二氯卡宾与甲醇及甲硫醇插入与氢抽提反应的量子化学计算

利用密度泛函和自然键轨道理论及电子密度拓扑分析方法，对单、三重态CCl2与CH3MH（M=O，S）中C—H和M—H键的插入反应及抽提氢反应进行了研究．在B3LYP／6-311G（d，p）水平上优化了势能面上构型，并以频率分析和内禀反应坐标法进行了确认．计算了各物种的CCSD（T）／6-211G（d，p）能量．结果表明，主反应通道主要发生在单重态势能面中，单重态CCl2既可以与C-H及M—H键发生插入反应，存在四条主反应通道，分别生成P1[CH3OCHCl2，反应Ⅰ（1）]，P3[Cl2HCCH2OH，反应Ⅰ（2）]和PS[CH3SCHCl2，反应Ⅱ（1）]，P7[Cl2HCCH2SH，反应Ⅱ（2）]，也可以与CH3MH发生抽提氢反应，分别生成P4[CH2O＋CH2Cl2，反应Ⅰ（3）]和P8[CH2S＋CH2Cl2，反应Ⅱ（3）]．同时，存在三重态CCl2与CH3SH插入生成^3P4[CH3SCHCl＋Cl]的反应通道．进一步对反应通道上的关键点进行了自然键轨道和电子密度拓扑分析．     

三氯化铝固载化的新方法

Al Cl3是化工、石油炼制和制药工业中广泛应用的重要催化剂之一 .但由于它具有腐蚀性 ,与产物分离麻烦以及产生大量污水等缺点 ,其使用日益受到限制 .为解决上述问题 ,人们对其固载化进行了长达 50多年的研究 ,研究的重点是通过化学反应把 Al Cl3嫁接到 γ-Al2 O3和 Si O2 等常用载体上 .主要方法有两种 :一种是气 -固反应法 [1～ 4 ] :先将 Al Cl3升华 ,再与固体载体反应 ;另一种是溶剂反应法[5～ 6] :将 Al Cl3溶解于 CCl4 ,CHCl3等溶剂中 ,通过浸泡、回馏等方法使 Al Cl3与固体载体反应 .一般认为 ,Al Cl3固载化机理是 Al Cl3…     

[Sm(CH_3CN)_9]·(AlCl_4)3·CH_3CN的合成和晶体结构

关于过渡金属乙腈配合物的合成和催化性能的研究在文献中已有很多报道。但是,含稀土元素的这类配合物的合成及催化性能的研究直到1986年才见报道。Thomas利用金属Eu和NOBF_4在乙腈中的反应制得了配合物[Eu(CH_3CN)_3(BF_4)_3]_x。本文报道了新乙睛稀土配合物[Sm(CH_3CN)_9]·(AlCl_4)_3·CH_3CN的合成及其晶体结构与分子结构。 (一) 实验 所有操作都在氩气保护下进行。无水SmCl_3用NH_4Cl法制得。AlCl_3经升华后使用。CH_3CN经P_2O_5干燥蒸馏。IR用Perkin-Elmer FTS-20红外光谱仪测定。     

CCl4的光解微观机制研究

利用激光光解瞬态吸收光谱技术,研究有氧和无氧条件下CCl4的激光光解.结果表明,在248 nm激光作用下, CCl4发生了单光子吸收,反应生成{CCl4－Cl}σ电荷转移复合物、(CCl3＋…Cl－)离子对、CCl3O2过氧自由基等瞬态物种,它们的衰减过程是表观一级反应. {CCl4－Cl}σ电荷转移复合物在有氧/无氧条件下的拟合衰减速率常数分别是3.38×106 s－1和3.65×106 s－1,它的形成不受氧气含量影响. (CCl3＋…Cl－)离子对在有氧/无氧条件下的拟合衰减速率分别为3.73×107 s－1和3.02×107 s－1,它的形成也不受氧气含量影响, CCl3O2过氧自由基需在有氧条件下形成,拟合衰减速率是2.32×104 s－1.     

