Fe_3O_4/Ce~(3+)-TiO_2复合光催化材料的制备及其光催化性能研究

采用溶胶-凝胶法,以钛酸四丁酯、硝酸铈为主要原料,无水乙醇为溶剂,冰醋酸为抑制剂,浓硝酸为催化剂制得稳定的Ce3+掺杂TiO2溶胶,其凝胶经不同温度煅烧3 h后制得Ce3+掺杂量不同的TiO2粉体。用XRD对TiO2进行了测试对比分析,以紫外光为光源,亚甲基蓝溶液为模拟有机染料废水,研究了TiO2的光催化性能。用化学共沉淀法制备了具有强磁性的纳米Fe3O4水基磁流体,再与Ce3+掺杂TiO2进行复合,制备了Fe3O4负载量不同的磁性Ce3+掺杂TiO2,研究了其对亚甲基蓝的光催化降解效果、磁分离回收率的影响。结果表明,TiO2凝胶热处理温度、Ce3+掺量、TiO2晶型及Fe3O4负载量对亚甲基蓝的光催化活性均有影响。掺Ce3+量为1%,热处理温度650℃的Ce3+掺杂TiO2粉体光催化活性最高。Fe3O4负载量为10%的Fe3O4/Ce3+-TiO2对亚甲基蓝的降解率8 h时达到90.3%,磁分离回收率达96.8%。     

静电纺丝法制备Fe3+/TiO2纳米纤维及表征

以聚乙烯吡咯烷酮(PVP)为纤维模板,钛酸四丁酯(Ti[O(CH2)3CH3]4)和Fe3+为前驱体,乙醇为溶剂,醋酸为催化剂,采用静电纺丝法制备不同含铁量的复合纳米纤维Fe3+/TiO2,经500℃煅烧得到以锐钛矿为主的Fe3+/TiO2纳米纤维。采用扫描电子显微镜(SEM)和X射线衍射仪(XRD)分别表征了Fe3+/TiO2纳米纤维的形貌与晶态,计算了样品的晶粒尺寸和锐钛矿所占的比例,并比较了5%Fe3+/TiO2纳米纤维、5%Fe3+/TiO2粉体以及纯TiO2纳米纤维三者光催化降解亚甲基蓝(MB)的效果。研究表明:由静电纺丝法制备的5%Fe3+/TiO2纳米纤维的光催化降解效果比相同含铁量的粉体的降解效果好,TiO2纳米纤维比5%Fe3+/TiO2纳米纤维的光催化活性高。     

磁性La3+掺杂TiO2的制备及性能

利用溶胶-凝胶法,在室温条件下,以钛酸四丁酯、硝酸镧为主要原料,无水乙醇为溶剂,冰醋酸为抑制剂,浓硝酸为催化剂制得稳定的掺La3+TiO2溶胶,陈化后的凝胶经不同温度煅烧3h后制得不同掺La3+量的TiO2。通过XRD对不同煅烧温度及不同掺La3+量的TiO2进行了表征;以紫外光为光源,研究了掺La3+-TiO2对甲基橙溶液的光降解效果。用化学共沉淀法制备了具有强磁性的Fe3O4水基磁流体,再与La3+掺杂TiO2进行复合,制备了Fe3O4负载量不同的磁性La3+掺杂TiO2,研究了Fe3O4负载量不同的La3+掺杂TiO2对甲基橙的光催化降解效果、磁分离回收率的影响。结果表明,掺La3+量及煅烧温度对TiO2的晶型、各晶型TiO2的相对含量及对甲基橙的光降解效果均有影响。La3+掺杂TiO2比纯TiO2显示出更强的光催化性能,掺La3+量2%,热处理温度450℃的La3+掺杂TiO2光催化活性最高。Fe3O4负载量为10%的Fe3O4/La3+-TiO2对甲基橙的降解率8h时为99.4%;磁分离回收率达97.39%。     

