铁氧化物/草酸/UVA体系中2-硫醇基苯骈噻唑的光化学降解

 用水热法合成纯γ-FeOOH粉末, 然后分别在250, 320, 420和520 ℃下煅烧得到IO-250等4种铁氧化物. XRD结果表明, 煅烧后得到的IO-250和IO-320为γ-Fe2O3和α-Fe2O3混合相, IO-420和IO-520为纯α-Fe2O3相. N2吸附结果表明, 随煅烧温度升高,铁氧化物比表面积减小. 铁氧化物与草酸悬浮液在紫外光照射下建立了一个铁氧化物/草酸/长波紫外线(UVA)类光Fenton体系,以2-硫醇基苯骈噻唑(MBT)为目标污染物测试了该体系的催化活性. 结果表明, 该体系能有效降解MBT, 不同铁氧化物组成的体系光化学活性依次为IO-320＞IO-250＞IO-420＞IO-520＞γ-FeOOH. 铁氧化物剂量和草酸的初始浓度显著影响体系的光化学活性,不同铁氧化物最佳剂量不同; 草酸能显著促进MBT光化学降解, 在各体系中其最佳浓度均为1.0 mmol/L. 反应过程中Fe2+和Fe3+的浓度及溶液pH值的变化均与铁氧化物的种类和草酸的初始浓度有关.     

低温下Fe(II)对Ferrihydrite相转化的催化作用研究

研究了在低温、近中性条件下,在微量Fe(II)离子存在下Ferrihydrite(又称为水合氧化铁hydrousironoxide)的相转化过程.结果表明,微量Fe(II)离子的存在不仅可以加速Ferrihydrite的相转化过程,而且其相转化产物的组成也与没有Fe(II)离子存在时产物的组成有所不同,即除了α-FeOOH和α-Fe2O3外,还形成了γ-FeOOH;相转化过程既与阴离子的种类、反应温度、反应时间等因素有关,也与Fe(II)离子存在状态有关;Fe(II)离子通过催化Ferrihydrite的溶解过程,从而加速整个相转化过程.对该过程的深入研究将对认识和了解自然条件下铁氧化物的形成与相互转化具有重要意义.     

球形α-Fe2O3纳米粉体的超声水解法合成与表征

0引言纳米Fe2O3因在磁性、气敏、催化、染料、抗腐蚀等领域显示出广阔的应用前景而备受瞩目[1￣3]。Fe2O3存在α-Fe2O3、β-Fe2O3、γ-Fe2O3、ε-Fe2O3等多种构型,它们在性能上差异较大,如α-Fe2O3具有良好的磁性和气敏性,可用作气敏材料和磁记录材料;γ-Fe2O3具有独特的电、磁、光等性质而在信息存贮器、彩色显像管、生物处理、磁制冷等方面得到广泛应用。由于其各种应用都与性能有直接关系,所以研究Fe2O3的制备方法具有重要意义。尽管不少学者采用溶胶-凝胶法[4]、电化学合成法[5]、微波辐射法[6]、燃烧合成法[7]、水热法等[8]不…     

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.     

纳米铁氧化物合成的实验设计

设计了一个不同纳米铁氧化物（α-FeOOH、γ-FeOOH、α-Fe2O3、Fe3O4）合成的简单方法,该方法可用于中级无机化学实验中,使学生掌握纳米材料常见的合成方法及表征手段,有利于学生实践能力和创新能力的提高。     

气相色谱法研究配位化合物的热稳定性IX.Fe2(C2O4)3一HZSM一5和Fe2(C2O4)3一HY的热分解

本文研究了早酸铁(III)负载在HZSM-5和HY沸石上的性质和热分解,早酸铁(III)在沸石表面发生离解吸附,C2O[2-][4]与表面的Al配位,热分解时产生β峰,草酸铁(III)与HZSM-5沸石作用较弱,在氢气中500℃时的还原产物为α-Fe,而Fe2(C2O4)3-HY体系在氢气中500℃时除得到α-Fe外,还有少量高分散的零价铁和部分难以还原的铁离子。     

单分散α-Fe_2O_3纳米结构空心亚微球的制备及表征

采用一种新的溶液生长法结合多步包覆法在自制的不同粒径SiO2单分散亚微球表面包覆不同厚度的β-FeOOH涂层,得到单分散β-FeOOH/SiO2核壳结构亚微球.实验结果表明,SiO2核心颗粒尺寸对表面涂层的形态和包覆均匀性有很大影响.当SiO2核心颗粒的平均粒径为250 nm左右时,β-FeOOH表面涂层均匀,颗粒间团聚较少,一次包覆后涂层厚度约为35 nm.涂层中β-FeOOH纳米棒的尺寸随着所选SiO2核心颗粒粒径的增大而相应增大.经多次包覆能够显著提高涂层的厚度,3次包覆后β-FeOOH表面涂层厚约100 nm.β-FeOOH/SiO2核壳结构亚微球与质量分数5%的NaOH溶液反应后,于600℃焙烧2 h得到了单分散α-Fe2O3空心微球.单分散α-Fe2O3空心亚微球表层是由α-Fe2O3纳米棒搭建而成的三维网络结构,α-Fe2O3纳米棒的尺寸与核壳结构中β-FeOOH纳米棒的尺寸基本一致.     

