Element Partitioning (Mineral-Melt, Metal-/Sulfide-Silicate) in Planetary Sciences

B. Mahan
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In planetary sciences, the phase pairs typically considered are mineral-melt, metal-silicate, and sulfide-silicate, owing largely to the ubiquity of their coexistence in planetary materials across scales and context, from the micrometer-sized components of meteorites up to the size of planets (thousands of kilometers).\n It is common to speak of trace elements in terms of their tendency toward forming metallic, sulfidic, or oxide phases, and the terms “siderophile,” “chalcophile,” and “lithophile” (respectively) are used to define these tendencies under what is known as the Goldschmidt Classification scheme. The metric of an element’s tendency to concentrate into one phase relative to another is expressed as the ratio of its concentration (as a weight or molar fraction) in one phase over another, where convention dictates the reference frame as solid over liquid, and metal or sulfide over silicate; this mathematical term is the element’s partition coefficient, or distribution coefficient, between the two respective phases,DMPhaseBPhaseA (where M is the element of interest, most often reported as molar fraction), or simply DM. In general, trace elements obey Henry’s Law, where the element’s activity and concentration are linearly proportional. Practically speaking, this means that the element is sufficiently dilute in the system such that its atoms interact negligibly with one another compared to their interactions with major element phases, and thus the trace element’s partition coefficient in most settings is not appreciably affected by its concentration.\n The radius and charge of an element’s ionized species (its ionic radius and valence state)—in relation to either the major element ion for which it is substituting or the lattice site vacancy or interstitial space it is filling—generally determine the likelihood of trace element substitution or vacancy/interstitial fill (along with the net charge of the lattice space). The key energy consideration that underlies an element’s partitioning is the Gibbs free energy of reaction between the phases involved. Gibbs free energy is the change in internal energy associated with a chemical reaction (at a given temperature and pressure) that can be used to do work, and is denoted as ΔGrxn. Reactions with negative ΔGrxn values are spontaneous, and the magnitude of this negative value for a given phase, for example, a metal oxide, denotes the relative affinity of the metal toward forming oxides. That is to say, an element with a highly negative ΔGrxn for its oxide species at relevant pressure-temperature conditions will tend to be found in oxide and silicate minerals, that is, it will be lithophile (and vice versa for siderophile elements).\n Trace element partitioning systematics in mineral-melt and metal-/sulfide-silicate systems have boundless applications in planetary science. A growing collective understanding of the partition coefficients of elements has been built on decades of physical chemistry, deterministic theory, petrology, experimental petrology, and natural observations. Leveraging this immense intellectual, technical, and methodological foundation, modern trace element partitioning research is particularly aimed at constraining the evolution of plate tectonics on Earth (conditions and timing of onset), understanding the formation history of planetary materials such as chondrite meteorites and their constituents (e.g., chondrules), and de-convolving the multiply operating processes at play during the accretion and differentiation of Earth and other terrestrial planets.","PeriodicalId":304611,"journal":{"name":"Oxford Research Encyclopedia of Planetary Science","volume":"152 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-06-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Oxford Research Encyclopedia of Planetary Science","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1093/acrefore/9780190647926.013.202","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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Abstract

