柔性双三氮唑配体构筑的二维镉(Ⅱ)配合物的合成、结构和荧光性质

水热条件下,合成了1个镉的配位聚合物{[Cd(L)(HBTC)(H₂O)]·H₂O}_n(1)(L=1,2-二(1,2,4-三氮唑-1-亚甲基)苯,H₃BTC=1,3,5-均苯三酸)并对其进行了元素分析,红外光谱,热重以及X射线单晶衍射分析。结构分析表明,镉中心为六配位八面体结构,赤道平面上,4个配位O原子分别来自,2个HBTC^2-二价阴离子和配位水,轴向上的2个配位N原子来自2个不同的L配体。该配合物是1个二维(4,4)网络结构,并进一步被分子间的O-H…O氢键作用构筑成三维超分子结构。同时研究了配合物的荧光性质。     

一个双核镍配合物[Ni2(Htda)2(H2O)6]·4H2O的合成、晶体结构和性质

双核金属配合物对于生物化学和磁化学都是非常重要的。在本文中,1,2,3-三氮唑-4,5-二羧酸(H₃tda)配体和硝酸镍在常温常压下反应得到了1个三氮唑桥联的双核镍配合物[Ni₂(Htda)₂(H₂O)₆]·4H₂O (1),并通过元素分析、红外光谱、X-射线单晶衍射、热重分析以及超导量子干涉仪(SQUID)对其晶体结构和磁、热性质进行了表征。晶体数据表明该配合物属三斜晶系,空间群为P1。在配合物1中,2个1,2,3-三氮唑-4,5-二羧酸配体利用2个相邻的氮原子桥联2个金属镍离子形成一个双桥的双核镍配合物。这些双核镍单元又通过体系中存在的大量的氢键相互作用形成了三维超分子骨架。磁性分析显示双核镍单元内镍镍之间存在反铁磁相互作用。     

2-(1H-1，2，4-三氮唑)乙酸-稀土配合物的合成与结构

利用柔性含氮配体羧酸2-(1H-1,2,4-三氮唑)乙酸(HL)与稀土氧化物在水热条件下反应得到了2个稀土配位聚合物 [Gd(L)₃H₂O]_n(1)和[Nd(L)₃H₂O]_n(2)。利用元素分析、红外光谱、X射线单晶衍射结构分析等方法对其进行了表征。晶体结构表明2个配合物晶体同属三斜晶系,空间群P1,具有一维链状结构。     

两个由1H-苯并三氮唑-1-乙酸构筑的镉、银配合物的合成及晶体结构

合成了2个配位聚合物{[Cd(btaa)(phen)(CH₃COO)]·H₂O}_n(1)和{[Ag₂(btaa)(4,4-bpy)₂](NO₃)·2H₂O}_n(2)(Hbtaa=1H-苯并三氮唑-1-乙酸,phen=1,10-邻菲啰啉,4,4-bpy=4,4-联吡啶),采用单晶X-射线、红外光谱、元素分析和热重分析对配合物进行了表征。配合物1中的镉离子通过1H-苯并三氮唑-1-乙酸根桥连成一位螺旋链状结构。在配合物2中,银离子被4,4-联吡啶连接成一维链状结构,这些一维链通过1H-苯并三氮唑-1-乙酸根桥连以及Ag···Ag作用和π-π堆积连接成一维梯子状结构。此外,还研究了配合物1的荧光性质。     

三维羧基氧桥联双核铜配合物[Cu2(nta)(Phen)3]NO3·6H2O的合成、表征与晶体结构

由H₃nta(H₃nta=nitriloriacetic acid)、Phen(Phen=1,10-phenanthroline)与Cu²⁺离子反应,合成标题配合物[Cu₂(nta)(Phen)₃]NO₃·6H₂O。该配合物的晶体属单斜晶系,空间群为P2₁/c。在配合物中,2个中心铜原子分别与配位原子构成变形八面体和变形三角双锥结构。晶体中结构单元通过分子间氢键和π-π堆积,形成了三维网络结构。TG分析结果表明标题配合物在194 ℃以下是稳定的。     

