Iron K-edge X-ray absorption near-edge structure spectroscopy of aerodynamically levitated silicate melts and glasses

被引:41
作者
Alderman, O. L. G. [1 ,2 ]
Wilding, M. C. [3 ]
Tamalonis, A. [1 ]
Sendelbach, S. [1 ]
Heald, S. M. [2 ]
Benmore, C. J. [2 ]
Johnson, C. E. [4 ]
Johnson, J. A. [4 ,5 ]
Hah, H. -Y. [4 ,5 ]
Weber, J. K. R. [1 ,2 ]
机构
[1] Mat Dev Inc, Arlington Hts, IL 60004 USA
[2] Argonne Natl Lab, Adv Photon Source, Xray Sci Div, Argonne, IL 60439 USA
[3] UCL, Dept Chem, 20 Gordon St, London WC1H 0AJ, England
[4] Univ Tennessee, Inst Space, Ctr Laser Applicat, Tullahoma, TN 37388 USA
[5] Univ Tennessee, Inst Space, Dept Mech Aeronaut & Biomed Engn, Tullahoma, TN 37388 USA
关键词
Silicate; Melt; Glass; Iron; XANES; Redox; FE OXIDATION-STATE; FERRIC-FERROUS RATIO; MQ-MAS NMR; OXYGEN FUGACITY; REDOX EQUILIBRIA; ALUMINOSILICATE GLASS; MOLECULAR-DYNAMICS; LOCAL ENVIRONMENT; XAS DETERMINATION; K/T BOUNDARY;
D O I
10.1016/j.chemgeo.2017.01.020
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
The local structure about Fe(II) and Fe(III) in silicate melts was investigated in-situ using iron K-edge X-ray absorption near-edge structure (XANES) spectroscopy. An aerodynamic levitation and laser heating system was used to allow access to high temperatures without contamination, and was combined with a chamber and gas mixing system to allow the iron oxidation state, Fe3+/Sigma Fe, to be varied by systematic control of the atmospheric oxygen fugacity. Eleven alkali-free, mostly iron-rich and depolymerized base compositions were chosen for the experiments, including pure oxide FeO, olivines (Fe, Mg)(2)SiO4, pyroxenes (Fe, Mg)SiO3, calcic FeO-CaSiO3, and a calcium aluminosilicate composition, where total iron content is denoted by FeO for convenience. Melt temperatures varied between 1410 and 2160 K and oxygen fugacities between FMQ - 2.3(3) to FMQ + 9.1(3) log units (uncertainties in parentheses) relative to the fayalite-magnetite-beta-quartz (FMQ) buffer. Remarkably, XANES preedge peak areas imply mean Fe-O coordination numbers (n(FeO)) close to 5 in all cases, with only a slight tendency toward higher values in the most iron rich melts, suggesting an intermediate role for both Fe(II) and Fe(III) in terms of network formation. End member coordination numbers for Fe(II)-O and Fe(III)-O are estimated to be similar, having means (and standard deviations) of 5.0(2) and 4.9(1), respectively. As such, the preference for ferric iron to occupy lower coordination sites than ferrous is weak, in contrast to published behavior in some alkali-rich systems, which may explain the larger published viscosity variations with Fe3+/Sigma Fe in alkali-, compared to alkaline earth-iron silicates. Temperature effects on nFeO are inferred to be small based on the melt data, as well as by comparison to glasses formed on quenching. Positive shifts of the pre-edge peak centroids observed in many cases on quenching are attributed to rapid oxidation enabled by the stirring of the melt droplets by the levitation gas jet. Fe3+/Sigma Fe values were estimated from XANES pre-edge peaks using published calibrations and compared to semi-empirical thermodynamic model calculations and Mossbauer measurements on quench products. Whilst showing positive correlation, the comparisons highlight the limitations involved in applying XANES calibrations and models for Fe3+/Sigma Fe derived from measurements on glasses, to high temperature basic melts. Fe3+/Sigma Fe varies from approximately zero up to about 65% in the high temperature melts and 75% in the glasses. (C) 2017 Elsevier B.V. All rights reserved.
引用
收藏
页码:169 / 185
页数:17
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