A simple and generalised P–T–V EoS for continuous phase transitions, implemented in EosFit and applied to quartz
PETROLOGICAL INTEREST
105113 Crystallography
CONSISTENT THERMODYNAMIC DATA
530
Continuous phase transition
01 natural sciences
105116 Mineralogy
105113 Kristallographie
Geochemistry and Petrology
EosFit
HIGH-PRESSURE
Continuous phase transition; Elasticity; EosFit; Equation of state; Quartz; Geophysics; Geochemistry and Petrology
Geophysic
105116 Mineralogie
0105 earth and related environmental sciences
Equation of state
LAMBDA-TRANSITION
Quartz
SPONTANEOUS STRAIN
EQUATION-OF-STATE
Elasticity
MOLECULAR-DYNAMICS
BETA-QUARTZ
THERMAL-EXPANSION
SINGLE-CRYSTAL QUARTZ
DOI:
10.1007/s00410-017-1349-x
Publication Date:
2017-04-11T11:11:50Z
AUTHORS (4)
ABSTRACT
Continuous phase transitions in minerals, such as the α–β transition in quartz, can give rise to very large non-linear variations in their volume and density with temperature and pressure. The extension of the Landau model in a fully self-consistent form to characterize the effects of pressure on phase transitions is challenging because of non-linear elasticity and associated finite strains, and the expected variation of coupling terms with pressure. Further difficulties arise because of the need to integrate the resulting elastic terms over pressure to achieve a description of the P–T–V equation of state. We present a fully self-consistent simplified description of the equation of state of minerals with continuous phase transitions based on a purely phenomenological adaptation of Landau theory. The resulting P–T–V EoS includes the description of the elastic softening occurring in both phases with the minimum number of parameters. By coupling the volume and elastic behaviour of the mineral, this approach allows the EoS parameters to be determined by using both volume and elastic data, and avoids the need to use data at simultaneous P and T. The transition model has been incorporated in to the EosFit7c program, which allows the parameters to be determined by simultaneous fitting of both volume and elastic data, and all types of equation of state calculations to be performed. Quartz is used as an example, and the parameters to describe the full P–T–V EoS of both α- and β-quartz are determined.
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