基于2,4,6-吡啶三羧酸配体桥连的铁(Ⅱ)/镍(Ⅱ)配位聚合物的水热合成及结构表征

在水热反应条件下FeCl₂·6H₂O、2,4,6-吡啶三羧酸(H₃pyta)和NaOH反应合成了1种一维链状铁配位聚合物[Fe₃(pyta)₂(H₂O)₈] (1);同样条件下Ni(OAc)₂·4H₂O、2,4,6-吡啶三羧酸(H₃pyta)、NaOH和4-氨基-3,5-二(4-吡啶基)-1,2,4-三氮唑(abpt)反应合成了1种二维网状镍配合物[Ni₃(pyta)₂(abpt)₂(H₂O)₃]·2H₂O (2)。通过元素分析和红外光谱对这2个配位聚合物进行了表征。单晶结构表明：配合物1的晶体属于单斜晶系,Cc空间群;配合物2的晶体属于单斜晶系,P2₁/c空间群。在配合物1中,pyta^3-配体采取μ₂-和μ₄-pyta^3- 2种桥连模式将Fe原子连成了沿c轴方向延伸的Fe-pyta链。而在配合物2中,pyta^3-配体仅采取μ₂-桥连模式将Ni原子连成线型三核[Ni₃(pyta)₂]单元,这些三核单元进一步通过abpt辅助配体桥连成二维 (4,4)层状结构。     

一种双肟四核铜(Ⅱ)配合物的合成、结构及热稳定性研究

由螯合双肟配体3,3′-二甲氧基-2,2′-[(1,3-亚丙基)二氧双(氮次甲基)]二酚(H₂L)与四水合苦味酸铜作用,合成了一种新的四核铜(Ⅱ)配合物 [Cu₄L₂(pic)₄(H₂O)₂]·2CH₃COCH₃·2H₂O(pic^-=苦味酸根)。用X-射线单晶衍射仪测定了该配合物的晶体结构：配合物属单斜晶系,P2₁/c空间群,由4个Cu^Ⅱ离子,2个四齿的L2-单元,4个配位的苦味酸根(pic^-),2个配位的水分子,2个结晶的丙酮分子和2个结晶的水分子组成。Cu^Ⅱ离子的配位数为6,都具有稍微扭曲的八面体结构。且配合物分子通过分子间O-H…O氢键作用形成了1个二维超分子结构。     

喹啉和吡啶取代三芳基三唑的两个铜配合物的合成与晶体结构

分别以3-（2-吡啶基）-4-（4-甲基苯基）-5-（2-喹啉基）-1，2，4-三氮唑（L¹）和3-（2-吡啶基）-4-（4-氟苯基）-5-（2-喹啉基）-1，2，4-三氮唑（L²）作为配体，合成了2个新的单核铜配合物：trans-[Cu（L¹）₂（NO₃）（H₂O）]NO₃·H₂O（1）和trans-[Cu（L²）₂（NO₃）（H₂O）]NO₃·H₂O（2），对其进行了红外、元素分析和单晶结构表征。2个配合物都属于三斜晶系，P1空间群。单晶结构表明，配合物1和2中的铜离子均处于一个扭曲的八面体配位环境[CuN₄O₂]，轴向上各有一个水分子和一个硝酸根配位。配体的吡啶氮原子和三氮唑的一个氮原子参与配位，而喹啉的氮原子不配位。配合物晶体中存在O-H…O、C-H…O、C-H…N氢键和C-H…π相互作用，从而连接单核配合物形成三维网络。     

