静电纺丝法制备PAN/Fe3O4磁性纳米纤维

采用化学共沉淀法制备纳米四氧化三铁,选用曲拉通X-100为分散剂,利用静电纺丝法制备PAN/Fe3O4磁性纳米复合材料。X射线衍射仪(XRD)验证了四氧化三铁在复合纳米纤维中的存在。同时使用扫描电镜(SEM)和透射电镜(TEM)对复合纳米纤维的微观形貌和Fe3O4在纤维中的分布进行了观察,利用热重(TGA)对纳米复合材料的热稳定性进行分析;通过磁性实验分析了纳米复合材料的磁性性能。结果表明,所制备PAN/Fe3O4磁性纳米纤维成型良好,且Fe3O4磁性颗粒在纤维中分散均匀,其与PAN是物理复合。纳米复合材料具有一定磁性,并可由磁性颗粒的加入量进行控制。     

复合纳米纤维静电纺丝法的制备及其磁性

以聚乙烯吡咯烷酮（PVP）和金属盐为原料,利用静电纺丝法成功制备出了摩尔比为1：1的SrTiO3-SrFe12O19磁电复合纳米纤维。并通过FT-IR,XRD,SEM和VSM等技术对纤维前驱体及其产物的结构、热处理产物的物相、形貌及磁性能进行了表征。结果表明,样品经900℃焙烧2h后,即可得到纯的SrTiO3和SrFe...     

M型锶铁氧体纳米纤维静电纺丝和磁性能

以聚乙烯吡咯烷酮(Polyvinylpylrrolidone,PVP)和金属盐为原料,采用静电纺丝法制备了SrFe12O19/PVP复合纤维前驱体,前驱体经焙烧后得到M型锶铁氧体纳米纤维.通过FTIR、TG/DSC、XRD、SEM和VSM技术对复合纤维前驱体及所制备的M型锶铁氧体纳米纤维进行了表征.结果表明,复合纤维前驱体的直径与溶液中金属盐浓度有关,随盐浓度的升高纤维直径增大;经800℃焙烧2h后,得到纯相M型锶铁氧体纳米纤维,直径在100～150nm,组成纤维的平均晶粒大小约为49nm,且随焙烧温度的升高,晶粒长大;经1000℃焙烧2h后得到的锶铁氧体纤维的磁性能最佳,此时纤维平均直径约为100nm,晶粒尺寸约为61nm,室温下测得的饱和磁化强度为68.5A.m2/kg,矫顽力为503kA/m.     

静电纺丝法制备Sr1-xLaxFe12-xCoxO19纳米纤维及其磁性研究

采用溶胶?凝胶过程和静电纺丝技术相结合的方法,制得了PVP/Sr1-xLaxFe12-xCoxO19(x=0～0.5)复合纳米纤维,经过煅烧处理过程,获得了Sr1-xLaxFe12-xCoxO19(x=0～0.5)纳米纤维.通过SEM、TEM、XRD和VSM等技术对样品的形貌、物相、结构以及磁性能进行了表征.结果表明,800℃煅烧后的Sr1-xLaxFe12-xCoxO19(x=0.5)纳米纤维的直径主要分布在80～150 nm;这些纤维在室温下都具有硬磁特性,化学组成对铁氧体的磁性能有着显著的影响,当x≥0.3时,样品中同时出现M型的SrFe12O19、LaFeO3和CoFe2O4;在适当范围内(x≤0.1),La3+-Co2+的掺杂有利于改善锶铁氧体纤维的永磁性能,相应的矫顽力、饱和磁化强度和剩余磁化强度分别为Hc=432.02kA/m,Ms=54.7A.m2/kg,Mr=28.9A.m2/kg,与传统溶胶?凝胶法在相同条件下制得的Sr0.9La0.1Fe11.9Co0.1O19粉体样品相比,磁性能也有显著提高.     

