稀土对MoSi2力学性能和抗氧化性能的影响

采用自蔓延和真空烧结方法制备了掺杂0．9％La2O3的MoSi2基复合材料，利用热重分析法，SEM和X射线考察了La2O3颗粒对MoSi2力学性能、抗氧化特性以及循环氧化后力学性能的影响。结果表明，与纯MoSi2相比，RE／MoSi2材料的弯曲强度和断裂韧性分别提高了46％和78％；稀土对MoSi2材料的强韧化机制主要是细晶强化、弥散强化和细晶韧化。RE／MoSi2的氧化增重是纯MoSi2的2．5倍，稀土使MoSiz材料的抗氧化性能降低。由于纯MoSi2材料氧化后的晶粒长大，其抗弯强度比氧化前降低了17％。稀土对MoSi2氧化时的晶粒长大倾向有抑制作用，使得RE／MoSi2材料的抗弯强度基本不变。     

La2O3对Mo5Si3/MoSi2复合材料的改性研究

通过粉末冶金方法制备了Mo5Si3/MoSi2和La2O3/Mo5Si3/MoSi2复合材料,探讨了其烧结工艺.检测了其密度、维氏硬度、抗弯强度和断裂韧性,运用X射线衍射仪和扫描电镜（SEM）研究了La2O3对Mo5Si3/MoSi2复合材料显微结构和力学性能的改性影响.结果表明,La2O3/Mo5Si3/MoSi2复合材料的合理烧结温度为1600 ℃,比MoSi2材料提高了100 ℃; 稀土氧化物的加入细化了晶粒,且明显提高了材料的致密度、维氏硬度和抗弯强度; 其强化机制为细晶强化和弥散强化; 韧化机制为细晶韧化、裂纹偏转、裂纹分支和微桥接.     

稀土/MoSi2复合材料的干摩擦磨损性能

运用M－2型摩擦磨损试验机测定了不同载荷条件下稀土／MoSi2复合材料与45钢配对件的干摩擦磨损性能，采用SEM观察了摩擦副表面的形貌和X射线分析了磨屑相组成，并探讨了其磨损机制。结果表明：稀土／MoSi2和MoSi2与45钢干摩擦时，在负荷不超过150N的范围内，其摩擦系数μ和磨损率W与负荷p间较好地满足关系式：W（或μ）＝a bp cp^2 p^3 ep^4，两种均具有优异的耐磨性能，在80－120N范围，稀土／MoSi2复合材料的磨损率比纯MoSi2材料的至少降低了65％；稀土／MoSi2材料的磨损机制主要是粘着磨损。     

Al2O3-30％TiCN-0.2％Y2O3复相陶瓷的氧化性研究

对热压法制备的Al2O3-30％TiCN-0.2％Y2O3复合陶瓷抗高温氧化性能的研究。结果表明：该材料在空气中静态氧化时的氧化增重符合抛物线规律，氧化产物主要随氧化时间增加，氧化温度的提高而增加，该材料具有较好的抗氧化性能。Al2O3-30％TiCN-0.2％Y2O3复相陶瓷的氧化产物为TiO2。由于氧化产物TiO2存在以及氧化反应的体积膨胀效应，使氧化膜中产生残余应力并导致氧化膜的破坏，适当的氧化处理可使Al2O3-30％TiCN-0.2％Y2O3陶瓷材料的抗弯强度得到一定程度的提高，强度提高可达4．5％。     

MC尼龙-纳米La2O3复合材料的制备及性能研究

用原位分散聚合法制备了一系列MC尼龙／纳米La2O3复合材料，研究了纳米La2O3用量对复合材料力学性能的影响，用SEM观察了La2O3粒子在MC尼龙基体中的分散情况，用XRD对复合材料的晶体结构进行了表征。SEM观察结果表明，当纳米La2O3用量小于1％时，纳米La2O3均匀分散于MC尼龙基体中，团聚情况很少，当纳米La2O3用量大于1％时，纳米La2O3开始团聚；XRD研究结果表明，纳米La2O3没有改变MC尼龙的结晶形态；力学性能的研究结果表明，随着纳米La2O3用量的增加，复合材料的拉伸强度、断裂伸长率、缺口冲击强度、弯曲强度和弯曲模量都呈先升后降的趋势，当纳米La2O3用量为0．5％时，复合材料的拉伸强度和断裂伸长率达到最大值，分别比MC尼龙提高17．9％和52．1％，当纳米La2O3的用量为1．0％时，复合材料的缺口冲击强度、弯曲强度和弯曲模量达到最大值，分别比MC尼龙基体提高36，6％．12．7％和16．3％。     

Y2O3和CeO2对氮化硅烧结性能的影响

研究了Y2O3,CeO2的添加量在不同烧结温度下对Si3N4烧结性能的影响，分析了其助烧作用及晶界二次小晶粒形成的机制。结果表明，添加Y2O3,CeO2的Si3N4其烧结性能良好。Y2O3添加5％（此时Al2O3含量为4％）及CeO2为8％时对制品烧结促进作用最大。热处理后在Si3N4晶界获得结晶完美的二次小晶粒，使晶界玻璃相大为下降，为Si3N4高温力学性能的提高奠定结构基础。     