N-苯基亚氨基二乙酸桥联的双核铜配合物的合成、表征与晶体结构

由Cu(Ⅱ)、2，2′-联吡啶(邻菲咯啉)与N-苯基亚氨基二乙酸在溶液中组装得到2个双核配合物[Cu₂(L)₂(2，2′-bipy)₂]·8H₂O (1)、[Cu₂(L)₂(phen)₂]·2H₂O (2)(H₂L=N-苯基亚氨基二乙酸，2，2′-bipy=2，2′-联吡啶，phen=邻菲咯啉)。用元素分析、红外光谱、热重分析等进行了表征，并测定了其晶体结构。晶体结构表明，配合物1的晶体属三斜晶系，空间群P1;配合物2的晶体属单斜晶系，空间群P2₁/c。在这2个双核配合物中，中心铜离子的配位形式均为五配位的畸变四方锥构型，配体L中的N原子没有参与配位，而是采用1个羧基的1个氧原子与Cu²⁺离子螯合、另1个羧基上的1个氧原子以μ₂-桥联的配位模式连接2个Cu²⁺离子。     

(5，7，7，12，14，14-六甲基-1，4，8，11-四氮杂环十四-4,11-二烯)·双(O，O′-二(2-苯乙基)二硫代磷酸根)合铜(Ⅱ)的合成与晶体结构

本文首次报道了标题配合物［Cu(hmtade｛SSP(OCH₂CH₃ph)₃｝₃］(hmtade=5,7,7,12,14,14-六甲基-1，4，8，11-四氮杂环十四-4，11-二烯)的合成和晶体结构。该配合物属三斜晶系。空间群为P1。晶胞参数为：a=0.9457(1)mm, b=1.3001(5) nm, c=1.3182(3) nm; α=58.24(2)°, β=73.65(2)°, γ=66.27(3)°。Z=1, R=0.059, R_W=0.067。结构测定表明：(phCH₂CH₂O)₂PSS^-为单齿配体，Cu²⁺与硫和氮形成了六配位的拉长的八面体配合物，该配合物分子具有中心对称性。对其热分解进行了讨论。     

Synthesis of a New Two-dimensional Cd（Ⅱ） Coordination Compound by Benzotriazole-5-carboxylate Acid and 1,10-Phenanthroline and Its Crystal Structure and Characterization

A mixed-ligand metal-organic complex [Cd（C7H3N3O2）（C12H8N2）]n was synthesized by cadmium（Ⅱ） nitrate, 1,10-phenanthroline（phen） and benzotriazole-5-carboxylate acid（H2btca）. Single crystal X-ray analysis indicates that complex 1 has a two-dimensional layer structure and crystallizes in an orthorhombic space group（Pbca）, with cell parameters, a=1.7422（6） nm, b=0.9264（3） nm, c=2.0729（7） nm, α=90°, β=90°,γ=90°, V=3.346（2） nm^3, Z=8. Each central Cd（Ⅱ） is six-coordinated by four N atoms, two of which are from 1,10-phenanthroline, and the other two from two different triazole nitrogen atoms and two O atoms from benzotriazole-5-carboxylate, forming a distorted octahedral geometry. Adjacent Cd（Ⅱ） centers are bridged by benzotriazole-5-carboxylate molecules to form a one-dimensional chain, which is further connected by the nitrogen atoms of btca^2- to form an extended two-dimensional wave-like layer, with OFF（offset face-to-face） stacking interactions between phen ligands in adjacent layers, which are helpful to forming the three-dimensional supramolecular structure.     

