配合物[Cu(H2O)(C12H8N2)2]·2ClO4的合成、性质及晶体结构

合成了配合物 [Cu(H2 O) (C12 H8N2 ) 2 ]·2ClO4 (C12 H8N2 为 1,10 邻菲咯啉 ) ,用元素分析、摩尔电导、红外光谱及电子光谱进行了表征 ,并测定了配合物的晶体结构。该晶体属单斜晶系 ,空间群为CC;晶胞参数 :a =1.9177(2 )nm ,b =0 .81994(0 )nm ,c=1.6 2 45 8(14)nm ,β =10 0 .10 4(6 )° ;V =2 .5 419(4)nm3,Z =4,F(0 0 0 ) =130 0 ,DC=1.6 93g/cm3,R =0 .0 430 ,wR =0 .1195。中心铜 (Ⅱ )离子与两个 1,10 邻菲咯啉的四个N原子和一个水分子的氧原子配位 ,形成了一个变形的三角双锥结构     

三维网状配位聚合物{[Cd2(phen)2(H2O)2(C6H5NO2)2]·(ClO4)}n的水热合成、晶体结构及荧光性质

以异烟酸和邻菲咯啉(phen)为原料,采用水热合成方法,合成了一个新的配位聚合物{[Cd2(phen)2(H2O)2(C6H5NO2)2]·(ClO4)}n,测定了其晶体结构.结果表明:该配合物晶体属单斜晶系,空间群P21/n.与中心镉(Ⅱ)离子配位的3个氧原子分别来自2个异烟酸根和1个水分子,3个氮原子分别来自1个异烟酸根和1个邻菲咯啉,形成六配位变形八面体结构.由于异烟酸的桥联作用及氢键作用,配合物堆积成三维网状结构;同时配合物通过异烟酸的羧基双齿桥联配位以及邻菲咯啉和水分子作为端基配位.形成了双核笼状结构,其Cd(Ⅱ)…Cd(Ⅱ)距离为0.8798 nm.此外,还研究了该聚合物的荧光性质.     

新型混价铜配合物[CuⅠCuⅡ(Ophen)2Cl]·H2O(HOphen=2-羟基-1,10-邻菲咯啉)的水热合成和晶体结构

报道了一种新型混价铜配合物[CuⅠCuⅡ(Ophen)2Cl]·H2O(HOphen=2-羟基-1,10′-邻菲咯啉)的水热合成和晶体结构.该化合物属于三斜晶系,P1空间群,a=0.91667(18)nm,b=1.0546(2)nm,c=1.1705(2)nm,α=80.50(3)°,β=80.56(3)°,γ=66.87(3)°,V=1.0202(3)nm3,Z=2,Dc=1.872Mg/m3,R1=0.0508,(wR2)=0.1481.标题化合物由一种新型的双核铜配合物和一个结晶水组成.邻菲咯啉在水热反应中发生羟基化,形成新型的羟基化邻菲咯啉.两个这样的配合物通过Cu…Cu间的范德华力相互作用形成二聚体.二聚体之间通过Ophen基团的π-π堆积以及C—H…Cl弱相互作用构筑成三维超分子网络.水分子处于网络的孔穴中.该化合物为邻菲咯啉的羟基化提供又一个新的范例.     

双核银配合物[Ag2(μ-(4-MeC6H4O)2PS2)2(Phen)2]的光谱性质和晶体结构

合成了双核银配合物[Ag2(μ-(4-MeC6H4O)2PS2)2(Phen)2](phen为1,10-邻菲咯啉),用元素分析、红外光谱、紫外-可见光谱和热重分析进行了表征,并用X-射线衍射法测定了晶体结构。该晶体属于正交晶系,Pbca空间群,晶胞参数为:a=1.2035(2)nm,b=1.638 3(3)nm,c=2.517 1(5)nm,V=4.963 1(17)nm 3,Dc=1.599 g.m-3,Z=4,F(000)=2 416,μ(Mo Kα)=1.072 mm-1,S=1.066,(Δ/σ)max=0.001,R1=0.037 6,wR2=0.088 8(I>2σ(I))。晶体结构研究表明每个Ag原子与不同配体(4-MeC6H4O)2PS2-的2个S原子和1个phen配体的2个N原子配位形成了具有椅式构型的八元环Ag2S4P2,Ag原子为畸变四面体AgS2N2构型,配合物通过phen的π-π堆积形成了一维结构,分子间的弱氢键C-H…O和C-H…π作用使分子进一步形成了三维网络结构。     

