Japan Geoscience Union Meeting 2025

Presentation information

[J] Poster

S (Solid Earth Sciences ) » S-CG Complex & General

[S-CG62] Rheology, fracture and friction in Earth and planetary sciences

Thu. May 29, 2025 5:15 PM - 7:15 PM Poster Hall (Exhibition Hall 7&8, Makuhari Messe)

convener:Osamu Kuwano(Japan Agency for Marine-Earth Science and Technology), Hiroaki Katsuragi(Department of Earth and Space Science, Osaka University), Sando Sawa(Deparment of Earth Science, Graduate School of Science, Tohoku Univeristy), Dan Muramatsu(Earthquake Reserch Institute, The University of Tokyo)

5:15 PM - 7:15 PM

[SCG62-P09] High-strain deformation experiments on olivine aggregates using the rotational diamond anvil cell

*Keishi Okazaki1,3, Shintaro Azuma2, Masahiro Yasutake5, Bunrin Natsui2, Kentaro Uesugi5, Naotaka Tomioka3,1, Ryuichi Nomura4 (1.Earth and Planetary Systems Science Program, Hiroshima University, 2.Department of Earth & Planetary Sciences, Institute of Science Tokyo, 3.Kochi Institute for Core Sample Research, JAMSTEC, 4.Kyoto University, 5.JASRI/SPring-8)

To understand the dynamics of the plate tectonics, it is important to constrain the rheology of olivine in the mantle peridotites, and how it evolves under high-strain deformation imposed during plate motions and mantle flows. We performed a series of high-strain deformation experiments on olivine aggregates using a rotational diamond anvil cell (rDAC). Experiments were conducted at the beamline BL47XU, SPring-8. The experimental conditions are the confining pressure of 8–22 GPa, the temperature of 300–1000 K, and the equivalent shear strain rate of ~10^–4 1/s. During the deformation experiments, X-ray diffraction (XRD) patterns and X-ray radiographs were taken every 2–3 minutes. Stresses in the olivine aggregates were calculated from the lattice strain estimated from XRD. Since we applied a torsional deformation to the sample, there are some stress and strain gradients in the sample. We adopted the stress at the position 2/3 of the radius from the center of the sample as a representative stress in the sample, because this position is the area-averaged radius of the sample. As the shear strain increased, the stress increased and then reached a steady-state stress condition. The steady-state shear stress and equivalent stress at the temperature of 300 K and the pressure of 8 GPa were about 1.8 GPa and 7.0 GPa, respectively. The steady-state shear stress and equivalent stress at the temperature of 673 K and the pressure of 12 GPa were about 1.2 GPa and 3.0 GPa, respectively. The steady-state stress obtained in the present study is consistent with a Peierls’s flow law reported in a previous study. We will also present data on crystallographic preferred orientations of olivine aggregates in this presentation.