LaAl1-xFexO3/Al2O3/FeCrAl催化剂的制备及其对甲烷燃烧的催化性能

 以FeCrAl合金薄片为载体,以LaAl1-xFexO3为活性组分,以Al2O3为过渡层,制备了LaAl1-xFexO3/Al2O3/FeCrAl金属基整体式催化剂,并用XRD和SEM等方法对催化剂的物相和形貌进行了表征,对催化剂上甲烷催化燃烧活性进行了评价. 结果表明,催化剂物相中有LaAl1-xFexO3型钙钛矿及 α-Al2O3 和 γ-Al2O3; 催化剂的颗粒小于2 μm, 并且颗粒的尺寸及形貌与LaAl1-xFexO3中的Fe/Al摩尔比有关; 催化剂样品对甲烷催化燃烧活性的大小顺序为LaAl0.3Fe0.7O3/Al2O3/FeCrAl＞LaFeO3/Al2O3/FeCrAl＞LaAl0.5Fe0.5O3/Al2O3/FeCrAl＞LaAl0.7Fe0.3O3/Al2O3/FeCrAl＞LaAlO3/Al2O3/FeCrAl.     

沉淀铁催化剂在F-T合成反应过程中的物相变化

 采用元素分析、X射线衍射和穆斯堡尔谱等手段研究了喷雾干燥沉淀Fe-Cu-K/SiO2催化剂在F-T合成反应过程中的物相变化. 结果表明,新鲜催化剂样品主要由α-Fe2O3组成,且81.1%的α-Fe2O3粒径小于13.5 nm. 随着反应时间的延长,催化剂表面碳沉积物的含量逐渐增多,不饱和度逐渐增大; χ-Fe5C2的含量逐渐增多,Fe3O4的含量逐渐减少并趋于稳定. 超顺磁Fe3+的含量呈先增加后减少的变化趋势. 由于碳沉积物是由CO生成的,而χ-Fe5C2是由α-Fe2O3经Fe3O4生成的,故催化剂表面碳沉积物的生成先于χ-Fe5C2的生成.     

Al掺杂α-Fe2O3材料的制备、表征和气敏特性

采用均相沉淀法制备了纯α-Fe2O3(300 ℃煅烧)和Al掺杂α-Fe2O3(300和400 ℃煅烧), 使用SEM, XRD, ICP和红外光谱等手段进行表征, 并利用气敏仪测试无水乙醇和90＃汽油在不同条件下对材料的响应性能. 结果表明, 微量Al掺杂不改变α-Fe2O3材料的物相, 但会阻碍晶粒生长, 使颗粒变小及Fe2O3晶格间隙中的铁原子数目增多, 材料的导电率增大, 从而显著提高材料的气敏性能. Al掺杂α-Fe2O3对乙醇的响应性能优于对汽油的响应性能, 在乙醇气氛中, 材料对湿度仍然不敏感. 经400 ℃煅烧的Al掺杂α-Fe2O3稳定性较好, 可作为检测乙醇气体的半导体气敏材料.     

γ′-Fe_4N纳米晶薄膜的磁性及热稳定性研究

采用直流磁控溅射方法,在Si(100)单晶衬底上获得了γ′-Fe4N纳米晶薄膜样品.将样品在真空中分别于300,400,500,600,700和800℃下进行热处理,利用XRD,SEM和VSM等测试手段对样品的结构、形貌和磁性进行表征.结果表明,热处理温度在300～500℃时,在γ′-Fe4N纳米晶粒的界面处形成了Fe8N包裹层,600℃时,Fe8N包裹层转变为α-Fe,当热处理温度≥700℃时,样品全部转变为α-Fe.γ′-Fe4N薄膜样品在600℃以下温度热处理可保持其主相γ′-Fe4N的结构稳定,而其软磁性能并未发生明显的减弱.     

高温煤气脱硫 Ⅰ.铁基脱硫剂的相态特征和活性

用穆斯堡尔谱考察了氧化铁脱硫剂在高温煤气中还原及硫化时的铁形态变化规律。在反应开始阶段，原脱硫剂中的α-Fe2O3即被迅速还原成Fe3O,Fe3O4可进一步还原转化成α-Fe。反应初期Fe3O4和α-Fe都参与脱硫反应，其中α-Fe具有较高的脱硫活性，对整个脱硫过程而言α-Fe是主要的脱硫活性相。铁化合物与硅铝氧化物载体间存在相互作用，形成磁微 晶颗粒及少量γ-Fe。在高温煤气条件下，FeS是唯一的铁硫化物，θ－Fe3C则是α－Fe转化中的主要产物。适量的θ－F e3C对脱硫有促进作用。     

