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首页> 外文期刊>Minerals Engineering >(106451)Monte Carlo simulations of electron-sample interactions at phase boundaries and implications for automated mineralogy
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(106451)Monte Carlo simulations of electron-sample interactions at phase boundaries and implications for automated mineralogy

机译:(106451)Monte Carlo仿真电子样品相互作用的相互作用和自动矿物学的影响

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Automated mineralogy instrumentation (QEMSCAN, MLA, TIMA) is routinely used for materials characterization in the mining industry. All current techniques identify minerals based on a combination of backscattered electron and chemical (energy-dispersive spectroscopy) signals read from the sample. Boundary zones, where two or more minerals are touching, yield signals that reflect a mix of the characteristics of multiple minerals and that may or may not match anything in the mineral database. These phase boundaries, varying in width, are known to cause errors in automated mineralogy analyses, but what mineral and boundary characteristics affect phase boundary width and how much error phase boundaries can cause remain poorly understood.New Monte Carlo modeling of electron-sample interactions at and near phase boundaries shows that the width of the zone of mixed signals, and hence the amount of error, depends on the grain size and texture of the sample;;the densities of the minerals and the ionization potentials of their constituent elements;;and the position and orientation of the boundary between the minerals, as well as various instrumental factors such as beam accelerating voltage. Error induced by phase boundaries is high when a high accelerating voltage is used to examine fine-grained samples with complex (intergrowth, exsolution) textures that involve low-density minerals with low-ionization-potential elements. Error is low when the sample is coarse-grained, lacks complex textural relationships that create boundary area, and consists of high-density minerals with high-ionization-potential elements, which have a higher electron stopping power and prevent the beam from spreading out as much. Where low- and high-density minerals are in contact at an angled boundary, the width of the boundary zone is low when the high-density mineral is on top and high when the low-density phase is on top.Calculations based on these simulations indicate that the amount of area that could fall within phase boundary zones depends strongly on grain size, shape, and width of boundary zone. Boundary phases may contribute significantly to overall analytical error for fine-grained minerals with low densities and composed of elements with low ionization potentials, but for most samples the boundary phase area is likely to be < 5% of the total surface area and the error relatively small. Errors induced by boundary phases will probably continue to annoy geometallurgists for some time, but with proper laboratory procedures for validating and cross-checking automated mineralogy results, they should not be a major component of error for most samples.
机译:自动化矿物学仪器(QEMSCAN,MLA,TIMA)经常用于采矿业的材料表征。所有电流技术都识别基于从样本读取的背散射电子和化学(能量分散光谱)信号的组合的矿物质。边界区,其中两个或更多矿物触摸,屈服的信号反映多种矿物质的特征的混合,并且可能或可能与矿物数据库中的任何东西匹配。已知这些相界,宽度不同,在自动矿物学分析中引起误差,但是矿物和边界特性影响相位边界宽度以及有多少误差相界可能导致仍然持久理解。电子样品相互作用的新蒙特卡罗建模。电子样品相互作用近相界面表明,混合信号区域的宽度,并因此取决于样品的晶粒尺寸和质地;;矿物质的密度和它们的组成元素的电离电位;;和矿物质之间边界的位置和取向,以及诸如光束加速电压的各种仪器因素。当使用高加速电压来检查具有涉及低密度矿物的低密度矿物质的复合物(栖分裂)纹理的细粒样品,相相边界引起的误差高。当样品粗糙颗粒时误差低,缺乏创造边界区域的复杂纹理关系,并且由具有高电离电位元件的高密度矿物质组成,具有更高的电子停止电源并防止光束散布很多。当低密度矿物在成角度边界处接触的情况下,当高密度矿物在顶部和高时,边界区的宽度低,当低密度相位在顶部的顶部时。基于这些模拟表示可能落在相边界区内的区域的量强烈地取决于边界区的晶粒尺寸,形状和宽度。边界阶段可显着对具有低密度的细粒矿物的整体分析误差以及由具有低电离电位的元件组成,但对于大多数样本,边界相位可能是总表面积的<5%,相对误差小的。边界阶段引起的错误可能会继续惹恼几何矿物质一段时间,但具有适当的实验室程序来验证和交叉检查自动化矿物学结果,它们不应该是大多数样本错误的主要成分。

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