首页> 外文会议>Proceedings of the 12th China International Geo-electromagnetic Induction Workshop >Proton conduction and hydrogen diffusion in olivine: An attempt to reconcile laboratory and field observations and implications for the role of grain boundary diffusion in enhancing conductivity
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Proton conduction and hydrogen diffusion in olivine: An attempt to reconcile laboratory and field observations and implications for the role of grain boundary diffusion in enhancing conductivity

机译:橄榄石中的质子传导和氢扩散:试图调和实验室和现场观察以及对晶界扩散在增强电导率中的作用的启示

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Proton conduction is directly related to the diffusion of hydrogen through the Nernst-Einsteinrnequation, but prior attempts to use this relationship have always invoked additional terms to try to reconcilernproton conduction and hydrogen diffusion data. However, experimental data on hydrogen diffusion throughrnthe mineral lattice only constrain the rate of proton migration coupled with defects (such as vacancies) orrncoupled to polarons (electron holes mostly associated to ferric iron) and not the diffusion of uncoupled freernprotons. New diffusion experiments on olivine demonstrate that lattice diffusion associated to vacancies isrnindeed highly dependent on the defect site where hydrogen is bonded, but from none of the sites is fastrnenough to explain the observed laboratory proton conduction experiments. Hydrogen diffusion associated tornpolarons (redox-exchange) is significantly faster but still cannot explain the low activation energy typical ofrnelectrical conductivity measurements. A process of bulk diffusion, which combines lattice diffusion (eitherrnassociated to redox-exchange or vacancies) with the far faster grain boundary diffusion, explains thernlaboratory results, but does not explain the field observations with an average grain size of 0.5-2 cm at 100rnkm below the Jagersfontein kimberlite field on the Kaapvaal craton, consistent with petrological observationsrnon xenolith material. Another conduction mechanism must be responsible for the field observations.
机译:质子传导与通过Nernst-Einsteinrnequation进行的氢扩散直接相关,但是以前使用这种关系的尝试总是引用其他术语来调和质子传导和氢扩散数据。然而,关于氢穿过矿物晶格扩散的实验数据仅限制了质子迁移的速度,以及与极化子(主要与三价铁相关的电子空穴)耦合的缺陷(例如空位),而对未耦合的游离质子的扩散没有限制。在橄榄石上进行的新扩散实验表明,与空位相关的晶格扩散高度依赖于结合氢的缺陷位点,但是没有一个位点能充分解释所观察到的实验室质子传导实验。氢与极化极化子(氧化还原交换)的扩散明显更快,但仍不能解释电导率测量中典型的低活化能。体扩散的过程将晶格扩散(与氧化还原交换或空位相关)与更快的晶界扩散相结合,解释了实验室的结果,但没有解释在100rnkm处平均晶粒尺寸为0.5-2 cm的现场观察结果在Kaapvaal克拉通的Jagersfontein金伯利岩层下方,与岩石学观察结果一致。另一个传导机制必须负责现场观察。

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