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1.
采用改进的水热法成功合成了单分散的纯相锶铁氧体纳米片。借助DLS、XRD、FTIR、SEM、EDS和VSM等分析测试手段对SrFe12O19铁氧体粉体的粒度、结构、形貌和磁性能进行表征。研究结果表明,在240℃保温5 h,物质的量之比nFe3+/nSr2+(RF/S)和nOH-/nNO3-(RO/N)分别为5和2时,所得产物为单分散的纯相六角SrFe12O19铁氧体纳米片。随着RF/SRO/N的变化,合成样品中有少量SrCO3和Fe2O3杂相存在,这主要与反应条件和离子比例有关。磁性能测试结果显示,所得纯相的六角SrF12O19铁氧体纳米片具有优异的磁性能,其饱和磁化强度和矫顽力分别达到60.91 emu·g-1和94.83 kA·m-1,使其在医疗、催化和生物等高技术领域具有潜在的应用。  相似文献   

2.
采用静电纺丝法成功制备了La3+掺杂CaFe2O4材料。通过X射线衍射、扫描电子显微镜和X射线光电子能谱对La3+掺杂CaFe2O4材料的结构和形貌进行了表征。随后,研究了La3+的掺杂量(质量分数)对CaFe2O4气敏性能的影响。研究表明,3% La3+掺杂CaFe2O4材料在室温下对100 μL·L-1甲醛的响应最高(Ra/Rg=14.1)。更为重要的是,对甲醛的最低检测限低至0.1 nL·L-1,并且响应/恢复时间仅为4.3 s/8.4 s。  相似文献   

3.
针状纳米SrFe12O19的溶胶-凝胶法制备及磁性研究   总被引:1,自引:0,他引:1  
采用柠檬酸-EDTA的联合络合溶胶-凝胶法制得了针状纳米锶铁氧体磁性微粒。利用XRD对样品的物相进行分析,利用TEM对样品形貌和粒径进行表征,并利用振荡样品磁强计(VSM)对样品进行了磁性能研究。结果表明,相对于柠檬酸法制备的纯锶铁氧体微粒,EDTA加入后制备的SrFe12O19微粒仍保持六方磁铅石型结构,但是粒径减小,形貌向一维发展,且内禀矫顽力Hc显著提高。并直接对凝胶加热,使其发生自蔓延燃烧,省去了凝胶的干燥过程,制备周期缩短1/4以上,同时自蔓延燃烧使SrFe12O19的内禀矫顽力提高10%左右,通过洗涤前驱体使得SrFe12O19纯度得到提高,进而使比剩余磁化强度和比饱和磁化强度提高20%左右,最终制得了粒径为30 nm,长径比为5∶1,内禀矫顽力、比饱和磁化强度与比剩余磁化强度分别为6 446.9 Oe、68.9 emu·g-1和40.2 emu·g-1的针状纳米SrFe12O19。  相似文献   

4.
以乙二醇为溶剂,氯化铁、氯化钴、氯化镍和醋酸铵为反应试剂,采用溶剂热法制备纳米NixCo1-xFe2O4(x=0、0.3、0.5、0.7、1)铁氧体空心微球,研究镍含量对铁氧体空心球的磁性与吸波性能的影响。借助X射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、振动样品磁强计(VSM)和网络分析仪对试样的物相组成、微观形貌和电磁特性进行表征。结果表明制备的镍钴铁氧体为尖晶石结构,且形貌为空心球,粒径在200nm左右。当x=0时,镍钴铁氧体空心球饱和磁化强度最大为81.7emu·g-1,反射损耗在1658.8MHz有最小值为-16.9dB。  相似文献   

5.
以乙二醇为溶剂,氯化铁、氯化钴、氯化镍和醋酸铵为反应试剂,采用溶剂热法制备纳米NixCo1-xFe2O4(x=0、0.3、0.5、0.7、1)铁氧体空心微球,研究镍含量对铁氧体空心球的磁性与吸波性能的影响。借助X-射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、振动样品磁强计(VSM)和网络分析仪对试样的物相组成、微观形貌和电磁特性进行表征。结果表明制备的镍钴铁氧体为尖晶石结构,且形貌为空心球,粒径在200 nm左右。当x=0时,镍钴铁氧体空心球饱和磁化强度最大为81.7 emu·g-1,反射损耗在1 658.8 MHz有最小值为-16.9 dB。  相似文献   

