Chemical States of Lanthanum in Carbonized La2O3-Mo Thermionic Cathode Materials

The chemical reaction between lanthanum oxide and molybdenum carbide was studied by thermodynamic calcu-lation, thermal analysis and in-situ X-ray Photoelectron Spectroscopy. The theoretical results show that at the environment allowing for the evaporation of lanthanum, such as in high vacuum, La2O3 in the La2O3-Mo materials can be reduced to metallic lanthanum by molybdenum carbide (Mo2C). To confirm the conclusion, many analysis methods such as XRD, SPS, and TG-DTA were taken. The experimental results show that the chemical state of lanthanum changes during heat-ing. It was proved, for the first time, that reacted metallic lanthanum appears at the surface of this kind of material at high temperature.     

放电等离子烧结工艺对Ca3Co4O9陶瓷织构及电性能的影响

采用溶胶-凝胶与放电等离子烧结(SPS)相结合的方法制备了Ca3Co4O9陶瓷.通过X射线衍射、扫描电镜等表征手段,研究了放电等离子烧结工艺对Ca3Co4O9物相、显微结构和性能的影响.实验结果表明片状颗粒和放电等离子烧结工艺,特别是烧结温度的提高有利于Ca3Co4O9织构的形成.初步认为是片状颗粒在脉冲电流所产生的脉冲磁场作用下发生重排,使颗粒定向排列.本实验范围内,当烧结温度从700℃提高到900℃时,Ca3Co4O9晶粒取向度从0.75增大到0.87,700℃下的电阻率从6.24×10-5 Ωm降低到5.59×10-5 Ωm.此外,Ca3Co4O9块体表现出典型的半导体电学特征,电导率随着SPS烧结温度和测量温度的升高而增大,当SPS烧结温度为850℃时,P型Ca3Co4O9化合物在700℃有最大电导率.     

放电等离子烧结Fe3B／（Pr,Tb）2Fe14B块体纳米晶双相复合永磁体的性能

采用放电等离子烧结技术将非晶Pr4.2Tb0.3Fe78B17.5薄带制备成块状纳米晶复合磁体。研究了烧结条件对磁体密度、微观结构和磁性能的影响。结果表明，烧结温度的升高可使磁体得到高致密度，但同时由于其晶粒长大，结果导致磁性能的恶化。在最佳烧结条件下得到磁体的磁性能为Br=1．02T，JHc=220kA／m。磁体具有较好的微观结构，平均晶粒尺寸为20nm。     

富钕相对烧结NdFeB磁体耐腐蚀性的影响

研究了Nd2Fe14B单晶、传统烧结NdFeB磁体和放电等离子烧结（简称SPS）NdFeB磁体在电解液溶液中的电化学特性。采用扫描电子显微镜和电子能谱分析了磁体的微观组织成分。结果表明在3．5％NaCI溶液的极化曲线中，Nd2Fe14B单晶具有最高的电化学腐蚀电位，放电等离子烧结NdFeB磁体的腐蚀电位高于传统烧结NdFeB磁体。与传统烧结NdFeB磁体相比，放电等离子烧结NdFeB磁体富Nd相具有独特的分布形态，主相Nd2Fe14B晶粒细小、均匀，富钕相在主相晶粒边界上分布较少，主要集中在三角晶界处。这种组织结构有效地抑制了磁体沿富钕相发生晶间腐蚀的过程，磁体因此具有良好的耐腐蚀性能。此外，从不同稀土含量的烧结NdFeB磁体的高压加速实验中可以看出磁体的腐蚀速度随稀土含量的增加而增大。以上结果表明富Nd相的化学特性及其分布状态和含量是决定合金耐蚀性能的关键，它在合金中以网络状分布在主相晶粒边界上，并决定了烧结NdFeB易于发生选择性晶间腐蚀，从而导致耐蚀性差。     