Element partitioning—at its most basic—is the distribution of an element of interest between two constituent phases as a function of some process. Major constituent elements generally affect the thermodynamic environment (chemical equilibrium) and therefore trace element partitioning is often considered, as trace elements are present in minute quantities and their equilibrium exchange reactions do not impart significant changes to the larger system. Trace elements are responsive to thermodynamic conditions, and thus they act as passive tracers of chemical reactions without appreciably influencing the bulk reactions themselves. In planetary sciences, the phase pairs typically considered are mineral-melt, metal-silicate, and sulfide-silicate, owing largely to the ubiquity of their coexistence in planetary materials across scales and context, from the micrometer-sized components of meteorites up to the size of planets (thousands of kilometers). It is common to speak of trace elements in terms of their tendency toward forming metallic, sulfidic, or oxide phases, and the terms “siderophile,” “chalcophile,” and “lithophile” (respectively) are used to define these tendencies under what is known as the Goldschmidt Classification scheme. The metric of an element’s tendency to concentrate into one phase relative to another is expressed as the ratio of its concentration (as a weight or molar fraction) in one phase over another, where convention dictates the reference frame as solid over liquid, and metal or sulfide over silicate; this mathematical term is the element’s partition coefficient, or distribution coefficient, between the two respective phases,DMPhaseBPhaseA (where M is the element of interest, most often reported as molar fraction), or simply DM. In general, trace elements obey Henry’s Law, where the element’s activity and concentration are linearly proportional. Practically speaking, this means that the element is sufficiently dilute in the system such that its atoms interact negligibly with one another compared to their interactions with major element phases, and thus the trace element’s partition coefficient in most settings is not appreciably affected by its concentration. The radius and charge of an element’s ionized species (its ionic radius and valence state)—in relation to either the major element ion for which it is substituting or the lattice site vacancy or interstitial space it is filling—generally determine the likelihood of trace element substitution or vacancy/interstitial fill (along with the net charge of the lattice space). The key energy consideration that underlies an element’s partitioning is the Gibbs free energy of reaction between the phases involved. Gibbs free energy is the change in internal energy associated with a chemical reaction (at a given temperature and pressure) that can be used to do work, and is denoted as ΔGrxn. Reactions with negative ΔGrxn values are spontaneous, and the magnitude of this negative value for a given phase, for example, a metal oxide, denotes the relative affinity of the metal toward forming oxides. That is to say, an element with a highly negative ΔGrxn for its oxide species at relevant pressure-temperature conditions will tend to be found in oxide and silicate minerals, that is, it will be lithophile (and vice versa for siderophile elements). Trace element partitioning systematics in mineral-melt and metal-/sulfide-silicate systems have boundless applications in planetary science. A growing collective understanding of the partition coefficients of elements has been built on decades of physical chemistry, deterministic theory, petrology, experimental petrology, and natural observations. Leveraging this immense intellectual, technical, and methodological foundation, modern trace element partitioning research is particularly aimed at constraining the evolution of plate tectonics on Earth (conditions and timing of onset), understanding the formation history of planetary materials such as chondrite meteorites and their constituents (e.g., chondrules), and de-convolving the multiply operating processes at play during the accretion and differentiation of Earth and other terrestrial planets.
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行星科学中的元素划分(矿物-熔体,金属/硫化物-硅酸盐)
元素划分——最基本的是——作为某种过程的函数,在两个组成阶段之间分配感兴趣的元素。主要组成元素通常影响热力学环境(化学平衡),因此经常考虑微量元素分配,因为微量元素以微量存在,它们的平衡交换反应不会给更大的系统带来重大变化。微量元素对热力学条件有反应,因此它们作为化学反应的被动示踪剂,对主体反应本身没有明显的影响。在行星科学中,通常考虑的相对是矿物熔体、金属硅酸盐和硫化物硅酸盐,这主要是因为它们在不同尺度和背景下的行星物质中普遍存在,从陨石的微米大小的成分到行星的大小(数千公里)。人们通常根据微量元素形成金属相、硫化物相或氧化物相的倾向来谈论它们,而“亲铁”、“亲铜”和“亲石”这三个术语(分别)被用来根据所谓的戈德施密特分类方案来定义这些倾向。一种元素相对于另一种元素浓缩成一相的趋势的度量,表示为其在一相中的浓度(重量或摩尔分数)与另一相的比率,惯例规定参考框架为固体比液体,金属或硫化物比硅酸盐;这个数学术语是元素在两相之间的分配系数或分配系数,DMPhaseBPhaseA(其中M是感兴趣的元素,通常以摩尔分数表示),或简称DM。一般来说,微量元素遵循亨利定律,元素的活度和浓度成线性比例。实际上,这意味着该元素在系统中被充分稀释,使得其原子之间的相互作用与它们与主要元素相的相互作用相比可以忽略不计,因此在大多数情况下,微量元素的分配系数不受其浓度的明显影响。元素电离态的半径和电荷(它的离子半径和价态)——与它所取代的主元素离子或它所填充的晶格空位或间隙有关——通常决定了微量元素取代或空位/间隙填充的可能性(以及晶格空间的净电荷)。决定元素分配的关键能量因素是相关相之间反应的吉布斯自由能。吉布斯自由能是指化学反应(在给定温度和压力下)的热力学能的变化,它可以用来做功,用ΔGrxn表示。负ΔGrxn值的反应是自发的,对于给定相,例如金属氧化物,该负值的大小表示金属形成氧化物的相对亲和力。也就是说,在相关的压力-温度条件下,氧化态具有高度负ΔGrxn的元素往往存在于氧化物和硅酸盐矿物中,也就是说,它将是亲石的(亲铁元素反之亦然)。矿物-熔体和金属/硫化物-硅酸盐体系的微量元素分配系统在行星科学中有着广泛的应用。在几十年的物理化学、确定性理论、岩石学、实验岩石学和自然观测的基础上,对元素分配系数的集体理解日益加深。利用这一巨大的智力、技术和方法基础,现代微量元素划分研究特别旨在限制地球上板块构造的演化(条件和开始的时间),理解行星材料的形成历史,如球粒陨石及其成分(如球粒),并对地球和其他类地行星在吸积和分化过程中发挥作用的多重操作过程进行解卷积。
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