LiCl-KCl-MgCl2-Gd2O3熔盐共电沉积制备Mg-Li-Gd合金

在823 K和973 K的条件下,采用恒电流密度共电沉积法在LiCl-KCI-MgCl2-Gd2O3熔盐体系中制备Mg-Li-Gd合金,并运用XRD、SEM、EDS和OM对所制备合金进行微观组织分析.结果表明:在开始的30 min内,主要是Mg和Gd的沉积,所得合金含96.53%Mg,3.20%Gd和0.27%Li(质量分数),然后Li迅速沉积.可以通过控制电解时间或改变Gd2O3的浓度调节Mg-Li-Gd合金的组成.XRD分析可知,在Mg-Li-Gd合金中存在Mg3Gd相和Mg2Gd相.从Gd元素的面扫描分析可知,Gd元素主要分布在Mg-Li-Gd合金的晶界处.Gd的添加增强了合金的抗腐蚀能力.     

氯化物熔盐体系共电沉积法制备Mg-Li-Gd合金的研究

在LiCl-KCl-MgCl2-Gd2O3熔盐体系中采用电化学共沉积法制备Mg-Li-Gd合金,借助循环伏安和计时电位技术对熔盐电化学行为进行探讨,并运用XRD,SEM,EDS和OM对所得合金进行测试.研究结果表明,Gd2O3在LiCl-KCl熔盐体系中几乎不溶,而在LiCl-KCl-MgCl2熔盐中有一定的溶解度,而...     

稀土对La0.6R0.2Mg0.2（NiCoAlMn）3.3储氢合金相结构和电化学性能的影响

以La0.6R0.2Mg0.2Ni2.8Co0.2Al0.2Mn0.1(R=La、Ce、Pr、Nd、Y)合金为研究对象,研究稀土元素R部分替代La后对合金相结构和相组成及电化学性能的影响。X射线衍射(XRD)和显微电子探针(EPMA)方法分析结果表明,合金La0.8Mg0.2Ni2.8Co0.2Al0.2Mn0.1退火组织主要由Ce2Ni7型相(或Gd2Co7型)、PuNi3型相和CaCu5型相组成;Pr、Ce、Nd元素的替代对合金的相组成没有明显影响,而Y元素替代使合金中CaCu5型相明显减少,Ce2Ni7型(或Gd2Co7型)相显著增加,其相丰度达到79.03%。Y元素替代时合金中Gd2Co7型相基本消失。电化学测试和分析表明,稀土元素R替代La后对合金电极活化性能影响不大,其中Pr、Nd、Y部分替代La在一定程度上提高了合金的最大放电容量,而元素Y替代时合金电极容量最高达到392.6mAh/g;Y元素部分替代La使合金电极的循环稳定性得到明显提高,S100达到90.3%。     

Microstructures and Properties of As-Cast Mg92Zn4Y4 and Mg92Zn4Y3Gd1 Alloys with LPSO Phase

采用普通凝固技术制备了含有长周期堆垛有序 (long period stacking ordered, LPSO) 结构相的Mg92Zn4Y4和Mg92Zn4Y3Gd1合金。通过OM、SEM、EDS、XRD和TEM分析了合金中各相形貌、微区成分及结构。结果表明：Zn/RE原子比为1的2种铸态镁合金中均存在14H-LPSO结构相;在Mg-Zn-Y合金中添加稀土元素Gd增加了合金的形核质点并促进了长周期堆垛有序结构相的形成,14H-LPSO相体积分数由12.1%增至30.4%;LPSO结构相在高温形成时分割了a-Mg树枝晶,基体平均晶粒尺寸由50 μm降至10 μm以下;铸态Mg92Zn4Y4合金的凝固组织为a-Mg固溶体+Mg12ZnY+Mg3Zn3Y2+Mg-Y;铸态Mg92Zn4Y3Gd1合金的凝固组织主要为a-Mg固溶体+Mg12Zn(Y,Gd)+Mg3Zn3(Y,Gd)2;室温条件下,Mg92Zn4Y4和Mg92Zn4Y3Gd1合金的压缩率达到12.4%和15.5%,热导率分别为99.233和88.639 W·(m·K)-1。     

