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1.
以P123为模板剂,采用溶胶-凝胶的溶剂热合成方法制备了H3PW12O40掺杂TiO2介孔材料H3PW12O40/TiO2.利用紫外可见漫反射吸收光谱(UV-vis/DRS)、X射线粉末衍射(XRD)、N2吸附和透射电子显微镜(TEM)手段对所制备的材料进行结构表征,罗丹明B(RB)为模型污染物评价其光催化性能.结果表明,所制备的介孔材料具有锐钛矿与板钛矿复合的晶型结构、大的BET比表面积和孔径均匀分布的介孔结构.光催化实验表明,H3PW12O40/TiO2可将罗丹明B完全矿化.  相似文献   

2.
利用螯合剂乙二胺四乙酸二钠(EDTA-Na2)作为致孔剂,以三氯化钛(TiCl3)为前驱体.利用水热法直接合成了氮掺杂的纳米多孔TiO2.通过SEM、XRD、IR、低温N2吸附-脱附、XPS、热重分析(TG)和紫外可见(UV)光谱对样品进行了表征与分析.结果表明所合成TiO2以锐钛矿相形式存在,氮掺在TiO2晶面之间,具有典型的介孔结构和较高的比表面积,通过改变EDTA-Na2的浓度,比表面积口1控制在95~216 m2·g-1之间.这种纳米多孔TiO2在光降解甲基橙的实验中表现出很好的光催化活性,且随着EDTA-Na2的浓度增大而逐渐增加.  相似文献   

3.
酸法纳米纤维素模板剂合成介孔TiO2及光催化活性   总被引:1,自引:0,他引:1  
以生物可再生资源的酸法纳米纤维素为模板剂,四氯化钛为钛源,采用液相水解-沉淀法制备了具有介孔结构的TiO2光催化剂。采用低温N2物理吸附-脱附、透射电镜(TEM)、X射线衍射(XRD)、热重-量热扫描(TG/DSC)、傅里叶变换红外(FTIR)、X射线光电子能谱(XPS)等对介孔TiO2进行了表征,并以甲基橙为模型物,考察了介孔TiO2光催化活性。结果表明,以酸法纳米纤维素为模板剂合成的TiO2光催化活性显著提高,且具有良好的孔隙结构,平均孔径5.03 nm、总孔容积0.35 cm3.g-1、比表面积192m2.g-1;纤维素模板剂合成的TiO2表面羟基数量降低;纤维素长链分子结构之间的羟基与TiO2表面羟基的键合,可有效限制TiO2前驱体的生长和团聚,并抑制锐钛矿相TiO2向金红石相转变。  相似文献   

4.
掺杂TiO2介孔材料的合成与表征   总被引:2,自引:0,他引:2  
基于溶胶-凝胶过程, 以非表面活性剂有机小分子三乙醇胺为模板剂, 合成了TiO2及Fe3+/V5+-TiO2介孔材料. 利用XRD, TEM, BET, UV-Vis DRS等手段表征了材料的结构、形貌、比表面积、孔径分布及吸光性能. 研究结果表明, 用乙醇萃取法脱除模板剂可形成具有蠕虫状孔道结构的TiO2介孔材料, 而利用焙烧法在450 ℃脱除模板剂时可引起孔道的塌陷. 掺杂Fe3+或V5+可稳定材料的介孔结构, 适宜的掺杂摩尔分数为0.5%. 于450 ℃下焙烧后, 掺杂Fe3+/V5+的TiO2的平均孔径分别为10.5和9.6 nm, 比表面积分别达到103.59和90.80 m2/g. 相对于P25光催化剂, 掺杂Fe3+或V5+的TiO2吸光带边红移至可见光区, 说明掺杂离子在此合成过程中可有效地进入TiO2的晶格结构而引起其微观电子结构的改变.  相似文献   

5.
La掺杂TiO2光催化剂的制备与表征   总被引:5,自引:0,他引:5  
用共沉淀法和溶胶-凝胶法制备了La掺杂TiO2光催化剂(La3 -TiO2),并以罗丹明B为模型反应物,进行了光催化降解实验.结果发现,共沉淀法制备的La3 -TiO2具有较高的光催化活性,当掺La量为1.0%、于800℃煅烧2 h时获得的催化剂活性最佳.用X射线衍射、N2吸附、扫描电镜和电子探针等手段测定了两种方法制备的典型样品的结构和粒度分布.两种方法制备的催化剂都是含有锐钛矿和金红石型TiO2的混合晶体,但共沉淀法制备的催化剂具有较高的锐钛矿含量、较大的晶粒和大孔/介孔的多级孔结构,这是其具有较高光催化活性的主要原因.  相似文献   