（±）—1—[（2—羟基基—5—甲基苯基）（苯基）甲基]—2—吡啶苯并咪唑的合成及晶体结

自 Hobrecker通过还原 2 -硝基 -4 -甲基乙酰苯胺得到 2 ,5 -二甲基苯并咪唑后 ,苯并咪唑化合物一直NNNCH3HOScheme 1　 Structure of compound 1被人们关注[1] .近年来 ,此类杂环化合物的合成及其生物活性的研究日益成为杂环化学研究的热门课题 [2～ 4 ] .文献 [5～ 9]报道 ,苯并咪唑具有广谱的生物活性及其它用途 .因此 ,对这类化合物的合成及其性质的研究具有广阔的开发前景 .本文通过不对称双Schiff碱中氢原子的重排与成环 ,合成了一种新的外消旋苯并咪唑衍生物 (1 ,结构见 Scheme1 ) ,并报道其晶体结构 .1　实验部分1 .1　仪器与…     

固相配位化学反应研究ⅩⅩⅩⅩⅢ.[Co(NH_3)_4CO_3]Cl、[Co(en)_2CO_3]Cl与NH_4SCN的固相取代反应

本文研究了[Co(NH_3)_4CO_3]Cl、[Co(en)_2CO_3]C1分别与NH_4SCN在100℃发生的固相取代反应.[Co(NH_3)_4CO_3]Cl与NH_4SCN反应生成trans-[Co(NH_3)_4(NCS)_2]~+;[Co(en)_2CO_3]Cl与NH_4SCN反应先生成cis-[Co(en)_2(NCS)_2]~+,然后转化成trans-(Co(en)_2(NCS)_2]~+。采用气相色谱、红外光谱、X粉末衍射和核磁共振法对相应反应体系及其产物进行了测试,推测反应按S_(N~2)机理进行。     

La(ClO4)3-BAPOAP-H2O(30 ℃)三元体系的相平衡和Ln2(BAPOAP)3(ClO4)6的合成与表征

安替比林 ( AP)衍生物可用于稀土的分析测定及协同萃取[1] ,安替比林稀土配合物的合成 [2 ] 及其发光性质和磁学性质等 [3,4 ]的研究已有报道 .在对具有芳基侧链的 4- (邻氯苯甲酰基 )氨基安替比林 [5]、4- (对氯苯甲酰基 )氨基安替比林 [6] 及长链桥联的 N ,N -二安替比林 - 1 ,6-己二酰二胺[7,8] 等与稀土盐相互作用进行研究的基础上 ,本文对短链桥联的 N,N -二安替比林乙二酰二胺与镧系高氯酸盐在水溶液中全浓度范围内的相互作用进行了研究 .1　实验部分1 .1　试剂及仪器　L a( Cl O4 ) 3· 8H2 O用 La2 O3( 99.9% )和 1∶ 1高氯…     

三种离子液体的合成及其对棉纤维素溶解性能的比较研究

合成了三种含有羧基或醚基的离子液体, 1-羧甲基-3-乙基咪唑氯化物([CmEIM]Cl)、1-甲氧乙基-3-乙基咪唑氯化物([C2OC1-EIM]Cl)和1-[2-(2-氯乙氧基)乙基]-3-乙基咪唑氯化物([Cl-C2OC2-EIM]Cl), 用FT-IR和1H NMR对它们的化学结构进行了表征. 测定并比较了这三种离子液体对棉纤维素的溶解能力, 并用FT-IR, SEM和XRD研究了溶解前和再生后纤维素的化学结构、形貌及晶体结构的变化. 结果表明, 在三种离子液体中, [C2OC1-EIM]Cl对棉纤维素的溶解性最好. 在溶解过程中, 随着温度的升高, 纤维素在离子液体中的溶解度增加, 但聚合度下降, 特别是在[Cl-C2OC2-EIM]Cl中溶解时, 纤维素的聚合度下降最严重. 研究结果表明, 含羧基的离子液体会由于分子间氢键的缔合作用降低其对纤维素的溶解性. 侧基较大的离子液体对纤维素的溶解性也较差.     