LPSO相增强铸态Mg_(92)Zn_4Y_4和Mg_(92)Zn_4Y_3Gd_1合金组织与性能分析（英文）

采用普通凝固技术制备了含有长周期堆垛有序(long period stacking ordered,LPSO)结构相的Mg92Zn4Y4和Mg92Zn4Y3Gd1合金。通过OM、SEM、EDS、XRD和TEM分析了合金中各相形貌、微区成分及结构。结果表明:Zn/RE原子比为1的2种铸态镁合金中均存在14H-LPSO结构相;在Mg-Zn-Y合金中添加稀土元素Gd增加了合金的形核质点并促进了长周期堆垛有序结构相的形成,14H-LPSO相体积分数由12.1%增至30.4%;LPSO结构相在高温形成时分割了αMg树枝晶,基体平均晶粒尺寸由50μm降至10μm以下;铸态Mg92Zn4Y4合金的凝固组织为α-Mg固溶体+Mg12Zn Y+Mg3Zn3Y2+Mg-Y;铸态Mg92Zn4Y3Gd1合金的凝固组织主要为α-Mg固溶体+Mg12Zn(Y,Gd)+Mg3Zn3(Y,Gd)2;室温条件下,Mg92Zn4Y4和Mg92Zn4Y3Gd1合金的压缩率达到12.4%和15.5%,热导率分别为99.233和88.639W·(m·K)-1。     

固相反应Gd2Zr2O7陶瓷的形成机理研究

以ZrO2,Gd2O3粉体为原料,采用固相合成工艺制备了Gd2Zr2O7陶瓷,通过在不同温度(1273 K～1873 K)下进行混合料的烧结以及对不同温度下合成产物的XRD相分析,来研究Gd2Zr2O7陶瓷的合成过程和形成机理.结果表明ZrO2和Gd2O32种粉体在1473 K开始发生相互固溶,随着温度升高,固溶程度逐渐加大,在1673 K时ZrO2和Gd2O3之间的固溶达到饱和,开始析出Gd2Zr2O7相,当温度达到1773 K时固溶结束,此时产物为Gd2Zr2O7,1873 K时ZrO2和Gd2O3烧结完成,产物为单相的Gd2Zr2O7.     

掺杂离子对Gd2O2S:Eu3+磷光体结构和发光性能的影响

采用高温固相反应法制备出新型红色长余辉发光材料Gd2O2S:Eu3+,Xn+(X为Mg、Si、Ti中的一种或两种),研究掺杂离子对Gd2O2S:Eu3+磷光体的晶体结构、形貌粒度和发光性能的影响。通过X射线粉末衍射(XRD)、扫描电镜(SEM)和分光光度计等对合成产物进行分析与表征。结果表明:掺杂离子没有改变Gd2O2S:Eu3+磷光体的晶体结构,颗粒的形貌为类球形,分散性良好。同时,掺杂离子显著地延长发光材料Gd2O2S:Eu3+的余辉时间,并显示纯正的红色发光。     

氯化物熔盐体系共电沉积法制备Al-Li-Gd合金的研究

在773K时,采用循环伏安法、方波伏安法和计时电位法研究了Gd(III)和Al(III)在LiCl-KCl-AlCl3-GdCl3熔盐体系中的电化学行为及共电沉积制备Al-Li-Gd合金,并借助XRD,SEM-EDS对所得合金进行表征.结果表明,Gd(III)在预先沉积的Al上欠电位沉积形成了两种Al-Gd金属间化合物,当电流密度超过-279.5 mA/cm2时,Al,Gd和Li能同时析出.通过调节熔盐中AlCl3的含量可以获得不同相的Al-Li-Gd合金.Al-Li-Gd合金含有Al2Gd和Al2Gd3,Gd在合金中分布不均匀,而Al的分布相对均匀.     

(Gd0.8Ca0.2)2Ce2O6.6陶瓷的制备及热导率

以Gd2O3、CeO2和CaO为原料,采用固相反应法制备(Gd0.8Ca0.2)2Ce2O6.6陶瓷材料。用X射线衍射(XRD)技术和扫描电镜(SEM)研究样品的相组成和微观组织,用激光脉冲法测试样品的热扩散系数。结果表明,所制备的样品具有单一的萤石结构,组织致密且晶界清晰,其在800℃的热导率仅为YSZ陶瓷的89%,较低热导率表明该材料有潜力用作新型热障涂层用陶瓷材料。     

高强Mg-Gd-Y-Zn-Zr合金的微观组织和力学性能

通过金属模铸、热挤压和时效处理(T5)工艺过程制备出高强Mg-7Gd-4Y-1.6Zn-0.5Zr合金,并利用光学显微镜、XRD、SEM及TEM分析研究Mg合金不同状态下的显微组织和力学性能。结果表明:Mg-7Gd-4Y-1.6Zn-0.5Zr合金的铸态组织主要由α-Mg基体和沿晶界分布的片层状第二相Mg12Zn(Gd,Y)组成,经过热挤压变形后,合金晶粒显著细化,时效处理过程中Mg12Zn(Gd,Y)相上析出少量细小的颗粒状Mg3Zn3(Gd,Y)2相。时效态合金的抗拉强度、屈服强度和伸长率分别达到446 MPa、399 MPa和6.1%,其强化方式主要为细晶强化和第二相强化。     

