Japan Geoscience Union Meeting 2014

Presentation information

Oral

Symbol S (Solid Earth Sciences) » S-IT Science of the Earth's Interior & Techtonophysics

[S-IT40_1PM1] Geofluids: their distribution and role in the Earth's dynamics

Thu. May 1, 2014 2:15 PM - 4:00 PM 416 (4F)

Convener:*Michihiko Nakamura(Division of Earth and Planetary Materials Science, Department of Earth Science, Graduate School of Science, Tohoku University), Hiroshi Sakuma(Department of Earth and Planetary Sciences, Graduate School of Science and Engineering, Tokyo Institute of Technology), Masahiro Ichiki(Graduate School of Science, Tohoku University), Tsutomu Takahashi(Institute for Research on Earth Evolution Japan Agency for Marine-Earth Science and Technology), Chair:Tetsuya Yokoyama(Department of Earth and Planetary Sciences, Graduate School of Science and Engineering, Tokyo Institute of Technology), Keika Horiguchi(Crustal Fluid Research Group, The Institute of Geology and Geoinformation, Geological Survey of Japan, National Institute of Advanced Industrial Science and Technology)

2:15 PM - 2:30 PM

[SIT40-P08_PG] Diffusive kinetic isotope fractionaion of water in silicate glasses

3-min talk in an oral session

*Minami KURODA1, Daiki YAMAMOTO1, Shogo TACHIBANA1, Michihiko NAKAMURA2, Satoshi OKUMURA2, Miho ASAKI2, Atsuko ISHIBASHI1, Naoya SAKAMOTO1, Hisayoshi YURIMOTO1 (1.Department of Natural History Science, Hokkaido Unicersity, 2.Deparement of Earth Science, Tohoku University)

Keywords:eruption dynamics, silicate glass, water, diffusion, hydrogen isotope, isotopic fractionation

Oversaturation of dissolved volatiles in an ascending magma leads to bubble nucleation and growth, which depend on volatile solubility and diffusivity, and drives explosive volcanic eruptions in the Earth. It is thus important to clarify the behaviors of volatiles in silicate melts in understanding the mechanism and dynamics of volcanic eruptions. Hydrogen isotopes record the degassing processes of hydrous magmas due to isotopic fractionation between dissolved and exsolved water. The degree of hydrogen isotopic fractionation is correlated with the water content in natural volcanic rock samples; Deuterium is more deficient in water-poor samples, and the degree of D-deficiency increases as the water content decreases. This trend has been interpreted to reflect the transition of degassing model from that in a closed-system to in an open-system. However, these two extreme degassing schemes do not take the diffusive transport of water in magmas into account, which should be included in a realistic degassing model, because the timescale of diffusion is not necessarily negligibily small compared to that of degassing during magma ascent. Moreover, diffusion of water in silicate melts may cause kinetic isotope fractionation between silicate melt and explosive fluid phases because H2O is likely to diffuse faster than HDO, of which effect can be overprinted in the D/H ratios of natural samples. The hydrogen isotopic fractionation during water diffusion in silicate melts, however, has not yet been fully determined. In order to determine the isotopic fractionation factor of hydrogen due to water diffusion in silicate melts, we performed diffusion experiments of water in SiO2 and synthetic rhyolite glasses in a D-enriched systems(H/D=10, 5 and 1). The experiments were performed for SiO2 and rhyolite glasses at 850℃ and water pressure of 50 bar in sealed silica tubes and at 650℃ and water pressure of 500 and 1000 bar in a hydrothermal furnace developed at Tohoku University. Concentration profiles of H and D in run products were measured with the ion microprobe (Cameca ims-6f at Hokkaido University) to evaluate diffusion coefficients of water (including H2O and HDO) in glasses. The obtained diffusivity (a diffusion coefficient divided by a water content) in SiO2 glass at 650 and 850℃ were consistent with the values reported in previous studies (Davis and Tomozawa, 1995; Berger and Tomozawa, 2003). The D/H ratios along the diffusion profile were also analyzed for SiO2 glasses with the ion microprobe. The D/H ratio first decreases, but apparently increases along the profile. The decrease of D/H ratio may imply the kinetic isotope fractionation during diffusion. However, the increase of D/H ratio cannot be explained simply by diffusion and may reflect the change of instrumental mass fractionation with water content (Hauri et al., 2006), which should be precisely determined to correct the profile of hydrogen isotopic ratio.