静电纺丝法制备磁性纳米纤维材料的研究进展

磁性纳米纤维材料不但具有普通纳米粒子的特殊效应,而且具有独特的形状各向异性和磁晶各向异性效应,在高密度磁记录、电磁波吸收、催化剂、医学和生物功能材料等领域具有重要应用。静电纺丝技术已被证明是一种制备纳米纤维最简单有效的方法。结合最新文献,重点阐述了以静电纺丝技术为主的磁性纳米纤维制备工艺以及不同工艺对磁性纳米纤维的形貌和性能的影响。简要介绍了磁性纳米纤维的应用,指出了发展新型结构可控磁性纳米纤维材料、研究其定向排布及组装技术、开发其在各领域的实际应用是未来主要的研究方向。     

静电纺丝制备磁性碳纳米复合纤维及其表征

以聚丙烯腈(PAN)、乙酰丙酮铁(AAI)、N, N-二甲基甲酰胺(DMF)为原料, 采用静电纺丝-煅烧技术成功制备出磁性碳纳米复合纤维。通过TEM分析发现CF900的直径约为130~210 nm, 磁性纳米颗粒均匀地分散在碳纳米纤维中, 并探讨了碳化温度对碳纳米复合纤维磁性能的影响。结果显示: 饱和磁化强度(M_s)和剩余磁化强度(M_r)均随温度的升高而增大, 样品CF900的饱和磁化强度(M_s)高达27.55 A·m²/kg, 比表面积(S_BET)和总孔容积(V_total)达354.0 m²/g和0.315 mL/g。     

静电纺丝法制备Fe3+/TiO2纳米纤维及表征

以聚乙烯吡咯烷酮(PVP)为纤维模板,钛酸四丁酯(Ti[O(CH2)3CH3]4)和Fe3+为前驱体,乙醇为溶剂,醋酸为催化剂,采用静电纺丝法制备不同含铁量的复合纳米纤维Fe3+/TiO2,经500℃煅烧得到以锐钛矿为主的Fe3+/TiO2纳米纤维。采用扫描电子显微镜(SEM)和X射线衍射仪(XRD)分别表征了Fe3+/TiO2纳米纤维的形貌与晶态,计算了样品的晶粒尺寸和锐钛矿所占的比例,并比较了5%Fe3+/TiO2纳米纤维、5%Fe3+/TiO2粉体以及纯TiO2纳米纤维三者光催化降解亚甲基蓝(MB)的效果。研究表明:由静电纺丝法制备的5%Fe3+/TiO2纳米纤维的光催化降解效果比相同含铁量的粉体的降解效果好,TiO2纳米纤维比5%Fe3+/TiO2纳米纤维的光催化活性高。     

静电纺丝制备的ZrO2纳米纤维及其应用的研究进展

制备超细、高性能ZrO2纤维是实现其在催化、能源及环境等领域工程应用的关键。静电纺丝技术是一种近年来兴起的氧化物陶瓷纳米纤维制备新方法,能够制备直径较小、均一性高、连续性好的ZrO2纳米纤维,并且可通过控制前驱体纺丝液组成、静电纺丝工艺及热处理参数,对ZrO2纤维的组成、结构及性能进行调控。介绍了ZrO2纳米纤维制备、结构及性能方面的研究进展,并对经由原料组成、静电纺丝工艺及热处理条件调控的ZrO2纳米纤维结构、性能以及应用进行了综述和分析。     

CoFe2O4-SiO2电纺纳米纤维的对喷制备技术与磁性研究

将溶胶-凝胶法和新型双喷丝头静电纺丝技术相结合,制备了CoFe2O4-SiO2电纺纳米纤维材料。利用热分析法(TG-DTA)、X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)和振动样品磁强计(VSM)等测试手段,表征了所研制纳米纤维的晶型结构、纤维形貌以及磁学性能。研究结果表明,样品中CoFe2O4为单畴结构,纤维直径在100nm左右,非晶态SiO2的存在有效抑制了CoFe2O4晶粒的生长;煅烧温度对纤维形貌和晶型结构有较大影响,随着煅烧温度的升高,饱和磁化强度(Ms)和剩余磁化强度(Mr)均增大,但矫顽力(Hc)和剩磁比(Mr/Ms)呈波动变化。     

