镧锶锰氧的电磁性能与吸波特性

用溶胶-凝胶法制备了LaxSr1-xMnO3超微粉末.测量数据表明随着x值的增大,其磁导率的实部、虚部及损耗角正切的波峰均向低频端偏移,峰值增加;对x=0. 5样品的吸波特性研究表明其片状在 2. 2mm厚时吸波较好,峰高达 25dB;而对于柱状样品,当柱高 2. 2mm时,吸收峰高却达 34dB,这可能与电磁波在柱间的多次反射吸收有关。     

Fe69.5Cu1.5V7Si12B8Al2合金机械合金化研究

采用机械合金化的方法，制备了Fe69.5Cu1.5V7Si12B8Al2纳米合金样品。研究了球磨时间对样品非晶化程度的影响，并测量了这些样品压结体的高频特性。结果发现，球磨可形成合金化，随球磨时间的增加，样品的非晶化逐渐加强。当球磨超过一定时间后，出现新的相，引起样品磁特性的变化。复数磁导率实部μ1随球磨时间t的增加而增大，超过72h后，μ1开始下降。在4－13MHz范围内，μ1值随频率f的变化不大。损耗角正切tgδ随t的增加而减小。     

射频等离子体制备球形Ti—6Al—4V粉末性能表征

以不规则形状的Ti—6Al—4V(TC4)粉末为原料,通过射频等离子体球化处理制备了球形TC4粉末,并研究了球化处理对粉末特性及加料速率对粉末球化率的影响.利用扫描电子显微镜、激光粒度分析和霍尔流速计分别对其粉末微观结构、粒度分布和粉体性能进行了测试和分析.结果表明:TC4粉末经等离子球化处理后得到表面光滑、球形度好及球化率可达到100%的球形粉末;球化处理后,粉末的松装密度、振实密度和粉末流动性得到明显改善,粒度略微增大;随着加料速率的增加,TC4粉的球化率逐渐降低.     

罐形磁芯法测量软磁薄膜复数磁导率的研究

介绍了罐形磁芯法测量软磁薄膜材料磁导率的磁路结构原理,根据磁路磁通分布,给出了计算的等效磁路;推导了复数磁导率的计算表达式;利用罐形磁芯法在阻抗分析仪上测量了几种软磁薄膜样品的复数磁导率,并与冲击法的实验结果做了比较,获得了较为一致的结果。     

Fe1-xBx磁性纳米膜的制备和微波物性分析

为获得具有较高复磁导率虚部的磁性材料并研究其微波物性，采用磁控溅射方法，制备Fe1-xBx磁性纳米膜，以Landau-Lifshitz-Gibert方程研究复磁导率虚部随纳米膜各向异性场、饱和磁化强度和阻尼系数的变化规律，采用谐振腔法开展点频测试。结果表明，测试数据与理论计算值吻合较好。结合Fe1-xBx样品的制备，分析了其磁导率虚部随制备工艺、组分、厚度等的变化规律，这对于获得高磁导率（虚部）的磁性纳米膜具有指导意义。     

尖晶石铁氧体吸波材料的复数磁导率

为了设计高效和宽频的微波吸波体,本文研究了吸波体对吸波材料的要求。研究结果表明:要想设计得到高质量的吸波体,要求材料的复数磁导率(包括其实部和虚部)具有适当高的数值。本文还研究了Ni铁氧体系列。首先研究了Co对Ni的替代对复数磁导率的影响,其次,研究了烧结温度对复数磁导率的影响,结果表明:选择适当的Co含量和烧结温度,可以得到较高的磁导率。     

掺Ho纳米TiO2粉晶的结构及光学特性

采用溶胶一凝胶法制备了掺lat%Ho的纳米TiCl2粉末,并分别在400℃、600℃与800℃下对样品进行热处理,通过XRD和紫外可见吸收测试,对掺杂纳米TiO2粉末的晶体结构与光学性质进行了研究.分析发现掺杂提高了样品的相变温度,减小了样品的晶粒尺寸,使样品的吸收明显增强,光学带隙增加.而且随着热处理温度的升高,样品的晶粒尺寸增大,晶格常数a值减小,c值增大,吸收减小而光学带隙增大.     