铋（Ⅲ）苯乙酸-1,10-邻菲罗啉三元配合物[Bi2（PPA）6·（Phen）2]的合成、晶体结构及抑菌活性

合成了铋(III)苯乙酸-1,10-邻菲罗啉[Bi2(PPA)6·(Phen)2](HPPA=苯乙酸(C8H7O2),Phen=l,10-邻菲罗啉(C12H8N2))三元配合物,并通过元素分析和红外(IR)光谱对其进行了表征,用单晶X-射线衍射测定了配合物的晶体结构.配合物属于三斜晶系,P-1空间群,a=0.9100(6)nm,b=1.2617(8)nm,c=1.3324(9)nm,α=89.757(8)°,β=87.277(8)°,γ=81.155(8)°,V=1.5099(17)nm3,Dc=1.748g·cm-3,μ=5.890mm-1,Z=1,F(000)=780,残差因子R1=0.0484,wR2=0.1090[I>2σ(I)],S=1.002.标题化合物为双核铋(III)配合物,金属中心Bi(III)原子与三个苯乙酸根(PPA)中的6个氧原子、一个1,10-邻菲罗啉分子中的两个氮原子和一个桥连氧原子进行配位,形成九配位的扭曲三帽三方柱配位十四面体,围绕铋原子的价键总数VBi(1)=2.897,两个Bi(III)原子通过两个桥连氧原子连结成中心对称的分子,Bi…Bi间距离为0.4469(2)nm.初步抑菌试验结果显示,配合物对大肠杆菌(E.Coli)、金黄色葡萄球菌(S.Aureus)、枯草芽孢杆菌(B.Subtilis)表现出相似且良好的抑菌效果.     

[Ag(4，4′-bpy)]+及[Zn(phen)2(H2O)2]2+两种配合物的合成、结构与荧光性质

用水热法和溶液法分别合成了2个新的配合物{[Ag(4,4′-bpy)]·3-HSBA.H2O}n(1)和[Zn(phen)2(H2O)2]·(A-2,5-DSA)·3H2O(2)(3-HSBA=3-羧基苯磺酸根,A-2,5-DSA=苯氨-2,5-二磺酸根,4,4′-bpy=4,4′-联吡啶,phen=1,10-邻菲咯啉),用X-射线单晶衍射结构分析方法测定了其晶体结构。配合物1是一维链状结构。在1个不对称单元中包含1个[Ag(4,4′-bpy)]+阳离子,1个3-羧基苯磺酸根阴离子和1个晶格水分子。Ag髣离子与2个4,4′-联吡啶的2个氮原子配位。配合物2是单核结构。在1个不对称单元中包含1个[Zn(phen)2(H2O)2]2+阳离子,1个苯氨-2,5-二磺酸根阴离子和3个晶格水分子。Zn髤离子与2个1,10-邻菲咯啉的4个氮原子和2个水氧原子配位。配合物1和2中,配位阳离子、抗衡阴离子以及晶格水分子之间存在丰富的氢键,进而构筑成超分子网络结构。配合物的荧光均来自于配体的π-π*电子跃迁。     