稀土对Si3N4陶瓷力学性能和显微组织的影响

研究了Y2 O3,La2 O3,Nd2 O3等稀土氧化物对Si3N4 陶瓷力学性能和显微组织的影响。添加稀土氧化物的Si3N4 陶瓷可以获得较好的力学性能。添加复合稀土氧化物 (Y2 O3 La2 O3)后 ,断裂韧性达 7 8MPa·m1 2 ,抗弯强度达 962MPa,其性能提高的主要原因是稀土氧化物改善了材料的显微组织 ,提高了 β Si3N4 晶粒的长径比。     

Y2O3提高Al2O3-30％TiCN复合材料的抗热震性能

研究采用热压法制备含Y2O3的Al2O3-30％TiCN复合材料的热震性能。结果表明：材料的抗热震性是由材料的显微结构及增韧机制所决定。通过SEM观察及热震理论计算可知：Al2O3-30％TiCN复合材料断口起伏较大。由于稀土Y2O3的加入，生成少量的YAC相，抑制了Al2O3和TiCN晶粒长大，有助于提高含稀土Y2O3的Al2O3-30％TiCN复合材料断裂韧性。有效地阻止了热震裂纹的进一步扩展及合并，提高了复合材料的抗热震性。200～800℃淬火温度范围内添加Y2O3的Al2O3-30％TiCN复合材料的残留压痕强度明显高于未加Y2O3的复合材料，且抗热震阻力较大。含Y2O3的Al2O3-30％TiCN复合材料的裂纹萌生阻力R’比不含Y2O3的复合材料提高12％，而裂纹扩展阻力R‘‘‘‘则提高5％，这是由于Y2O3的加入生成少量的YAC相，抑制了Al2O3晶粒长大，复合材料的强度和韧性以及热震时裂纹萌生和扩展的阻力得到提高，从而提高了复合材料的抗热震性。     

铁电-铁磁复合材料xLa5／8Ca3／8MnO3：（1-x）ErMnO3的电磁学性能

系统研究了xLa5／8Ca3／8MnO3：（1-x）ErMnO3（x=0、0．2、0．4、0．5、0．6、0．8、1）铁电铁磁复合材料的晶体结构和低温下的电磁输运性质．X光衍射结果表明金属铁磁相La5／8Ca3／8MnO3和绝缘铁电相ErMnO3由于晶体结构上的巨大差异几乎完全不相溶．电阻率随x的增大而降低,其导电特性可用经典的渗流理论来解释．当x〉xc时,样品电阻特性山La5／8Ca3／RMnO3主导,电阻温度曲线会出现金属绝缘体转变．磁性测试表明,由于La5／8Ca3／8MnO3的掺入,复合材料的磁性相比单相ErMnO3得到加强．从电磁性质综合分析认为这利复合材料是一种新的多铁性材料,相比单相多铁性材料ErMnO3,它具有更强的磁性和更广的使用温度范围．     

稀土改性Pd/Al2O3催化剂的性能:甲醇分解的活性和选择性

用稀土金属氧化物CeO2和La2O3改性γ-Al2O3担载Pd制备了一系列甲醇分解催化剂，并考察了Pd盐前驱体（氯盐或硝酸盐），稀土种类（镧或／和铈），经的含量（0％－30％），浸渍方法（顺序浸渍或共浸渍）地催化剂性能的影响。结果表明：CeO2能提高Pd/Al2O3催化剂的甲醇分解活性，La2O3能提高催化剂的CO和H2选择性，而CeO2和La2O3在γ-Al2O3上对Pd的催化性能表现出一种协同作用。在10％的La2O3和22％的CeO2共同改性的催化剂上，250℃，甲醇液体空速1.8h^-1条件下反应甲醇转化率达到91．4％，CO（H2）的选择性几乎为100％。     

2-Formyl-3-Methoxymethylindole, 3-Ethoxymethyl-2-Formylindole and 2-Formyl-3-Methylindole

Base-catalysed hydrolysis of 2-formyl-3-methyl-1-phenyl-sulphonylindole results in the formation of 3-alkoxy-methyl-2-formylindoles. Cleavage of the 1-phenyl-sulphonyl group with sodium amalgam produces 2-hydroxymethyl-3-methylindole.     

Reciprocal system 3Tl2S + Bi2Se3 ↔ 3Tl2Se + Bi2S3

The reciprocal system 3Tl₂S + Bi₂Se₃ ? 3Tl₂Se + Bi₂S₃ has been investigated by DTA, X-ray powder diffraction analysis, and emf measurements. Some polythermal sections and the isothermal section at 500 K of the phase diagram and the projection of the liquidus surface of this system have been constructed, and the types and coordinates of the invariant and univariant equilibria have been determined. The existence of wide regions of quaternary solid solutions based on the binary compounds Tl₂S, Tl₂Se, Bi₂S₃, and Bi₂Se₃, and solid solutions between the temary compounds TlBiS₂ and TlBiSe₂ have been established.     

