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1.
以乙酰丙酮盐为前驱体,三乙二醇为溶剂,采用多元醇法制备了纳米Ni0.5-xCoxZn0.5Fe2O4(x=0,0.1,0.2,0.3和0.4)铁氧体.通过X射线衍射仪(XRD)、透射电子显微镜(TEM)、傅里叶变换红外光谱仪(FTIR)和振动样品磁强计(VSM)等对样品的结构、形貌和磁性能进行了表征.结果表明,所得纳米Ni0.5-xCoxZn0.5Fe2O4铁氧体的分散性较好,尺寸均一.在室温下产物的剩磁和矫顽力均较小,表现出亚铁磁性.纳米Ni0.3Co0.2Zn0.5Fe2O4铁氧体的饱和磁化强度达到41.34 A·m2·kg-1,其在交变磁场中升温可达到55℃,表现出较好的磁热性能.  相似文献   

2.
基于尖晶石晶体结构信息,本文采用热力学三亚晶格模型,将材料热力学计算和第一性原理计算相结合,研究了Zn_xMn_(1-x) Fe_2O_4和Ni_xMn_(1-x)Fe_2O_4立方相中的Zn~(2+)、Ni~(2+)、Mn~(2+)以及Fe~(3+)在8a和16d亚晶格上的占位有序化行为。结果表明:在锰铁氧体中,室温下Mn~(2+)完全占据在8a亚晶格上,Fe~(3+)完全占据在16d亚晶格上,属于正尖晶石结构;随着热处理温度升高,在1 273 K达到热处理平衡时的占位构型为(Fe~(3+)0.09Mn~(2+)0.91)[Fe~(3+)1.91Mn~(2+)0.09]O_4,在热处理温度升至1 473 K时,达到热处理平衡时的占位构型为(Fe~(3+)0.11Mn~(2+)0.89)[Fe~(3+)1.89Mn~(2+)0.11]O_4,均与实验结果符合较好。在锌铁氧体中,室温下Zn~(2+)完全占据在8a亚晶格上,Fe~(3+)完全占据在16d亚晶格上,属于正尖晶石结构;在热处理温度较高时,Zn~(2+)和Fe~(3+)发生部分置换,符合实验结果。在镍铁氧体中,半数的Fe~(3+)在室温下占据在8a亚晶格上,Ni~(2+)与剩下另一半的Fe~(3+)共同占据在16d亚晶格上,仅在热处理温度较高的时候发生微弱变化,亦与已有的实验结果吻合。在此基础上,本文进一步通过热力学模型研究了立方相尖晶石结构的Zn_xMn_(1-x)Fe_2O_4、Ni_xMn_(1-x)Fe_2O_4复合体系中阳离子占位行为与热处理温度对占位的影响规律。  相似文献   

3.
采用温和的反应条件,制备出三明治结构rGO/Fe_3O_4@mSiO_2,利用SEM、TEM、FTIR、XRD和N_2吸附-脱附等对其形貌和性能进行表征,考查了其对Hela细胞的毒性和细胞荧光成像效果,并探讨了其形成机理。实验结果表明:rGO/Fe_3O_4@mSiO_2具有较高的比表面积(217 m~2·g~(-1)),对抗癌药物五氟尿嘧啶(5-FU)的载药率达到57.34%;它还具有较好的磁性,磁饱和强度为32 emu·g-1;而且rGO/Fe_3O_4@mSiO_2纳米复合物在光照条件下具有优异的光热转换性能,对He La细胞表现出明显的杀伤效果。  相似文献   

4.
采用喷雾干燥法结合后续的热处理,成功地制备了一系列新型的基于富锂层状固溶体Li_2MnO_3和Li[Ni_(0.8)Co_(0.15)Al_(0.05)]O_2结合的xLi_2MnO_3-(1-x)Li[Ni_(0.8)Co_(0.15)Al_(0.05)]O_2(0.5≤x≤0.8)材料,并对其晶体结构、表面形貌、元素价态以及电化学性能进行了一系列的研究。实验结果表明,随着x值的增大,材料的晶体结构逐渐从层状的Li[Ni_(0.8)Co_(0.15)Al_(0.05)]O_2过渡到类Li_2MnO_3结构。对样品进行淬火处理对晶粒的微观晶体结构和元素价态产生复杂影响,这种变化使得淬火的样品表现出较好的电化学性能。其中x=0.6的样品淬火后表现出较好的电化学性能,100次循环后可逆容量可达209 mAh·g~(-1)。  相似文献   

