Table 1.
Parameter | Designation | Units | Diamond | Coesite |
---|---|---|---|---|
Bulk modulus | Ko = −V(dP/dV)T | GPa | 442† | 99.8‡ |
Its pressure derivative | K′o = (dKo/dP)T | 4† | 6.3‡ | |
Its temperature derivative | (dKo/dT)P | GPa/K | −0.0188† | −0.020§ |
Shear modulus | μd | GPa | 538† | |
Thermal expansivity | α = 1/V(dV/dT)P = a + bT + cT2 + dT3 | 1/K | ||
Coefficients in equation for α | a*106 | 6.828¶ | 5.43‖ | |
b*106 | 0.042¶ | 0.005‖ | ||
c*1010 | −0.309¶ | 0 | ||
d*1015 | 8.88¶ | |||
Raman shift vs. pressure | dν/dP | cm−1/GPa | 2.9 (±0.1)‡‡ |
The ΔV/V term at constant temperature, for both diamond and coesite, can be found from a simple Murnaghan equation of state, P = K′o/Ko[(Vo/V)Ko + 1], where K(P) = Ko + K′oP and K(T) = Ko + (dK/dT)dT. The temperature dependence of the diamond bulk modulus is below the error limits and can be effectively neglected. The pressure dependence of thermal expansivity may also be neglected, especially taking into account the very small difference in thermal expansion between coesite and diamond.
Ref. 51.
Ref. 53.
Ref. 54.
Ref. 52.
Ref. 27.