RbLi2Ga2(BO3)3

The structure of rubidium dilithium digallium tris­(borate), RbLi₂Ga₂(BO₃)₃, contains two‐dimensional sheets of open‐branched rings of GaO₄ tetrahedra and planar BO₃ triangles that are joined by LiO₄ tetrahedra to form a three‐dimensional framework. Ten‐coordinate Rb atoms lie on twofold axes and occupy channels within the framework that extend along the b axis.     

Kinetics of gas‐phase reactions of CH3OCH2CF3, CH3OCH3, CH3OCH2CH3, CH3CH2OCH2CH3, and CHF2CF2OCH2CF3 with NO3 radicals at 298 K

Rate constants for the gas‐phase reactions of CH₃OCH₂CF₃ (k₁), CH₃OCH₃ (k₂), CH₃OCH₂CH₃ (k₃), and CH₃CH₂OCH₂CH₃ (k₄) with NO₃ radicals were determined by means of a relative rate method at 298 K. NO₃ radicals were prepared by thermal decomposition of N₂O₅ in a 700–750 Torr N₂O₅/NO₂/NO₃/air gas mixture in a 1‐m³ temperature‐controlled chamber. The measured rate constants at 298 K were k₁ = (5.3 ± 0.9) × 10^?18, k₂ = (1.07 ± 0.10) × 10^?16, k₃ = (7.81 ± 0.36) × 10^?16, and k₄ = (2.80 ± 0.10) × 10^?15 cm³ molecule^?1 s^?1. Potential energy surfaces for the NO₃ radical reactions were computationally explored, and the rate constants of k₁–k₅ were calculated according to the transition state theory. The calculated values of rate constants k₁–k₄ were in reasonable agreement with the experimentally determined values. The calculated value of k₅ was compared with the estimate (k₅ < 5.3 × 10^?21 cm³ molecule^?1 s^?1) derived from the correlation between the rate constants for reactions with NO₃ radicals (k₁–k₄) and the corresponding rate constants for reactions with OH radicals. We estimated the tropospheric lifetimes of CH₃OCH₂CF₃ and CHF₂CF₂OCH₂CF₃ to be 240 and >2.4 × 10⁵ years, respectively, with respect to reaction with NO₃ radicals. The tropospheric lifetimes of these compounds are much shorter with respect to the OH reaction. © 2009 Wiley Periodicals, Inc. Int J Chem Kinet 41: 490–497, 2009     

Ga2O3-La2O3-Yb2O3-Er2O3(HO2O3)体系光谱性质的研究

根据稀土离子能级的特点,对Ga2O3-La2O3-Yb2O3-Er2O3(HO2O3)体系的光谱性质进行了探讨,发现它们有二类发光性质:Stokes发光和反Stokes发光,研究了发光强度和发射波长与掺杂离子的依赖关系,观察到由能量的共振转移引起的荧光浓度猝灭现象,并取得了最大发光强度时的掺杂离子浓度和一些规律性结果.     

PbCu3(OH)(NO3)(SeO3)3·1/2H2O und Pb2Cu3O2(NO3)2(SeO3)2: Synthese und Kristallstrukturuntersuchung

Crystals of PbCu₃(OH)(NO₃)(SeO₃)₃·1/2H₂O [a=7.761(3)Å,b=9.478(4)Å,c=9.514(4)Å, =66.94(2)°, =69.83(2)°, =81.83(2)°, space group P ,Z=2] and Pb₂Cu₃O₂(NO₃)₂(SeO₃)₂ [a=5.884(2)Å,b=12.186(3)Å,c=19.371(4)Å, space group Cmc2₁,Z=4] were synthesized under hydrothermal conditions. Their crystal structures were refined with three-dimensional X-ray data toR _w=0.033 resp. 0.055. In PbCu₃(OH)(NO₃)(SeO₃)₃·1/2H₂O the Cu atoms are [4+1] and [4+2] coordinated and via SeO₃ groups a three-dimensional atomic arrangement is built up. In Pb₂Cu₃O₂(NO₃)₂(SeO₃)₂ there are sheets, which are connected only via Pb-O bonds ranging from 2.98 Å to 3.16 Å.

     

Die Systeme Tl3SbS3-Tl3AsS3 und TlSbS2-TlAsS2

The influence of structural relationships between the components of (pseudo)binary systems with no intermediate compounds on the type of phase diagram was investigated. Structurally and chemically closely related Tl₃SbS₃ and Tl₃AsS₃ form a complete solid solution series whereas crystallographically different TlSbS₂ and TlAsS₂ constitute an eutectic type system.