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1.
采用超声粉碎分散团聚磁性纳米Fe3O4粒子,用油酸对分散好的磁性粒子表面进行改性.结果表明,在纳米Fe3O4中油酸用量为0.5mL、超声次数为15次、每次2min、间隔时间为15s、pH值为7.5的条件下,改性效果最好,改性指数为0.87.红外光谱分析证明,油酸通过-COOH的"均化"与纳米Fe3O4粒子的表面结合实现了包覆改性,无分解和其它化学反应发生,改性效果良好.  相似文献   

2.
聚苯乙烯/Fe3O4纳米复合材料的制备与表征   总被引:2,自引:0,他引:2  
采用油酸为表面活性剂表面处理Fe3O4纳米粒子,将其分散在苯乙烯单体中,进行原位聚合,制备PS/Fe3O4纳米复合材料,对该复合材料的分散均匀性和结构进行了表征.实验结果显示,Fe3O4粒子在PS基体中分散均匀;包覆油酸的Fe3O4纳米粒子在基体中起到物理和化学交联点的作用,使得聚合物产生交联,并提高了其耐热性.  相似文献   

3.
油酸钠/Fe纳米粒子的制备及其脱氯性能研究   总被引:3,自引:0,他引:3  
采用油酸钠作为包覆剂,在液相体系中制备油酸钠/Fe纳米复合粒子,并用TEM、XRD、FT-IR、DSC-TGA对所制得的纳米复合粒子进行结构表征.结果表明,油酸钠/Fe纳米复合粒子呈核壳结构,粒度分布窄,其粒径在90nm左右;T-IR和DSC-TGA分析证明纳米铁与油酸钠之间发生了化学键合,具有空气稳定性,而且憎水亲油;将油酸钠/Fe纳米复合粒子与三氯乙烯(TCE)模拟水样反应,发现油酸钠/Fe纳米复合粒子能够与水相中的三氯乙烯(TCE)有良好的接触性,其脱氯效果优于未修饰的纳米铁粒子.  相似文献   

4.
油酸对微波水热法制备的纳米Fe_3O_4的影响   总被引:1,自引:0,他引:1  
采用微波水热法制备纳米Fe3O4,并用油酸对其进行表面改性,获得油酸包覆的Fe3O4纳米粒子。利用XRD、FT-IR、TEM和振动样品磁强计对Fe3O4纳米粒子的结构、形貌、磁性能进行表征。结果表明:表面改性使得油酸分子中—COOH和Fe离子形成化学键;改性后的纳米Fe3O4粒子为粒度均匀的球形,具有良好的分散性,平均粒径约8nm;该产物具有超顺磁性,饱和磁化强度为61.8emu/g。  相似文献   

5.
关晓辉  王雪  鲁敏  赵会彬 《材料导报》2013,27(16):70-73
基于膜分散技术,以Fe2+、Fe3+的混合溶液和NaOH溶液为分散相,利用中空纤维膜将分散相均匀分散到水中并发生微混合反应,连续制备粒径均匀、球形度好的纳米Fe3O4颗粒。考察了铁混合溶液与NaOH溶液的流量以及表面活性剂油酸钠和十二烷基硫酸钠对制备纳米Fe3O4的影响;同时,对纳米Fe3O4进行了XRD、IR、SEM表征。结果表明:控制铁混合溶液的平均流量为68mL/h,NaOH溶液的平均流量为132mL/h,制得的纳米Fe3O4平均产量为420g/(m2·h),平均粒径在10~20nm之间;通过添加分散剂可以有效减轻纳米Fe3O4的团聚,其中油酸钠的修饰效果优于十二烷基硫酸钠。  相似文献   

6.
张利杰  顾银君  马倩  刘勇健 《功能材料》2013,44(11):1588-1592
采用共沉淀法制得Fe3O4溶胶,用γ-缩水甘油醚氧丙基三甲氧基硅烷(KH-560)对其表面进行改性,制得有机硅改性的纳米Fe3O4磁性粒子;用L-半胱氨酸盐酸盐(L-Cys)将油相的CdSe/CdS转成水相并带上氨基的CdSe/CdS纳米晶;将其复合制备了Fe3O4/CdSe/CdS荧光磁性双功能纳米复合物颗粒。该Fe3O4/CdSe/CdS复合物颗粒平均尺寸约为40nm,饱和磁化强度为21.287A.m2/kg,该纳米粒子既具有优异的荧光特性,也具有较强的超顺磁性。  相似文献   

7.
一种高磁含量磁性聚合物粒子的制备方法。属于生物和医学领域。本发明首先合成油酸包缚的Fe3O4粒子的辛烷分散液,其次通过细乳化制备水基磁性聚集体胶束,将油酸包缚的Fe3O4粒子的辛烷分散液在水相中,用十二烷基硫酸钠作为乳化剂、十二醇为助乳剂细乳化,再蒸去辛烷后,得到表面由油酸/十二烷基硫酸钠双层覆盖的水基磁性聚集体。  相似文献   