超声辐射下二(2''''-氯喹啉)-乙二醇的合成

()呐醇是有机合成中的重要中间体[1],广泛应用于农药、医药等精细化工品的合成;作为能够构建碳碳键的一个重要反应,羰基化合物还原偶联为()呐醇的反应一直是有机合成领域中的一个重要研究课题;同时又形成了两个手性中心,光学活性的邻二醇可作为手性配体广泛应用于手性拆分与不对称合成,特别是在生物活性的天然化合物[2]的合成.1973年,Mukaiyama[3]首次将低价钛运用于醛酮的还原偶联反应,此后随着还原体系的改进和扩充,利用低价钛配合物合成()呐醇的研究也在逐步深入,近年来已有诸多文献报道[4,5].     

尾式金属卟啉配合物的研究IV: 含氮配体与尾式铁(III)卟啉轴向配位反应热力学及其配位模式

用分光光度法研究了咪唑或吡啶类配体与5-[邻-(4-(1-咪唑基)丁氧基)苯基]-10,15,20-三苯基卟啉合铁(III)氯化物[[Fe^I^I^I(ImTPP)]Cl]和5-[对-(4-(3-吡啶氧基)丁氧基)苯基]10,15,20-三苯基卟啉合铁(III)氯化物[[Fe^I^I^I(PyTPP)]Cl]两种尾式铁(III)卟啉的轴向加合作用, 测定了平衡常数、热力学参数及含氮配体的加合分子数。结果表明, [Fe^I^I^I(PyTPP)Cl与[Fe^I^I^I(TPP)]Cl相类似, 均与咪唑、吡啶类配体生成1:2低自旋六配位加合物。含氮配体与[Fe^I^I^I(ImTPP)]Cl的轴向加合反应平衡常数比与{Fe^I^I^I(TPP)]Cl相应的平衡常数大10-10^3倍, 这是因为含氮配体与[Fe^I^I^I(ImTPP)]Cl的轴向配位诱导了尾端咪唑基与配合物中的Fe^I^I^I离子的轴向配位, 这种配位横式增强了含氮配体与Fe^I^I^I离子的键合; 尾端咪唑基与配合物中的Fe^I^I^I离子配位的模式得到了UV-vis、^1H NMR及EPR实验数据的进一步证实。     

Mixed-metal single-molecule magnets: Syntheses, structure, and magnetic properties of [Mn8Fe4O12(O2CR)16(H2O)4] (R = CH2Cl, CH2Br, CHCl2)

Three mixed-metal single-molecule magnets containing [Mn₈Fe₄O₁₂]¹⁶⁺ cores are synthesized and characterized. The reaction of FeCl₂·4H₂O with KMnO₄ and RCOOH (R = CH₂Cl, CH₂Br) in H₂O gives [Mn₈Fe₄O₁₂(O₂CR)₁₆(H₂O)₄] (R = CH₂Cl (1), CH₂Br (2)) in yields of 43% and 40%, respectively. Treatment of complex 1 with an excess of CHCl₂COOH in CH₂Cl₂ gives [Mn₈Fe₄O₁₂(O₂CCHCl₂)₁₆(H₂O)₄]·CH₂Cl₂·10H₂O (3·CH₂Cl₂·10H₂O) in a yield of 83%. The X-ray structure analysis reveals that all three complexes consist of a trapped-valence dodecanuclear core comprising 4Mn^III, 4Fe^III, and 4Mn^IV ions. DC magnetic susceptibility and magnetization measurements indicate that all three complexes exhibit intramolecular antiferromagnetic interaction, resulting in an S = 4 ground state. In addition, frequency-dependent out-of-phase AC magnetic susceptibility signals at low temperature for complexes 1, 2, and 3 are indicative of their single-molecule magnetism behavior.     