金属配位聚合物[Mn2（C8H3NO6）2(C12H8N2)2]n的合成及其催化氧化性能

以5-硝基间苯二甲酸,1,10-邻菲啰啉,硫酸锰(MnSO4.H2O)为原料合成了一种结构新颖的金属配位聚合物——[Mn2(C8H3NO6)2(C12H8N2)2]n(1),其结构经IR,XRD,TG-DTG和元素分析表征。X-射线单晶衍射测试结果表明,1属三斜晶系,空间群Pī,晶胞参数a=10.060 2(1),b=14.343 5(2),c=14.663 7(2),α=104.052(1)°,β=102.633(1)°,γ=110.460(1)°,Mr=888.52,V=1 812.69(4)3,Z=2,Dc=1.628 g.cm-3,F(000)=900。以30%H2O2为氧化剂,初步研究了1在苯乙烯氧化反应中的催化氧化性能。     

配合物[Cu2(C4H2O6)(Phen)2(H2O)]·8H2O的合成、晶体结构和抗菌活性

在pH≈10的乙醇-水溶液中以硫酸铜、酒石酸和邻菲咯啉反应合成了分子式为[Cu₂(C₄H₂O₆)(Phen)₂(H₂O)]·8H₂O的配合物单晶。用X-射线单晶衍射测定了晶体结构，并研究了配合物对大肠杆菌、金黄色葡萄球菌、枯草杆菌的抗菌活性。晶体属单斜晶系，空间群P2₁。标题化合物为双核铜配合物，2个铜原子配位数不同。Cu(1)是五配位的，具有扭曲的四方锥结构，5个配位原子分别是酒石酸的去质子的羟基氧和羧基氧、邻菲咯啉的2个氮原子及1个水分子的氧原子。Cu(2)为四配位的，配位原子分别是酒石酸的去质子的羟基氧和羧基氧和邻菲咯啉的2个氮原子。分子中Cu(1)…Cu(2)间的距离为0.354 8 nm。存在分子内邻菲咯啉-邻菲咯啉的面—面π-π相互作用，面间距为0.381 3 nm。配合物对大肠杆菌、金黄色葡萄球菌、枯草杆菌具有较强的抗菌活性。     

锌配合物Zn(phen)(H2O)(3-mba)2的合成、结构表征及荧光性质

常温下,溶液法合成了一个单核结构的锌配合物Zn (phen)(H2O)(3-mba)2(phen:邻菲咯啉;3-Hmba∶3-甲基苯甲酸),并用红外光谱、元素分析、热重分析以及X射线单晶衍射表征了其结构.结果表明,配合物属于三斜晶系,空间群P1,晶胞参数:a=10.893(2)(A),b=11.461(2)(A),c=11.505(2)(A),α=95.54(3)°,β=115.80(3)°,γ =100.25(3)°,V=1247.9(4) (A)3,C28H24N2O5Zn,Mr=533.86,Z =2,Dc=1.421 g·cm-3,F(000) =552,最终偏离因子[I≥2σ(I)]R1=0.0471,wR2 =0.0954.在配位物分子中,中心锌离子是五配位模式,双分子间先通过O—H…O氢键形成二聚体,继而二聚体间通过相邻分子中的邻菲咯啉芳环的π-π堆积作用沿着a方向形成了一维超分子链.对配合物的荧光性能进行了测试.CCDC 1023439.     

