11:45 AM - 12:00 PM
[SMP29-10] Stractural investigation on viscosity difference between albite and anorthite melts
Keywords:plagioclase, melt・glass, viscosity, melt structure
Plagioclase is a basic component of volcanic magma and albite (NaAlSi3O8) and anorthite (CaAl2Si2O8) are the end members. NaAlSi3O8 and CaAl2Si2O8 melts have the same NBO/T (Number of non-bridging oxygen/tetrahedral atom, T is Si and Al) value, 0, though they have largely different viscosity (e.g., Li et al., 2021, Chem. Geol.). In previous studies, NBO/T has been considered as an important parameter which dominates viscosity of silicate melts (e.g., Mysen, 1983, AREPS). However, we cannot interpret the viscosity difference of NaAlSi3O8 and CaAl2Si2O8 melts with the conventional understanding. Therefore, investigating the mechanism which causes the viscosity difference of NaAlSi3O8 and CaAl2Si2O8 melts is essential to understand mobility of magma in the Earth’s interior and process of volcanic eruption.
In this study, we conducted viscosity measurements of CaAl2Si2O8 melt, for which viscosity data are limited, from air pressure to around 4 GPa, and carried out pair distribution function analyses to investigate melt structures of NaAlSi3O8 and CaAl2Si2O8 melts from air pressure to around 7 GPa, at 16-BM-B beamline of Advanced Photon Source. As a result, the CaAl2Si2O8 melt has around two orders of magnitude lower viscosity than NaAlSi3O8 melt at air pressure, and the viscosity of CaAl2Si2O8 melt does not change with increasing pressure up to around 4 GPa. For the melt structure, the FSDP (First Sharp Diffraction Peak) of S(Q) is clearly different between the NaAlSi3O8 and CaAl2Si2O8 melts. In order to interpret the viscosity and structure differences between the NaAlSi3O8 and CaAl2Si2O8 melts, we conducted high precision pair distribution function analyses of plagioclase glasses with different content of anorthite component. From structural data of the plagioclase glasses, we carried out Molecular Dynamics simulation and Reverse Monte-Carlo calculation, and constructed structural model of plagioclase melts. In this presentation, we discuss the structural occurrence of viscosity difference between NaAlSi3O8 and CaAl2Si2O8 melts and mechanism of viscosity changes in NaAlSi3O8 and CaAl2Si2O8 melts with increasing pressure.
In this study, we conducted viscosity measurements of CaAl2Si2O8 melt, for which viscosity data are limited, from air pressure to around 4 GPa, and carried out pair distribution function analyses to investigate melt structures of NaAlSi3O8 and CaAl2Si2O8 melts from air pressure to around 7 GPa, at 16-BM-B beamline of Advanced Photon Source. As a result, the CaAl2Si2O8 melt has around two orders of magnitude lower viscosity than NaAlSi3O8 melt at air pressure, and the viscosity of CaAl2Si2O8 melt does not change with increasing pressure up to around 4 GPa. For the melt structure, the FSDP (First Sharp Diffraction Peak) of S(Q) is clearly different between the NaAlSi3O8 and CaAl2Si2O8 melts. In order to interpret the viscosity and structure differences between the NaAlSi3O8 and CaAl2Si2O8 melts, we conducted high precision pair distribution function analyses of plagioclase glasses with different content of anorthite component. From structural data of the plagioclase glasses, we carried out Molecular Dynamics simulation and Reverse Monte-Carlo calculation, and constructed structural model of plagioclase melts. In this presentation, we discuss the structural occurrence of viscosity difference between NaAlSi3O8 and CaAl2Si2O8 melts and mechanism of viscosity changes in NaAlSi3O8 and CaAl2Si2O8 melts with increasing pressure.