氧化钐掺杂氧化铈纳米材料的导电性

利用溶胶-凝胶法制备了Sm2O3掺杂CeO2系列固体电解质.通过粉末X射线衍射谱对所制备的电解质材料进行了平均晶粒尺寸和晶格常数分析,并利用交流阻抗谱测试结果分析了样品的电导率机理.研究表明,粉末样品晶粒尺寸较小,属于纳米级材料,且具有立方萤石型结构.另外,随温度的升高,Sm2O3掺杂CeO2样品中的氧离子通过空位移动速度增大,而使其电导率也随之线性增大;Sm2O3掺杂CeO2样品随掺杂比例变化而导致空位变化,使其导电率也在一定程度上受到了影响.     

负磁导率材料的微波反射行为

采用波导法研究了开口谐振环(split resonator rings,SRRs)负磁导率材料X波段(8-12 GHz)的微波反射行为.通过电路板刻蚀技术制备了六边形SRRs为单元的二维及三维样品.实验表明:二维负磁导率材料样品反射率曲线形成反射峰,其峰值点对应频率与材料谐振频率一致,反射率变化达到10 dB,在谐振频率两侧较窄的区域反射微弱;三维样品反射率曲线形成反射峰,其峰值点位置与材料谐振频率一致,调节晶格常数时材料反射行为变化较大;负磁导率材料反射相位随频率增大,二维样品在谐振频率处反射相位存在一个拐点.     

旋转喷镀法制备GHz高磁导率NiZn铁氧体膜

用自研设备将加压的反应溶液Fe2 Cl2( Fe3 Cl3) NiCl2 ZnCl2和缓冲溶液CH3COONH4以一定流量同时喷镀在90℃转盘上的玻璃衬底上以单质氧为氧化剂生成了厚度1～2 μm的NiZn铁氧体薄膜.X射线衍射数据表明制备的NiZn铁氧体薄膜具有尖晶石结构.氧化液pH值等于8.8时制备的薄膜的组成是Ni0.25Zn0.09Fe2.66O4,有313 kA/m的大的饱和磁化强度和692.5 A/m的低的矫顽力.在0.1 GHz到3.5 GHz频率范围内用Agilent 8722ES矢量网络分析仪通过短路微带线微扰法测量了薄膜的复数磁导率.薄膜的复磁导率的实部μ'r在0.5 GHz为36.1,虚部μ"r在0.8 GHz达最大值55.5.磁导率虚部值在0.5～2 GHz频率范围大于20,制备的薄膜将可以应用于微波频段的电磁干扰抑制器.     

Fe_(78)Si_9B_(13)非晶磁粉芯工艺

研究了粉末制备方法、粉末粒度、绝缘剂添加量等因素对Fe78Si9B13非晶磁粉芯性能的影响.结果表明,气流磨法得到的粉末比机械法得到的粉末棱角少,多数粉末呈圆片状,利于绝缘包覆,因此,其粉芯磁性能比后者高;粉末粒度越大磁粉芯磁导率越高,但是损耗也越大,所以需要粒级调配,最终确定最佳配比为75~100μm占70%,61~75μm占10%,45~61μm占20%.添加绝缘剂可提高粉末的固有电阻,降低涡流损耗.但绝缘剂含量过大时会降低粉芯的磁导率,本实验确定最佳添加量为4%.     

