顺丁烯二酸-co-苯乙烯微球对Cd(Ⅱ)的吸附行为研究

以火焰原子吸收光谱法(FAAS)为检测手段,研究了本实验室合成的顺丁烯二酸-苯乙烯共聚物微球对Cd(Ⅱ)的静态吸附性能,考察了影响吸附率的相关因素以及不同浓度的各种解吸剂对Cd(Ⅱ)的解吸效果.溶液pH为6、吸附时间为2h时吸附基本达到平衡,吸附率可达到95%以上.以3 mol/,L的HCI溶液作为解吸剂对Cd(Ⅱ)进...     

纳米TiO2分离富集Mo(Ⅵ)和Re(Ⅶ)

本文研究了纳米TiO2吸附剂对Mo(VI)、Re(VII)的吸附行为,考察了溶液的pH值、吸附时间、温度等因素对吸附的影响。结果表明：纳米TiO2对Mo(VI)的吸附在pH 1～8条件下,吸附率超过99%,2 mL 0.05mol/L NaOH溶液可将吸附的Mo(VI)离子完全洗脱,解吸率能达到97%。在pH 1～10范围内,纳米TiO2不吸附Re(VII), 从而达到Mo(VI)、Re(VII)分离。在2℃～50℃温度范围内,Mo(VI)的吸附过程符合Langmiur等温式,纳米TiO2对Mo(VI)的最大吸附容量从11.51mg g-1增加到14.19 mg g-1;纳米TiO2分离钼后,溶液剩余的铼,用活性炭吸附,在pH1～10范围内, Re(VII)的吸附率可达99%,用浓氨水进行洗脱,洗脱率可达96%;吸附过程可用准二级反应动力学模型描述,是以化学吸附为控制步骤的吸附过程;吸附等温线与Freundlich模型有较好的拟合。     

纳米二氧化钛对水中Sn(Ⅱ)、Sn(Ⅳ)和二丁基锡吸附性能的研究

采用流动注射-氢化物发生-原子吸收光谱法研究纳米TiO2对Sn(Ⅱ)、Sn(Ⅳ)和二丁基锡(DBT)的吸附作用,探讨在不同pH值、吸附时间、试样浓度和试样体积下,不同用量的纳米TiO2的吸附效果以及试样的洗脱条件和效率。结果表明,Sn(Ⅱ)和Sn(Ⅳ)的浓度≤6.0μg/mL、体积≤500 mL、pH=3.0;DBT的浓度≤0.2μg/mL、体积≤50 mLp、H=4.0,30 mg纳米TiO2对Sn(Ⅱ)、Sn(Ⅳ)和DBT的吸附率≥90.0%。在25℃条件下,纳米TiO2对Sn(Ⅱ)、Sn(Ⅳ)和DBT的饱和吸附容量分别为23.6μg/mg、13.7μg/mg和0.628μg/mg,适用于无机锡和二丁基锡污染的吸附去除及对水中无机及丁基锡的定量富集。用4 mol/L HCl对吸附的Sn(Ⅱ)、Sn(Ⅳ)和DBT进行洗脱,洗脱率达到98%以上,可做为样品分析的前处理方法。     

硫脲基纳米螯合纤维对水溶液中Cd(Ⅱ)的吸附和密度泛函理论计算

以聚丙烯腈为原料, 利用静电纺丝技术和化学接枝制备得到硫脲基纳米螯合纤维, 并用于水溶液中 Cd(Ⅱ)的去除. 结合样品的表征和密度泛函(DFT)理论计算结果, 揭示了所制备纳米纤维材料对Cd(Ⅱ)的吸附机理. 借助静态吸附和动态吸附实验, 考察了硫脲基纳米螯合纤维对Cd(Ⅱ)的吸附性能. 结果表明, 纳米纤维吸附材料对Cd(Ⅱ)的最大吸附容量可达349.46 mg/g, 吸附过程在90 min以内即可达到基本平衡. 整个吸附过程符合准二级动力学模型和Langmuir等温吸附模型. 硫脲基纳米螯合纤维吸附Cd(Ⅱ)的吸附机理为表面配位络合, 增加纳米纤维表面硫脲基团的含量是提高吸附容量的重要途径. 该吸附材料经6次循环使用后, 最大动态吸附容量并未发生明显改变.     