Molecular dynamics simulation on the interaction between polymer inhibitors and anhydrite surface

Investigation on the microscopic interaction between polymer inhibitors and calcium sulfate will be helpful for understanding its scale inhibition mechanism and can provide a theoretical guidance to developing new scale inhibitors. In this work, molecular dynamics simulations with COMPASS force field have been performed to simulate the interaction between hydrolyzed polymaleic anhydride (HPMA), polyaspartic acid (PASP), polyepoxysuccinic acid (PESA), polyacrylic acid (PAA) and the (001) and (020) surfaces of anhydrite (AD) crystal with and without water. The results show that the sequence of binding energies between four polymer inhibitors and AD (001) and (020) with water is PESA > PASP > HPMA > PAA. The binding energy of the same polymer inhibitor on AD (001) is smaller than that on AD (020). Water molecules weaken the deformations of HPMA and PAA but aggravate those of PASP and PESA. Natural bond orbital (NBO) charges of the repeat units of polymer inhibitors were calculated by B3LYP/6‐31G* method. The Coulomb interaction is formed between the O atoms of polymer inhibitors and the Ca atoms of AD crystal. The system of polymer–AD is mainly contributed from the non‐bonding interaction. Polymer inhibitors do not interact directly with AD crystal, but indirectly through the interactions between inhibitor–H₂O and H₂O–AD, i.e. water molecules participate in scale inhibition of polymer inhibitors to AD crystal. Water molecules cannot be ignored when the interaction models are constructed, i.e. solvent effect cannot be ignored. Copyright © 2015 John Wiley & Sons, Ltd.     

Molecular Dynamics Study of Interaction between Acrylamide Copolymers and Alumina Crystal

Four acrylamide polymer flocculants, anionic polyacrylamide P(AA-co-AM), cationic poly-acrylamide P(DMB-co-AM), nonionic polyacrylamide P(AM), and hydrophobical polyacry-lamide P(OA-co-AM) have been prepared by copolymerizing with acrylic acid, cationic monomer dimethylethyl (acryloxyethyl) ammonium bromide (DMB) and hydrophobical monomer octadecyl acrylate with acrylamide. The interactions between the flocculants withthe (012) surface of alumina crystal (Al₂O₃) have been simulated by molecular dynamics method. All the polymers can bind tightly with Al₂O₃ crystal, the interaction between the O of polymers and Al of the (012) surface of Al₂O₃ is significantly strong. The order of binding energy is as follows: P(DMB-co-AM)>P(OA-co-AM)>P(AA-co-AM)>P(AM), implying a better flocculation performance of P(DMB-co-AM) than the others. Analy-sis indicates that binding energy is mainly determined by Coulomb interaction. Bonds are found between the O atoms of the polymers and the Al atoms of Al₂O₃. The poly-mers' structures deform when they combine with Al₂O₃ crystal, but the deformation en-ergies are low and far less than non-bonding energies. Flocculation experiments in sus-pension medium of 1%Kaolin show a transmittancy of 90.8% for 6 mg/L P(DMB-co-AM) and 73.0% for P(AM). The sequence of flocculation performance of four polymers is P(DMB-co-AM)>P(OA-co-AM)>P(AA-co-AM)>P(AM), which is in excellent agreement with the simulation results of binding energy.     

Molecular dynamics simulation of the interaction between methyl benzotriazole and Cu2O crystal

In circulating water system , methyl benzotriazole (TTA) is one of the common corrosion inhibitors for copper. But the inhibition mechanisms have not been clearly understood so far. In different number of water molecules, the interaction between TTA and Cu₂O (copper surface) was investigated with molecular dynamics (MD) method. The results showed that the MD simulation result with water was more consistent with the experiment results. In different number of water molecules, the sequence of the interaction energies between TTA and Cu₂O (001) was ? E ₁ (150H₂O) > ? E ₁(200H₂O) > ? E ₁(100H₂O) > ? E ₁(50H₂O) > ? E ₁(0H₂O). The number of water molecules had an important influence on the interaction between corrosion inhibitors and Cu₂O crystal. From non‐bond energy and pair correlation functions, the interaction energies of the model system were mainly contributed by the non‐bond interaction. Strong adsorption could be raised by the Coulomb interaction between the negatively charged functional groups in TTA and the positive copper ions in the Cu₂O (001) face, and further interaction between aggressive media and copper could be restricted. So, copper corrosion could be avoided. Chemical bonds and non‐bond interactions were formed between TTA and Cu₂O (001) in different number of water molecules. Water molecules could not be ignored during the MD simulation, too. The results obtained here may provide theoretical supports for developing new corrosion inhibitors.     