冷却速率对高碳铬铁粉电磁性能的影响

采用矢量网络参数法在1~18 GНz频段内分别对电阻炉、空气和水浴中冷却的高碳铬铁粉的电磁性能进行研究.随着冷却速率的提高,高碳铬铁粉的相对复介电常数实部和虚部在大多数频率下均增大.空冷和水冷粉料的相对复介电常数虚部在12~18 GНz频率范围内因极化弛豫而产生较大的峰值.同一频率下相对复磁导率实部随冷却速率变化的趋势与相对复介电常数相反.水冷粉料的相对复磁导率虚部在3~5GНz以外的频段内均大于另两组冷却粉料,且三组粉料的虚部在低频及高频条件下均具有峰值.在2.45 GНz的微波加热频率下,炉冷、空冷及水冷粉料的反射损耗分别为-2.30、-2.15和-2.07 dB.水冷粉料的介电损耗因子及磁损耗因子最大,微波场下具有最佳的升温速率与反应效果.     

Bi1-xLaxFeO3多铁体系的微波吸收性能

采用溶胶-凝胶法制备Bi1-xLaxFeO3(x=0,0.05,0.10,0.15)粉晶样品,用X线衍射仪表征样品的晶体结构,用扫描电镜观察样品的颗粒形貌与尺寸,用微波矢量网络分析仪测试样品在2～18 GHz微波频率范围内的复介电常数、复磁导率,并计算损耗角正切及微波反射率.研究结果表明:Bi1-xLaxFeO3晶体结构为钙钛矿型,颗粒形貌为直径约200nm、长度约700nm的不规则短棒状;La的A位掺杂有利于提高体系的微波吸收性能;当样品厚度为2.6 mm,x=0.10时,吸收峰值为27.7 dB,小于-10 dB吸收带宽为3.4 GHz,该材料的电磁损耗来自介电损耗和磁损耗,但介电损耗较大.     

固液反应球磨制备Al-Cu-Co三元金属间化合物

利用固液反应球磨技术制备了Al-Cu-Co三元合金．分别采用Co球球磨Al-33．2％Cu(此文中的百分比为质量分数),Al-54％Cu(A12Cu)和Al-70％Cu(A1QJ)二元合金熔体,在923K和973K球磨Al-33．2％Cu熔体12h后生成Al65Co15Cu20粉末;在923K和1023K球磨24h后生成Al69Co25Cu6粉末,在893K和993K分别球磨Al-54％Cu(A12Cu)合金熔体12h和24h后均生成Al65Co15Cu2n粉末;在1123K球磨Al-70％Cu合金熔体24h后生成Al65Co15Cu20粉末．采用Al-Cu-Co固液反应球磨得到的金属间化合物粉末为纳米粒子．同时,对Al-Cu-Co三元合金相形成的规律进行了研究,对固液反应球磨机理进行了探讨．在固液反应球磨过程中,三元合金产物的元素摩尔比接近于二元母合金中的元素摩尔比;三元合金产物成分中固相第三组元的成分含量与二元母合金熔体成分有很大关系;提高反应球磨温度、延长球磨时间有利于三元合金产物的形成;延长球磨时间,形成的三元合金产物中磨球的成分增加;反应球磨温度超出二元母合金熔点越高,球磨反应越容易进行．     

钴铁氧体的溶胶凝胶燃烧法制备及其物性检测

通过溶胶凝胶燃烧法制备了钴铁氧体（CoFe₂O₄）纳米颗粒,并通过压片退火成型.XRD图谱显示样品成分无杂相.通过介电测试仪和振动样品磁强计测试了样品在室温下的介电性能和磁性能.试验结果表明,其介电常数和损耗都随着频率的变化而变化并展现出频散的行为,在低频范围内随着频率的增加而急剧减小,在高频范围内减小不明显.此外,其磁滞回线显示该类材料的饱和磁化强度、剩余磁化强度和矫顽力场分别为81.8 emu·g^-1,29.4 emu·g^-1和834.9 Oe.样品展现出良好的磁性能.     

