UV-Vis-草酸铁络合物-H_2O_2体系产生羟自由基的Fe(phen)_3~(2+)光度法测定

UV-Vis-草酸铁络合物 -H2O2 法是一种新的高级氧化工艺 ,该工艺产生的羟自由基·OH具有极强的氧化能力 ,可与水中大多数有机物迅速反应而使其降解 ;用Fe(phen)32+ 光度法研究了该体系中羟自由基·OH产生的规律 ,·OH可将Fe(phen)32+(Fe2 +-菲咯啉络合物)氧化成Fe(phen)33+(Fe3 +-菲咯啉络合物),通过测定Fe(phen)32+ 在508nm处吸光度的变化可间接求出·OH的生成量 ;结果表明 ,在 pH=4.0,n(Fe2+)∶n(H2O2)∶n(C2O42-)=1∶5∶10(化学计量数 )时 ,·OH的生成量最大;该分析方法具有简单、快速的优点     

普利沙星与Co(phen)_3~(2+)及DNA间结合作用的电化学和光谱

利用电化学和紫外光谱法研究了邻菲咯啉合钴(Co(phen)32+)与普利沙星(PLFX)及DNA间在pH=7.4的三羟甲基氨基甲烷-盐酸缓冲溶液中的结合作用。紫外光谱测量结果表明,普利沙星与Co(phen)32+发生了结合作用形成二元络合物,结合常数为2.0×104L/mol。电化学测量表明,在Co(phen)32+-普利沙星络合物中加入DNA后,Co(phen)32+-普利沙星络合物的峰电流下降,峰电位差增大了17 mV,式电位负移了3.5 mV,推断络合物与DNA作用方式主要为静电作用。     

铜(Ⅱ)-邻菲咯啉-(邻菲咯啉-5,6-二酮)络合物的合成及其同脱氧核糖核酸的作用

以邻菲咯啉（phen)、邻菲咯啉－5，6－二酮（dione)为配体首次合成了高氯酸邻菲咯啉－邻菲咯啉－5，6－二酮（Ⅱ）。用荧光光谱，摩尔比，粘度，MLCT减色效应，平衡常数以及荧光能量转移研究了各合物与鱼精子DNA的结合情况，证实了该络合物与DNA存在插入作用。基于络合物对DNA能量转移造成荧光量子产率比值（Φλ/Φ320）的降低，解释了不同波长激发光下，荧光发射峰在加入DNA后产生猝灭和增强两种绝然不同的现象。     

SDS-乙醇-水中［Fe（phen）3］2+介导双酚A的伏安检测

应用循环伏安法和微分脉冲伏安法研究了十二烷基硫酸钠(SDS)-乙醇-水体系中[Fe(phen)3]2+(phen=1,10-邻菲咯啉)介导双酚A(BPA)氧化的反应机理及其伏安检测。结果表明:在SDS-乙醇-水体系中,铟锡氧化物(ITO)电极上[Fe(phen)3]2+对BPA呈现出良好的电催化氧化活性,电催化效果受乙醇-水体积比、SDS及BPA浓度的影响。在乙醇-水(1∶5)体系中,0.25 mmol·L-1SDS的加入增强了ITO电极上[Fe(phen)3]2+对BPA的电催化氧化作用。在乙醇-水(1∶5)和0.25 mmol·L-1SDS体系中,BPA在微分脉冲伏安图上约0.731 V处有明显的电催化氧化峰,峰电流在0.2~20μmol·L-1内呈良好的线性关系(r=0.999 9),检出限为0.034μmol·L-1,相对标准偏差(n=3)为2.1%。将该体系用于水样中BPA的测定,回收率为96.9%~100.7%。该文还讨论了SDS-乙醇-水体系中[Fe(phen)3]2+介导BPA氧化的反应机理。该研究有助于更好地理解微乳体系中氧化还原媒介体对酚类污染物的电催化氧化机理,可为电化学传感器的构建提供新思路。     

普利沙星与Co(phen)2+3及DNA间结合作用的电化学和光谱

利用电化学和紫外光谱法研究了邻菲咯啉合钴(Co(phen)2+3)与普利沙星(PLFX)及DNA间在pH=7.4的三羟甲基氨基甲烷-盐酸缓冲溶液中的结合作用. 紫外光谱测量结果表明,普利沙星与Co(phen)2+3发生了结合作用形成二元络合物,结合常数为2.0×104 L/mol. 电化学测量表明,在Co(phen)2+3-普利沙星络合物中加入DNA后,Co(phen)2+3-普利沙星络合物的峰电流下降,峰电位差增大了17 mV,式电位负移了3.5 mV,推断络合物与DNA作用方式主要为静电作用.     