含氰基聚合物微球对铜离子吸附性能的研究

以火焰原子吸收光谱法(FAAS)为检测手段,研究了聚丙烯腈微球(PANMS)对溶液中Cu2+的吸附及其影响因素,并建立了PANMS分离富集-FAAS法。实验结果表明,溶液pH为5、静态吸附时间为1.5 h、温度为20℃时,其对Cu2+的吸附达到饱和而稳定,吸附容量为30.2 mg/g,吸附率可达到87.5%。随着吸附时间的延长吸附率有所提高,但幅度不是很大。以0.1 mol/LHC l溶液作为解吸剂,解吸率可达到96.5%。经富集50倍后,测Cu2+工作曲线的回归方程为A=0.0025C(μg/L)-0.0026(r=0.9993),方法的检出限为1.68μg/L,相对标准偏差(RSD)小于2.9%。加标回收率为91.4%~97.0%。     

凹凸棒土应用于水样中铜和铅测定的研究

本文以凹凸棒土为固相萃取剂,与火焰原子吸收光谱(FAAS)法联用,富集并检测样品中的痕量金属离子。研究了凹凸棒土对痕量Cu(Ⅱ)和Pb(Ⅱ)的吸附作用,考察了吸附时间、凹凸棒土加入量等影响其吸附和解吸的主要因素、并考察了静态饱和吸附容量,及共存离子的影响。结果表明,当pH 6.0、凹凸棒土用量为0.25 g时,凹凸棒土对Cu(Ⅱ)和Pb(Ⅱ)的吸附率达到90.3%和92.1%;用20 mL 0.1 mol.L-1的HNO3可将吸附在凹凸棒土上的Cu(Ⅱ)和Pb(Ⅱ)定量洗脱。凹凸棒土对Cu(Ⅱ)和Pb(Ⅱ)的静态饱和吸附容量分别为15.8 mg.g-1、23.7 mg.g-1;本法对Cu(Ⅱ)和Pb(Ⅱ)的检出限分别为2.80μg.L-1、0.25μg.L-1;相对标准偏差分别为1.9%和2.1%(Cu(Ⅱ)、Pb(Ⅱ):0.40μg.mL-1,n=5)。在优化的实验条件下,实测了水样中Cu(Ⅱ)和Pb(Ⅱ)的含量,加标回收率均在96%～105%之间,结果令人满意。     

Cu(Ⅱ)印迹丙烯腈-co-苯乙烯微球的制备与对Cu(Ⅱ)的选择性吸附

以Cu(Ⅱ)为模板离子、丙烯腈为功能单体,苯乙烯(St)为骨架单体,偶氮二异丁腈为引发剂,二乙烯苯为交联剂制备了铜离子印迹丙烯腈-co-苯乙烯微球(Cu-I-AN-co-St);用UV、FTIR、SEM和FAAS表征了聚合物和分析了Cu-I-AN-co-St对Cu(Ⅱ)的选择性吸附;结果表明,在室温下溶液pH为5～6,吸附时间为60 min时吸附达到平衡,最佳吸附条件下,饱和吸附容量可达到49.1 mg/g;以1 mol/L HCl溶液作为解吸剂其解吸率可达98%;与相应非印迹微球(NI-AN-co-St)相比,Cu(Ⅱ)I-AN-co-St对Cu(II)的吸附量增大并具有选择性;与电荷相同及离子半径相近的Zn(Ⅱ)、Ni(Ⅱ)、Cd(Ⅱ)共存时,其相对选择性系数分别为28.2,24.8,44.4。     

纳米Cu(OH)2分解温度对CuO粒度的影响

以CuSO4.5H2O和NaOH为原料,采用沉淀法制备得到Cu(OH)2纤维,再进行Cu(OH)2的分解反应.考察了在不同实验条件下温度对Cu(OH)2热分解过程的影响.结果表明:在反应温度20℃,反应终点pH值为12,搅拌速度为1 200 r.min-1,NaOH溶液的滴加速度为50 mL.min-1的反应条件下,得到的样品为纳米Cu(OH)2纤维,其直径为10~30 nm、长度为1~6μm;在固相纳米Cu(OH)2热分解制备CuO过程中CuO粒径随温度的升高而增大,在温度不超过200℃时CuO的粒径约为20 nm左右;在液相中先沉淀后升温时,产物的形貌为球形,CuO粒径随温度的升高而增大,低于80℃可得到纳米级的CuO.     