水热法合成TiO2/Fe3+光催化剂及其氧化降解亚甲基蓝

以硫酸钛为钛源,采用水热法合成了TiO2/Fe3+光催化剂,利用XRD对产物晶体结构进行表征,研究在紫外光(365nm)照射下用合成的TiO2/Fe3+粉末催化降解亚甲基蓝的效果,分析了亚甲基蓝初始浓度、TiO2/Fe3+用量、掺Fe3+量、光照时间和溶液初始pH值等因素的影响;考察了溶液初始pH值对TiO2/Fe3+粉末的吸附性能和光催化活性的影响。结果表明:合成的TiO2/Fe3+晶体为锐钛矿型(A-TiO2)。在4mg/L的亚甲基蓝溶液(pH=8)中,加入掺Fe3+量0.8%(摩尔分数)合成的TiO2/Fe3+粉末使其用量为0.6g/L,室温下紫外光照反应6h,亚甲基蓝的降解率达到98.2%。在上述优化条件下,当溶液的pH<6时,催化剂对亚甲基蓝的吸附量和光催化效率均较低,且二者随pH升高而显著增加;当pH≥6时,对亚甲基蓝的吸附作用较大,因此较明显地提高了光催化活性。     

铁掺杂纳米TiO2的制备及其光催化性能研究

采用溶胶-凝胶法制备了掺杂Fe3 的纳米TiO2微粒,采用X光衍射仪对粉体进行了表征.以甲基橙为目标降解物,研究了Fe3 掺杂纳米TiO2光催化性能.结果表明,掺杂适量Fe3 能够提高TiO2的光催化活性,当Fe3 的掺入量为摩尔比0.41%时催化活性最高.以紫外灯为光源,降解初始浓度为20mg·L-1的250mL甲基橙溶液,催化剂0.41%(摩尔分数)Fe3 -TiO2投加量为0.5g时,甲基橙的光催化降解效果最好.     

Fe掺杂纳米ZnO的制备及其光催化性能研究

以醋酸锌和Fe(NO)_3·9H_2O为原料,采用水热法制备了Fe掺杂的纳米ZnO。利用XRD、SEM等方法对所制得的样品的结构及形貌进行表征,以亚甲基蓝为模拟染料废水,分别考察了反应温度、pH、掺杂比例、催化剂用量和亚甲基蓝pH对其光催化性能的影响。结果表明,在反应温度为150℃,Fe/Zn掺杂比为0.05,pH为11时,催化剂光催化性能较优;催化剂投加量为1.00g/L,亚甲基蓝废水pH为11时,亚甲基蓝的降解率达到93%。Fe~(3+)掺杂到ZnO晶格中。     

柔性YAG-Al2O3纳米纤维膜负载C3N4的水处理性能研究

采用溶胶-凝胶法和静电纺丝技术制备了柔性钇铝石榴石-氧化铝(YAG-Al₂O₃)纳米纤维膜，然后使用尿素包埋法将石墨相氮化碳(g-C₃N₄)引入到纤维膜孔隙中，制备了自支撑光催化降解钇铝石榴石-氧化铝/氮化碳(YAG-Al₂O₃/C₃N₄)复合材料，表征了材料的形貌结构和力学行为，并研究了其在亚甲基蓝污水处理中的可见光催化降解性能。结果表明，YAG-Al₂O₃纳米纤维膜具有优异的柔韧性，YAG-Al₂O₃/C₃N₄复合材料在厚度方向具有良好的弹性，两者均为自支撑材料。100min内复合材料对亚甲基蓝的降解率可达96%以上，循环3次后降解率仍保持在94%左右。催化反应动力学符合Langmuir-Hinshelwood(L-H)模型，说明复合材料具有长期稳定且高效的催化降解效果。     

纳米Ni-TiO2光催化剂的制备及其性能研究

采用溶胶-凝胶法制备了过渡金属Ni掺杂纳米TiO2光催化剂(Ni-TiO2),采用XRD、纳米粒度、UVVis和PL对其进行了表征和分析,并以亚甲基蓝(MB)作为目标降解物,研究了Ni掺杂量以及热处理温度对NiTiO2性能的影响。结果表明:当pH=2.5、n(Ni)∶n(Ti)=1%、热处理温度为500℃时制备的样品在普通日光灯下、5h内对MB的光催化降解率达到92.54%,明显优于Degussa P25在相同条件下的降解率(50.69%)。     