5.
采用缓冲溶液法制备Mn掺杂Ni_(1-x)Mn_x(OH)_2(x=0.1,0.2,0.3,0.4)。X射线衍射(XRD)测试表明x=0.1和0.2的样品主要是由β相组成;扫描电子显微镜(SEM)和氮气吸附-脱附测试表明掺杂Mn样品比不掺Mn的商用β-Ni(OH)2的颗粒更细小、多孔;恒流充放电测试表明,这种电极具有优良的高倍率性能,当x=0.2,电流密度800 mA·g-1时放电比容量为288.8 mAh·g-1,同等条件测试的商用β-Ni(OH)2放电比容量为198.7 mAh·g-1,循环580圈后仍有276 mAh·g-1的放电比容量,其衰减率为4.1%,而同等测试条件下的其它4种样品衰减率分别为46.1%(商用β-Ni(OH)2)、13.0%(x=0.1)、25.6%(x=0.3)、34.1%(x=0.4),可见这种Mn掺杂电极材料适合大电流密度充放电,能够改善镍电极的循环稳定性,降低镍电极成本。  相似文献   

6.
采用一锅共缩聚法制备了不同N原子个数的硅烷偶联剂改性并且SiO_2包覆的球形磁性Fe_3O_4@SiO_2-x N(x=1,2,3)复合吸附剂,其中1N、2N、3N分别代表γ-氨丙基三甲氧基硅烷、γ-氨乙基氨丙基三甲氧基硅烷、二乙烯三胺基丙基三甲氧基硅烷。采用XRD、SEM、N2吸附-脱附、元素分析、FT-IR和ζ电位等手段对典型样品的物理化学性质进行了对比表征。结果表明,改性后的复合材料均具有良好的球形形貌和较高的等电点,其含N量呈现出Fe_3O_4@SiO_2-1NFe_3O_4@SiO_2-2NFe_3O_4@SiO_2-3N的趋势。对Cr(Ⅵ)的静态吸附实验表明,其最大吸附量随着N含量的增加而降低,即Fe_3O_4@SiO_2-1N(79.74 mg·g~(-1))Fe_3O_4@SiO_2-2N(63.05 mg·g~(-1))Fe_3O_4@SiO_2-3N(55.37 mg·g~(-1)),并对其呈现这种趋势的机理进行了分析。对模拟废水的吸附实验表明,样品Fe_3O_4@SiO_2-1N可以同时吸附废水中的多种重金属离子,并且可以在30 s内实现磁性分离。  相似文献   

7.
通过静电纺丝技术制备了多孔软硬磁Ni_(0.5)Zn_(0.5)Fe_2O_4/SrFe_(12)O_(19)复合纤维,利用综合热重分析仪(TG-DSC)、X射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、X射线能谱仪(EDS)和矢量网络分析仪(VNA)等对复合纤维的晶体结构、微观形貌和电磁性能进行了表征,研究了不同软硬磁质量比对纤维结构和性能的影响。结果表明:900℃下制备的复合纤维具有立体多孔结构,软硬磁质量比为1∶3时,复合纤维的比表面积达到55 m~2·g~(-1)。吸波性能测试结果显示,当吸波剂涂层厚度为3.5 mm时,复合纤维在10.6 GHz处反射损失(RL)值达到-31.9 dB,在2~18 GHz频率范围内,RL值小于-10 dB的吸收带宽达到10.5 GHz,覆盖了整个X波段(8.2~12.4 GHz)和Ku波段(12.4~18 GHz),显示出优异的宽波段吸收性能。  相似文献   

