Isothermal compression of grossular garnets to 250 Kbar and the effect of calcium on the bulk modulus

The effect of pressure on the lattice parameter, and hence on the volume, of two samples of grossularite garnet (Ca3Al2Si3O12) has been measured at room temperature up to 250 kbar with the use of a diamond anvil highpressure X ray diffraction camera. The pressure to which the sample was subjected was measured by means of the NaCl internal pressure standard. A least squares fit of the pressure-volume to the Birch-Murnaghan equation yields a bulk modulus value of KO = 1.74 ± 0.04 Mbar when a (∂K/∂P)∣P=0 value of 4.25 (Halleck, 1973) is used. This KO value is in agreement with the value of 1.704 Mbar obtained by Halleck [1973], using ultrasonic techniques. A comparison of the bulk moduli of grossularite, pyrope, and almandite shows that KO∝ Vo−1 for Ca and Mg garnets as expected from static lattice models. On the other hand, KO∝ Vo−5 for the Mg-Fe garnet solid solutions. This behavior has not been explained by available theories.

[1]  Don L. Anderson,et al.  Brief report: The bulk modulus‐volume relationship for oxides , 1970 .

[2]  Naohiro Soga,et al.  A restriction to the law of corresponding states , 1967 .

[3]  Naohiro Soga,et al.  Elastic properties of CaO under pressure and temperature. , 1968 .

[4]  Taro Takahashi,et al.  Effect of pressure and temperature on the molar volumes of Wüstite and of three (Fe, Mg)2SiO4 spinel solid solutions , 1969 .

[5]  P. W. Bridgman The linear compressibility of thirteen natural crystals , 1928 .

[6]  R. Verma,et al.  Elasticity of some high-density crystals , 1960 .

[7]  Anthony W. England,et al.  Universal equations of state for oxides and silicates , 1969 .

[8]  Gene Simmons,et al.  Velocity of compressional waves in various minerals at pressures to 10 kilobars , 1964 .

[9]  Dae H. Chung,et al.  Birch's Law: Why Is It So Good? , 1972, Science.

[10]  L. Orgel,et al.  Electronic properties of transition-metal oxides-II: Cation distribution amongst octahedral and tetrahedral sites , 1957 .

[11]  D. Chung,et al.  Effects of iron/magnesium ratio on P- and S-wave velocities in olivine , 1970 .

[12]  C. R. Knowles,et al.  X-Ray Emission Microanalysis of Rock-Forming Minerals. VII. Garnets , 1969, The Journal of Geology.

[13]  R. Kearney,et al.  Elastic Constants of SrO , 1970 .

[14]  Taro Takahashi,et al.  X‐Ray Diffraction and Optical Observations on Crystalline Solids up to 300 kbar , 1967 .

[15]  P. R. Son,et al.  CaO and SrO single crystal elastic constants and their pressure derivatives , 1972 .

[16]  T. Shankland,et al.  Velocity‐density systematics: Derivation from Debye theory and the effect of ionic size , 1972 .

[17]  William A. Bassett,et al.  Effect of pressure on the crystal structure and the lattice parameters of BaO , 1972 .

[18]  J. C. Jamieson,et al.  X‐Ray Diffraction Studies in the 100 Kilobar Pressure Range , 1962 .

[19]  C. Pistorius,et al.  Stability relations of grossularite and hydrogrossularite at high temperatures and pressures , 1960 .

[20]  O. Anderson,et al.  Pressure Derivatives of Elastic Constants of Single‐Crystal MgO at 23° and ‐195.8°C , 1966 .

[21]  R. A. Bartels,et al.  BaO single crystal elastic constants and their temperature dependence , 1973 .

[22]  D. L. Anderson A Seismic Equation of State , 1967 .

[23]  B. Skinner Physical properties of end-members of the garnet group , 1956 .

[24]  Naohiro Soga,et al.  New measurements on the sound velocity of calcium oxide and its relation to Birch's law , 1967 .

[25]  P. W. Bridgman Linear Compressions to 30,000 Kg/Cm, including Relatively Incompressible Substances , 1949 .

[26]  D. Chung,et al.  Elasticity and Equations of State of Olivines in the Mg2SiO4-Fe2SiO4 System , 1971 .

[27]  Taro Takahashi,et al.  Compression of ferromagnesian garnets and the effect of solid solutions on the bulk modulus , 1970 .

[28]  O. Anderson,et al.  The bulk modulus-volume relationship for oxide compounds and related geophysical problems , 1965 .