均分散超微细α-Fe2O3水溶胶的制备

均分散微米、亚微米或纳米级α-Fe_2O_3的制备包括静态水解法［1－3］、沸腾回流水解法[4]以及微乳液反应法[5]．随着粒子尺寸的减少,则体系具有明显的表面和体积效应[6]以及光电化学性质[7]．预计均分散超微细α-Fe_2O_3将会在催化、材料等许多新技术领域获得重要的应用．但以FeCl3为原料的水解法,Fb3十浓度一般在0．02－0．04mol·L－1很窄的浓度范围之内,超出该浓度范围将得到足β-FeOOH而不是α-Fe_2O_3[8]．以Fe（NO3）3为原料,虽然Fe3十浓度可增至0．2mol·L－1,但随之而来的不利因素：（1）水解时间增加几倍;（2）产率…     

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。     

一步水热法合成三种形貌纳米α-Fe2O3的机理及磁性能研究（摘要）

纳米α-Fe2O3以其优良的生物相容性、环境友好性、稳定性、催化性、以及磁性被广泛的应用于生物医学、颜料、催化、传感以及半导体等领域.为了实现不同形貌纳米α-Fe2O3的工业化可控合成,我们采用一步水热法,通过控制体系的反应时间,依次制备出了纺锤体状、管状和轮胎状的α-Fe2O3纳米结构,并利用X射线衍射仪、扫描电子显微镜和透射电子显微镜对产物进行了表征.体系中磷酸根离子在α-Fe2O3晶面上的特异性吸附是主导α-Fe2O3形貌演进的关键性因素.其作用主要体现在两个方面：一是使α-Fe2O3颗粒产生各向异性生长,形成纳米纺锤体;二是阻止某些晶面参与质子轰击反应,形成α-Fe2O3纳米管,进而促进体系中Fe4（PO4）3（OH）3相的形成与α-Fe2O3相的再结晶,最终形成轮胎状纳米结构.通过超导量子干涉仪对产物的磁性能表征,发现产物的不同形貌以及形状各项异性会对矫顽力、磁化强度以及低温磁性相变温度等磁学参量产生显著的影响.     

α-Fe(Ga)OOH的液相催化合成及表征

采用液相催化相转化法, 以Fe(III)与Ga(III)的共沉淀为前驱物合成了α-Fe(Ga)OOH微粒. 探讨了镓离子的掺杂浓度和Fe(II)离子用量等因素对合成α-Fe(Ga)OOH微粒的影响, 并对产物进行了X射线衍射(XRD)、红外光谱(IR)、扫描电镜(SEM)、透射电镜(TEM)、电子衍射(ED)表征. 结果表明: 初始pH＝9, nFe(II)/nFe(III)＝0.02, nGa(III)/nFe(III)＝0.18时, 在沸腾回流条件下可制备出类多面体形的α-Fe(Ga)OOH微粒, 镓离子的掺杂对α-FeOOH的形成起了形貌调控作用, 电子衍射数据表明该α-Fe(Ga)OOH为单晶粒子.     

纺锤形β-FeOOH纳米结构和α-氧化铁亚微米/微米粒子的合成与转变

使用一种简易的无表面活性剂辅助的水热合成方法,在温度为140 ℃时实现了纺锤形β-FeOOH纳米结构向α-氧化铁亚微米/微米粒子的转变。研究表明,通过实验参数的简单调控,实现了单晶α-氧化铁亚微米粒子与β-FeOOH的纺锤形纳米结构和纳米棒的控制制备。基于实验结果,提出了该过程中的相转变机理。     

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.     

Rechargeable battery using a novel iron oxide nanorods anode and a nickel hydroxide cathode in an aqueous electrolyte

A rechargeable battery using novel α-Fe(2)O(3)/CNFs composite as the anode, β-Ni(OH)(2) as the cathode and LiOH/KOH solution as the electrolyte in an aqueous rechargeable battery has been proposed. The Fe(2)O(3)/Ni(OH)(2) prototype cell exhibits a high average operational voltage of 1.5 V, high rate capability and good cycling performance.     