Spheroidization of silica powders by radio frequency inductively coupled plasma with Ar-H2 and Ar-N2 as the sheath gases at atmospheric pressure

Amorphous spherical silica powders were prepared by inductively coupled thermal plasma treatment at a radio frequency of 36.2 MHz.The effects of the added content of hydrogen and nitrogen into argon (serving as the sheath gas),as well as the carrier gas flow rate,on the spheroidization rate of silica powders,were investigated.The prepared silica powders before and after plasma treatment were examined by scanning electron microscopy,X-ray diffraction,and laser granulometric analysis.Results indicated that the average size of the silica particles increased,and the transformation of crystals into the amorphous state occurred after plasma treatment.Discharge image processing was employed to analyze the effect of the plasma temperature field on the spheroidization rate.The spheroidization rate of the silica powder increased with the increase of the hydrogen content in the sheath gas.On the other hand,the spheroidization rate of the silica power first increased and then decreased with the increase of the nitrogen content in the sheath gas.Moreover,the amorphous content increased with the increase of the spheroidization rate of the silica powder.     

Spheroidization of silica powders by radio frequency inductively coupled plasma with Ar-H2 and Ar-N2 as the sheath gases at atmospheric pressu

Amorphous spherical silica powders were prepared by inductively coupled thermal plasma treatment at a radio frequency of 36.2 MHz. The effects of the added content of hydrogen and nitrogen into argon (serving as the sheath gas), as well as the carrier gas flow rate, on the spheroidization rate of silica powders, were investigated. The prepared silica powders before and after plasma treatment were examined by scanning electron microscopy, X-ray diffraction, and laser granulometric analysis. Results indicated that the average size of the silica particles increased, and the transformation of crystals into the amorphous state occurred after plasma treatment. Discharge image processing was employed to analyze the effect of the plasma temperature field on the spheroidization rate. The spheroidization rate of the silica powder increased with the increase of the hydrogen content in the sheath gas. On the other hand, the spheroidization rate of the silica power first increased and then decreased with the increase of the nitrogen content in the sheath gas. Moreover, the amorphous content increased with the increase of the spheroidization rate of the silica powder.     

Spheroidization of silica powders by radio frequency inductively coupled plasma with Ar–H_2 and Ar–N_2 as the sheath gases at atmospheric pressure

Amorphous spherical silica powders were prepared by inductively coupled thermal plasma treatment at a radio frequency of 36.2 MHz. The effects of the added content of hydrogen and nitrogen into argon(serving as the sheath gas), as well as the carrier gas flow rate, on the spheroidization rate of silica powders, were investigated. The prepared silica powders before and after plasma treatment were examined by scanning electron microscopy, X-ray diffraction, and laser granulometric analysis. Results indicated that the average size of the silica particles increased, and the transformation of crystals into the amorphous state occurred after plasma treatment. Discharge image processing was employed to analyze the effect of the plasma temperature field on the spheroidization rate. The spheroidization rate of the silica powder increased with the increase of the hydrogen content in the sheath gas. On the other hand, the spheroidization rate of the silica power first increased and then decreased with the increase of the nitrogen content in the sheath gas. Moreover, the amorphous content increased with the increase of the spheroidization rate of the silica powder.     

双稀土掺杂BCST陶瓷的研制及其性能结构的研究

采用溶胶—凝胶法合成了BCST（Ba0.62 Ca0.08 Sr0.3 TiO3）粉体,再经过二次固相掺杂稀土Pr6O11和Nd2O3获得BCST∶0.001Pr6 O11.xNd2 O3系列纳米粉体及陶瓷;采用XRD和SEM,等对粉体的相组成和陶瓷的微观形貌进行了表征,并用介电频谱仪测试了陶瓷的介电性能.结果表明：所得BCST∶0.001Pr6O11.0.002Nd2O3粉体主要为四方相纳米粉体;随着稀土Nd2O3掺杂量的增加,所获得的陶瓷的晶粒先逐渐变小随后又逐渐增大;当钕的掺杂量x=0.002时,所获得陶瓷的室温介电常数最高,而介电损失最小;各试样的介电常数随烧结温度的升高增大,在1 330℃,1 360℃和1 400℃温度下烧结所获得的S1-陶瓷,介电常数的峰值εmax分别为10 360、12 490、13 750;其居里温度显著降低（10℃）,介温曲线呈单峰,介电常数随温度的变化敏感而对称,有望在温度敏感陶瓷方面发现其应用.