8.
为制备稳定的水基磁流体,分别以月桂酸、油酸钠、十二烷基苯磺酸钠作为外层表面活性剂,对包油酸的Fe3O4粒子进行了再包覆.将得到的双层包覆的Fe3O4粒子分别分散在水中,发现以十二烷基苯磺酸钠为外层表面活性剂的磁粒子制成的水分散液的稳定性最佳.利用IR研究其吸附机理,结果显示:内层的油酸通过化学键合吸附在磁粒子表面,外层的十二烷基苯磺酸钠通过物理作用吸附在包油酸的Fe3O4粒子表面.  相似文献   

9.
制备了尺寸为30nm,具有磁响应的单分散Fe3O4@SiO2/Au核壳纳米颗粒,并研究其光学性质。首先利用热分解法制备油酸修饰的Fe3O4纳米粒子,再用反相微乳法制备Fe3O4@SiO2纳米粒子,最后利用表面修饰的氨基还原性,获得Fe3O4@SiO2/Au核壳复合纳米颗粒。分别用TEM、XRD、Zeta电位与粒度分析仪对产物形貌、结构、表面电位和粒径分布进行表征,用紫外-可见分光光度计对光学性质进行了测试。  相似文献   

10.
纳米Fe3 O4颗粒改性详析   总被引:12,自引:0,他引:12  
详细解析了Fe3O4纳米颗粒的改性条件,并对表面活性剂的用量进行了理论估算,实验确定了表面活性剂的用量。研究结果表明:pH值对改性效果影响明显,酸性或强碱性环境对改性均不利;油酸和硬脂酸按一定比例混合使用,可提高改性效果;IR图谱显示了油酸的羧基发生了漂移,表明油酸与纳米Fe3O4粒子间存在化学键结合。  相似文献   

11.
K. Zhao  J.F. Feng  H. Li 《Thin solid films》2005,476(2):326-330
La0.67Ca0.33MnO3 (LCMO)/La0.67Sr0.33CoO3 (LSCO)/LCMO trilayer films are fabricated on single-crystal substrates NdGaO3 (110) and the interlayer coupling are investigated. Compared with LCMO single layer, sandwiches showed the enhanced metal-insulator transition temperature of LCMO layers. The magnetoresistance is dependent on spacer thickness and the peak value dramatically decreases when LSCO layer is thick enough because of shorting by the LSCO layer. The magnetic coercivity HC shows a nonmonotonic behavior with changing spacer layer thickness and the waist-like hysteresis indicates that there is an indirect exchange coupling between the top and bottom LCMO layers across the spacer layer.  相似文献   

12.
The varistor properties of the ZnO-Pr6O11-CoO-Cr2O3-Y2O3-In2O3 ceramics were investigated for different concentrations of In2O3. The increase of In2O3 concentration slightly increased the sintered density (5.60-5.63 g/cm3) and slightly decreased the average grain size (3.4-2.9 μm). The breakdown field increased from 6023 to 14822 V/cm with increasing concentration of In2O3. The nonlinear coefficient increased from 17.6 to 44.6 for up to 0.005 mol%, whereas the further doping caused it to decrease to 36.8. In2O3 acted as an acceptor due to the donor concentration, which decreases in the range of 1.02 × 1017 to 0.24 × 1017/cm3 with increasing concentration of In2O3.  相似文献   

13.
Transparent glasses in the system (100−x)Li2B4O7x(SrO---Bi2O3---Nb2O5) (10≤x≤60) (in molar ratio) were fabricated by a conventional melt-quenching technique. Amorphous and glassy characteristics of the as-quenched samples were established via X-ray powder diffraction (XRD) and differential thermal analyses (DTA) respectively. Glass–ceramics embedded with strontium bismuth niobate, SrBi2Nb2O9 (SBN) nanocrystals were produced by heat-treating the as-quenched glasses at temperatures higher than 500 °C. Perovskite SBN phase formation through an intermediate fluorite phase in the glass matrix was confirmed by XRD and transmission electron microscopy (TEM). Infrared and Raman spectroscopic studies corroborate the observation of fluorite phase formation. The dielectric constant (r) and the loss factor (D) for the lithium borate, Li2B4O7 (LBO) glass comprising randomly oriented SBN nanocrystals were determined and compared with those predicted based on the various dielectric mixture rule formalism. The dielectric constant was found to increase with increasing SBN content in LBO glass matrix.  相似文献   

14.
Hollandite-type compounds, Rb2Cr8O16, K2Cr2V6O16 and K2V8O16, were synthesized under high P-T conditions up to 1200°C and 7GPa. The structural refinement using a single crystal of Rb2Cr8O16 confirms that the structure is similar to that of K2Cr8O16. Magnetic measurements indicate that Rb2Cr8O16 is ferromagnetic below 295K, K2Cr2V6O16 paramagnetic down to 77K and K2V8O16 has susceptibility anomaly at 175K. These compounds are all semiconductive and show discontinuities in temperature-resistivity curves at points corresponding to magnetic anomalies.  相似文献   