碳化温度对MOFs基碳材料吸附性能的影响

本文以均苯三酸和二水合醋酸锌、苯并咪唑/苯并三氮唑作为反应物,在50℃条件下合成了两种金属有机框架结构MOFs-Bm/MOFs-Bt。分别在不同温度下氮气氛围中煅烧得到纳米多孔碳材料Bm-t/Bt-t。利用红外光谱仪、同步热分析仪对配合物的结构以及热稳定性进行了表征;对煅烧后样品采用场发射扫描电子显微镜、比表面及孔径分析仪等进行表征,并通过对亚甲基蓝的脱除来测试其吸附性能。结果表明:煅烧温度越高碳材料对亚甲基蓝的吸附性越好;相同煅烧温度下Bm-t比Bt-t具有更好的吸附效果;煅烧温度在600℃-750℃间吸附速率发生了断崖式变化,说明虽然根据热重分析,600℃时配合物的框架结构完全坍塌,但并未碳化完全。     

纳米氧化镁对Cr(Ⅵ)、Cr(Ⅲ)和Cu(Ⅱ)的吸附特性

采用乳液法制备不同形貌的花状和片状MgO纳米粒子并研究其对Cr(Ⅵ)、Cr(Ⅲ)和Cu(Ⅱ)的吸附性能。运用静态吸附实验考察吸附时间和吸附剂MgO用量对Cr(Ⅵ)、Cr(Ⅲ)和Cu(Ⅱ)的去除率影响,探讨MgO纳米粒子的微观机构对其吸附性能的影响机制。结果表明,花状MgO和片状MgO对Cu(Ⅱ)、Cr(Ⅵ)和Cr(Ⅲ)离子表现出优异的吸附性能,对金属离子的去除效果是Cu(Ⅱ)Cr(Ⅵ)Cr(Ⅲ),5min基本达到吸附平衡;花状MgO对金属离子Cr(Ⅵ)和Cr(Ⅲ)的吸附性能明显优于片状MgO,这归因于比表面积大、多孔结构的花状MgO为金属离子提供更多的吸附活性位。与Temkin模型和Freundlich模型相比,Langmuir等温吸附模型更符合MgO样品在含Cu(Ⅱ)离子溶液体系中对Cr(Ⅵ)和Cr(Ⅲ)离子的吸附过程,这意味着Cr(Ⅵ)和Cr(Ⅲ)离子在MgO纳米粒子表面的吸附属于单分子层吸附。花状和片状MgO对金属铬离子的吸附行为符合伪一级动力学模型。     

OH(3) (-) and O(2)H(5) (-) double Rydberg anions: predictions and comparisons with NH(4) (-) and N(2)H(7) (-)

A low barrier in the reaction pathway between the double Rydberg isomer of OH(3) (-) and a hydride-water complex indicates that the former species is more difficult to isolate and characterize through anion photoelectron spectroscopy than the well known double Rydberg anion (DRA), tetrahedral NH(4) (-). Electron propagator calculations of vertical electron detachment energies (VEDEs) and isosurface plots of the electron localization function disclose that the transition state's electronic structure more closely resembles that of the DRA than that of the hydride-water complex. Possible stabilization of the OH(3) (-) DRA through hydrogen bonding or ion-dipole interactions is examined through calculations on O(2)H(5) (-) species. Three O(2)H(5) (-) minima with H(-)(H(2)O)(2), hydrogen-bridged, and DRA-molecule structures resemble previously discovered N(2)H(7) (-) species and have well separated VEDEs that may be observable in anion photoelectron spectra.     

Bis(trifluoroacetyl) peroxide, CF(3)C(O)OOC(O)CF(3)

Pure, highly explosive CF(3)C(O)OOC(O)CF(3) is prepared for the first time by low-temperature reaction between CF(3)C(O)Cl and Na(2)O(2). At room temperature CF(3)C(O)OOC(O)CF(3) is stable for days in the liquid or gaseous state. The melting point is -37.5 degrees C, and the boiling point is extrapolated to 44 degrees C from the vapor pressure curve log p = -1875/T + 8.92 (p/mbar, T/K). Above room temperature the first-order unimolecular decay into C(2)F(6) + CO(2) occurs with an activation energy of 129 kJ mol(-1). CF(3)C(O)OOC(O)CF(3) is a clean source for CF(3) radicals as demonstrated by matrix-isolation experiments. The pure compound is characterized by NMR, vibrational, and UV spectroscopy. The geometric structure is determined by gas electron diffraction and quantum chemical calculations (HF, B3PW91, B3LYP, and MP2 with 6-31G basis sets). The molecule possesses syn-syn conformation (both C=O bonds synperiplanar to the O-O bond) with O-O = 1.426(10) A and dihedral angle phi(C-O-O-C) = 86.5(32) degrees. The density functional calculations reproduce the experimental structure very well.     