6.
在理论研究方面,采用基于密度泛函理论(DFT)的第一性原理方法对CaMn7O12的晶体结构进行了计算和表征,对螺旋桨型磁序的电子结构及相变机制进行了理论分析和研究;在实验方面以TG-DSC为指导,采用固相反应法制备了单相多铁性体CaMn7O12,并检测表征其磁、电学性能。磁学方面验证了CaMn7O12的2个磁相转变温度(TN1=90 K和TN2=45 K),测得其在10 K温度下存在磁滞回线(Mr=0.02 emu·g-1,Hc≈1000 Oe);电学方面在室温条件下表征其在10 MHz频率时εr=280,tanδ=1.69。  相似文献   

7.
以硝酸锶、硝酸铁、硝酸钐、硝酸钴为原料,采用低热固相法制备出前驱体,经灼烧后得到最终产物,使用XRD、EDX、SEM对其表征,表明产物为Sm-Co共掺杂的Sr1-xSmxCoxFe12-xO19x=0~0.5)锶铁氧体;并发现所制产物具有单一的六方相晶体结构,粒子尺寸在40~100 nm,随着Sm-Co掺杂量的增大,晶粒尺寸逐渐减小。经VSM测试:产物的磁性能(Ms,Mr,Hc)随Sm-Co的共掺杂量的增加(0~0.5),先增大后减小,在x=0.1时表现为最大值(Ms=64.32 A·m2·kg-1Mr=36.17 A·m2·kg-1、Hc=417.45 kA·m-1)。将制得的共掺杂锶铁氧体磁粉,添加到醇酸清漆中形成防蜡涂层,通过拉伸强度测试、涂层防蜡率实验、以及晶相显微表征,发现该涂层随磁粉用量增加,抗拉强度提高;同时随磁粉磁性的增强,涂层的防蜡效果增加,在磁粉用量为2%时,涂层磁性最大,防蜡率也达到最大值77.3%。  相似文献   

8.
以水热法制备的高磁饱和强度Fe3O4纳米颗粒为核,正硅酸乙酯(TEOS)为前驱体,采用改进的Stöber法,制备介孔SiO2包覆Fe3O4磁性核壳复合微球。利用XRD、SEM、TEM、N2吸-脱附、FTIR和VSM对制备样品的物相结构、形貌和磁性能进行了测试表征。研究结果表明,制备的复合材料呈球形,粒径分布均一,材料的比表面积和磁饱和强度分别为413 m2·g-1和68.93 emu·g-1。研究了TEOS的添加量对复合微球形貌的影响,随着TEOS添加量的增加,SiO2壳层增厚,复合粒子形貌均匀,饱和磁化强度有所下降,仍具有良好的超顺磁性。在此基础上,通过接枝法在复合微球的表面接枝-NH2,制备了一种新型磁性纳米吸附剂(Fe3O4@SiO2@mSiO2-NH2),进而研究了其对水中重金属离子Cr(Ⅳ)的吸附性能。通过动力学拟合,Fe3O4@SiO2@mSiO2-NH2对Cr(Ⅳ)的吸附过程是准二级动力学模型占主导地位。探究了该材料对Cr(Ⅳ)的吸附过程和吸附机理。结果表明,其吸附机理及吸附容量与Cr(Ⅳ)的离子形态及-NH2有关,并通过吸附剂与吸附质之间的电子共用或静电吸附实现。  相似文献   

9.
采用改进的Stober法合成了多孔结构的双层SiO2包覆Fe3O4复合材料,利用TEM、XRD、VSM和氮吸附-脱附实验对其结构与性能进行分析,进而研究其对染料的吸附性能。研究结果表明,双层SiO2包覆Fe3O4复合材料的比表面积和磁饱和强度分别为308 m2·g-1和45.5 emu·g-1;当罗丹明B的初始浓度从25 mg·L-1提高到250 mg·L-1时,复合材料对其饱和吸附量从24.0 mg·g-1增大到112.4 mg·g-1,而亚甲基蓝的初始浓度从25 mg·L-1提高到500 mg·L-1时,对其饱和吸附量从22.0 mg·g-1增大到235.1 mg·g-1;随着溶液pH值增大,复合材料对罗丹明B的饱和吸附量增加,而对亚甲基蓝的饱和吸附量变化不明显;温度在20~40 ℃范围内复合材料的吸附量较大。  相似文献   

10.
采用溶剂热法成功制备了纳米CuFe2O4-rGO复合材料。通过X射线衍射(XRD),扫描电子显微镜(SEM)、透射电子显微镜(TEM)和电化学工作站对样品的结构、形貌及电容特性进行表征。结果表明,CuFe2O4纳米粒子均匀地分散在石墨烯片层间,其中CuFe2O4-20% rGO复合材料具有最优的电化学性能,当电流密度1 A·g-1时,其比电容为1 952.5 F·g-1,当电流密度为1 A·g-1时,CuFe2O4-20% rGO复合材料经1 000次充放电后的比电容保持率为86.17%。  相似文献   