8.
将镍铁金属配位聚合物前驱体在惰性气氛下热分解制备了富氮洋葱碳(ONC)包覆的Ni/Ni Fe_2O_4多孔纳米棒复合析氧电催化剂,与Ni@ONC,Ni Fe_2O_4材料及传统Ru O_2催化剂相比,得益于这种富氮洋葱碳包覆的Ni/Ni Fe_2O_4一维多孔纳米异质结构,Ni/Ni Fe_2O_4@ONC材料拥有更优异的导电性能和更大的电化学活性面积(0.149 m F),因而表现出更优异的析氧电催化性能。Ni/Ni Fe_2O_4@ONC纳米棒在1 mol·L~(-1) KOH溶液中,10 m A·cm-2下的析氧过电位仅为299 m V,塔菲尔斜率为73 m V·dec-1,展现出优异的析氧稳定性能。  相似文献   

9.
采用改进的Hummers法制备了氧化石墨烯,用水热法首次制备了Fe_3O_4/GO/PPy(聚吡咯)三元复合粒子用于处理含2-硝基-1,3-苯二酚(NRC)的废水,研究了其对水中NRC的吸附性能。采用紫外-可见吸收光谱(UV-Vis)、透射电子显微镜(TEM)、傅里叶变换红外光谱(FT-IR)、X射线衍射(XRD)、振动样品磁强计及ζ电位等对所制备复合粒子的结构进行了表征;研究了溶液pH值、吸附剂用量、NRC的初始浓度、吸附时间和温度对吸附NRC的吸附性能的影响,并对吸附过程进行了吸附动力学模拟。结果表明:制备的Fe_3O_4/GO/PPy复合材料为层状分散结构,PPy及Fe_3O_4颗粒无规则地镶嵌在石墨烯片层之间。Fe_3O_4颗粒为多面体晶体结构,尺寸为100~300 nm。Fe_3O_4/GO/PPy具有超顺磁性,40 s可以磁分离,NRC移除率达91.6%;在NRC浓度为200 mg·L~(-1)、pH=5±0.05、温度T=318 K、吸附剂用量10 mg·L~(-1)和吸附时间6 h的条件下Fe_3O_4/GO/PPy对NRC的吸附量最大,达到163.3mg·g~(-1)。NRC吸附动力学符合二级动力学模型,吸附等温线符合Langmuir模型。循环使用5次后,NRC的移除率由最初的91.6%下降至77.6%,说明Fe_3O_4/GO/Ppy磁性复合物的结构具有较好的稳定性,且可以再重复利用。  相似文献   

10.
采用溶胶-凝胶法用SO~(2-)_4部分代替Li_3Fe_2(PO_4)_3中的PO~(3-)_4阴离子制得Li_(3-x)Fe_2(PO4)_(3-x)(SO_4)_x(x=0~0.90)正极材料,通过X射线衍射、充放电技术、循环伏安特性测试及电化学阻抗谱表征了掺杂材料的相组成及电化学性能.结果表明,SO~(2-)_4主要以固溶形式存在于Li_3Fe_2(PO_4)_3中,产物中还伴有少量Fe_2O_3第二相析出.SO~(2-)_4掺杂使Li_3Fe_2(PO_4)_3的放电容量呈抛物线形规律变化,并在掺杂浓度x=0.60时达到最佳值,该样品在0.5C倍率下的首次放电容量为111.59 mA·h/g,比未掺杂的样品提高了18.4%;60次循环充放电后的容量保持率为96%;将该样品的放电倍率由0.5C逐渐提高至5C,再降至0.5C,并在每个倍率下循环10次,材料的最终放电容量仍能达到首次放电容量的97%.导致这些变化的原因是SO~(2-)_4掺杂使材料的氧化还原性能增强,电池内阻减小,极化程度降低及Li~+扩散系数增大.  相似文献   