不同晶化度γ-FeOOH的合成及其液相转化研究

进行了空气氧化Fe(OH)2悬浮液, EDTA作用下可见光诱导, 不同温度(14～20 ℃)制备不同晶化度γ-FeOOH的研究, 进行了其沸腾回流液相转化历程的探讨. 结果表明: 随温度的升高, γ-FeOOH的晶化程度变差; 而γ-FeOOH的晶化程度越差, 在液相沸腾回流时就越易转化成α-Fe2O3, 反之则易转化为α-FeOOH. 在pH近中性, 微量Fe(II)存在条件下低晶态的γ-FeOOH可以快速转化为均匀球形的α-Fe2O3.     

不同制备方法和反应条件对Fe_2O_3形貌和晶型转变的影响

研究了吸附相反应技术、浸渍法以及沉淀法制备Fe2O3的过程中,反应环境的变化对粒子形貌和晶型转变过程的影响。当吸附层是主要反应场所时,生成的粒子与SiO2表面以较强的化学键键合,焙烧过程中Fe2O3的晶型变化和粒子团聚被有效地抑制,焙烧后Fe2O3粒子维持稳定的γ-Fe2O3晶型和高分散的小粒子。而在乙醇体相中反应生成的粒子,仅通过物理作用与SiO2表面结合,不能有效抑制其向α-Fe2O3晶型的转变和粒子的团聚。吸附相反应制备过程中,当水量持续增加或者体系温度升高,反应环境逐渐从吸附层向乙醇体相中转变,SiO2对Fe2O3晶型转变的抑制作用减弱,从而导致样品中逐渐出现α-Fe2O3晶型。     

纳米Al2O3颗粒对纯Fe液诱导凝固过程的分子动力学模拟

采用分子动力学(MD)方法模拟了不同半径大小的纳米Al2O3颗粒夹杂在三个温度下(1750、1730和1710K)对纯Fe液的诱导凝固过程,并分析了作为诱导核心的纳米Al2O3颗粒的结构演变及其对Fe原子体系的凝固过程的影响.发现在诱导过程中,纳米Al2O3颗粒的内部保持较好的晶型结构,仅表面原子有结构变形;诱导凝固的Fe原子主要为面心立方(fcc)和密排六方(hcp)原子;纳米Al2O3颗粒的尺寸越大,发生诱导凝固的温度越高;诱导凝固得到的Fe晶体的晶格取向受纳米Al2O3颗粒在Fe液中的漂移程度影响.     

添加Al2O3对Ni0.5Zn0.5Fe2O4纳米纤维结构和磁性能的影响

采用静电纺丝技术制备了添加0～20wt%Al2O3的Ni0.5Zn0.5Fe2O4纳米纤维。通过XRD、FESEM、TEM和VSM对样品的物相结构、形貌和磁性能进行了表征。结果表明,所合成的复合纳米纤维的直径都分布在40～150 nm之间,添加到纤维中的Al2O3主要以非晶态形式分布于铁氧体晶粒边界;随着Al2O3添加量的增加,可观察到γ-Fe2O3相逐渐析出,Ni-Zn铁氧体的晶格常数单调减小,说明有一些Al2O3进入到尖晶石晶格中取代了B位的Fe3+离子,Ni-Zn铁氧体的平均晶粒尺寸先增大后减小,在Al2O3添加量为8wt%时达到最大值39.2 nm;比饱和磁化强度和矫顽力随Al2O3添加量的增加呈现出相同的变化规律,先减小后增大,当Al2O3添加量超过5wt%时又开始变小。     

低温燃烧法合成掺钕钇铝石榴石（Nd：YAG）纳米粉末

以Nd2O3,Y2O3,Al(NO3)3·9H2O,氨水和柠檬酸为原材料,采用低温燃烧法合成出分散均匀、团聚轻的掺钕钇铝石榴石(Nd∶YAG)纳米粉末,该方法有效地解决了固相合成的高反应温度以及化学沉淀法的颗粒团聚问题。采用TG-DTA,XRD,FT-IR和TEM测试手段对纳米粉末进行了表征,同时测量了(Nd0.01Y0.99)3Al5O12陶瓷素胚以及烧结体的荧光发射光谱。研究结果表明:YAG晶相的形成温度为850℃,在煅烧过程中出现YAP中间相,并于1050℃完全转化为YAG晶相。采用低温燃烧法合成的粉末材料其颗粒尺寸随热处理温度的不同在20~50nm范围波动。(Nd0.01Y0.99)3Al5O12陶瓷体的有效激发发射截面积(σin)为4.03×10-19cm2,比同组成的单晶高44%。     