Thermodynamics and phase diagrams in the binary systems Na2O-SiO2, Na2O-GeO2, Na2O-B2O3, Li2O-B2O3, CaO-B2O3, SrO-B2O3, and BaO-B2O3

We applied our model to the enthalpy of mixing data of the binary systems Na₂O-SiO₂, Na₂O-GeO₂, Na₂O-B₂O₃, Li₂O-B₂O₃, CaO-B₂O₃, SrO-B₂O₃, and BaO-B₂O₃. The most stable composition in the liquid, that is where the enthalpy of mixing is most negative, is with a metal-oxygen ratio of 4 to 3, for monovalent metals (Na and Li) and 3 to 4 for divalent metals (Ba and Ca) in liquid silicates or borates. The same applies to the CaO-SiO₂, CaO-Al₂O₃, PbO-B₂O₃, PbO-SiO₂, ZnO-B₂O₃, and ZnO-SiO₂ systems. The oxygen to metal ratio, its constant value in various types of systems, reflects and describes the structure of the liquid. Using the analyzed enthalpies of mixing data and the available phase diagrams, we calculated the enthalpies of formation of the various binary compounds. The results are in excellent agreement with data in the literature that were obtained from direct solid-solid calorimetry.     

Fe2+-Ni2+-NH3-NH4+-C2O42-H2O体系的沉淀配合平衡热力学

针对草酸盐配位共沉淀热分解还原法制备超细铁镍合金粉过程中Fe2+-Ni2+-NH3-NH4+-C2O42--H2O体系的溶液平衡建立热力学分析模型,并根据模型进行相关计算,揭示反应体系中各物质随pH值、氨及草酸浓度的变化关系。结果表明:溶液中的Fe主要以[Fe(C2O4)n]2 2n络合物形式存在,而铁氨络合物含量很低。当氨含量较低时,溶液中的Ni主要以[Ni(C2O4)n]2 2n存在;氨含量较高时,在酸性条件下,溶液中的Ni主要以[Ni(C2O4)n]2 2n存在,在碱性条件下,则主要以[Ni(NH3)n]2+存在。低pH值下,Ni的沉淀率较Fe的高,而高pH值下,Ni的沉淀率则较Fe的低。     

Al2O3-Sm2O3-CeO2电解质的性能（英文）

采用溶胶-凝胶法和低温燃烧技术制备Ce1-xSmxO2（x=0,0.1,0.2,0.3）和掺杂Sm和（2%-8%）Al2O3的二氧化铈;研究其合成、结构、致密化、导电性和热膨胀等性能,并利用XRD研究其结构和相组成。结果表明,于1300°C烧结球团,获得致密的陶瓷,于1250°C在Ce0.8Sm0.2O0.2中加入2%和4%的Al2O3以促进烧结。利用扫描电子显微镜观察烧结后球团的表面形貌,使用双探针交流阻抗谱研究总离子电导率。     

Al2O3包覆改善P2型Na2/3Fe1/2Mn1/2O2正极材料的存储性能

采用超声喷雾热解与高温固相烧结相结合的方法合成P2型Na_2/3Fe_1/2Mn_1/2O₂材料。通过X射线衍射仪、扫描电子显微镜和电化学充放电设备对材料的结构、形貌和电化学性能进行全面的表征。此外,在Na_2/3Fe_1/2Mn_1/2O₂表面包覆Al₂O₃薄层,该包覆层可以抑制Na₂CO₃·H₂O的形成,提高Na_2/3Fe_1/2Mn_1/2O₂材料的存储性能,从而改善其电化学性能。这种简单的表面改性方法为合成高性能钠离子电池正极材料提供了新思路。     

Synthesis and properties of CaCd2Sb2 and EuCd2Sb2

High density polycrystalline CaCd₂Sb₂ and EuCd₂Sb₂ intermetallics are synthesized by Spark Plasma Sintering and their thermoelectric properties are investigated. X-ray diffraction measurements reveal both materials have a structure in space group, containing a small amount of CdSb as a second phase. Thermoelectric measurements indicate both are p-type conductive materials. The figure of merit value of CaCd₂Sb₂ is 0.04 at 600 K and that of EuCd₂Sb₂ is 0.60 at 617 K. Theoretical calculations show that CaCd₂Sb₂ is a degenerate semiconductor with a band gap of 0.63 eV, while EuCd₂Sb₂ is metallic with DOS of 13.02 electrons/eV. For deeper understanding of the better thermoelectric properties of EuCd₂Sb₂, its low temperature magnetic, transport and heat capacity properties are investigated. Its Nèel temperature is 7.22 K, convinced by heat capacity anomaly at 7.13 K. Hall effect convinced that it is a p-type conductive material. It has high Hall coefficient, high carrier concentration and high carrier mobility of +1.426 cm³/C, 4.38 × 10¹⁸/cm³ and 182.40 cm²/Vs, respectively. They are all in the magnitude of good thermoelectric materials. The Eu 4f level around Fermi energy and antiferromagnetic order may count for the better thermoelectric properties of EuCd₂Sb₂ than that of CaCd₂Sb₂.     