11.
A nitrogen doped TiO2/Ni0.5Zn0.5Fe2O4 core–shell structure nanoparticles was prepared by low temperature sol–gel-hydrothermal process. The characterizations of the catalyst indicate that the Ni0.5Zn0.5Fe2O4 nanocrystals of about 25 nm are well-coated with crystalline N-doped titania. The absorption edges in the diffusion reflectance spectra of TiO0.98N1.02 and TiO1.37N0.63/Ni0.5Zn0.5Fe2O4 shift to visible light region. The core–shell nanocatalysts can effectively photodegrade organic pollutants in the dispersion system and can be recycled easily by an external magnetic field.  相似文献   

12.
完全还原的NixCu1-xFe2O4(x=0.25,0.5,0.75)可用来分解CO2。采用共沉淀法制备了NixCu1-xFe2O4(x=0.25,0.5,0.75)系列铁酸盐的纳米微粒,利用H2-TG数据分析NixCu1-xFe2O4(x=0.25,0.5,0.75)中Cu2+的还原反应动力学数据,得出表观活化能Ea并不是单纯随着Ni2+或Cu2+含量的变化而变化,当x=0.25时反应活化能具有最大值。通过CO2-TG比较不同样品经H2完全还原后分解CO2的活性,得出Ni0.5Cu0.5Fe2O4具有最低的起始反应温度和最大的分解活性,并采用XRDRietveld拟合方法对Ni0.5Cu0.5Fe2O4的完全还原产物和分解CO2产物进行物相分析。  相似文献   

13.
MnxNi0:5-xZn0:5Fe2O4 nanorods were successfully synthesized by the thermal treatment of rod-like precursors that were fabricated by the co-precipitation of Mn2+, Ni2+, and Fe2+ in the lye. The phase, morphology, and particle diameter were examined by the X-ray diffrac-tion and transmission electron microscopy. The magnetic properties of the samples were stud-ied using a vibrating sample magnetometer. The results indicated that pure Ni0:5Zn0:5Fe2O4 nanorods with a diameter of 35 nm and an aspect ratio of 15 were prepared. It was found that the diameter of the MnxNi0:5-xZn0:5Fe2O4 (0≤x≤0.5) samples increased, the length and the aspect ratio decreased, with an increase in x value. When x=0.5, the diameter and the aspect ratio of the sample reached up to 50 nm and 7~8, respectively. The coercivity of the samples first increased and then decreased with the increase in the x value. The coer-civity of the samples again increased when the x value was higher than 0.4. When x=0.5,the coercivity of the MnxNi0:5-xZn0:5Fe2O4 sample reached the maximal value (134.3 Oe)at the calcination temperature of 600 oC. The saturation magnetization of the samples first increased and then decreased with the increase in the x value. When x=0.2, the satura-tion magnetization of the sample reached the maximal value (68.5 emu/g) at the calcination temperature of 800 oC.  相似文献   

14.
Nanocomposites of ferrite and ferroelectric phases are attractive functional ceramic materials. In this work, the nanocomposite Ni1−x Co x Fe2O4–BaTiO3(x = 0.2, 0.3, 0.4, 0.5) fibers with fine diameters of 3 ~ 7 μm and high aspect ratios were synthesized by the organic gel-thermal decomposition process from the raw materials of citric acid and metal salts. The structure, thermal decomposition process and morphologies of the gel precursors and the resultant fibers derived from thermal decomposition of the gel precursors were characterized by Fourier transform infrared spectroscopy, thermogravimetric differential thermal analysis, X-ray diffraction and scanning electron microscopy. The magnetic properties of the nanocomposite fibers were measured by vibrating sample magnetometer. The nanocomposite fibers of ferrite Ni1−x Co x Fe2O4 and perovskite BaTiO3 are formed at the calcination temperature of 900 °C for 2 h. The average grain sizes of Ni1−x Co x Fe2O4 and BaTiO3 in the nanocomposite fibers increase from about 15 nm to approximately 67 nm with the increasing calcination temperatures from 900 to 1,180 °C. The saturation magnetization of the nanocomposite Ni1−x Co x Fe2O4–BaTiO3(x = 0.2, 0.3, 0.4, 0.5) fibers increases with the increase of grain sizes of Ni1−x Co x Fe2O4 and Co content, while the coercivity reaches a maximum value at the single-domain size of about 65 nm of Ni0.5Co0.5Fe2O4 obtained at the calcination temperature of 1,100 °C.  相似文献   

