Fe_(78)Si_9B_(13)/Ni层状复合材料的制备及其拉伸性能

采用脉冲电沉积的方法制备了Fe78Si9B13/Ni层状复合材料(Ni-Fe78Si9B13-Ni三层结构)。用SEM和TEM对层状复合的微观组织进行观察,Ni层的晶粒尺寸平均约为50 nm,非晶层和纳米Ni层具有良好的界面结合。Fe78Si9B13/Ni层状复合材料的室温断裂强度达到2090 MPa,断裂伸长率达到8.5%,其伸长率远大于单相Fe78Si9B13非晶带的伸长率(1.39%);在450℃高温拉伸,复合材料的延伸率达到了115.5%,远大于单相非晶带的高温延伸率(36.3%),实现了通过制备层状复合材料来提高非晶带塑性的目的。     

Ni-Fe-(Nb)-Si-B非晶合金的等温晶化与结构转变

采用旋铸急冷工艺在大气环境中制备出(Ni0.75Fe0.25)78-xNbxSi10B12(x=0,5)非晶合金带材.X射线衍射(XRD)分析表明样品为完全非晶态.用差热分析仪(DTA)在高纯氩气保护下测量了非晶薄带的Tg、Tx、Tm,并分析了其热稳定性.根据DTA结果分析表明,(Ni0.75Fe0.25)78Si10B12非晶合金退火温度为695,715,745和765K,在715和745K退火时,非晶基体上析出了单一的γ-(Fe, Ni)固溶体,平均晶粒尺寸分别约为10.3和18.5nm;765K退火后的结晶相为γ-(Fe, Ni)固溶体,Fe2Si,Ni2Si和Fe3B.(Ni0.75Fe0.25)73Nb5Si10B12非晶合金的退火温度为720,750和800K,退火后不能在非晶基体上析出单一的晶化相,晶化析出相为γ-(Fe, Ni)固溶体,(Fe, Ni)23B6,Ni31Si12和Nb2NiB0.16.     

非晶Fe_(78)Si_9B_(13)合金涂层及涂层对磁性能的影响

研究了非晶Fe78Si9B13合金涂层工艺及涂层对非晶Fe78Si9B13合金磁性能的影响。结果表明:使用适当的涂层工艺涂层后的非晶Fe78Si9B13合金带材涂层厚度均匀,显示出良好的耐电压性;X射线衍射实验结果表明,纵向磁场热处理后,涂层及未涂层的Fe-Si-B合金衍射花样特征基本相同;与未涂层的非晶Fe78Si9B13合金相比,经涂层的Fe78Si9B13非晶合金静态磁性能有所下降,但经涂层处理后的非晶合金有效的降低了其在高频下的铁损,对于高频率工作条件下的非晶合金器件,具有一定的应用价值。     

薄带宽度对(Fe_(0.9)Co_(0.1))_(76.9)Cu_(0.6)Nb_(2.5)Si_(11)B_9非晶合金阻抗效应的影响

研究了薄带宽度对(Fe0.9Co0.1)76.9Cu0.6Nb2.5Si11B9非晶合金薄带阻抗效应的影响。样品长度为40mm,宽度分别为8和4.4mm。淬态下4.4mm宽的样品在f=3.75MHz的条件下达到最大值28%,而8mm宽的样品在f=4.34MHz的条件下达到最大值17%;各频率下4.4mm宽的样品的阻抗效应均8mm宽的样品。(Fe0.9Co0.1)76.9Cu0.6Nb2.5Si11B9非晶合金薄带阻抗效应远大于Co68Fe5Si12B15非晶合金阻抗效应。     