The standard free energy of formation of YbFe2O4, Yb2Fe3O7, YbFeO3, and Yb3Fe5O12 at 1200°C

The standard free energy of formation of YbFe₂O₄, Yb₂Fe₃O₇, YbFeO₃, and Yb₃Fe₅O₁₂ from metallic iron, Yb₂O₃, and oxygen was determined to be ?100.38, ?158.38, ?58.17, and ?283.40 kcal/mole, respectively, at 1200°C on the basis of the phase equilibria in the FeFe₂O₃Yb₂O₃ system. The FeFe₂O₃-Lanthanoid sesquioxide systems were classified into four types with respect to the assemblage of the ternary compounds in stable existence at 1200°C, and the standard free energy of formation of YbFeO₃ was compared with those of the other lanthanoid-iron perovskites.     

Syntheses, crystal structures and optical properties of the first strontium selenium(IV) and tellurium(IV) oxychlorides: Sr3(SeO3)(Se2O5)Cl2 and Sr4(Te3O8)Cl4

Two new quaternary strontium selenium(IV) and tellurium(IV) oxychlorides, namely, Sr₃(SeO₃)(Se₂O₅)Cl₂ and Sr₄(Te₃O₈)Cl₄, have been prepared by solid-state reaction. Sr₃(SeO₃)(Se₂O₅)Cl₂ features a three-dimensional (3D) network structure constructed from strontium(II) interconnected by Cl⁻, SeO₃²⁻ as well as Se₂O₅²⁻ anions. The structure of Sr₄(Te₃O₈)Cl₄ features a 3D network in which the strontium tellurium oxide slabs are interconnected by bridging Cl⁻ anions. The diffuse reflectance spectrum measurements and results of the electronic band structure calculations indicate that both compounds are wide band-gap semiconductors.     

Crystal structure and magnetic properties of Co2TeO3Cl2 and Co2TeO3Br2

The crystal structures of the two new synthetic compounds Co₂TeO₃Cl₂ and Co₂TeO₃Br₂ are described together with their magnetic properties. Co₂TeO₃Cl₂ crystallize in the monoclinic space group P2₁/m with unit cell parameters a=5.0472(6) Å, b=6.6325(9) Å, c=8.3452(10) Å, β=105.43(1)°, Z=2. Co₂TeO₃Br₂ crystallize in the orthorhombic space group Pccn with unit cell parameters a=10.5180(7) Å, b=15.8629(9) Å, c=7.7732(5) Å, Z=8. The crystal structures were solved from single crystal data, R=0.0328 and 0.0412, respectively. Both compounds are layered with only weak interactions in between the layers. The compound Co₂TeO₃Cl₂ has [CoO₄Cl₂] and [CoO₃Cl₃] octahedra while Co₂TeO₃Br₂ has [CoO₂Br₂] tetrahedra and [CoO₄Br₂] octahedra. The Te(IV) atoms are tetrahedrally [TeO₃E] coordinated in both compounds taking the 5s² lone electron pair E into account. The magnetic properties of the compounds are characterized predominantly by long-range antiferromagnetic ordering below 30 K.     

Synthesis, crystal structure and magnetic property of a new nickel selenite chloride: Ni5(SeO3)4Cl2

The new nickel selenite chloride, Ni₅(SeO₃)₄Cl₂, was obtained by high-temperature solid state reaction of NiCl₂, Ni₂O₃ and SeO₂ in a 1:2:4 molar ratio at 700 °C in an evacuated quartz tube. Its structure was established by single-crystal X-ray diffraction. Ni₅(SeO₃)₄Cl₂ crystallizes in the triclinic system, space group P-1 (No. 2) with cell parameters of a=8.076(2), b=9.288(2), c=9.376(2) Å, α=101.97(3), β=105.60(3), γ=91.83(3)° and Z=2. All nickel(II) ions in Ni₅(SeO₃)₄Cl₂ are octahedrally coordinated by selenite oxygens or/and chloride anions (([Ni(1)O₅Cl], [Ni(2)O₄Cl₂], [Ni(3)O₅Cl], [Ni(4)O₆] and [Ni(5)O₄Cl]). The structure of the title compound features a condensed three-dimensional (3D) network built by Ni(II) ions interconnected by SeO₃²⁻ anions as well as Cl⁻ anions. Magnetic property measurements show strong antiferromagnetic interaction between nickel(II) ions.     

