1971
DOI: 10.2475/ajs.271.4.370
|View full text |Cite
|
Sign up to set email alerts
|

Stability of the assemblage iron-rich orthopyroxene-olivine-quartz

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
8
1

Year Published

1971
1971
2024
2024

Publication Types

Select...
7
3

Relationship

0
10

Authors

Journals

citations
Cited by 37 publications
(11 citation statements)
references
References 0 publications
2
8
1
Order By: Relevance
“…To keep the 1-bar enthalpy difference to within the uncertainty of Navrotksy et al's (1979) data, and additionally the heat of formation of fayalite to within experimental uncertainty, allows destabilizing fayalite by about 828-900 J/mol, which has the effect that the fayalite-ringwoodite boundary is lowered by − 0.23 GPa. Additionally the phase boundary between fayalite + quartz and orthoferrosilite is moved to pressures − 0.28 GPa below our present result, which is twice the difference between the boundaries determined by Bohlen et al (1980) and Smith (1971). Stabilizing quartz or destabilizing orthoferrosilite to keep this boundary at the same location results in the same effect as the first possibility for changing the fayalite-ringwoodite boundary, that the ringwoodite + coesite field becomes stable at temperatures below 1473 K. Our present result represents the boundary of Bohlen et al (1980), which is the lowest in pressure relative to previous measurements and the conclusion is that we can change the fayalite-ringwoodite boundary by only − 0.13 GPa, leaving a difference of 0.25 GPa relative to Ono et al's (2013) data points.…”
Section: Phase Diagramscontrasting
confidence: 57%
“…To keep the 1-bar enthalpy difference to within the uncertainty of Navrotksy et al's (1979) data, and additionally the heat of formation of fayalite to within experimental uncertainty, allows destabilizing fayalite by about 828-900 J/mol, which has the effect that the fayalite-ringwoodite boundary is lowered by − 0.23 GPa. Additionally the phase boundary between fayalite + quartz and orthoferrosilite is moved to pressures − 0.28 GPa below our present result, which is twice the difference between the boundaries determined by Bohlen et al (1980) and Smith (1971). Stabilizing quartz or destabilizing orthoferrosilite to keep this boundary at the same location results in the same effect as the first possibility for changing the fayalite-ringwoodite boundary, that the ringwoodite + coesite field becomes stable at temperatures below 1473 K. Our present result represents the boundary of Bohlen et al (1980), which is the lowest in pressure relative to previous measurements and the conclusion is that we can change the fayalite-ringwoodite boundary by only − 0.13 GPa, leaving a difference of 0.25 GPa relative to Ono et al's (2013) data points.…”
Section: Phase Diagramscontrasting
confidence: 57%
“…Other workers [3][4][5] have shown that FeSiO3 is a stable phase at high pressures. More recently Smith [1 ] and Wood and Strens [6] have attempted to experimentally calibrate parts of the Fe2 SiO4-SiO2 and Fe2SiO4-Mg2SiO4-SiO2 systems. Smith [1 ] has determined the pres- and has also experimentally evaluated the effect of MgO on the orthopyroxene-olivine-quartz system at 900°C.…”
Section: Introductionmentioning
confidence: 99%
“…6" needs some explanation as well. In experiments SMITH (1971) has shown that at relatively low pressures and temperatures between 600 and 1000 ~ C the reaction orthopyroxene --olivine + quartz proceeds to the right in systems with high Fe/(Fe § ratios. In experiments SMITH (1971) has shown that at relatively low pressures and temperatures between 600 and 1000 ~ C the reaction orthopyroxene --olivine + quartz proceeds to the right in systems with high Fe/(Fe § ratios.…”
Section: Thermometamorphism--m1mentioning
confidence: 99%