Y2O3-BaO-SiO2-B2O3-Al2O3 glass sealant for solid oxide fuel cells

A glass based on Y₂O₃-BaO-SiO₂-B₂O₃-Al₂O₃ (named YBA) has been investigated as sealant for planar solid oxide fuel cells (SOFCs). The YBA glass has been systematically characterized by differential thermal analysis, dilatometer, scanning electron microscopy, impedance analysis, and open circuit voltage to examine their suitability as sealant. The coefficient of thermal expansion of YBA is 11.64 × 10⁻⁶ K⁻¹ between 323 and 873 K. The resistivity is 9.1 × 10⁴ Ω cm at 800 °C. The glass sealant is found to be well adhered with other cell components, such as electrolytes and stainless steels, at an optimum sealing temperature of 800 °C. All measured results showed that the YBA glass appears to be a promising sealant for SOFCs.     

New Zr6CoAs2-type compounds: Y6CoBi2, Ho6CoBi2 and Tm6CoBi2

Results of a powder X-ray diffraction investigation of new ternary compounds are reported. The compounds Y₆CoBi₂ [a=0.8312(1) nm, c=0.4144(1) nm], Ho₆CoBi₂ [a=0.8246(2) nm, c=0.4095(1) nm], and Tm₆CoBi₂ [a=0.8155(2) nm, c=0.4066(1) nm] crystallize in the hexagonal Zr₆CoAs₂-type structure (space group P6b2m No. 189). The Zr₆CoAs₂-type structure is a superstructure of the Fe₂P-type structure.     

Electronic structures and Eu photoluminescence behaviors in Y2Si2O7 and La2Si2O7

The electronic structures and linear optical properties of Y₂Si₂O₇ (YSO) and La₂Si₂O₇ (LSO) are calculated by LDA method based on the theory of DFT. Both YSO and LSO are direct-gap materials with the direct band gap of 5.89 and 6.06 eV, respectively. The calculated total and partial density of states indicate that in both YSO and LSO the valence band (VB) is mainly constructed from O 2p and the conduction band (CB) is mostly formed from Y 4d or La 5d. Both the calculated VB and CB of YSO exhibit relatively wider dispersion than that of LSO. In addition, the CB of YSO presents more electronic states. Meanwhile, the VB of LSO shows narrower energy distribution with higher electronic states density. The theoretical absorption of YSO shows larger bandwidth and higher intensity than that of LSO. The results are compared with the experimental host excitations and impurity photoluminescence in Eu³⁺-doped YSO and LSO.     

Phase equilibria in the system La2O3-BaO-P2O5: The partial system LaPO4-Ba2P2O7-Ba(PO3)2

The LaPO₄-Ba₂P₂O₇-Ba(PO₃)₂ portion of the oxide La₂O₃-BaO-P₂O₅ system has been investigated. Important parts of this investigation were the determination of equilibria in the LaPO₄-Ba(PO₃)₂ subsystem and the addition of liquidus data to the partially known LaPO₄-Ba(PO₃)₂-Ba₂P₂O₇ subsystem. These data were combined with known data from the LaPO₄-Ba₂P₂O₇ subsystem and with measurements of the equilibria within the LaPO₄-Ba₃P₄O₁₃ isopleth to determine the nature of the phase equilibria in the quasi-ternary LaPO₄-Ba₂P₂O₇-Ba(PO₃)₂ system.     

载体中ZrO2/Al2O3比对Pt/ZrO2-Al2O3催化剂性能的影响

相比汽油车而言,柴油车具有高效、低油耗的优势已得到广泛应用。本实验以ZrO₂作为改性剂,探究了ZrO₂与Al₂O₃的质量比对催化剂的影响。研究结果表明：随着ZrO₂的加入,Pt粒子先减小后增大;Pt粒子与载体的交互作用先增大后减小。活性实验数据分析表明,ZrO₂的最佳添加量为40 wt%,CO和C₃H₆完全氧化温度分别降低20 _oC 、25 _oC。贵金属在催化剂的分散度以及贵金属与载体的相互作用随着ZrO₂与Al₂O₃质量比的变化而变化。Pt粒子越小,其与载体的交互作用越强,这表明催化剂性能越强。