Bulk modulus of Fe-rich olivines corrected for non-hydrostaticity

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Abstract

In situ X-ray diffraction was used to measure the isothermal bulk modulus at room conditions (KT0)of synthetic olivines with different iron contents. The chemical formulae of the olivine samples were (Fex,Mg1−x)2SiO4 with x = 0.45; 0.64; 0.82; 1, with 1% standard deviation (referenced as Fa45, Fa64, Fa82 and Fa100, respectively). All experiments were performed in the multi-anvil apparatus installed at NSLS beamline X17B2, to pressures up to about 7 GPa. Unit-cell volumes under hydrostatic conditions and differential stresses present in the samples were calculated using the method developed by Singh et al. (1998), and pressures measured using NaCl as a standard were then corrected for these stresses. Using a second-order Birch–Murnaghan equation of state, we obtained the isothermal bulk modulus of each composition: KT0Fa45=131.4±2.6 GPa, KT0Fa64=132.1±3.1 GPa, KT0Fa82=136.3±1.7 GPa and KT0Fa100=134.8±1.4 GPa. These values combined with data available in the literature show that the KT0 of Fe-rich olivines increases very slowly with the Fe content, but possibly not in a simple linear trend.

Figures

  • Table 1 Characteristics of sintered samples before the experiments and highpressure run conditions.
  • Fig. 2. Microstructure of sample Fa100 reconstructed from EBSD data acquired with a step size of 0.1 mm. The horizontal field of view is 80 mm. The sample has a very low porosity and a homogeneous grain size.
  • Fig. 3. XRD patterns of sample Fa100 and Fa peak positions at room pressure (bottom) and at 5 GPa (top), both at room temperature after background subtraction. Orange and red lines show the fit of the full spectra and the grey lines show their residuals. Extra peaks come from cell assembly materials. Light-grey data points were masked during peak fitting. The peaks used to calculate unit cell volumes are listed in the text.
  • Fig. 6. Volumes of Fa82 and NaCl (colored data, left axis), and stress in Fa82 (grey data, right axis) as a function of pressure. The top part of the plot is for Fa82 (down-pointing triangles), the bottom part for NaCl (crosses). Orange and green colors indicate volume data from detectors 5 and 9, respectively, as a function of PFa. Volumes (V) calculated from dP (see Eq. (3)) are shown in blue as a function of PNaCl and in red as a function of PFa after correction using Eq. (4). The grey points show the stress in Fa82 as a function of PFa. The higher stress levels correspond to the cold-compression phase. After relaxation heating, stress lowers but remains measurable throughout the experiments. One can see that the differential stress present in Fa82 does not allow the determination of an EoS from one detector only, unlike for NaCl where stress is low (not shown).
  • Fig. 5. Differential stress measured in both NaCl (orange crosses) and samples (blue triangles) Fa100 (a) and Fa45 (b) at room T, and pressure (grey squares, right-hand axis) as a function of time. See the text for a description of stress determination. The stress drop visible after 20,000 s for Fa100 (a) and after 10,000 s for Fa45 (b) is due to the flow of cell assembly materials as a result of the relaxation heating. The samples remained under extension until the very end of the experiment.
  • Fig. 7. Unit-cell volumes of the four specimens as a function of pressure PFa. Uncertainties are shown as one standard deviation. Pressures are corrected for differential stresses both in NaCl and in the samples. Lines show the orthogonal distance regression (ODR) fits of a BM2 EoS for each dataset. The results are listed in Table 3.
  • Fig. 8. Selected values of the bulk modulus of olivines from the literature that show a possible trend for KT0 as a function of Fe content (blue dashed line). KT0 could present a plateau around 125 GPa for XFe9 20% and around 133 GPa for XFe0 80%, with a linear increase in between (slope ’ 0.15 GPa/% Fa). Red diamonds are our KT0 values with dK/ dP = 5.3 in order to compare with Nestola et al. (2011)’s data (green circles), and the red-blue diamond is our K_{T0}^{Fa} with dK/dP = 4 to compare with the results of Zhang et al. (2017) (grey down triangle). The yellow diamond represents data from Angel et al. (2017, from their BM3 isothermal EoS, dK/dP = 4.5), and the green square is from Speziale et al. (2004, dK/dP = 4.85). These two points would have lower values if recalculated with dK/dP = 5.3. A more complete figure with all published KT0 is given in the Supplementary Materials.
  • Fig. 9. V/V0 as a function of pressure for all four specimens. Uncertainties are shown as one standard deviation. The black line shows the ODR fit of BM2 EoS to all data points and giving KT0 = 135 . 3 GPa. The barely visible dashed line is a BM3 EoS fit with a fixed K0 = 5.3 (Nestola et al., 2011) leading to KT0 = 132 . 4 GPa. The four light-blue squares (data from Fa45) were considered as outliers and excluded from the fit.

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APA

Béjina, F., Bystricky, M., Tercé, N., Whitaker, M. L., & Chen, H. (2019). Bulk modulus of Fe-rich olivines corrected for non-hydrostaticity. Comptes Rendus - Geoscience, 351(2–3), 86–94. https://doi.org/10.1016/j.crte.2018.06.002

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