[Eu(C10H9N2O4)(C10H8N2O4)(H2O)3]2·phen·4H2O超分子化合物的晶体结构、荧光性质及热稳定性

在水-乙醇混合体系中,以2-羰基丙酸水杨酰腙(C10H10N2O4,简作H3L)、1,10-菲啰啉C12H8N2,简作phen)与Eu(NO3)3·4H2O反应,首次培养出黄色单晶[Eu(C10H9N2O4)(C10H8N2O4)(H2O)3]2·phen·4H2O.该晶体属三斜晶系,P1空间群,晶胞参数a=1.378 6(12) nm,b=1.398 8(12) nm,c=1.759 7(16) nm,α=73.977(11)°,β=68.598(12)°,γ=71.224(12)°,V=29.42(4) nm3,Z=2,μ=2.208 mm-1,Dc=1.746 Mg/m3,F(000)=1 556,R=0.037 7,ωR=0.074 4,GOF=0.916.每个配合物晶体中均有两个相似的结构单元,每个结构单元中铕(Ⅲ)配位数为9,分别与两个2-羰基丙酸水杨酰腙和3个水分子配位; 每个2-羰基丙酸水杨酰腙中的羧基氧、酰胺基中的羰基氧和CN中的氮与Eu3+配位,形成两个共边的稳定的五元环,另3个配位原子则分别来自3个水分子中的氧原子,该结构单元在空间呈扭曲的单帽四方反棱柱,而在每两个铕的九配位单元周围还有一个游离的1,10-菲啰啉分子和4个水分子.IR,1H NMR及热分解结果佐证了配合物的组成.该配合物具有很好的荧光特性.     

Intermolecular forces for D2, N2, O2, F2 and CO2

The intermolecular potentials for D₂, N₂, O₂, F₂ and CO₂ are determined on the basis of the second virial coeffincients, the polarizabilities parallel and perpendicular to the molecular axes, and the electric quadrupole moment. The repulsive parts of the potentials are taken from the corresponding Kihara core-potentials. Effects of the octopolar induction are taken into consideration in a unique way. The potential depends on relative orientations of the two molecules as well as the distance r between the molecular centers. This dependence is shown in graphs. A measure of the anisotropy of the potential depth is 0.72 for CO₂ 0.36 for D₂, and smaller than 0.27 for N₂ O₂ and F₂. The remarkable anisotropy for CO₂ and D₂ is due to strong electrostatic quadrupole interactions.     

Ba3 (VO4)2-K2 Ba(MoO4)2 and Pb3 (VO4)2-K2 Pb(MoO4)2 systems

Phase equilibria in the Ba₃(VO₄)₂-K₂Ba(MoO₄)₂ and Pb3(VO₄)₂-K₂Pb(MoO₄)₂ systems have been investigated. In the first system, a continuous series of substitutional solid solutions with the palmierite structure is formed, and in the second one, the polymorphic transition in lead orthovanadate at 100°C restricts the extent of the palmierite-type solid solution to 10–100 mol % K₂Pb(MoO₄)₂. Original Russian Text ? V.D. Zhuravlev, Yu.A. Velikodnyi, A.S. Vinogradova-Zhabrova, A.P. Tyutyunnik, V.G. Zubkov, 2008, published in Zhurnal Neorganicheskoi Khimii, 2008, Vol. 53, No. 10, pp. 1746–1748.     

The preparation of NbH5(Me2PCH2CH2Me2)2 and NbHL2(Me2PCH2CH2PMe2)2 (L = CO or C2H4)

MMe₅(dmpe) (M = Nb or Ta, dmpe = Me₂PCH₂CH₂PMe₂) reacts with H₂ (500 atm) and dmpe in THF at 60°C to give MH₅(dmpe)_2? NbH₅(dmpe)₂ readily reacts with two mol of CO or ethylene (L) to give NbHL₂(dmpe)₂. The exchange of the hydride ligand with the ethylene protons in NbH(C₂H₄)₂(dmpe)₂ is not rapid on the ¹H NMR time scale (60 MHz) at 95°C.     