连续压应力下Fe基非晶合金带材的压磁效应

通过对Fe基非晶合金带材连续施加压力,测试其附近闭合回路电感变化,研究了Fe基非晶合金带材的电感式压磁效应。结果表明,通过测试Fe基非晶合金带材附近闭合回路电感变化可用来测试和表征Fe基非晶合金带材的压磁性能;在f=1kHz时,Fe基非晶合金带材压磁性能稳定性好,随着压力的增大带材压磁性能升高,在同一压力情况下,Fe73.5Cu1Nb3Si13.5B9带材压磁性能优于Fe78Si9B13带材;在f=100kHz时,Fe73.5Cu1Nb3Si13.5B9带材压磁性能稳定性优于Fe78Si9B13带材,并且Fe73.5Cu1Nb3-Si13.5B9带材在f=1kHz、压应力为0.69MPa时具有最佳的压磁性能;在压应力<0.1MPa条件下,随着压应力增大,线圈电感值Ls有一个剧增的上升趋势,铁基非晶带材压磁性能对微小应力更加敏感。     

FeCuNbSiBV非晶纳米晶合金带材压磁特性研究

研究了Fe71.5Cu1Nb3Si13.5B9V2非晶带材经不同退火工艺处理后的压磁特性,并对不同成分带材的压磁特性进行了对比分析。研究表明,在测试频率f=1 kHz、压应力σ≤0.2 MPa条件下,Fe71.5Cu1Nb3Si13.5B9V2非晶带材闭合回路的电感值随压应力的增大而增大,带材具有良好的压磁稳定性,当退火温度为550℃时,带材的压磁特性稳定性最好,电感值与加载时间、SI(%)与压应力均具有良好的线性关系;热处理工艺对Fe71.5Cu1Nb3Si13.5B9V2带材的压磁性能具有显著影响,退火工艺为300℃×30 min时SI(%)达到最大值0.183;带材的压磁效应与其成分有关,相同测试条件下,Fe73.5Cu1Nb3Si13.5B9带材具有最大的压磁效应,Fe78Si9B13带材次之,Fe71.5Cu1Nb3Si13.5B9V2带材压磁效应最小。     

高Fe含量FeCuNbSiB系非晶/纳米晶合金制备及其磁性研究

研究了过渡金属元素(Zr,Nb,Mo)和Cu元素对Fe78Si9B13合金系非晶形成能力、热稳定性和磁性的影响;在Fe74Cu1Nb3Si13B9合金的基础上,通过逐步提高Fe含量,利用单辊甩带法制备Fe(76+x)Cu1Nb3Si(11-x)B9(x=0,2,4)和Fe(79+x)Cu1Nb2Si(6-x)B12(x=0,2,4)非晶/纳米晶合金薄带;利用XRD、DSC、TEM和VSM研究了高Fe含量Fe-Cu-Nb-Si-B系非晶/纳米晶合金的微观结构和磁性,并通过添加Nb元素优化了高Fe含量合金的磁性。研究结果表明:Zr和Nb元素的添加能明显提高Fe78Si9B13合金的非晶形成能力和热稳定性;高Fe含量的Fe-Cu-Nb-Si-B系纳米晶合金为典型的非晶/纳米晶双相结构,合金的饱和磁化强度Ms180 emu/g,且合金的矫顽力Hc在2Oe-9Oe之间,具有良好的软磁性能;Nb元素能显著细化Fe-Cu-Nb-Si-B系合金晶粒尺寸,从而能显著降低合金的矫顽力,改善合金的软磁性能;当Fe含量在80%-83%(原子百分比,下同)之间时,合金具有良好的软磁性能,但当Fe含量达到85%时,会有Fe2B、Fe3B相析出,从而显著恶化其软磁性能。     

Fe78Si13B9/铁氧体复合材料磁粉芯制备及其软磁性能

用Mn-Zn铁氧体溶胶对非晶Fe78Si13B9粉体包覆,模压成型制备了复合磁粉芯,并研究了复合材料磁粉芯的软磁性能.实验结果表明,铁氧体粉体在500℃×2h的热处理条件下逐渐生成,并在非晶Fe78Si13B9颗粒表面较好包覆;铁氧体溶胶的加入,大大提高了非晶Fe78Si13B9磁粉芯的品质因数Q值.当铁氧体溶胶量为7%、30℃的测试温度时,Fe78Si13B9/铁氧体复合材料磁粉芯的磁导率在1MHz时达到最大值32,Q值高达23.     