稀土La掺杂TiO2纳米纤维高响应光催化降解染料研究

为了提高TiO₂光催化性能,并研究金属离子掺杂对TiO₂光催化性能的影响,采用静电纺丝技术和煅烧工艺制备稀土元素La掺杂TiO₂无机纳米纤维膜,通过SEM、XRD、FT-IR、TG测试对材料的形貌、结构进行表征,以亚甲基蓝为靶向降解剂,进一步深入研究La³⁺改性TiO₂光催化氧化降解染料的机理。结果表明,当染料浓度为10 mg/L,La³⁺掺杂改性纳米TiO₂纤维的浓度为15 mg/10 mL条件下,催化10 min的降解率为63.41%,催化70 min的降解率即可达到99.87%,比未掺杂TiO₂纳米纤维的降解率提高了6.36%,可见,La³⁺的掺杂提高了TiO₂光催化降解速率,所需要的时间减少了。     

Yb,N共掺杂TiO_2光催化剂的制备及可见光下降解亚甲基蓝的研究

采用微波辅助溶胶-凝胶法制备了Yb,N共掺杂的纳米(Yb,N)-TiO2光催化剂,通过XRD、XPS、UV-Vis-DRS、PL等对(Yb,N)-TiO2样品进行了表征和分析,并以亚甲基蓝(MB)作为目标降解物,考察了不同Yb掺杂浓度的(Yb,N)-TiO2对MB的光催化降解效果。结果表明,Yb和N的掺入减小了TiO2的禁带宽度,降低了光生电子-空穴对的复合,使其吸收光谱的阈值波长红移至可见光区,提高了TiO2的光催化活性。当p H值=1.5、m(H2NCONH2)=10 g、热处理温度为650℃、n(Yb)∶n(Ti)=0.005时,(Yb,N)-TiO2粉体在普通日光灯下对亚甲基蓝在5 h内的光催化降解效率达93.55%,明显高于同等条件下P25的降解率45.72%。     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Thermal diffusion in binary mixtures H2-CCl2F2 and H2-CHClF2

Thermal diffusion coefficients were measured in two gaseous mixtures, in which one component was close to the critical temperature, in the pressure range (19.6–127.4)·10⁴ N/m² and at a freon concentration of 0.25–0.8.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Radial GRIN glasses in Li2O-Na2O-Al2O3-TiO2-SiO2 systems

A series of GRIN glass rods have been developed in Li2O-Na2O-Al2O3-TiO2-SiO2 systems. Negative radial refractive index profiles were generated by exchanging Na+ for Li+ ions in these glass rods. It has been observed that TiO2 plays a vital role in increase in the profile depth and maximum change in the refractive index because of its ambivalent nature. Change in the refractive index can be further increased by increasing the concentration of exchanging cation in the base glass.     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.     

Si_2N_2O-Al_2O_3-La_2O_3和Si_2N_2O-Al_2O_3-CaO系统的亚固相关系

本文给出了 Si_2N_2O-Al_2O_3-La_2O_3和 Si_2N_2O-Al_2O_3-CaO 系统的亚固相图。实验结果表明:在 Si_2N_2O-Al_2O_3-CaO 系统中有一个未知结构的新化合物 CaO·Si_2N_2O,在3CaO·Si_2N_2O 和3CaO·Al_2O_3两化合物之间形成连续立方固溶体。而 Si_2N_2O-Al_2O_3-La_2O_3系统中则没有发现新化合物。在两个系统的富 Si_2N_2O区,过量的 Si_2N_2O 与 La_2O_3和 CaO 分别反应形成 Si_3N_4与 La_(10)[SiO_4]_(?)N_2(H-相)(和 CaSiO_3。所研究的这两个三元系统中,分别形成了如下几个四元相容性区。在 Si_2N_2O-Al_2O_3-La_2O_3系统内有:H-Si_3N_4-La_2O_3·Si_2N_2O-La_2O_3·Al_2O_3;H-Si_3N_4-La_2O_3·Al_2O_3-La_2O_3·11 Al_2O_3;H-Si_3N_4-La_2O_3·11 Al_2O_3-Al_2O_3;H-Si_3N_4-Al_2O_3-O′s.s;H-Si_3N_4-O′s.s-Si_2N_2O在 Si_2N_2O-Al_2O_3-CaO 系统内有:Si_3N_4-CaSiO_3-CaO·Si_2N_2O-3CaO·Al_2O_3;Si_3N_3-CaSiO_3-3CaO·Al_2O_3-2CaO·Al_2O_3·SiO_(?);Si_(?)N_(?)-CaSiO_3-2CaO·Al_2O_3·SiO_2-Al_2O_3;Si_3N_4-CaSiO_3-Al_2O_(?)-O′s.s;Si_3N_4-CaSiO_3-O′s.s-Si_(?)N_(?)O