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American Mineralogist; March 1999; v. 84; no. 3; p. 384-388
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Elastic wave velocities at Mg 3 Al 2 Si 3 O 13 -pyrope garnet to 10 GPa

Ganglin Chen, Joseph A. Cooke, Gabriel D. Gwanmesia, and Robert C. Liebermann

State University of New York at Stony Brook, Mineral Physics Institute, Stony Brook, NY, United States

Elastic wave velocities of Mg 3 Al 2 Si 3 O 12 pyrope garnet were measured to 10 GPa at ambient temperature, using ultrasonic interferometry in a 1000 ton split-cylinder, multi-anvil apparatus (USCA-1000). The sample used in the ultrasonic measurements was a polycrystalline specimen hot-pressed at 5 GPa and 1350 degrees C in a 2000 ton uniaxial split-sphere apparatus (USSA-2000) from a homogeneous glass of pyrope composition. Special P-T paths used during synthesis minimized effects of decompressing and thermal cracking; the bulk density of the sample was indistinguishable from the X-ray density. The elastic wave velocities measured at the ambient condition agree with the Hashin-Shtrikman averages of the single crystal values within the mutual uncertainties. The high-pressure experiments yielded the elastic moduli and their pressure derivatives (finite strain fit) for the shear modulus G 0 = 92+ or -1 GPa. G' 0 = (theta G/theta P)T = 1.6+ or -0.2 and for the longitudinal modulus L 0 = 294+ or -1 GPa, L' 0 = (theta L/theta P)T = 7.4 + or - 0.5, (L = K s +4/3G), from which the bulk modulus K 0 = 171+ or -2 GPa, K' 0 = (theta K s /theta P)T = 5.3+ or -0.4 was calculated. The pressure derivative for the shear modulus of pyrope did not differ from those of natural pyrope-almandine-grossular garnets. For the bulk modulus, the pressure derivative for pyrope agreed with that for pyrope-almandine but was substantially higher (25%) than that for the Ca-bearing garnet. In the pyrope-majorite series, K' 0 remained constant, whereas G' 0 increased by 25 for 38% majorite content.

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