11.
以乙酰丙酮金属盐为前驱体,三乙二醇为溶剂,采用多元醇法制备了镍锌不同配比的Ni_xZn_(1-x)Fe_2O_4(x=0,0.3,0.5,0.7和1.0)铁氧体,并通过X射线衍射仪(XRD),透射电子显微镜(TEM)和振动样品磁强计(VSM)等对样品的结构、形貌、磁性能和磁热性能进行了表征。结果表明:Ni_xZn_(1-x)Fe_2O_4铁氧体分散性较好,尺寸均一,形状近似球形,平均粒径为4~5 nm。Ni_xZn_(1-x)Fe_2O_4纳米颗粒在室温下表现出亚铁磁性,饱和磁化强度随着镍含量的增加先增大后减小,当x=0.5时达到最大值29.38 emu·g~(-1)。在382k Hz交变磁场作用下,Ni_(0.5)Zn_(0.5)Fe_2O_4铁氧体温度可升温至313 K,表现出较好的磁热性能。  相似文献   

12.
 Magnetic properties of nanocrystalline Fe78B13Si9 alloys are studied for three series prepared by ball milling starting from amorphous ribbons, crystallized ribbons, and elemental powders. Temperature variation of static magnetization results in strong ferromagnetic interaction which is weakly dependent on the initial material. Magnetic hysteresis loops show that saturation magnetization, magnetic remanence, and coercive field increase with frequency for both series of ribbon samples, whereas they decrease for alloys prepared from elemental powders. Power losses raise faster for the alloys prepared from elemental powders than for the two other alloys.  相似文献   

13.
Magnetic glass-ceramic composites containing micron-sized particles of lanthanum strontium manganite in the matrix of borate-silicate phases were prepared by thermal treatment of amorphous samples of nominal composition 28La2O3-22SrO-25MnO x -17SiO2-8B2O3at 800–1150°C. The samples obtained exhibit high magnetization up to 25 A m2/kg at a magnetic field strength of 720 kA/m. The relative magnetoresistance amounts to 17% at 77 K and a magnetic field strength of 160 kA/m.  相似文献   

14.
Catalytic activities of ferrites MFe2O4 (M = Cu, Co, Ni, Mg, and Zn) and M1 0.5M2 0 .5Fe2O4 (M1 = CU; M2 = Co, Zn, and Mg) in oxidation of CO and ethylbenzene were investigated, and their dependences on the cation nature were established. Higher activities were observed for catalysts containing ions with variable valence (Cu, Co, and Ni). A correlation between catalytic and adsorption properties of ferrites was found.Translated fromIzvestiya Akademii Nauk, Seriya Khimicheskaya, No. 1, pp. 49–52, January, 1996.  相似文献   

15.
Nanocrystalline magnetic particles of Ni0.8−xZn0.2MgxFe2O4 ferrites with x lying between 0.0 and 0.8 were synthesized using metal nitrates and freshly extracted egg-white. The synthesized powders were characterized using X-ray diffraction (XRD), Fourier transform infrared (FT-IR) and transmission electron microscopy (TEM). With increasing magnesium concentration, the lattice constant increases while X-ray density decreases. The average crystallite size determined from XRD data using Scherrer formula lie in the range of 35–59 nm. TEM image shows spherically agglomerated particles with average crystallite size agreed well with that obtained from XRD. Magnetic properties measured at room temperature by vibrating sample magnetometer (VSM) reveal a decrease in saturation magnetization up to Mg content of 0.6. In agreement with FT-IR results, the unexpected increase in the magnetization at Mg content of 0.8 can be attributed to the tendency of Mg2+ ions to occupy the tetrahedral site. The decrease in the value of coercivity with increasing magnesium content can be explained based on the magneto-crystalline anisotropy.  相似文献   

