NdF3-LiF-Nd2O3体系表面张力的研究

用拉筒法研究了NdF3-LiF体系的表面张力。采用二因子二次回归正交设计,得出表面张力(σ)与NdF3含量(C)、温度(t)的回归方程,讨论了NdF3含量、温度对表面张力的影响,并考察了加入Nd2O3对体系表面张力的影响。     

NdF3—LiF—Nd2O3体系表面张力数学模型的研究

用拉筒法研究了低NdF3浓度下NdF3-LiF体系的表面张力,采用二因子二次回归正交设计,得出表面张力（σ）与NdF3含量（C）、温度（t) 的回归方程,讨论了NdF3含量、温度对表面张力的影响,并考察了加入Nd2O3对体系表面张力的影响。     

NdF3-LiF-Nd2O3体系表面张力的研究

用拉筒法研究了 Nd F3- L i F体系的表面张力。采用二因子二次回归正交设计 ,得出表面张力 (σ)与Nd F3含量 (C)、温度 (t)的回归方程 ,讨论了 Nd F3含量、温度对表面张力的影响 ,并考察了加入 Nd2 O3 对体系表面张力的影响     

NdF3-LiF-Nd2O3体系粘度的研究

采用坩埚扭摆法研究了NdF3-LiF熔盐体系的粘度,讨论了NdF3含量及温度对体系粘度的影响,并考察了加入Nd2O3对体系粘度的影响。合理地解释了个别组分熔盐粘度出现异常的现象。     

NdF_3-LiF二元系相图测定和计算的再研究

氟盐-氧化钕熔盐电解是目前稀土金属钕工业生产的主要方法,优化工艺的确定、产品质量的保证以及更好综合性能熔盐组成的选择直接有赖于NdF3-LiF二元系相图的分析和应用。为了获得精确的NdF3-LiF二元系相图和热力学信息,采用差热分析法(DTA)测定不同配比NdF3-LiF二元熔盐体系的初晶温度,同时通过扫描电子显微镜(SEM)表征方法观察确认初晶温度的准确性,并依据DTA测试结果绘制出实验相图;再根据CALPHAD法利用FactSage软件中的Compound、Solution、Equilib、OptiSage和Phase diagram等模块优化计算最终确定出NdF3-LiF二元系的相图,发现实际的NdF3-LiF熔盐体系符合正规溶液;在1000~1100℃下,LiF的活度系数趋于稳定,而NdF3的活度系数随温度升高有明显增多的趋势,其电离形成离子的多寡与电解过程密切相关。另外,用计算机处理拟合出相图中NdF3-LiF二元系初晶温度的数学模型,讨论提出了工业熔盐电解钕适合的配比为w(NdF3)∶w(LiF)=10∶1或者是比之略小的w(NdF3)∶w(LiF)=9∶1。     

NdF3-LiF-Nd2O3系熔盐密度的研究

用阿基米德法研究了ＮｄＦ３－ＬｉＦ体系熔盐的密度。采用二因子二次回归正交设计，得出密度（ρ）与ＮｄＦ３含量（ｃ）、温度（ｔ）的回归方程，讨论了ＮｄＦ３含量及温度对熔体密度的影响，并考察了加入Ｎｄ２Ｏ３对体系密度的影响。     

钕电解相关物质理论分解电压的计算

本文计算了NdF3-LiF-Nd2O3体系各物质的理论分解电压。结果表明,采用惰性阳极,理论分解电压按Nd2O3、NdF3、LiF顺序依次增大,温度升高,理论分解电压降低;采用活性阳极(石墨)时,Nd2O3与石墨反应生成CO和CO2,其理论分解电压较小,反应较易发生,尤以生成CO的反应更易发生。但当电流密度较高或Nd2O3浓度较低时,可能生成碳氧氟化合物及氟碳化合物,并发生阳极效应,各物质的理论分解电压也随温度的升高而降低。     

Na_3AlF_6-AlF_3-LiF-MgF_2-Al_2O_3-Sm_2O_3熔盐体系表面张力的研究

采用拉筒法测定了在905~1055℃温度范围内Na_3AlF_6-AlF_3(12%)-LiF(5%)-MgF_2(5%)-Al_2O_3-Sm_2O_3熔盐体系的表面张力,研究了温度、Al_2O_3和Sm_2O_3添加量对熔盐表面张力的影响,并用最小二乘法建立了熔盐表面张力与温度、Al_2O_3与Sm_2O_3添加量之间的回归数学模型,确定了熔盐电解制备Al-Sm中间合金较为适宜的电解条件。研究结果表明:熔盐体系表面张力与温度有良好的线性关系,并随着温度的升高而下降;Al_2O_3添加量的递增对熔盐体系表面张力产生线性减小的影响,而Sm_2O_3添加量的递增却对熔盐表面张力产生线性增加的影响;当ω_(Al_2O_3)∶ω_(Sm_2O_3)=9∶1,7∶3或1∶1时,熔盐表面张力随混合氧化物添加量的增大而线性减小,当ω_(Al_2O_3)∶ω_(Sm_2O_3)=3∶7时,熔盐表面张力却随混合氧化物添加量的增大而线性增加;表面张力回归方程为σ=0.21813-0.00146ω_(Al_2O_3)+0.000553343ω_(Sm_2O_3)-0.0000774912 t。     

NdF3-LiF-Nd2O3体系粘度的研究

采用坩埚扭摆法研究了 Nd F3- L i F熔盐体系的粘度 ,讨论了 Nd F3含量及温度对体系粘度的影响 ,并考察了加入 Nd2 O3对体系粘度的影响。合理地解释了个别组分熔盐粘度出现异常的现象     

