共查询到20条相似文献，搜索用时 140 毫秒
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用等压法测定了298.15 K下氯化物型含铷卤水的三元子体系KCl-Rb Cl-H2O的等压平衡浓度,混合溶液的离子强度范围从0.5 mol·kg-1到4.9 mol·kg-1。由实验结果计算了混合溶液的渗透系数、水活度,根据Pitzer离子相互作用模型对实验结果进行参数化研究,拟合得到了描述KCl-Rb Cl-H2O混合溶液中离子间相互作用的Pitzer混合参数。用Pitzer模型计算的混合溶液的渗透系数、水活度与实验结果相一致。 相似文献
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报道由硫酸钠水溶液实验径向分布函数通过理论模型计算,解析溶液结构参数的方法。其中包括建立理论结构模型的基本依据,专用KURLVR程序使用和结构参数最小二乘精修,以及高斯多峰拟合等实用方法,最终给出能够阐述溶液本质的微观结构参数。结果表明,硫酸钠溶液中水合Na+有2个水合层,第一水合层Na+-OH2(I)距离为0.243 nm,配位数6.0;第二水合层距离为0.448 nm,配位数为13.3;SO2-4存在第一水合层,SO2-4-H2O距离为0.374 nm,配位数为9.1;水合硫酸根原子团中氧原子与水分子的作用距离和配位数按OS-W(1)、OS-W(2)、OS-W(3)、OS-W(4),距离依次为0.283、0.322、0.375和0.486 nm,配位数除OS-W(2)为12.9,其余都在8左右;除此之外溶液中还存在NaOSO-3接触离子对,Na-S距离为0.348 nm,配位数0.20,与晶体结构比较证实SO2-4以单齿形式配位到Na+;水共享离子对Na+-W-SO2-4中Na-S距离精修为0.491 nm,配位数0.62。精修的R因子为0.16,表明获得了很好的精修结果。 相似文献
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用高精度振动管密度仪测定二元系统(LiCl-H2O 和 MgCl2-H2O)和三元系统(LiCl-MgCl2-H2O)在273.15 至 308.15 K下溶液密度。采用VFT方程关联了LiCl和MgCl2溶液密度与温度、摩尔浓度关系。利用Young理想混合规则,根据二元体积性质计算计算了三元系统溶液密度。采用Pitzer离子相互模型拟合了LiCl-MgCl2-H2O,得到Pitzer单盐参数(β(0)VMX,β(1)VMX,and CVMX,MX=LiCl 和 MgCl2)和混合离子相互作用参数(θVLi,Mg、ψVLi,Mg,Cl)。在本工作中确定了三元体系在恒定离子强度下的混合体积 (ΔVm)。 相似文献
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X射线散射法是溶液结构研究的重要手段,是研究物质微观结构起源较早的一种方法。从X射线散射图解析出的径向分布函数可以得到具体的结构参数,因此这种方法在溶液结构的研究中得以广泛应用。国内外学者应用X射线散射法对溶液结构进行了大量的研究,确定了不同离子的水合数和水合离子半径,研究了温度、浓度、压力等因素对离子水化结构的影响,发现部分离子存在第二水合层。本文将按照碱金属离子、碱土金属离子、重金属离子、稀土元素离子、卤素离子、含氧酸根离子进行分类,对X射线散射法在溶液结构研究中取得的成果进行总结。在此基础上,分析了应用X射线散射法对水溶液结构研究的现状及其面临的挑战,讨论了该领域的发展前景。 相似文献
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盐湖卤水提锂工艺的难点之一在于卤水中镁锂比过高。采用红外光谱对非平衡动态降温过程中溶液结构变化进行分析,测定不同类型单盐溶液和卤水的结构变化,并基于此规律强化盐湖尾卤的镁锂分离。结果表明,MgSO4 溶液在40 ℃及以上时, 984 cm-1 处的特征峰显示可能出现接触式离子对结构(Mg2+-SO42-);1 280 cm-1处出现溶剂共享型离子对结构( Mg2+-H2O-SO42-);Li2SO4溶液中出现溶剂共享型离子对结构的可能性低,镁锂之间会出现结构差异。基于如上溶液结构的变化,通过非平衡动态降温过程,实现盐湖尾卤中的镁锂分离,镁锂质量比值可由最初的40降至20左右,Mg2+以MgSO4·nH2O型混合结晶产品的形式从卤水中析出,而液相中Li+的损失率可低至5.01%以下,以此达到了脱镁及锂富集的效果。 相似文献
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碳酸铷、硼酸化学计量比混合,蒸发溶液,直至五硼酸铷RbB5O8·4H2O晶体析出。经粉末X射线衍射（XRD）、拉曼光谱（Raman spectroscopy）、热重/微商热重/差示扫描量热（TG/DTG/DSC）、原子吸收光谱等实验方法,确定其化学组成及结构。298.15、333.15K时测量溶液的物理化学性质（密度、电导、pH）,并与经验方程进行拟合,研究五硼酸铷溶液的物化性质随浓度、温度的变化规律。根据文献报道的平衡常数,实验测量的pH数据,采用牛顿迭代法进一步研究五硼酸铷溶液中主要存在的硼酸根离子对类型、含量以及物种的形成。 相似文献
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We consider the two coupled differential equations of the two radial functions appearing in the displacement components of spheroidal oscillations for a transversely isotropic (TI) medium in spherical coordinates. Elements of the layer matrix have been explicitly written—perhaps for the first time—to extend the use of the Thomson-Haskell matrix method to the derivation of the dispersion function of Rayleigh waves in a transversely isotropic spherical layered earth. Furthermore, an earth-flattening transformation (EFT) is found and effectively used for spheroidal oscillations. The exponential function solutions obtained for each layer give the dispersion function for TI spherical media the same form as that on a flat earth. This has been achieved by assuming that the five elastic parameters involved vary as r p and that the density varies as r p-2 , where p is an arbitrary constant and r is the radial distance. A numerical illustration with p = - 2 shows that, in spite of the inhomogeneity assumed within layers, the results for spherical harmonic degree n , versus time period T , obtained here for the Primary Reference Earth Model (PREM), agree well with those obtained earlier by other authors using numerical integration or variational methods. The results for isotropic media derived here are also in agreement with previous results. The effect of transverse isotropy on phase velocity for the first two modes of Rayleigh waves in the period range 20 to 240 s is calculated and discussed for continental and oceanic models. 相似文献