16.
The adsorption of Saccharomyces cerevisiae mandelated dehydrogenase (SCMD) protein on the surface-modified magnetic nanoparticles coated with chitosan was studied in a batch adsorption system. Functionalization of surface-modified magnetic particles was performed by the covalent binding of chitosan onto the surface of magnetic Fe3O4 nanoparticles. Characterization of these particles was carried out using FTIR spectra, transmission electron micrography (TEM), X-ray diffraction (XRD) and vibrating sample magnetometry (VSM). Magnetic measurement revealed that the magnetic Fe3O4–chitosan nanoparticles were superparamagnetic and the saturation magnetization was about 37.3 emu g−1. The adsorption capacities and rates of SCMD protein onto the magnetic Fe3O4–chitosan nanoparticles were evaluated. The adsorption capacity was influenced by pH, and it reached a maximum value around pH 8.0. The adsorption capacity increased with the increase in temperature. The adsorption isothermal data could be well interpreted by the Freundlich isotherm model. The kinetic experimental data properly correlated with the first-order kinetic model, which indicated that the reaction is the adsorption control step. The apparent adsorption activation energy was 27.62 kJ mol−1 and the first-order constant for SCMD protein was 0.01254 min−1 at 293 K.  相似文献   

17.
A study was carried out on the conditions of formation of highly crystalline, superparamagnetic, nanosized oxides, MII Fe 2 III O4 and γ-Fe2O3 (4.9–11.7 nm) by the thermal decomposition of complexes [MFe2O(CH3CO2)6(H2O)3] (M = Mn, Fe, Co, Ni) in tetraethylene glycol. The presence of surfactants leads to a decrease in the size and size distribution of the nanoparticles formed, while the use of microwave radiation significantly reduces the time for formation of the nanocrystalline oxides. The magnetic measurements showed ferrimagnetic ordering in the nanoparticles studied and their superparamagnetic behavior. __________ Translated from Teoreticheskaya i éksperimental’naya Khimiya, Vol. 43, No. 5, pp. 323–329, September–October, 2007.  相似文献   

18.
Cation distribution in quenched and furnace-cooled samples of composition NixM1?xFe2O4 (where M is either Mg2+ or Cu2+) has been studied through magnetization measurements. It has been found that cation distribution in these mixed ferrites cannot be predicted by site preference energies. In magnesium-nickel ferrites, cation distribution is controlled by heat treatment up to x = 0.5, beyond which the effect of heat treatment diminishes. Addition of Ni2+ ions in copper ferrite reduces the diffusibility of Cu2+ ions and the distribution tends toward inverse spinel in the high-nickel region.  相似文献   

19.
Ferrites-spinels of the MFe2O4 type (M = Co, Ni, Zn), produced by glycine-nitrate combustion were studied. A physicochemical study of ferrite samples was performed by X-ray fluorescence analysis, scanning electron microscopy, X-ray phase analysis, and X-ray spectroscopy. The average size of the coherent scanning region was found to be (nm): 28 ± 2 for CoFe2O4, 32 ± 2 for NiFe2O4, and 26 ± 2 for ZnFe2O4. Magnetic characteristics were determined by the NMR method. The specific residual magnetization, specific saturation magnetization, and coercive force were, respectively, 14.1 A m2 kg?1, 20.1 A m2 kg?1, 31800 A m?1 for CoFe2O4; 4.4 A m2 kg?1, 23.1 A m2 kg?1, 6550 A m?1 for NiFe2O4; and 5.1 A m2 kg?1, 18.3 A m2 kg?1, 3200 A m?1 for ZnFe2O4. Their magnetic properties show that the resulting ferrospinel powders can be used in the following fields of technology: CoFe2O4 in those areas where heat transfer is necessary (hyperthermia) and in development of data storage media; NiFe2O4 and ZnFe2O4 in those areas where low heat exchange is necessary, ZnFe2O4 for fast remagnetization and NiFe2O4 as a core or shell for transportation of other substances. The ferrospinel samples compare well in magnetic properties with their foreign commercial analogs, which makes these compounds commercially viable.  相似文献   

20.
Nanoparticles of MFe2O4 (M=Mn, Co and Ni), with diameters ranging from 5 to 10 nm, have been obtained through a solvothermal method. In this synthesis, an alcohol (benzyl alcohol or hexanol) is used as both a solvent and a ligand; it is not necessary, therefore, to add a surfactant, simplifying the preparation of the dispersed particles. We have studied the influence of the synthetic conditions (temperature, time of synthesis and nature of solvent) on the quality of the obtained ferrites and on their particle size. In this last aspect, we have to highlight that the solvent plays an important role on the particle size, obtaining the smallest diameters when hexanol was used as a solvent. In addition, the magnetic properties of the obtained compounds have been studied at room temperature (RT). These compounds show a superparamagnetic behaviour, as was expected for single domain nanoparticles, and good magnetization values. The maxima magnetization values of the MFe2O4 samples are quite high for such small nanoparticles; this is closely related to the high crystallinity of the particles obtained by the solvothermal method.  相似文献   

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