MR025-01
Kinetics study of dehydrogenation of pyrite-FeO2H above 1 Mbar using laser heating and time-resolved synchrotron x-ray diffraction

Wednesday, 16 December 2020: 08:30
Virtual
Jiuhua Chen, Florida International Univ., Miami, FL, United States, Ruilian Tang, Changchun University of Science and Technology, Changchun, China, Jin Liu, Center for High Pressure Science & Technology Advanced Research, Beijing, China, Ho-kwang Mao, Center for High Pressure Science & Technology Advanced Research, Shanghai, China, Qingyang Hu, Center for High Pressure Science and Technology Advanced Research, Shanghai, China, Bin Yang, Center for High Pressure Science and Technology Advanced Research, Changchun, China, Yan Li, Jilin University, Changchun, China, Haozhe Liu, HPSTAR, Beijing, China, Vadym Drozd, Florida International University, Miami, FL, United States, Vitali B Prakapenka, University of Chicago, Center for Advanced Radiation Sources, Chicago, IL, United States, Yue Meng, HPCAT, X-Ray Science Division, Argonne National Laboratory, Argonne, United States and Jinyuan Yan, Lawrence Berkeley National Laboratory, Berkeley, CA, United States
Abstract:
We have conducted time-resolved synchrotron x-ray diffraction of pyrite- FeO2H at high pressures of 110 GPa and 120 GPa and high temperatures of 2100K and 2300K in a laser-heated diamond anvil cell (DAC). The accumulated laser-heating time extended up to 12 hours. The hydrogen concentration in FeO2Hx is determined by comparing the cell volume of the sample after it was quenched to room temperature with those of the end members (FeOOH and FeO2) at the same pressure and assuming a linear relationship between the molar volume and hydrogen concentration x in pyrite-FeO2Hx. We found that pyrite-FeO2H experiences a slow dehydrogenation process at these conditions. The derived x values as a function of the heating duration are fitted based on the first-order reaction equation dx/dt=-kx (where k is a time(t)-independent constant for a given environment) for the dehydrogenation: FeOOH=FeO2Hx+½(1-x)H2. The hydrogen concentration x approaches 0.76 at 110 GPa and 2300K when the heating time approaches infinity. The equilibrium x value decreases with temperature and increases with pressure, which explains the discrepancies in the hydrogen concentration among the previous experiments. These results indicate that FeOOH loses hydrogen through a dehydrogenation process at lower-mantle conditions and stabilizes at an intermediate composition, which remains capable of storing water as a reservoir at the bottom of the lower mantle.