水溶性聚合物与硬石膏晶体相互作用的分子动力学模拟

用分子动力学(MD)方法, 模拟计算了6种水溶性聚合物阻垢剂{聚丙烯酸(PAA)、聚甲基丙烯酸(PMAA)、丙烯酸-丙烯酸甲酯共聚物[P(AA-co-MAE)]、丙烯酸-丙烯酸羟丙酯共聚物[P(AA-co-HPA)]、聚马来酸(HPMA)、丙烯酸-马来酸共聚物[P(AA-co-MA)]}与硬石膏晶体的相互作用. 结果发现, 聚合物与硬石膏晶体结合能的大小排序为P(AA-co-MA)＞HPMA＞P(AA-co-HPA)＞P(AA-co-MAE)＞PMAA＞PAA, 同种聚合物阻垢剂对硬石膏两晶面生长的抑制能力相差不大. 对体系各种相互作用以及对关联函数g(r)的分析表明, 体系结合能主要由库仑作用提供. 与硬石膏晶体结合的聚合物发生明显形变, 但形变能远小于体系的非键作用能. 聚合物中不同位置羧基的动力学行为差别很大, 链端羧基的运动翻转比链中部羧基剧烈得多, 因后者与硬石膏晶体的结合比前者牢固而能更有效地抑制垢晶体生长.     

羧酸共聚物与方解石晶体相互作用的MD模拟

用分子动力学方法, 模拟计算了丙烯酸-丙烯酸甲酯共聚物(AA-MAE)、丙烯酸-丙烯酸羟丙酯共聚物(AA-HPA)、丙烯酸-马来酸共聚物(AA-MA)及水解马来酸酐(HPMA)四种聚羧酸类阻垢剂与方解石晶体(110)晶面的相互作用. 结果表明, 聚羧酸与(110)晶面结合能的大小排序为AA-MA＞HPMA＞AA-HPA＞AA-MAE; 对体系各种相互作用以及径向分布函数的分析表明, 结合能主要由库仑作用(包括离子键)提供, 并含少量氢键成分. 与方解石晶面结合的聚合物发生扭曲变形, 但形变能远小于相应的非键作用能. 聚合物中不同位置羧基的动力学行为差别很大, 链端羧基的运动翻转比链中部羧基剧烈得多, 故后者与晶面的结合比前者更牢固而具有更强的阻垢能力.     

多氨基多醚基亚甲基膦酸的合成及其阻垢机理的MD模拟

以端氨基聚醚、亚磷酸、甲醛、浓盐酸等为原料合成了新型水处理剂多氨基多醚基亚甲基膦酸(PAPEMP), 并通过红外、核磁等手段对产品进行了表征. 采用分子动力学(MD)模拟退火方法, 研究了周期性边界条件下PAPEMP与方解石晶体的相互作用, 探讨了该相互作用的本质, 并初步阐释了PAPEMP的阻垢机理. 结果发现, PAPEMP分子(n＝1～8)与方解石 晶面的结合能强弱排序依次为(按聚合度) 5＞6＞4＞3＞8＞2＞7＞1. 对体系各种相互作用以及对关联函数g(r)的分析表明, 超分子体系的结合能主要由库仑作用(包括离子键)提供, 并含少量氢键成分; van der Waals作用为正值, 不利于结合体系的形成. 能量分析表明, 与方解石晶面结合的PAPEMP (n＝1～8)分子均发生了明显的扭曲变形.     