茜素红S催化动力学光度法测定痕量铁(Ⅲ)及反应机理探讨

在pH4.5的NaAc-HAc缓冲介质中,以邻菲咯啉(phen)作活化剂,痕量Fe(Ⅲ)对H2O2氧化茜素红S(ARS)的褪色反应存在明显的催化作用,由此建立了测定痕量铁(Ⅲ)的催化动力学光度法。采用固定时间法,在λmax=422nm处,对催化体系和非催化体系进行光度测定,应用了正交试验法确定最佳条件,测定了有关动力学参数。该方法的检出限为0.63μg/L;线性范围为0~20μg/L,应用于一次蒸馏水、分析纯盐酸中痕量铁的测定,结果令人满意。提出了Fe(Ⅲ)-ARS-phen三元络合物活性中间体的催化反应机理设想,并推测催化反应经历了羟自由基氧化反应的历程。     

钌(Ⅱ)-邻菲咯啉偶合化学发光法测定 Fenton反应产生的羟自由基

提出了一种测定Fenton反应产生羟自由基的偶合化学发光分析法.羟自由基与苯甲酸发生羟化反应后生成的羟基苯甲酸能增大钉(Ⅱ)邻菲咯啉-Ce(Ⅳ)化学发光反应的发光强度.用化学发光法测定羟基苯甲酸的含量可间接测定自由基的生成量.拟定的方法,简单、灵敏度高,可用于筛选羟自由基消除剂.     

配体的空间构型及疏水性对钌（Ⅱ）多吡啶配合物与DNA作用的影响

合成了4－氰基苯基咪唑并[5,6-f]邻菲咯啉（CYIP）和2－羧基苯基咪唑并[5, 6-f]邻菲咯啉（COIP）两种新配体及它们的钌混配配合物[Ru(bpy)2CYIP](ClO4)2 ·H2O（Rul）（bpy=2,2′-联吡啶），[Ru(phen)2CYIP](ClO4)2·H2O(Ru2) (phen=1,10-邻菲咯啉），[Ru(bpy)2COIP](ClO4)2·3H2O(Ru3)和[Ru(phen)2COIP] (ClO4)2·H2O(Ru4)，并用红外光谱、紫外光谱、核磁和质谱对它们进行了表征。 通过循环伏安法研究了这些配合物的电化学性质。采用电子吸收光谱、稳态荧光、 圆二色谱和粘度测定研究了配合物与小牛胸腺DNA的相互作用。结果表明配合物 Rul和Ru2通过CYIP配体以插入的方式与DNA结合，而配合物Ru3和Ru4则通过COIP配 体以部分插入的方式与DNA结合。     

超细粉体二硫纶·取代菲咯啉铁(Ⅱ)配合物的光敏性研究

报道了新近合成的二硫纶·取代菲咯啉铁 (Ⅱ )配合物FeLL′(L =mnt2 - ,1 ,2 二氰基乙烯 1 ,2 二硫醇离子 ,L′ =phen 5,6 dione,1 ,1 0 菲咯啉 5,6 二酮 ;5 NO2 phen ,5 硝基 1 ,1 0 菲咯啉 )的电子吸收光谱、电子发射光谱及对CdS的光敏性 ,研究了FeLL′对CdS的光敏化作用与其电子光谱间的关系     

钌（Ⅱ）—邻菲咯啉偶合化学发光法测定Fenton反应产生的羟自由基

提出了一种测定Ｆｅｎｔｏｎ反应产生羟自由基的偶合化学发光分析法。羟自由基与苯甲酸发生烃化反应后生成的羟基苯甲酸能增大钌（Ⅱ）邻菲咯啉－Ｃｅ（Ⅳ）化学发光反应的发光强度。用化学发光法测定羟基苯甲酸的含量可间接测定自由基的生成量。拟定的方法,简单,灵敏度高,可用于筛选羟自由基消除剂。     

Sc2MgGa2 and Y2MgGa2

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.     

Electrochemical study of (NEt4)2Cl2FeS2MoS2 and (NEt4)2Cl2FeS2MoS2FeCl2

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, K_D, was evaluated by differential pulse polarography. K_D is tightly related to the donor number of the solvent.     

The alkali hypophosphites KH2PO2, RbH2PO2 and CsH2PO2

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.     

Zur Kenntnis der Dialkalimetalldichalkogenide β-Na2S2, K2S2, α-Rb2S2, β-Rb2S2, K2Se2, Rb2Se2, α-K2Te2, β-K2Te2 und Rb2Te2

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.     

Formal [(2+2)+2] and [(2+2)+(2+2)] nonconjugated dienediyne cascade cycloadditions

[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.     

Crystal Structures of [Bu2Sn(O2PPh2)2], [Ph2Sn(O2PPh2)2], and [PhClSn(O2PPh2)OMe]2. Raman Spectra of [Ph2Sn(O2PPh2)2] and [PhClSn(O2PPh2)OMe]2

[(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.     

Die Photoionenspektren von SCl2, S2Cl2 und S2Br2

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.