静电纺丝法制备SiO2纳米纤维及其形貌的调控

一维SiO2纳米纤维以其独特的长径比,优异的力学性能以及热学性能,广泛应用于分离、催化以及传感器领域。以高压静电纺丝技术为基础,结合无模板剂的溶胶-凝胶法合成了直径均匀、连续无裂痕的SiO2纳米纤维。研究表明,合成的SiO2纳米纤维形貌良好,直径约为0.5～3μm,为无定形结构。通过改变陈化时间,调整凝胶的粘稠度,从而控制电纺SiO2的形貌与结构,得到了SiO2碗状结构和不同直径的纳米纤维,证明了利用无模板的溶胶-凝胶法静电纺丝的可行性。     

静电纺SF/PLA共混纳米纤维的形态结构及热性能

以六氟异丙醇(HFIP)为溶剂,通过静电纺丝方法纺制了不同比例的丝素蛋白/聚乳酸(SF/PLA)共混纳米纤维,并通过SEM、FT-IR、X射线衍射和TG-DTA研究了该纳米纤维非织造网的形态特征、分子结构和热性能。结果表明,纤维直径在246nm～2000nm之间,混纺纤维直径随着SF含量的增大而变粗;FT-IR和X射线衍射谱图都表明混纺纤维有着较高的结晶度,并有相分离发生;TG-DTA曲线中明显的SF和PLA分解峰,进一步证明了在本实验条件下SF与PLA的共混不能形成共溶体系,共混SF/PLA纳米纤维存在两个分离的结晶区,即SF晶区与PLA晶区。     

Fabrication and Magnetic Property of One-dimensional SrTiO3/SrFe12O19 Composite Nanofibers by Electrospinning

The composite nanofibers of SrTiO3/SrFe12O19 with a molar ratio of 1:1 and diameter about 120 nm were prepared by electrospinning. Effects of calcination temperature on the formation, crystallite size, morphology and magnetic property were studied by infrared spectroscopy, X-ray diffraction, scanning electron microscopy and vibrating sample magnetometer. The binary phase of strontium ferrite and titanate was formed after being calcined at 900℃ for 2 h and the composite nanofibers were fabricated from nanograins of SrTiO3 about 24 nm and SrFe12O19 around 33 nm. The crystallite sizes for the nanofibers increase with increasing calcination temperature and the addition of SrTiO3 has an obvious suppression effect on SrFe12O19 grain growth. The specific saturation magnetization and remanence tend to increase with the crystallite size. With increasing calcination temperature from 900 to 1050℃, the coercivity increases initially, achieving a maximum value of 520.2 kA·m-1 at 950℃, and then shows a reduction tendency.     

Magnetic properties and magnetoelectric effect in Ni0.8Co0.1Cu0.1Fe2O4 + PbZr0.2Ti0.8O3 composites

Composites with compositions x (Ni_0.8Co_0.1Cu_0.1Fe₂O₄) + (1−x) PbZr_0.2Ti_0.8O₃ (x-mole fraction varies as 0.15, 0.25, 0.35 and 0.45) were prepared by standard ceramic method. The presence of constituent phases, namely ferrite and the ferroelectric were confirmed by X-ray diffraction. The structural analyses were carried out using the obtained powder pattern X-ray data. The porosity of the samples was calculated and the values obtained lie between 10% to 19%. To date, the variations in the magnetic properties with variation in ferrite phase in composites and thereby its influence on magnetoelectric effect is not yet reported. The saturation magnetization (Ms) and magnetic moment (η_B) in Bohr magneton were calculated for all the composites. The static value of magnetoelectric voltage coefficient (dE/dH) was measured as a function of intensity of magnetic field. The maximum value of ME coefficient was observed for a composite with 35% ferrite + 65% ferroelectric phase.     

Effects of different magnetic flux densities on microstructure and magnetic properties of molecular-beam-vapor-deposited nanocrystalline Fe64Ni36 thin films

The nanocrystalline Fe₆₄Ni₃₆ thin films were prepared by molecular-beam-vapor deposition under different magnetic flux densities. The microstructure and magnetic properties of thin films were examined by AFM, TEM, HRTEM and VSM. The results show that with the increase of magnetic flux densities, the changing trend of the average particle size is the same as the coercive force except 6 T. Under 6 T condition, the thin film became the mixture of bcc and fcc phases, which leads to slight increase of the coercive force. In addition, the HRTEM result shows the short-range ordered clusters (embryos) or nucleation rate of thin films increase with increasing magnetic flux densities.     