NdF_3-LiF-Nd_2O_3体系熔盐电导率的研究

采用交流阻抗谱技术测定熔盐电阻,并通过CVCC法研究了在1 020～1 120℃的温度范围内NdF3-LiF-Nd2O3熔盐体系的电导率,确定了温度、Nd2O3含量与熔盐电导率之间的关系,分析了温度和Nd2O3含量之间的相互作用以及对熔盐电导率的影响。研究结果表明,温度增加、Nd2O3含量减少,则电导率增大;在温度为1 080℃,Nd2O3含量为1.5%、2%、3.5%时,熔盐电导率变化幅度小,体系较为稳定。     

Density and ionic structure of NdF3-LiF melts

NdF3-LiF melts are commonly used in the electrolysis process of metallic neodymium production. Research on the density and ionic structure of the electrolyte is important for its close connection with the electrolysis mechanism and process. In this paper, the density of LiF-NdF3 melts was studied by the Archimedes method. The results showed that the density decreased with increasing temperature and LiF contents. The changing law was discussed and explained in terms of the micro ionic structure of the melts....     

NdF3—NaF—LiF熔体电导率的研究

采用三因子一次正交回归设计实验，研究了NdF3-NaF－LiF熔体的电导率，得出了该体系电导率的数学模型，分析了温度、NdF3浓度、NaF与LiF的摩尔比对电导率的影响。结果表明，提高温度、降低NdF3浓度、降低NaF与LiF的摩尔比均能提高电导率。所得研究结果可为稀土氟盐电解选择廉价电解质成分提供依据。     

钕电解阳极过电位的测定

用慢扫描示波法测定了钕电解的阳极过电位 .考察了温度、阳极电流密度、Nd2 O3添加量、电解质组成等因素对阳极过电位的影响 ,探讨了降低阳极过电位的可能途径 .结果表明 ,阳极过电位随阳极电流密度的增加而增大 ,随温度的升高而减小 ,一定范围内 ,阳极过电位与阳极电流密度的对数呈线性关系 ,满足塔菲尔方程 ;电解质中LiF和Nd2 O3浓度增加 ,阳极过电位降低 ;适当控制阳极电流密度、升高温度、增加电解质中LiF和Nd2 O3的浓度并尽可能减小极间距 ,均有利于降低阳极过电位     

Surface Properties of Manganese – Tin Liquid Alloys

We used the sessile drop method to study the temperature and concentration dependences of the density and surface tension of melts in the manganese – tin system. The density polytherms are linear dependences which are consistent with those calculated by the additivity rule for the specific volumes of the pure components. The temperature dependences of the surface tension are also linear and their temperature coefficient changes from negative values for tin-rich melts to positive values for melts with high manganese content. The surface tension isotherm is satisfactorily described by the Popel-Pavlov equation. We calculated the composition of the surface layer of the studied melts as a function of the composition of the bulk phase. We have shown that the model for the surface layer of melts in the Mn – Sn system at 1300°C is close to monolayer.     

Al2O3和Cr2O3对自蔓延冶金法制备 CuCr合金冶炼渣性能的影响

自蔓延冶金法制备CuCr合金时,合金中的Al₂O₃和Cr₂O₃夹杂物会在熔渣精炼过程中被冶炼渣溶解,改变熔渣成分,从而影响冶炼渣的熔点、黏度、密度和表面张力等性能,给精炼过程带来不利影响.使用熔体物性测定仪针对Al₂O₃和Cr₂O₃含量变化对冶炼渣的性能影响规律进行了研究,结果表明:Al₂O₃和Cr₂O₃含量的增加均可以提高熔渣的黏度、凝固温度和表面张力,Cr₂O₃对黏度和表面张力的影响较大,Al₂O₃对凝固温度的影响较大;Al₂O₃使熔体密度上升,Cr₂O₃使熔体密度先上升后下降.      

Volume and Surface Properties of a Bismuth-Containing Separating Nickel Melt

The influence of a bismuth impurity on the properties of solid and liquid alloys in the concentration range that obeys Henry’s law is considered. The structural and physicochemical properties, specifically, the density and the surface tension, of real melts are studied on relatively pure metals. The changes in the properties of the melts are estimated from changes in the temperature dependences of the density and the surface tension upon heating and cooling and in the concentration dependences of these parameters at a constant temperature. These dependences exhibit a correlation between the volume and surface properties of the melts: the density and the surface tension increase or decrease simultaneously. The introduction of bismuth in the nickel melt is accompanied by the appearance of a relatively strong compression effect (i.e., a decrease in the melt volume). At a certain bismuth content in the melt, the compression effect weakens because of the appearance of an excess phase or its associates and melt separation.     

Effect of exogenous refractory nanophases on the structural properties of nickel melts

The surface tension and density of nickel and Ni-S melts containing Al₂O₃ and TiN refractory-phase nanoparticles (RPNPs) are studied by the sessile drop method using a digital camera and computer processing of images. The dependences of the structural properties of Ni, Ni-(Al₂O₃,TiN), Ni-S, and Ni-S-(Al₂O₃,TiN) melts on temperature and the type and size of RPNPs are determined. It is found that the surface tension decreases with increasing temperature, the temperature dependence of the surface tension is inverted, the degree of loosening in the Ni-S-(Al₂O₃,TiN) melts decreases, and Ni-S-RPNP ensembles affect the melt structure.