B对Pb-Mg-Al-B屏蔽功能材料的显微组织与屏蔽性能的影响

利用立式高频感应炉制备出铸造Pb-Mg-Al-B屏蔽材料,并对其显微组织和屏蔽性能进行了研究。结果表明,随着B的添加,材料组织中AlB2颗粒增多;室温抗拉强度可达105MPa,布氏硬度为160;厚度为20mm、B含量为2.0%(质量分数)的Pb-Mg-Al-B屏蔽材料对能量为250、118和65keV的X射线屏蔽率分别为90.29%、99.22%和97.9%,对γ射线的屏蔽率达到49.75%(137Cs源)和34.21%(60Co源),对中子的屏蔽率高达92.7%,说明屏蔽材料具有强度高、X(γ)射线与中子屏蔽性能优异,具备结构-功能(屏蔽)一体化的特点。     

非晶Fe_(78)Si_9B_(13)合金磁致低温纳米晶化的超精细结构研究

用低频脉冲磁场处理了非晶Fe78Si9B13合金,以红外非接触测温仪测量处理过程的温升,用Mssbauer谱、XRD和TEM等手段观察样品的超精细结构变化。结果表明,脉冲磁场处理过程中,非晶Fe78Si9B13合金发生了低温纳米晶化,试样温升均7℃,晶化析出相仅为α-Fe(Si),晶粒尺寸约为10nm,析出量为2.428%～6.992%,所形成的非晶-纳米晶双相合金的平均超精细磁场较原始非晶发生了明显变化,其单峰向低位场移动,在高位场又有出现另一单峰的迹象,脉冲处理参数不同,各峰出现的位置不同。     

La0.5Y0.5Ni4.8Mn0.1Al0.1和La0.5Y0.5Ni4.8Al0.2合金的储氢性能研究

针对两种新型稀土型储氢合金La0.5Y0.5Ni4.8Mn0.1Al0.1和La0.5Y0.5Ni4.8Al0.2的储氢特性进行研究分析。实验表明,相同温度下,La0.5Y0.5Ni4.8Mn0.1Al0.1和La0.5Y0.5Ni4.8Al0.2合金的PCT曲线基本重合,且都具有优良的吸氢动力学性能;相比之下,后者的滞后系数要小于前者,吸氢量较大,吸氢速率也较快,故其储氢性能较优。300次吸放氢循环实验结果表明,La0.5Y0.5Ni4.8Al0.2合金的吸氢动力学性能虽然略有下降,但抗粉化性能较好。     

Dy0.6Tb0.3Pr0.1(Fe0.95Mn0.05)x取向晶体的结构与磁致伸缩

采用Ｃｚｏｃｈｒａｌｓｋｉ方法生长了Ｄｙ０．６Ｔｂ０．３Ｐｒ０．１（Ｆｅ０．９５Ｍｎ０．０５）ｘ（１．８５≤ｘ≤１．９５）取向合金。所有合金主相为立方Ｌａｖｅｓ相结构,择优取向不完整择优取向的方向与Ｘ的大小有关。研究了沿着这些样品的生长方向的磁致伸缩性能以及磁致伸缩性能与压力之间的关系。     

Thermal Stability of Amorphous Hydride Mg_(50)Ni_(50)H_(54) and Mg_(30)Ni_(70)H_(45)

The thermal stability of amorphous ternary hydrides Mg_(50)Ni_(50)H_(54) and Mg_(30)Ni_(70)H_(45) and their corre-sponding amorphous binary alloys Mg_(50)Ni_(50) and Mg_(30)Ni_(70) were studied with X-ray diffraction(XRD) and differential scanning calorimetry(DSC). Samples of the amorphous alloys were preparedby mechanical alloying and the amorphous hydrides were obtained by charging the alloys with gas-eous hydrogen at 3.0 MPa and 423 K. It was found that the amorphous hydrides released most oftheir hydrogen before the crystallization of the essentially hydrogen depleted amorphous alloy. Thecrystallization temperature of amorphous Mg_(50)Ni_(50)H_(54) elevated and that of amorphousMg_(30)Ni_(70)H_(45) did not change in relation to the original binary amorphous alloy. This is very excep-tional for amorphous hydrides. The reason for the effects of hydrogen absorption/desorption on thecrystallization of amorphous alloys was discussed.     