Fe(OH)2悬浮液在EDTA作用下氧气氧化生成δ-FeOOH的机理研究

At room temperature and in the presence of trace EDTA, the formation of δ-FeOOH was studied by the rapid oxidation of Fe(OH)2 suspension with O2. The structural and morphological changes were characterized by various techniques such as XRD, FTIR and TEM. γ-FeOOH and (δ-FeOOH) formed simutaneously in the early period of oxidation. But as the rate of mass transfer was in equilibrium, trace (γ-FeOOH) vanished gradually. Accordingly, pure phase δ-FeOOH was obtained. At the same time, critical amount ratio K of EDTA to Fe2+ was verified. The experiments show that the reactivity, rate of the oxidizing agent and pH of the initial medium were important factors for the formation of pure phase (δ-FeOOH). Under the auxiliary effect of EDTA, the reactivity of O2 was nearly improved to that of H2O2. And the process of the oxidation that Fe(OH)2 suspension was oxidized by O2 under that condition was discussed.     

Rational solution growth of α-FeOOH nanowires driven by screw dislocations and their conversion to α-Fe2O3 nanowires

We report the rational synthesis of α-FeOOH (goethite) nanowires following a dislocation-driven mechanism by utilizing a continuous-flow reactor and chemical equilibria to maintain constant low supersaturations. The existence of axial screw dislocations and the associated Eshelby twist in the nanowire product were confirmed using bright-/dark-field transmission electron microscopy imaging and twist contour analysis. The α-FeOOH nanowires can be readily converted into semiconducting single-crystal but porous α-Fe(2)O(3) (hematite) nanowires via topotactic transformation. Our results indicate that, with proper experimental design, many more useful materials can be grown in one-dimensional morphologies in aqueous solutions via the dislocation-driven mechanism.     

Formation and transformation kinetics of amorphous iron(III) oxide during the thermally induced transformation of ferrous oxalate dihydrate in air

Focusing on the formation and transformation of amorphous Fe(2)O(3) in the course of the thermally induced transformations of ferrous oxalate dehydrate in air, the kinetics and physico-geometric mechanisms of the respective reaction steps were investigated systematically by means of thermoanalytical methods, complemented by other techniques. The final product of α-Fe(2)O(3) is produced by heating the sample to 700 K via intermediates of poorly crystalline anhydrous FeC(2)O(4) and amorphous Fe(2)O(3), where the external shape and size of the original sample particles are retained during the overall course of reactions. The initial parts of all the three distinguished reaction steps, that is, thermal dehydration of crystalline water, oxidative decomposition of anhydrous FeC(2)O(4) and crystallization of amorphous Fe(2)O(3), are controlled kinetically by the formation or reconstruction of the surface product layers. The surface product layers play important roles of regulating the physico-geometric kinetic behavior of the established parts of the reactions. The oxidative decomposition of intermediate anhydrous FeC(2)O(4), characterized as the formation process of amorphous Fe(2)O(3), arrests in the final stage of the reaction. The as-produced amorphous Fe(2)O(3), protected probably by the outer shell of the surface product layer and the residual anhydrous FeC(2)O(3), crystallizes to α-Fe(2)O(3) being induced by the surface crystallization. Aiming to contribute notably toward provision of the establishment of the novel fabrication routes of nanosized iron oxides by the controlled crystallization of amorphous Fe(2)O(3), the possible factors controlling and/or affecting the formation and transformation kinetics of amorphous Fe(2)O(3) were discussed.     

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.     

氧化铁和羟基氧化铁光催化还原银离子

在波长λ≥320 nm的紫外灯照射下, 水溶液中的银离子能在氧化铁和羟基氧化铁催化剂表面发生还原反应而生成颗粒银. 在这些催化剂上, Ag(I)的等温吸附线都符合Langmuir吸附方程; Ag(I)的初始还原速率均随其初始吸附量的增加而线性增大, 并且增大的幅度依α-Fe2O3>α-FeOOH>γ-Fe2O3>γ-FeOOH>δ-FeOOH的顺序降低. 但是, 在前三种催化剂上, 只有当Ag(I)的吸附量达到其饱和吸附量的一半时, Ag(I)的还原才能发生, 并且几乎不受氮气的影响. 在δ-FeOOH和TiO2体系中通入氮气, 能显著加快Ag(I)的光催化还原. 这说明O2与Ag(I)竞争催化剂上的吸附位点和还原物种, 且与催化剂的性质有关. XRD分析表明, α-Fe2O3和δ-FeOOH分别具有较好和较差的结晶度. 这说明氧化铁和羟基氧化铁的结晶度越高, 越有利于光生载流子的分离及其与表面目标物种发生氧化还原反应.