Sound velocities and elastic moduli have been measured on γ‐(Mg0.91Fe0.09)2SiO4 (ringwoodite) single‐crystals to 16 GPa and to 923K by Brillouin spectroscopy. A third‐order finite‐strain fit to the data yields pressure derivatives of 4.1(2) and 1.3(1) for the adiabatic bulk modulus (KS) and shear modulus (μ) respectively. Mg‐rich α, β, and γ (Mg,Fe)2SiO4 have identical values of ∂KS/∂P and of ∂μ/∂P within the experimental uncertainties. ∂KS/∂T and ∂μ/∂T for γ‐(Mg,Fe)2SiO4 are −0.021 and −0.016 GPa/K respectively. Our results indicate that the shear and compressional impedance contrasts associated with β‐ → γ‐(Mg,Fe)2SiO4 transition are sufficient to produce a visible discontinuity at 520 km even with a moderate (30–50%) amount of olivine. The generally low visibility of the 520 km discontinuity is likely due to its width and large amplitude topographic variations.
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Sinogeikin et al. (2001) studied this question.
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