Plasma surface treatments of poly(l-lactic acid) (PLLA) and poly(hydroxybutyrate-co-hydroxyvalerate) (PHBV)

The surfaces of poly(l-lactic acid) (PLLA) and poly(hydroxybutyrate-co-hydroxyvalerate) (PHBV) were modified by oxygen and nitrogen plasma treatments. The physical and chemical surface characteristics were evaluated by contact angle tests, scanning electron microscopy (SEM), atomic force microscopy (AFM), and X-ray photoelectron spectroscopy (XPS). The plasma treatments caused an increase in both contact angle and roughening, altered the surface morphology, inserted polar groups, and, consequently, enhanced the hydrophilicity for both PLLA and PHBV polymers.     

Nanomechanical characterization of one-step combustion-synthesized Al(4)B(2)O(9) and Al(18)B(4)O(33) nanowires

Two kinds of aluminum borate nanowires, Al(4)B(2)O(9) and Al(18)B(4)O(33), were successfully synthesized by a one-step combustion method through control of the Al:B atomic ratio and synthesis temperature. Both nanowires are single crystalline but have distinguishing growth habits. Nanoindentation tests were performed directly on individual nanowires to reveal their mechanical properties. A 70% reduction in elastic modulus was found in Al(18)B(4)O(33) nanowires compared with their bulk counterpart. Al(18)B(4)O(33) nanowires exhibited higher hardness and elastic modulus than Al(4)B(2)O(9) nanowires.     

Natural Passivity of Amorphous Fe_(40)Ni_(40)P_(14)B_6 and Fe_(54.6)Ni_(38)Si_(4.1)B_(2.3)V_1 Alloys

The natural passive films forrned on Fe_(40)Ni_(40)P_(14)B_6 and Fe_(54.6)Ni_(38)Si_(4.1)B_(2.3)V_1 amorphous alloys long-term exposed in air have been studied by X-ray photoelectron spectroscopy (XPS) and Auger electron (including Ar+ ion depth profiling) spectroscopy (AES). The following aspects have been investigated: (1) chemical states of the elements in the films. binding energies and the chemical shifts measured by XPSf (2) structure and composition of the films fand (3) thickness of the passive films determined by AES depth profiling and XPS analysis.     

非晶态半导体 As_(24)Se_(76)、As_(40)Se_(60)和 As_(50)Se_(50)的光量子效率研究

光量子效率是非晶态光电导材料的一个重要参数。本文利用静电放电的方法,探讨和研究了 As—Se 系统非晶态半导体材料的光量子效率与电场和组份的关系,得出的结果与 Onsager 理论描述的相一致。由分析而得到了等剂量组份、富 As 和富 Se 系统光量子效率的变化趋势。     

An SANS Study of Decomposition Kinetics in Amorphous Cu_(12.5)Ni_(10)Zr_(41)Ti_(14)Be_(22.5)

Phase decomposition in amorphous Cu12.5Ni10Zr411Ti14Be22.5 alloy as annealed in the super-cooled liquid range was studied by applying small angle neutron scattering (SANS). As annealed between 600 K and 700 K, the alloy was observed to decompose into two new amorphous phases,with the second phase precipitates embedded in the matrix of the first. Long time annealing of the alloy results in crystallization in addition to evolution of the decomposed microstructure.The kinetic diagram of the decomposition and crystallization for this alloy is given. The second phase precipitates have several nanometers in size and occupy a quite low volume fraction. The decomposition of the supercooled liquid in overall temperature range exhibits the features of spinodal reaction.     

Work Functions of Pd_(83.5)Si_(16.5)and Cu_(70)Ti_(30)Glassy Alloys

The work functions before and aftercrystallization of two glassy alloys,Pd_(83.5)Si_(16.5) andCu_(70)Ti_(30) have been measured by means of the con-tact potential difference method in the secondaryelectron field at room temperature under 10~(-5) Pavacuum.The results show that the work functionsof both glassy alloys are higher than those of thecorresponding crystalline alloys.