Syntheses and structures of the infinite chain compounds Cs(4)Ti(3)Se(13), Rb(4)Ti(3)S(14), Cs(4)Ti(3)S(14), Rb(4)Hf(3)S(14), Rb(4)Zr(3)Se(14), Cs(4)Zr(3)Se(14), and Cs(4)Hf(3)Se(14)

The alkali metal/group 4 metal/polychalcogenides Cs(4)Ti(3)Se(13), Rb(4)Ti(3)S(14), Cs(4)Ti(3)S(14), Rb(4)Hf(3)S(14), Rb(4)Zr(3)Se(14), Cs(4)Zr(3)Se(14), and Cs(4)Hf(3)Se(14) have been synthesized by means of the reactive flux method at 823 or 873 K. Cs(4)Ti(3)Se(13) crystallizes in a new structure type in space group C(2)(2)-P2(1) with eight formula units in a monoclinic cell at T = 153 K of dimensions a = 10.2524(6) A, b = 32.468(2) A, c = 14.6747(8) A, beta = 100.008(1) degrees. Cs(4)Ti(3)Se(13) is composed of four independent one-dimensional [Ti(3)Se(13)(4-)] chains separated by Cs(+) cations. These chains adopt hexagonal closest packing along the [100] direction. The [Ti(3)Se(13)(4-)] chains are built from the face- and edge-sharing of pentagonal pyramids and pentagonal bipyramids. Formal oxidation states cannot be assigned in Cs(4)Ti(3)Se(13). The compounds Rb(4)Ti(3)S(14), Cs(4)Ti(3)S(14), Rb(4)Hf(3)S(14), Rb(4)Zr(3)Se(14), Cs(4)Zr(3)Se(14), and Cs(4)Hf(3)Se(14) crystallize in the K(4)Ti(3)S(14) structure type with four formula units in space group C(2)(h)()(6)-C2/c of the monoclinic system at T = 153 K in cells of dimensions a = 21.085(1) A, b = 8.1169(5) A, c = 13.1992(8) A, beta = 112.835(1) degrees for Rb(4)Ti(3)S(14);a = 21.329(3) A, b = 8.415(1) A, c = 13.678(2) A, beta = 113.801(2) degrees for Cs(4)Ti(3)S(14); a = 21.643(2) A, b = 8.1848(8) A, c = 13.331(1) A, beta = 111.762(2) degrees for Rb(4)Hf(3)S(14); a = 22.605(7) A, b = 8.552(3) A, c = 13.880(4) A, beta = 110.919(9) degrees for Rb(4)Zr(3)Se(14); a = 22.826(5) A, b = 8.841(2) A, c = 14.278(3) A, beta = 111.456(4) degrees for Cs(4)Zr(3)Se(14); and a = 22.758(5) A, b = 8.844(2) A, c = 14.276(3) A, beta = 111.88(3) degrees for Cs(4)Hf(3)Se(14). These A(4)M(3)Q(14) compounds (A = alkali metal; M = group 4 metal; Q = chalcogen) contain hexagonally closest-packed [M(3)Q(14)(4-)] chains that run in the [101] direction and are separated by A(+) cations. Each [M(3)Q(14)(4-)] chain is built from a [M(3)Q(14)] unit that consists of two MQ(7) pentagonal bipyramids or one distorted MQ(8) bicapped octahedron bonded together by edge- or face-sharing. Each [M(3)Q(14)] unit contains six Q(2)(2-) dimers, with Q-Q distances in the normal single-bond range 2.0616(9)-2.095(2) A for S-S and 2.367(1)-2.391(2) A for Se-Se. The A(4)M(3)Q(14) compounds can be formulated as (A(+))(4)(M(4+))(3)(Q(2)(2-))(6)(Q(2-))(2).     

Mixed ligand titanium(IV) complexes. Chlorobis(dithiocarbamato)bis(methylsalicylato)titanium(IV) andbis(dithiocarbamato)bis(methylsalicylato)titanium(IV)

Summary Dichlorobis(methylsalicylato)titanium(IV) reacts with potassium or amine salts of dialkyl or diaryl dithiocarbamates in 11 and 12 molar ratios in anhydrous benzene (room temperature) or in boiling CH₂Cl₂ to yield mixed ligand complexes: (AcOC₆H₄O)₂ Ti(S₂CNR₂)Cl (1) and (AcOC₆H₄O)₂ Ti(S₂CNR₂)₂ (2), R=Et, n-Pr, n-Bu, cyclo-C₄H₈ and cyclo-C₅H₁₀. These compounds are moisture sensitive and highly soluble in polar solvents. Molecular weight measurement in conjunction with i.r.,¹H and¹³C n.m.r. spectral studies suggest coordination number 7 and 8 around titanium(IV) in (1) and (2) respectively.