Phase transitions in Ca3(BN2)2 and Sr3(BN2)2

α-Ca₃(BN₂)₂ crystallizes in the cubic system (space group: ) with one type of calcium ions disordered over of equivalent (8c) positions. An ordered low-temperature phase (β-Ca₃(BN₂)₂) was prepared and found to crystallize in the orthorhombic system (space group: Cmca) with lattice parameters: , , and . Structure refinements on the basis of X-ray powder data have revealed that orthorhombic β-Ca₃(BN₂)₂ corresponds to an ordered super-structure of cubic α-Ca₃(BN₂)₂. The space group Cmca assigned for β-Ca₃(BN₂)₂ is derived from by a group-subgroup relationship.DSC measurements and temperature-dependent in situ X-ray powder diffraction studies showed reversible phase transitions between β- and α-Ca₃(BN₂)₂ with transition temperatures between 215 and 240 °C.The structure Sr₃(BN₂)₂ was reported isotypic with α-Ca₃(BN₂)₂ () with one type of strontium ions being disordered over of equivalent (2c) positions. In addition, a primitive () structure has been reported for Sr₃(BN₂)₂. Phase stability studies on Sr₃(BN₂)₂ revealed a phase transition between a primitive and a body-centred lattice around 820 °C. The experiments showed that both previously published structures are correct and can be assigned as α-Sr₃(BN₂)₂ (, high-temperature phase), and β-Sr₃(BN₂)₂ (, low-temperature phase).A comparison of Ca₃(BN₂)₂ and Sr₃(BN₂)₂ phases reveals that the different types of cation disordering present in both of the cubic α-phases () have a directing influence on the formation of two distinct (orthorhombic and cubic) low-temperature phases.     

Zur Trennung von H2, O2, N2, NO, CO, N2O, CO2, C2H6, C2H4, C2H2, NO2(N2O4) und Feuchtigkeit

Ohne Zusammenfassung     

Conversion of NO in NO/N2, NO/O2/N2, NO/C2H4/N2 and NO/C2H4/O2/N2 Systems by Dielectric Barrier Discharge Plasmas

An experimental study on the conversion of NO in the NO/N₂, NO/O₂/N₂, NO/C₂H₄/N₂ and NO/C₂H₄/O₂/N₂ systems has been carried out using dielectric barrier discharge (DBD) plasmas at atmospheric pressure. In the NO/N₂ system, NO decomposition to N₂ and O₂ is the dominating reaction; NO conversion to NO₂ is less significant. O₂ produced from NO decomposition was detected by an on-line mass spectrometer. With the increase of NO initial concentration, the concentration of O₂ produced decreases at 298 K, but slightly increases at 523 K. In the NO/O₂/N₂ system, NO is mainly oxidized to NO₂, but NO conversion becomes very low at 523 K and over 1.6% of O₂. In the NO/C₂H₄/N₂ system, NO is reduced to N₂ with about the same NO conversion as that in the NO/N₂ system but without NO₂ formation. In the NO/C₂H₄/O₂/N₂ system, the oxidation of NO to NO₂ is dramatically promoted. At 523 K, with the increase of the energy density, NO conversion increases rapidly first, and then almost stabilizes at 93–91% of NO conversion with 61–55% of NO₂ selectivity in the energy density range of 317–550 J L⁻¹. It finally decreases gradually at high energy density. A negligible amount of N₂O is formed in the above four systems. Of the four systems studied, NO conversion and NO₂ selectivity of the NO/C₂H₄/O₂/N₂ system are the highest, and NO/O₂/C₂H₄/N₂ system has the lowest electrical energy consumption per NO molecule converted.     

Formation of [Cp2TiSbMe2]2, [Cp2TiSb(SiMe3)2]2 and [Cp2TiCl]2·2Mes4Sb2

Reactions of [Cp₂Ti(btmsa)] (btmsa = bis(trimethylsilyl)acetylene) with R₄Sb₂ (R = Me, Me₃Si) give [Cp₂TiSbMe₂]₂ (1) or [Cp₂TiSb(SiMe₃)₂]₂ (2) respectively. [Cp₂TiCl]₂·2Mes₄Sb₂ (3) is serendipitously formed from [Cp₂Ti(btmsa)] and Mes₂SbH containing NH₄Cl traces.     