Fe3O4的X射线微结构特征与催化活性间的关系

湿法工艺制备的不同晶型Fe2O3, 经水煤气还原后Fe3O4的X射线衍射微结构特征, 用分析微应变和晶粒尺寸的Voigt函数单峰分析法进行了测定。Fe3O4微应变大小同催化活性间存在一种对应关系。γ-Fe2O3还原的Fe3O4比α型还原的有更大的晶格畸变, 在325℃, 500空速条件下, CO转化率达97%以上, 比后者高出30%多。这种畸变结构在工业催化反应条件下能长期稳定, 但经600℃高温处理后, 畸变减小,活性下降。湿法工艺可以获得具有不同活性的Fe3O4前身, γ-Fe2O3与Fe3O4晶体结构上的类似, 使它在还原过程中, 能把这种高活性的结构状态保留下来。     

基于溶液配位化学过程调控的中空单晶氧化铁纳米材料

本文简要综述了本课题组近年来在单晶氧化铁空心纳米结构制备与生长机理研究方面的相关工作.通过采用磷酸根与硫酸根的双阴离子调节,结合反应时间、反应温度等条件的改变,实现了对α-Fe2O3单晶空心纳米结构形貌、尺寸和表面结构的良好调控,并提出一种针对非层状结构纳米环/纳米管新颖生长机理,即"配位辅助的定向溶解机理".以所制备的α-Fe2O3为前驱体,采用气相还原方法,成功制备得到了系列单晶Fe3O4和γ-Fe2O3管状及环状纳米结构,并对单个Fe3O4纳米环的磁学行为进行了考察.     

A 3D α-Fe2O3 nanoflake urchin-like structure for electromagnetic wave absorption

An α-Fe(2)O(3) nanoflake urchin-like structure is formed via the thermal oxidation of micrometre-sized iron spheres in air at temperatures of 300-400 °C. The material consists of α-Fe(2)O(3) nanoflakes grown perpendicularly to the sphere surface, a layer of a mixture of α-Fe(2)O(3) and Fe(3)O(4) as the oxidation shell, and an iron core. The ranges of the tip diameters of the nanoflakes are 20-30 nm (300 °C), 30-50 nm (350 °C), and 60-100 nm (400 °C). A composite consisting of the α-Fe(2)O(3) nanoflake urchin-like structure and an epoxy resin exhibits an excellent electromagnetic (EM) wave absorption ability. A small tip diameter (20-30 nm) and a high density (3 × 10(13) nanoflakes m(-2)) lead to a good network structure and good EM wave absorption. A minimum reflection loss (RL) of -33.8 dB (99.93% of EM wave absorption) at 7.8 GHz can be achieved using a 70 wt% urchin-like material as the filler in the resin matrix. In addition, a composite containing 60 wt% unchin-like material exhibits dual-frequency EM wave absorption. The peaks of the minimum RL values are located at 9.7 GHz (-26.2 dB) and 25.2 GHz (-21.0 dB). The unique morphology of the α-Fe(2)O(3) nanoflake urchin-like material is believed to be a key factor in the enhancement of the EM wave absorption.     

γ-Fe(2)O(3) and Fe(3)O(4) magnetic hierarchically nanostructured hollow microspheres: Preparation, formation mechanism, magnetic property, and application in water treatment

In this paper, we report the preparation of γ-Fe(2)O(3) and Fe(3)O(4) magnetic hierarchically nanostructured hollow microspheres by a solvothermal combined with precursor thermal conversion method. These γ-Fe(2)O(3) and Fe(3)O(4) magnetic hierarchically nanostructured hollow microspheres were constructed by three-dimensional self-assembly of nanosheets, forming porous nanostructures. The effects of experimental parameters including molar ratio of reactants and reaction temperature on the precursors were studied. The time-dependent experiments indicated that the Ostwald ripening was responsible for the formation of the hierarchically nanostructured hollow microspheres of the precursors. γ-Fe(2)O(3) and Fe(3)O(4) magnetic hierarchically nanostructured hollow microspheres were obtained by the thermal transformation of the precursor hollow microspheres. Both γ-Fe(2)O(3) and Fe(3)O(4) hierarchically nanostructured hollow microspheres exhibited a superparamagnetic property at room temperature and had the saturation magnetization of 44.2 and 55.4emu/g, respectively, in the applied magnetic field of 20 KOe. Several kinds of organic pollutants including salicylic acid (SA), methylene blue (MB), and basic fuchsin (BF) were chosen as the model water pollutants to evaluate the removal abilities of γ-Fe(2)O(3) and Fe(3)O(4) magnetic hierarchically nanostructured hollow microspheres. It was found that γ-Fe(2)O(3) hierarchically nanostructured hollow microspheres showed a better adsorption ability over SA than MB and BF. However, Fe(3)O(4) hierarchically nanostructured hollow microspheres had the best performance for adsorbing MB.     