Systematic investigations on magneto-structural correlations of copper(II) coordination polymers based on organic ligands with mixed carboxylic and nitrogen-based moieties

Reaction of copper(II) tetrazolate-5-carboxylate with different neutral N-donor spacer ligands under hydrothermal conditions leads to the formation of five new coordination polymers, [Cu(tzc)(pyz)(0.5)(H(2)O)(2)](n)·H(2)O (1), [Cu(tzc)(pyz)](n) (2), [Cu(tzc)(pym)(H(2)O)](n) (3), [Cu(tzc)(dpe)(0.5)(H(2)O)](n) (4) and [Cu(tzc)(azpy)(0.5)(H(2)O)](n) (5) (tzc = tetrazolate-5-carboxylate, pyz = pyrazine, pym = pyrimidine, dpe = 1,2-di(4-pyridyl)ethylene and azpy = 4,4'-azopyridine). All five structures were characterized by X-ray single-crystal measurements and bulk material can be prepared phase pure in high yields. The crystal structures of the hydrates 1, 3, 4 and 5 show dimeric [Cu(2)(N(tzc)-N(tzc))(2)] building units formed by μ(2)-N1,O1:N2 bridging tzc ligands as the characteristic structural motif. These six-membered entities in 1, 4 and 5 are connected by μ(2)-N,N' bridging N-donor ligands into 1D chains and in 3 into 2D layers. In the crystal structure of compound 2 adjacent Cu(II) cations are connected by μ(2)-N1,O1:N4,O2 bridging tzc ligands into chains, which are further connected by μ(2)-N,N' bridging pyz ligands forming 2D layers. Extensive hydrogen bonds in all compounds play an important role in the construction of their supramolecular networks. Investigations of their thermal properties reveal water release upon heating according to the formation of anhydrates before starting decomposing above 220 °C. Furthermore, the magnetic properties have been studied leading to consistent global antiferromagnetic exchange interactions with coupling constants of J = 3 ± 1 cm(-1) and long-range antiferromagnetic ordering states at lower temperatures.     

水溶性聚合物与方解石晶体相互作用的MD模拟

用分子动力学(MD)方法, 模拟计算了三种水溶性聚合物阻垢剂[聚丙烯酸(PAA)、聚甲基丙烯酸(PMAA)、丙烯酸-丙烯酸甲酯共聚物(AA-MA)]与方解石晶体的作用. 结果表明, 聚合物与方解石两晶面结合能的大小均为PAA ＞ AA-MA ＞ PMAA, 聚合物与(1 0)面的相互作用远比与(104)面的作用强. 对体系各种相互作用以及对关联函数g(r)的分析表明, 结合能主要由库仑作用决定. 与方解石晶面结合的聚合物发生扭曲变形, (1 0)面上的形变能约为(104)面上的2倍, 但均远小于相应的非键作用能. 聚合物中不同位置羧基的动力学行为差别很大, 链端羧基的运动翻转比链中部羧基剧烈得多, 后者与方解石晶体的结合比前者牢固而能更有效地抑制垢晶体生长.     

新型二氟甲基磷酸类酪氨酸蛋白磷酸酯酶1B抑制剂的分子动力学模拟和结合自由能计算

通过分子对接建立了一系列含二氟甲基磷酸基团(DFMP)或二氟甲基硫酸基团(DFMS)的抑制剂与酪氨酸蛋白磷酸酯酶1B(PTP1B)的相互作用模式, 并通过1 ns的分子动力学模拟和molecular mechanics/generalized Born surface area (MM/GBSA)方法计算了其结合自由能. 计算获得的结合自由能排序和抑制剂与靶酶间结合能力排序一致; 通过基于主方程的自由能计算方法, 获得了抑制剂与靶酶残基间相互作用的信息, 这些信息显示DFMP/DFMS基团的负电荷中心与PTP1B的221位精氨酸正电荷中心之间的静电相互作用强弱决定了此类抑制剂的活性, 进一步的分析还显示位于DFMP/DFMS基团中的氟原子或其他具有适当原子半径的氢键供体原子会增进此类抑制剂与PTP1B活性位点的结合能力.