Hydrothermal synthesis and magnetic properties of Co0.2Cu0.03Fe2.77O4 nanoparticles

Co_0.2Cu_0.03Fe_2.77O₄ nanoparticles with different morphologies have been synthesized directly via a simple hydrothermal method. The effects of pH value, precursor concentration, reaction temperature and surfactant on the particle size were discussed. X-ray diffraction analyses showed that the as-synthesized Co_0.2Cu_0.03Fe_2.77O₄ nanoparticles possessed typical spinel structure. Scanning electron microscope images showed different morphologies of the particles, including truncated octahedron and octahedron. It was indicated that well-dispersed Co_0.2Cu_0.03Fe_2.77O₄ nanoparticles can be synthesized at pH values ranging from 11 to 13, and reaction temperature of 160 °C. The particle size decreased from 18 to 10 nm after the addition of sodium dodecyl sulphate at the pH value of 9. The magnetic measurement showed that the as-prepared Co-Cu spinel ferrite nanoparticles possessed hard magnetic property.     

静电纺缓释抗菌纳米纤维的制备及抗菌性能研究

目的 解决天然抗菌剂精油封装到聚合物中的受控释放问题。方法 选用聚乙烯醇和纳米纤维素为主体材料,采用百里香精油为活性物质,通过静电纺丝技术制备纳米纤维。结果 采用质量比为3∶4的纳米纤维素水凝胶(质量分数1%)和聚乙烯醇水溶液(质量分数6%),并加入质量分数为4%~10%的百里香精油制备纺丝液,在纺丝电压为16 kV、纺丝速率为0.8 mL/h、纺丝距离为11 cm、针头直径为0.7 mm的条件下制备了直径为100~150 nm的纳米纤维,并成功将百里香精油包埋在纳米纤维中。结论 所制备的纳米纤维可以达到百里香精油缓慢释放的效果,对大肠杆菌、金黄葡萄球菌、黑曲霉和橘青霉均有抑制作用。     

Preparation, characterization and microwave absorption properties of polyaniline/Co0.5Zn0.5Fe2O4 nanocomposite

The polyaniline (PAni)/Co_0.5Zn_0.5Fe₂O₄ nanocomposite was prepared by an in situ polymerization in an aqueous solution. The products were characterized by Fourier transform infrared (FT-IR) spectrometer, ultraviolet-visible (UV-vis) spectrometer, X-ray diffraction (XRD) and transmission electron microscope (TEM). The average particle size of the PAni/Co_0.5Zn_0.5Fe₂O₄ was estimated to be about 70 nm by TEM. The reflection loss (dB) of the nanocomposite was measured at different microwave frequencies in X-band (8.2-12.4 GHz), U-band (12.4-18 GHz) and K-band (18-26.5 GHz) by radar cross-section (RCS) method according to the national standard GJB-2038-94. The results showed the reflection loss of the PAni/Co_0.5Zn_0.5Fe₂O₄ nanocomposite was higher than that of the PAni. The maximum reflection loss of the PAni/Co_0.5Zn_0.5Fe₂O₄ nanocomposite was about −39.9 dB at 22.4 GHz with a bandwidth of 5 GHz (full frequency width at about a half of the peak response). In conclusion, this sample is a good microwave shielding and absorbing materials at higher frequency.     

Irreversible Magnetic Properties of Ceramic Hgba2Ca2Cu3O8 at Very High Pulsed Magnetic Fields

The magnetic properties of ceramic HgBa₂Ca₂Cu₃O₈ have been investigated using pulsed magnetic fields up to 50 tesla. The irreversibility line H _irr (T) and the magnetic critical current J _c,m (H,T) have been extracted from the high field hysteresis loops. Irreversibility fields exceed available fields at temperatures below 15 K. The magnetic critical current J _c,m is strongly dependent on the granular structure of the ceramic superconductor. This is reflected in the moderate value of the critical current density and its significant field dependence.