite have been measured to high precision between 0 and 7 GPa using single-crystal X-ray diffraction. The isothermal bulk modulus of magnesite determined from fitting a Birch-Murnaghan third-order equation of state to the volume compression data is K T = 117(3) GPa with K' T = 2.3(7), and K T = 111(1) GPa if K' T is constrained to a value of 4. Crystal structure parameters have been determined from X-ray intensity data at room pressure. 2.26, 3.09, 4.16, 4.77, and 6.05 GPa. The principal structural change with increasing pressure is compression of the MgO 6 octahedra while the CO 3 group remains invariant (within the experimental uncertainty) throughout the pressure range studied. The effect of the polyhedral compression is reflected in the anisotropic compression of the unit-cell parameters with the c axis approximately twice as compressible as the c axis. The polyhedral bulk modulus of the MgO 6 octahedron is 113 GPa, which is greater than that observed in other rhombohedral carbonates, but significantly smaller than values observed in many oxides and silicates. The distortion of the octahedra, though already small, decreases slightly with pressure. No phase change or change in compression behavior was observed throughout the pressure range studied.
dc.title THE EQUATION OF STATE AND HIGH-PRESSURE BEHAVIOR OF MAGNESITE
dc.type Статья


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