γ-Fe2O3纳米粉的低热固相制备及其电磁损耗特性(英)

The Fe(OH)₃ precursor was prepared by solid -state reaction with Fe(NO₃)₃·9H₂O, NaOH and dispersed poly-ethylene glycol at low heating temperature(25 ℃). Synthesis of iron oxide (γ-Fe₂O₃) nanoparticle was achieved by thermal decomposition of Fe(OH)₃·xH₂O precursor. The nanoparticle was characterized by TG-DTA, X-ray diffra-ction, TEM etc. The results showed that the nanoparticle was composed of γ-Fe₂O₃ and was a better absorber for electromagnetic wave within the low frequency band.     

Iron oxyhydroxide nanoparticles formed by forced hydrolysis: dependence of phase composition on solution concentration

Nanoparticles of single-phase lepidocrocite (γ-FeOOH) and goethite (α-FeOOH) have been synthesized by forced hydrolysis of ferric nitrate with no other additives, and the particles have been characterized by XRD, FT-IR and TEM. At low Fe(NO(3))(3) concentrations the hydrolysis product is predominantly γ-FeOOH, while at high concentrations it is α-FeOOH. These particles are nanometers in size and fall within narrow particle size distributions. The dependence of the oxyhydoxide phase on ferric nitrate concentration is attributed to two thermodynamic factors, the enthalpy of formation and the surface enthalpy of hydration at the oxide-water interface (which is a function of surface area). Two potential mechanisms for the phase-specific growth are proposed that explain the solution concentration dependence of the phase formed. Three other common nanoscale particles (α-Fe(2)O(3), Fe(3)O(4) and γ-Fe(2)O(3)) have also been prepared by relatively simple thermal/chemical treatment of the γ-FeOOH nanoparticles.     

Quasiemulsion-templated formation of α-Fe2O3 hollow spheres with enhanced lithium storage properties

α-Fe(2)O(3) hollow spheres with sheet-like subunits are synthesized by a facile quasiemulsion-templated method. Glycerol is dispersed in water to form oil-in-water quasiemulsion microdroplets, which serve as soft templates for the deposition of the α-Fe(2)O(3) shell. When tested as anode materials for lithium-ion batteries, these α-Fe(2)O(3) hollow spheres manifest greatly enhanced Li storage properties.     

Reaction products and kinetics of the reaction of NO2 with γ-Fe2O3

The reaction of NO(2) with Fe(2)O(3) has relevance for both atmospheric chemistry and catalysis. Most studies have focused on hematite, α-Fe(2)O(3), as it is the thermodynamic stable state of iron oxide; however, other forms of Fe(2)O(3) naturally occur and may have different chemistries. In this study, we have investigated the reaction products and kinetics for NO(2) reacting with γ-Fe(2)O(3) powder using diffuse reflectance infrared Fourier transform spectroscopy and compared the results to those of previous studies of NO(2) reacting with α-Fe(2)O(3). Both α- and γ-Fe(2)O(3) produce surface-bound nitrate at the pressures examined in this study (24-212 mTorr); surface-bound nitrite products are observed at all pressures for γ-Fe(2)O(3) whereas nitrite was only observed on α-Fe(2)O(3) at lower pressures. Surface-bound NO(+) and Fe-NO products are observed on γ-Fe(2)O(3), which have not been observed with α-Fe(2)O(3). The reaction kinetics show a first-order dependence on NO(2) pressure and this is used to support the hypothesis of unimolecular reaction of adsorbed NO(2) with the γ-Fe(2)O(3) surface as the slow step in the reaction mechanism. The difference in product formation between NO(2) reacting with γ-Fe(2)O(3) and previous studies of α-Fe(2)O(3) illustrate the fact that care must be taken in generalizing reactivity of different polymorphs.     

Morphology- and phase-controlled iron oxide nanoparticles stabilized with maleic anhydride grafted polypropylene

About phase: Ferromagnetic γ-Fe(2) O(3) nanowires (left in the figure) with a saturation magnetization (M(s) ) of 54.0?emu?g(-1) and coercivity of 518?Oe at room temperature, and superparamagnetic hollow α-Fe(2) O(3) nanoparticles (right) with a room-temperature M(s) of 2.9?emu?g(-1) were synthesized by the thermal decomposition of [Fe(CO)(5) ] but with the stabilizing action of maleic anhydride grafted polypropylene.