钪系阴极基体的研究

采用氧化钪与钨机械混合、氧化钨与钪盐水溶液固液掺杂法制备了氧化钪-钨基体，采用扫描电镜及原位俄歇电子能谱方法研究了基体中钪的分布及阴极基体的抗离子轰击性能。结果表明，采用液固法制备的烧结体，氧化钪分布均匀，这样的结构有利于钪的扩散和补充，原位俄歇轰击实验结果表明，阴极基体具有良好的耐高温和耐离子轰击性。     

Heat treatment process of new NdFeB magnet prepared by spark plasma sintering

1　INTRODUCTIONTraditionallysinteredNdFeBmagnetcanmeettherequirementofdimensional precisionthroughpost machining ,whichusuallyresultsin 4 5 %ofma terialloss.Post machiningnotonlywastestherareearthresources ,butalsoincreasesthe productioncost .Moreover ,itisdifficulttopreparehomogeneousworkpieceswithlargedimensionandcomplicatedshapeduetosomeuncontrollablefactorsinthecon ventionalsintering process .Ontheotherhand ,al thoughthebondedNdFeBmagnethasbetterforma bilityanddimensionalprecision ,…     

稀土Nd超细纳米晶块体的制备及其物理性能

利用放电等离子烧结技术,制备了稀土金属Nd非晶、非晶与纳米晶双相结构和超细纳米晶的块体材料.利用高分辨透射电镜表征了制备材料的显微结构.通过热力学分析,得出Nd超细纳米晶块体材料由hcp相向bcc相转变的温度约为650℃,相对于传统的粗晶材料降低了约200℃.对传统粗晶和超细纳米晶的Nd块体材料分别测定了电阻率、热导率和热膨胀系数及其随温度的变化规律,表明超细纳米晶Nd的电阻率较传统粗晶结构明显升高,而热导率则降低约3倍.     

叠层加压SPS烧结制备梯度硬质合金

采用叠层加压SPS烧结法制备致密的YG10/YG20梯度结构硬质合金。通过调整WC粒度和添加微量元素B来调整烧结温度,使含钴量低的粉末与含钴量高的粉末的烧结温度相近。研究了烧结温度对致密度、组织形貌、显微硬度和断裂韧性的影响,分析了沿梯度截面上C,Co,W等成分、显微硬度的变化及YG10/YG20界面的结合情况。结果表明:原始WC粒度为1μm的YG10+0.05%B混合粉末和9μm的YG20混合粉末都能在1100℃~1160℃烧结致密,相对密度达到99%以上,晶粒尺寸均匀,梯度界面结合良好,没有开裂现象。低钴端的硬度达到了15500MPa~16000MPa,高钴端的硬度为11100MPa;在294N载荷的作用下低钴端的断裂韧性为12.62MPa·m1/2,而高钴端在这一载荷的作用下没有出现裂纹,断裂韧性较高,从而实现了硬质合金一端具有高硬度,另一端具有良好的韧性的有机结合。     

复合稀土氧化物-钼-铼金属陶瓷阴极的次级发射性能

研究了复合稀土氧化物-钼-铼金属陶瓷阴极的二次电子发射系数和抗暴露大气性能,对发射后的表面进行了表面分析,并与单元、复合稀土-钼金属陶瓷阴极进行了对比.研究结果表明:加入微量铼的复合稀土氧化物-钼金属陶瓷阴极的二次电子发射系数可提高8%,其最大次级发射系数δm为2.65,且具有较好的抗暴露大气性能.     

La2O3-Gd2O3-Mo secondary emission material

A new kind of materials La2O3-Gd2O3-Mo has been produced by powder metallurgy method.The composition and microstructure of the material were studied by XRD and SEM.It shows that no chemical reaction takes place among La2O3,Gd2O3,Mo and the rare earth oxides exist along molybdenum grain boundaries and in the pores.The emission property measurement results of this material show that adding rare earth oxide into molybdenum can improve the secondary emission coefficient of the emitter,and the emission property depends on the activation temperature.After La2O3-Gd2O3-Mo was activated at 1360℃,the maximum secondary emission coefficient can be high to 2.62,which has exceeded that for practical uses(2.0).