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Finite element analysis of flow patterns near geological lenses in hydrodynamic and hydrothermal systems 总被引：2，自引：0，他引：2
Chongbin Zhao B. E. Hobbs H. B. Mühlhaus & A. Ord 《Geophysical Journal International》1999,138(1):146-158
We use theoretical and numerical methods to investigate the general pore-fluid flow patterns near geological lenses in hydrodynamic and hydrothermal systems respectively. Analytical solutions have been rigorously derived for the pore-fluid velocity, stream function and excess pore-fluid pressure near a circular lens in a hydrodynamic system. These analytical solutions provide not only a better understanding of the physics behind the problem, but also a valuable benchmark solution for validating any numerical method.
Since a geological lens is surrounded by a medium of large extent in nature and the finite element method is efficient at modelling only media of finite size, the determination of the size of the computational domain of a finite element model, which is often overlooked by numerical analysts, is very important in order to ensure both the efficiency of the method and the accuracy of the numerical solution obtained. To highlight this issue, we use the derived analytical solutions to deduce a rigorous mathematical formula for designing the computational domain size of a finite element model. The proposed mathematical formula has indicated that, no matter how fine the mesh or how high the order of elements, the desired accuracy of a finite element solution for pore-fluid flow near a geological lens cannot be achieved unless the size of the finite element model is determined appropriately.
Once the finite element computational model has been appropriately designed and validated in a hydrodynamic system, it is used to examine general pore-fluid flow patterns near geological lenses in hydrothermal systems. Some interesting conclusions on the behaviour of geological lenses in hydrodynamic and hydrothermal systems have been reached through the analytical and numerical analyses carried out in this paper. 相似文献
Since a geological lens is surrounded by a medium of large extent in nature and the finite element method is efficient at modelling only media of finite size, the determination of the size of the computational domain of a finite element model, which is often overlooked by numerical analysts, is very important in order to ensure both the efficiency of the method and the accuracy of the numerical solution obtained. To highlight this issue, we use the derived analytical solutions to deduce a rigorous mathematical formula for designing the computational domain size of a finite element model. The proposed mathematical formula has indicated that, no matter how fine the mesh or how high the order of elements, the desired accuracy of a finite element solution for pore-fluid flow near a geological lens cannot be achieved unless the size of the finite element model is determined appropriately.
Once the finite element computational model has been appropriately designed and validated in a hydrodynamic system, it is used to examine general pore-fluid flow patterns near geological lenses in hydrothermal systems. Some interesting conclusions on the behaviour of geological lenses in hydrodynamic and hydrothermal systems have been reached through the analytical and numerical analyses carried out in this paper. 相似文献
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碳酸铷、硼酸化学计量比混合,蒸发溶液,直至五硼酸铷RbB_5O_8·4H_2O晶体析出。经粉末X射线衍射、拉曼光谱、热重/微商热重/差示扫描量热(TG/DTG/DSC)、原子吸收光谱等实验方法,确定其化学组成及结构,298.15、333.15K时测量溶液的物理化学性质(密度、电导、pH),并与经验方程进行拟合,研究五硼酸铷溶液的物化性质随浓度、温度的变化规律。根据文献报道的平衡常数、实验测量的p H数据,采用牛顿迭代法进一步探讨了五硼酸铷溶液中主要存在的硼酸根离子物种分布规律。 相似文献