6.
以硅酸钠、硝酸铈铵为原料,十六烷基三甲基溴化铵为模板剂,通过水热法合成铈掺杂的介孔分子筛CeMCM-41.分别采用X射线粉末衍射(XRD)、透射电子显微镜(TEM)、红外光谱(FT-IR)、紫外-可见分光光度计(UV-Vis)和N2吸附-脱附等技术对产物的晶相、结构、形貌、比表面积和孔径进行表征.同时研究硅铈物质的量比对合成材料结构性能的影响.实验结果表明:水热条件下成功合成出铈掺杂的MCM-41介孔分子筛,其比表面积为480.5~1 295.2m2/g,平均孔径在2.70~6.29 nm之间.随着稀土元素铈的掺杂量的增加,CeMCM-41介孔分子筛的比表面积和孔体积变小,介孔有序性变差.  相似文献   

7.
La3+-SiO2掺杂纳米TiO2的合成及其光催化降解甲基橙的研究   总被引:2,自引:1,他引:1  
以三嵌段非离子表面活性剂P123为模板,采用水热法合成了La3+-SiO2掺杂纳米TiO2,通过X射线衍射(XRD)、红外光谱(FT-IR)、紫外-可见漫反射吸收光谱(DRS)等手段,考察了La3+-SiO2掺杂纳米TiO2的结构与光学特性.实验结果表明,La3+和SiO2掺杂使TiO2的晶粒在生长过程中受到阻碍.Ti-O-Si键和Ti-O-La键的形成抑制了金红石相的形成和晶粒长大,提高了TiO2的热稳定性,有利于获得高纯度锐钛矿相纳米TiO2.La3+-SiO2掺杂将TiO2的光响应范围拓宽至可见光区,提高了纳米TiO2的光催化性能.与纯纳米TiO2相比,La3+-SiO2掺杂纳米TiO2光催化降解甲基橙的性能显著提高.  相似文献   

8.
以有序密堆积的聚甲基丙烯酸甲酯(PMMA)单分散微球为大孔模板剂、以三嵌段共聚物EO20PO70EO20(P123)为介孔模板剂、以硝酸亚铈和硝酸氧锆为金属源,采用溶剂挥发自组织法首次合成了具有介孔孔壁的三维有序大孔结构的Ce0.6Zr0.4O2固溶体,并利用XRD,TEM/SAED,N2吸附-脱附等技术表征了所合成的铈锫固溶体的物理性质.结果表明,经500℃灼烧所制得的Ce0.6Zr0.4O2固溶体为多晶单相立方结构,具有三维有序大孔结构,其大孔直径为50~200mm.壁厚为10~40nm,大孔孔壁具有孔径为3~4 nm的蠕虫状介孔结构.  相似文献   

9.
以纤维素为模板剂,TiCl4为钛源,采用液相水解-沉淀法制备了浅黄色的N、F共掺杂可见光响应介孔TiO2催化剂(TiONF)。以苯酚为模型物,考察了TiONF在紫外光区、可见光区及太阳光下催化活性;采用X射线光电子能谱(XPS)、傅里叶变换红外(FTIR)、紫外-可见漫反射光谱(UV-Vis DRS)、X射线衍射(XRD)、热重/量热扫描(TG/DSC)、透射电镜(TEM)及低温N2物理吸附-脱附等技术对TiONF催化剂的结构进行了表征。结果表明,以纤维素为模板剂合成适量N、F共掺杂的TiONF催化剂在紫外光区、可见光区及太阳光下均表现出较高的活性,且高于无模板剂合成的TiONF催化剂的活性。N、F共掺杂提高了TiO2表面羟基数量和锐钛矿相TiO2向金红石相转变的温度;N掺杂形成新的能级结构,诱发TiO2可见光催化活性;F掺杂促进TiO2粒子表面氧空穴产生,致使TiO2粒子表面酸度和Ti3+增加。另外,纤维素的加入可减小TiONF颗粒平均尺寸,改善催化剂分散性,提高催化剂比表面积。  相似文献   

10.
采用聚苯乙烯(PS)微球和EO20PO70EO20(P123)作为模板剂,通过溶胶-凝胶及煅烧后处理等方法制备了三维有序大孔复合材料Ag/TiO2(3DOM Ag/TiO2).经傅里叶变换红外光谱、X射线衍射、紫外-可见漫反射吸收光谱、X射线光电子能谱、N2吸附-脱附测试和扫描电子显微镜配合X射线能量色散谱等测试手段对其组成、结构及形貌等进行了表征.结果显示,该复合材料的孔结构排列整齐有序,孔壁呈现介孔结构且分布均匀,属于三维有序大孔材料.该3DOM Ag/TiO2具有锐钛矿晶相,其Ag以单质形式存在.与商用光催化剂(Degussa P-25)相比,3DOM Ag/TiO2对光的吸收红移至可见区.考察了3DOM Ag/TiO2在紫外光、可见光以及微波辅助等不同模式下光催化降解有机污染物的性能.结果显示,其活性明显高于P-25和Ag/TiO2,且针对不同类型的有机污染物均表现出较好的光催化性能.  相似文献   