15.
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   

16.
Zn1?xNixFe2O4 (0.0 ≤ x ≤ 1.0) nanoparticles are prepared by sol–gel method using urea as a neutralizing agent. The evaluation of XRD patterns and TEM images indicated fine particle nature. The average crystallite size increased from 10 to 24 nm, whereas lattice parameters and density decreased with increasing Ni content (x). Infrared spectra showed characteristic features of spinel structure along with a strong influence of compositional variation. Magnetic measurements reveal a maximum saturation magnetization for Zn0.5Ni0.5Fe2O4 (x = 0.5); however, reduced value of magnetization is attributed to the canted spin structure and weakening of Fe3+(A)–Fe3+(B) interactions at the surface of the nanoparticles. Impedance analysis for different electro-active regions are carried out at room temperature with Ni substitution. The existence of different relaxations associated with grain, grain boundaries and electrode effects are discussed with composition. It is suggested that x = 0.5 is an optimal composition in Zn1?xNixFe2O4 system with moderate magnetization, colossal resistivity and high value of dielectric constant at low frequency for their possible usage in field sensor applications.  相似文献   

17.
This work is devoted to a detailed analysis of the interconnection between composition, cation distribution and acidic properties of the surface of nanocrystalline ferrites NixZn1−xFe2O4 obtained by aerosol pyrolysis. The detailed analysis of the Mössbauer spectra allows us to determine the distribution of cations between tetrahedral and octahedral positions in spinel structure. Depending on samples composition, the tetrahedral positions can be occupied by only Fe3+ cations (inverse spinel, x≥0.4) or by Fe3+ and Zn2+ cations (mixed spinel, x=0, 0.2). Increasing the nickel concentration in the ferrite leads to decrease in the number of strong acid centers on the surface. It was found that the decrease in the contribution of strong surface acid sites leads to an increase in sensory sensitivity of the ferrite towards ammonia. For ethanol detection an inverse relationship between sensor signal and surface acidity was observed.  相似文献   

18.
The structure and crystal phase of the nanocrystalline powders of Ni1−xZnxFe2O4 (0 ≤ x ≤ 0.5) mixed ferrite, synthesized by ethylene glycol mediated citrate sol-gel method, were characterized by X-ray diffraction and microstructure by transmission electron microscopy. Further studies by Fourier transform infrared spectroscopy were also conducted. Moreover, DC electrical properties of the prepared nanoparticles were studied by DC conductivity measurements. The response of prepared Ni1−xZnxFe2O4 mixed ferrites to different reducing gases (ethanol, hydrogen sulfide, ammonia, hydrogen and liquefied petroleum gas) was investigated. In particular, Ni0.6Zn0.4Fe2O4 composition exhibited high response to 100 ppm ethanol gas at 300 °C. Incorporation of palladium further improved the response, selectivity and response time of Ni0.6Zn0.4Fe2O4 to ethanol gas with the blue shift in the operating temperature by 25 °C.  相似文献   

19.
PMMA/Ni0.5Zn0.5Fe2O4 nanocomposite with superparamagnetic behavior was synthesized by in situ emulsion polymerization of methylmethacrylate (MMA) monomer in the presence of Ni0.5Zn0.5Fe2O4 colloidal suspension assisted by ultrasonic irradiation. The obtained samples were characterized by X-ray diffraction (XRD), Fourier transform infrared spectra (FT-IR), transmission electron microscopy (TEM) and vibrating sample magnetometer (VSM). XRD and FT-IR spectra confirmed the formation of PMMA/Ni0.5Zn0.5Fe2O4 nanocomposite. TEM images showed that Ni0.5Zn0.5Fe2O4 nanoparticles with the particle sizes of about 12 nm were well dispersed in the polymer matrix. The nanocomposite at room temperature exhibited superparamagnetic behavior under applied magnetic field. The formation mechanism of PMMA/Ni0.5Zn0.5Fe2O4 nanocomposite was proposed as well.  相似文献   

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