Synthesis and structure of three manganese oxalates: MnC2O4·2H2O, [C4H8(NH2)2][Mn2(C2O4)3] and Mn2(C2O4)(OH)2

Three manganese oxalates have been hydrothermally synthesized, and their structures determined by single-crystal X-ray diffraction. MnC₂O₄·2H₂O (I) is orthorhombic, P2₁2₁2₁, , , , , Z=4, final R, R_w=0.0832, 0.1017 for 561 observed data (I>3σ(I)). The one-dimensional structure consists of chains of oxalate-bridged manganese centers. [C₄H₈(NH₂)₂][Mn₂(C₂O₄)₃] (II) is triclinic, , , , , α=81.489(2)°, β=81.045(2)°, γ=86.076(2)°, , Z=1, final R, R_w=0.0467, 0.0596 for 1773 observed data (I > 3σ (I)). The three-dimensional framework is constructed from seven coordinate manganese and oxalate anions. The material contains extra-framework diprotonated piperazine cations. Mn₂(C₂O₄)(OH)₂ (III) is monoclinic, P2₁/c, , , , β=91.10(3)°, , Z=1, final R₁, wR2=0.0710, 0.1378 for 268 observed data (I>2σ (I)). The structure is also three dimensional, with layers of MnO₆ octahedra pillared by oxalate anions. The hydroxide group is found bonded to three manganese centers resulting in a four coordinate oxygen.     

Investigation of phase equilibria in the systems K2SO4Sc2(SO4)3, Rb2SO4Sc2(SO4)3 and Cs2SO4Sc2(SO4)3

Phase diagrams of the systems K₂SO₄Sc₂(SO₄)₃, Rb₂SO ₄Sc₂(SO₄)₃ and Cs₂SO₄ Sc₂(SO₄)₃ have been investigated by X-ray diffraction phase analysis and differential thermal analysis techniques. A salient feature of all the systems is the formation of M₃Sc(SO₄)₃, which melt incongruently, and MSc(SO₄)₂, which on heating decompose in the solid state.     

Synthesis and structural investigation of the compounds containing HF2 anions: Ca(HF2)2, Ba4F4(HF2)(PF6)3 and Pb2F2(HF2)(PF6)

Three new compounds Ca(HF₂)₂, Ba₄F₄(HF₂)(PF₆)₃ and Pb₂F₂(HF₂)(PF₆) were obtained in the system metal(II) fluoride and anhydrous HF (aHF) acidified with excessive PF₅. The obtained polymeric solids are slightly soluble in aHF and they crystallize out of their aHF solutions. Ca(HF₂)₂ was prepared by simply dissolving CaF₂ in a neutral aHF. It represents the second known compound with homoleptic HF environment of the central atom besides Ba(H₃F₄)₂. The compounds Ba₄F₄(HF₂)(PF₆)₃ and Pb₂F₂(HF₂)(PF₆) represent two additional examples of the formation of a polymeric zigzag ladder or ribbon composed of metal cation and fluoride anion (MF⁺)_n besides PbF(AsF₆), the first isolated compound with such zigzag ladder. The obtained new compounds were characterized by X-ray single crystal diffraction method and partly by Raman spectroscopy. Ba₄F₄(HF₂)(PF₆)₃ crystallizes in a triclinic space group P1¯ with a=4.5870(2) Å, b=8.8327(3) Å, c=11.2489(3) Å, α=67.758(9)°, β=84.722(12), γ=78.283(12)°, V=413.00(3) Å³ at 200 K, Z=1 and R=0.0588. Pb₂F₂(HF₂)(PF₆) at 200 K: space group P1¯, a=4.5722(19) Å, b=4.763(2) Å, c=8.818(4) Å, α=86.967(10)°, β=76.774(10)°, γ=83.230(12)°, V=185.55(14) ų, Z=1 and R=0.0937. Pb₂F₂(HF₂)(PF₆) at 293 K: space group P1¯, a=4.586(2) Å, b=4.781(3) Å, c=8.831(5) Å, α=87.106(13)°, β=76.830(13)°, γ=83.531(11)°, V=187.27(18) Å³, Z=1 and R=0.072. Ca(HF₂)₂ crystallizes in an orthorhombic Fddd space group with a=5.5709(6) Å, b=10.1111(9) Å, c=10.5945(10) Å, V=596.77(10) Å³ at 200 K, Z=8 and R=0.028.