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Russian Geology and Geophysics

2015 year, number 1-2

DIAMOND THERMOELASTIC PROPERTIES AND IMPLICATIONS FOR DETERMINING THE PRESSURE OF FORMATION OF DIAMOND–INCLUSION SYSTEMS

R.J. Angel1, M. Alvaro1, F. Nestola1, M.L. Mazzucchelli2
1Department of Geosciences, University of Padua, Via G. Gradenigo, 6, Padua, 35131, Italy
2Department of Earth and Environmental Sciences, University of Pavia, Via A. Ferrata, 1, Pavia, 27100, Italy
Keywords: Diamond, equation of state, compressibility, thermal expansion, high pressure, high temperature

Abstract

The formation conditions of diamond can be determined from the residual pressure of inclusions trapped within the diamond, as measured in ambient conditions, and the equations of state (EoS) of the mineral inclusion and the host diamond. The EoS parameters of the diamond and the inclusion phase are therefore critical for determining the precision and accuracy of the calculation of formation conditions of diamonds. The questions we address are: (1) How precise are these calculations? and, in particular, (2) Do we know the EoS parameters of diamond to a precision and accuracy which do not contribute significantly to the geological conclusions drawn from these calculations? We present a review of the recentmost compressional data, simulations, and direct elastic measurements of diamond and show them to be consistent with a room temperature bulk modulus of K 0 T = = 444(2) GPa and a pressure derivative K′ = 4.0. In combination with a thermal-pressure model with parameters a V 300,0 = 2.672(3)·10 -6 K -1 and a single Einstein temperature θ E = 1500K, the volume variation of diamond from room conditions to pressures and temperatures exceeding those in the Earth’s transition zone is described to within the levels of uncertainty inherent in both experimental and computational determinations. For olivine inclusions in diamond, these uncertainties in the diamond EoS parameters lead to uncertainties in the entrapment pressures of no more than 0.001 GPa at low temperatures and 0.008 GPa at higher temperatures.

DOI: http://dx.doi.org/10.1016/j.rgg.2015.01.014