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Bulk moduli and pressure derivatives for binary borides

Bulk moduli and pressure derivatives for binary carbides and silicides

Bulk moduli and pressure derivatives for binary nitrides

Bulk moduli and pressure derivatives for binary oxides of the M Oni type

Bulk moduli and pressure derivatives for binary phosphides and arsenides

Bulk moduli and pressure derivatives for ternary oxides

Bulk moduli and pressure derivatives of elements

Bulk moduli and pressure derivatives of the MX2 hydrides, halides, oxides and chalcogenides

Bulk moduli and pressure derivatives of the MX3 hydrides, halides, and hydroxides

Bulk moduli for A B covalent crystals

Bulk moduli for ionic crystals 1, 12, 17, 18

Bulk moduli for multi-bond covalent crystals 1, 12, 14, 19-21

Bulk Moduli for standard Croup IV, lll-V, and ll-VI semiconductors. The theoretical values are from a semi-empirical formula requiring the measured bond length as input.

Bulk modulus and apparent density of sono-aerogels elaborated by hydrolysis and polycondensation of TMOS

Bulk modulus and its pressure derivative for HMX polymorphs.2

Bulk modulus and Poisson ratio v for unstable-moment compounds.

Bulk modulus and thermal expansion for various compositional terms of the garnet phase. The experimental range for bulk moduli is relative to a common value of K 4. The calculated values are from Ottonello et al. . References for thermal expansion are as follows

Bulk modulus at P 0 and its first derivative versus pressure for dioctahedral micas.

Bulk modulus Ko and compressibilities Pi.

Bulk modulus Kq for some olivine end-members.

Bulk modulus model for earth

Bulk optical properties of amorphous Si02 and crystalline Cap2 at the 193-nm wavelength.

Bulk Phase Handling Properties of Adipic Acid

Bulk Photolysis of Isopropanol Uranyl Zeolite Suspensions

Bulk polymerization of 1,4-anhydroerythritol using CF3SO3H or FSO3H



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