11.
Scandium magnesium gallide, Sc2MgGa2, and yttrium magnesium gallide, Y2MgGa2, were synthesized from the corresponding elements by heating under an argon atmosphere in an induction furnace. These intermetallic compounds crystallize in the tetragonal Mo2FeB2‐type structure. All three crystallographically unique atoms occupy special positions and the site symmetries of (Sc/Y, Ga) and Mg are m2m and 4/m, respectively. The coordinations around Sc/Y, Mg and Ga are pentagonal (Sc/Y), tetragonal (Mg) and triangular (Ga) prisms, with four (Mg) or three (Ga) additional capping atoms leading to the coordination numbers [10], [8+4] and [6+3], respectively. The crystal structure of Sc2MgGa2 was determined from single‐crystal diffraction intensities and the isostructural Y2MgGa2 was identified from powder diffraction data.  相似文献   

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15.
Summary The ability of [MoS4]2–, anions to be used as ligands for transition metal ions has been widely demonstrated, especially with Fe2+. The present study has been restricted to linear complexes such as (NEt4)2 [Cl2FeS2MoS2] and (NEt4)2[Cl2FeS2MoS2FeCl2]. Their electrochemical properties are described: upon electrochemical reduction, these compounds yield MoS2, as a black precipitate, and an iron complex in solution, assumed to be [SFeCl2]2–. The electrochemical reduction goes through two electron transfers, coupled with the breakdown of the molecular skeleton: a DISPl and an ECE mechanism. Depending on the solvent, the following equilibrium may be observed: [Cl4Fe2MoS4]2–[Cl2FeMoS4]2–+FeCl2. The equilibrium constant, KD, was evaluated by differential pulse polarography. KD is tightly related to the donor number of the solvent.  相似文献   

16.
On Dialkali Metal Dichalcogenides β-Na2S2, K2S2, α-Rb2S2, β-Rb2S2, K2Se2, Rb2Se2, α-K2Te2, β-K2Te2 and Rb2Te2 The first presentation of pure samples of α- and β-Rb2S2, α- and β-K2Te2, and Rb2Te2 is described. Using single crystals of K2S2 and K2Se2, received by ammonothermal synthesis, the structure of the Na2O2 type and by using single crystals of β-Na2S2 and β-K2Te2 the Li2O2 type structure will be refined. By combined investigations with temperature-dependent Guinier-, neutron diffraction-, thermal analysis, and Raman-spectroscopy the nature of the monotropic phase transition from the Na2O2 type to the Li2O2 type will be explained by means of the examples α-/β-Na2S2 and α-/β-K2Te2. A further case of dimorphic condition as well as the monotropic phase transition of α- and β-Rb2S2 is presented. The existing areas of the structure fields of the dialkali metal dichalcogenides are limited by the model of the polar covalence.  相似文献   

17.
The structures of the hypophosphites KH2PO2 (potassium hypophosphite), RbH2PO2 (rubidium hypophosphite) and CsH2PO2 (caesium hypophosphite) have been determined by single‐crystal X‐ray diffraction. The structures consist of layers of alkali cations and hypophosphite anions, with the latter bridging four cations within the same layer. The Rb and Cs hypophosphites are isomorphous.  相似文献   

18.
Wu YT  Linden A  Siegel JS 《Organic letters》2005,7(20):4353-4355
[reaction: see text] Fluoranthene 2 and heptacycle 3 are easily accessible from the reaction of diyne 1 and norbornadiene (NBD) in the presence of the rhodium catalyst. The unusual [(2+2)+(2+2)] adduct 3 was confirmed by the X-ray crystal structure analysis.  相似文献   

19.
[(n‐Bu)2Sn(O2PPh2)2] ( 1 ), and [Ph2Sn(O2PPh2)2] ( 2 ) have been synthesized by the reactions of R2SnCl2 (R=n‐Bu, Ph) with HO2PPh2 in Methanol. From the reaction of Ph2SnCl2 with diphenylphosphinic acid a third product [PhClSn(O2PPh2)OMe]2 ( 3 ) could be isolated. X‐ray diffraction studies show 1 to crystallize in the monoclinic space group P21/c with a = 1303.7(1) pm, b = 2286.9(2) pm, c = 1063.1(1) pm, β = 94.383(6)°, and Z = 4. 2 crystallizes triclinic in the space group , the cell parameters being a = 1293.2(2) pm, b = 1478.5(4) pm, c = 1507.2(3) pm, α = 98.86(3)°, β = 109.63(2)°, γ = 114.88(2)°, and Z = 2. Both compounds form arrays of eight‐membered rings (SnOPO)2 linked at the tin atoms to form chains of infinite length. The dimer 3 consists of a like ring, in which the tin atoms are bridged by methoxo groups. It crystallizes triclinic in space group with a = 946.4(1) pm, b = 963.7(1) pm, c = 1174.2(1) pm, α = 82.495(6)°, β = 66.451(6)°, γ = 74.922(6)°, and Z = 1 for the dimer. The Raman spectra of 2 and 3 are given and discussed.  相似文献   

20.
Photoionization Mass Spectra of SCl2, S2Cl2, and S2Br2 Photoionization mass spectra of SCl2, S2Cl2, and S2Br2 have been measured. Heats of formation, bond energies, and ionization potentials of fragments have been calculated from appearance potentials.  相似文献   

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