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钇(III)盐水溶液中的水合作用和离子对形成

Hydration and ion pair formation in aqueous Y(3+)-salt solutions.

作者信息

Rudolph Wolfram W, Irmer Gert

机构信息

Medizinische Fakultät der TU Dresden, Institut für Virologie im MTZ, Fiedlerstr. 42, 01307 Dresden, Germany.

出版信息

Dalton Trans. 2015 Nov 14;44(42):18492-505. doi: 10.1039/c5dt02586a. Epub 2015 Oct 7.

Abstract

Raman spectra of aqueous yttrium perchlorate, triflate (trifluoromethanesulfonate), chloride and nitrate solutions were measured over a broad concentration range (0.198-3.252 mol L(-1)). The spectra range from low wavenumbers to 4200 cm(-1). A very weak mode at 384 cm(-1) with a full width at half height at 50 cm(-1) in the isotropic spectrum suggests that the Y(3+)- octa-aqua ion is thermodynamically stable in dilute perchlorate solutions (∼0.5 mol L(-1)) while in concentrated perchlorate solutions outer-sphere ion pairs and contact ion pairs are formed. The octa-hydrate, Y(OH2)8 was also detected in a 1.10 mol L(-1) aqueous Y(CF3SO3)3 solution. Furthermore, very weak and broad depolarized modes could be detected which are assigned to Y(OH2)8(aq) at 100, 166, 234 and 320 cm(-1) confirming that a hexa-hydrate is not compatible with the hydrated species in solution. In yttrium chloride solutions contact ion pair formation was detected over the measured concentration range from 0.479-3.212 mol L(-1). The contact ion pairs in YCl3(aq) are fairly weak and disappear with dilution. At a concentration <0.2 mol L(-1) almost all complexes have disappeared. In YCl3 solutions, with additional HCl, chloro-complexes of the type Y(OH2)8-nCln (n = 1,2) are formed. The Y(NO3)3(aq) spectra were compared with a spectrum of a dilute NaNO3 solution and it was concluded that in Y(NO3)3(aq) over the concentration range from 2.035-0.198 mol L(-1) nitrato-complexes Y(OH2)8-n(NO3)ln (n = 1,2) are formed. The nitrato-complexes are weak and disappear with dilution <0.1 mol L(-1). DFT geometry optimizations and frequency calculations are reported for both the yttrium-water cluster in the gas phase and the cluster within a polarizable continuum model in order to implicitly describe the presence of the bulk solvent. The bond distance and angle for the square antiprismatic cluster geometry of Y(OH2)8 with the polarizable dielectric continuum is in good agreement with data from recent structural experimental measurements. The DFT frequency of the Y-O stretching mode of the Y(OH2)8 cluster, in a polarizable continuum, is at 372 cm(-1) in satisfactory agreement with the experimental value.

摘要

在较宽的浓度范围(0.198 - 3.252 mol L⁻¹)内测量了高氯酸钇、三氟甲磺酸钇(三氟甲烷磺酸盐)、氯化钇和硝酸钇水溶液的拉曼光谱。光谱范围从低波数到4200 cm⁻¹。在各向同性光谱中,384 cm⁻¹处有一个非常弱的模式,半高宽为50 cm⁻¹,这表明Y(³⁺)-八水合离子在稀高氯酸盐溶液(约0.5 mol L⁻¹)中热力学稳定,而在浓高氯酸盐溶液中会形成外层离子对和接触离子对。在1.10 mol L⁻¹的Y(CF₃SO₃)₃水溶液中也检测到了八水合物[Y(OH₂)₈]³⁺。此外,可以检测到非常弱且宽的去极化模式,它们在100、166、234和320 cm⁻¹处被归属于[Y(OH₂)₈]³⁺(aq),这证实了六水合物与溶液中的水合物种不兼容。在氯化钇溶液中,在0.479 - 3.212 mol L⁻¹的测量浓度范围内检测到了接触离子对的形成。YCl₃(aq)中的接触离子对相当弱,会随着稀释而消失。在浓度<0.2 mol L⁻¹时,几乎所有的配合物都消失了。在YCl₃溶液中,加入额外的HCl后,会形成[Y(OH₂)₈⁻ₙClₙ]⁺³⁻ⁿ(n = 1,2)类型的氯配合物。将Y(NO₃)₃(aq)的光谱与稀NaNO₃溶液的光谱进行了比较,得出在Y(NO₃)₃(aq)中,在2.035 - 0.198 mol L⁻¹的浓度范围内会形成硝酸根配合物[Y(OH₂)₈⁻ₙ(NO₃)ₗₙ]⁺³⁻ⁿ(n = 1,2)。硝酸根配合物很弱,在稀释至<0.1 mol L⁻¹时会消失。报道了气相中钇 - 水簇以及极化连续介质模型中的簇的密度泛函理论(DFT)几何优化和频率计算,以便隐含地描述本体溶剂的存在。[Y(OH₂)₈]³⁺的方形反棱柱簇几何结构与极化介电连续介质的键长和键角与最近结构实验测量的数据吻合良好。在极化连续介质中,[Y(OH₂)₈]³⁺簇的Y - O伸缩模式的DFT频率为372 cm⁻¹,与实验值吻合良好。

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