15.
Phase equilibria along the PbSbBiS4-Sb2S3 and PbSbBiS4-Bi2S3 joins of the PbS-Sb2S3-Bi2S3 system have been studied for the first time using differential thermal analysis, X-ray diffraction, microstructural analysis, microhardness tests, and density measurements, and the phase diagrams of the joins have been mapped out. The joins are shown to be pseudobinary with limited series of terminal solid solutions. The solid solutions are p-type semiconductors.  相似文献   

16.
Epitaxial YBa2Cu3O7/La0.7Ca0.3MnO3 (YBCO/LCMO) bi-layers and La0.7Ca0.3MnO3/YBa2Cu3O7 (LCMO/YBCO) bi-layers were grown on (001)LaAlO3 by pulsed laser deposition, and their microstructures were compared by transmission electron microscopy investigation. In the YBCO(100 nm)/LCMO(150 nm) bi-layers, the LCMO layer consists of columnar grains of ~ 17 nm in diameter and contains mixed orientation domains of [100]c, [010]c and [001]c. The YBCO layer is totally c-axis oriented and the YBCO lattices are tilted − 2.5° to + 2.5° as they grew on the rough surfaces of LCMO columnar grains. For the LCMO(140 nm)/YBCO(140 nm) bi-layers, the LCMO/YBCO interface is sharp and flat. The initial 12-nm thickness of the YBCO layer is composed of c-axis oriented domains, and the upper part of YBCO layer is [100] oriented. The LCMO layer was predominantly [001]c oriented while [100]c-oriented domains were occasionally observed.  相似文献   

17.
A systematic study was performed with mixtures consisting of N2, CH4, C2H6 and C3H8, to investigate experimentally phase equilibria and caloric properties and to test the accuracy of thermodynamic correlations. The first part of this Paper reports results of T---p---x---y measurements on ternary systems in the range 20 < p < 120 bar and 140 < T < 220 K. The results are compared with data calculated by generalized equations of state.  相似文献   

18.
We investigated the structural and superconducting properties ofc-axis oriented (YBa2Cu3O7) nY /(PrBa2Cu3O7) npr superlattices with thicknesses of the individual layers down to one unit cell (10nY1; 18>nPr 1). By transmission electron microscopy and X-ray diffraction we find an excellent structural quality of the samples, though the quantitative analysis shows the existence of defects. In superlattices with decoupled YBa2Cu3O7 layers of two unit cell thickness we find a highT c value of 75 K. We probed the flux line structure in the superlattices by measurements of the critical current density in magnetic fields. The experiments show that the flux-line dynamics is dominated by the movement of pancake vortices.  相似文献   

19.
Sr0.3Ba0.7Nb2O6 (SBN) and La0.030Sr0.255Ba0.700Nb2O6 (LSBN) ceramic compounds have been prepared using the traditional ceramic method at two different calcination temperatures (900 and 1000 °C) and later sintered both at 1400 °C. A study of the effects of the calcination temperatures and La substitution on the morphological, compositional, and structural properties of SBN and LSBN is presented using scanning electronic microscopy (SEM), energy dispersive spectroscopy (EDS), and X-ray diffraction (XRD) analysis. From Rietveld refinement processes, the XRD patterns were interpreted to evaluate such effects in the structural parameters and the site occupation factors of the heavy metals and oxygen atoms. The effect of the incorporation of La resulted in a 0.25% cell contraction and turned out to be higher than the 0.08% dilation effect produced by the increase of calcination temperature. The La ion with similar effective ionic radius and higher electronegativity is incorporated into the structure occupying the A1 site just like the Sr ions in the SBN compound. Differences in the site occupation factors between the SBN and LSBN samples lead to substantial changes in the physical properties such as temperature of relative dielectric constant maximum, relative dielectric constant, and dielectric loss, correlated with the distortion and the relative orientation of the oxygen octahedra.  相似文献   

20.
Bi1.5Zn0.5Nb0.5Ti1.5O7 (BZNT) thin films with different thicknesses as cover layers were deposited on the Ba0.6Sr0.4TiO3 (BST) thin films on the Pt/Ti/SiO2/Si substrates by radio frequency magnetron sputtering method. The microstructure, surface morphology, dielectric and tunable properties of BST/BZNT heterogeneous bilayered films were investigated as a function of the thickness of BZNT films and the effect of BZNT films on the asymmetric electrical properties of BST/BZNT bilayered films was discussed. It was found that BZNT cover layer significantly improved the leakage current and the dielectric loss, and the dielectric constant and tunability of BST/BZNT bilayered thin films simultaneously decreased with the increasing thickness of BZNT films. The BST/BZNT bilayered thin film with a 50 nm BZNT cover layer gave the largest figure of merit (FOM) of 33.48 with the upper tunability of 55.38%. The asymmetric electrical behavior of BST/BZNT bilayered films is probably related to an internal electric field caused by built-in voltages at Pt/BST and BZNT/Au interfaces.  相似文献   

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