35Cl Nqr spectroscopy of the [PO2Cl2]− and POCl3 groups in Me(PO2Cl2)2·2D (Me = Mg,Ca, Mn; D = POCl3,CH3COOC2H5,CH3COCH3)

³⁵Cl NQR spectra of dichlorophosphates Me(PO₂Cl₂)₂ · 2D (Me = Mg, Ca, Mn; D = CH₃COOC₂H₅, CH₃COCH₃, POCl₃) are studied in the temperature range 77 ? T (K) ? 305. It is shown that the three compounds with CH₃COOC₂H₅ as donor are isomorphic at 77 K, the crystal structure of Mn(PO₂Cl₂)₂· 2CH₃COOC₂H₅. The structure of Mg(PO₂Cl₂)_2^?· 2CH₃COCH₃ and of Mg(PO₂Cl₂)₂ · 2POCl₃ probably consists of infinite chains as found for Mn(PO₂Cl₂)₂· 2CH₃COOC₂H₅. Mg(PO₂Cl₂)₂· 2CH₃COOC₂H₅ shows phase transformations and a complicated dynamical behaviour leading to strong deviations from a Bayertype NQR function v = f(T). The donor capacity of POCl₃ in Mg(PO₂Cl₂)₂· 2POCl₃ is comparable with the donor strength in AsCl₃ · POCl₃ · A d_π-p_π overlap of the P-O bond influences the P-Cl bond.     

Beam-gas chemiluminescent reactions of Cu(2D) with Cl2, Br2, and I2

Chemiluminescent reactions involving copper and halogen molecules are shown to result from the bimolecular reaction of metastable Cu(²D) with Cl₂, Br₂, and I₂ under single-collision conditions. The collision-energy dependence of the reactions is described by a hard-sphere model with zero threshold energy. Cross sections for these reactions are compared with that for chemiluminescent reaction of Cu(²S) with F₂.     

Synthesis and characterization of ionic organotin compounds [R2SnCl2(2-quin)](HNEt3) and crystal structures of [(2,4-Cl2-C6H3CH2)2SnCl2(2-quin)](HNEt3)

Eight ionic organotin compounds [R₂SnCl₂(2-quin)]⁻(HNEt₃)⁺ have been synthesized by reactions of 2-quinH with R₂SnCl₂ (R = PhCH₂1, 2-Cl-C₆H₄CH₂2, 4-Cl-C₆H₄CH₂3, 2-F-C₆H₄CH₂4, 4-F-C₆H₄CH₂5, 4-CN-C₆H₄CH₂6, Ph 7, 2,4-Cl₂-C₆H₃CH₂8) in the presence of organic base NEt₃, and their structures have been characterized by elemental analysis, IR and multinuclear NMR (¹H, ¹³C, ¹¹⁹Sn) spectroscopies. The structure of [(2,4-Cl₂-C₆H₃CH₂)₂SnCl₂(2-quin)]⁻(NEt₃)⁺ (8) has been determined by X-ray diffraction study. Studies show that compound 8 has a monomeric structure with the central tin atom six-coordinate in a distorted octahedral configuration and the nitrogen atoms of the 2-quin ligands are coordinating to the tin atom in all the eight compounds.     

A new ferroelastic transition in some A2(MO4)3 molybdates and tungstates

We have found for the first time a ferroelastic transition in many molybdates and tungstates with the Sc₂(MoO₄)₃-type structure. Below the transition these phases are monoclinic ($\text{P2}{}_1\text{a}$), and above the transition they are orthorhombic (Pnca). Observed transition temperatures are: Al₂(MoO₄)₃, 200°C; Al₂(WO₄)₃, ?6°C; Cr₂(MoO₄)₃, 385°C; Fe₂(MoO₄)₃, 499°C; In₂(MoO₄)₃, 335°C; In₂(WO₄)₃, 252°C; and Sc₂(MoO₄)₃, 9°C.     

Standard free energy of formation of YFeO3, Y3Fe5O12, and a new compound YFe2O4 in the FeFe2O3Y2O3 system at 1200°C

The phase equilibria in the FeFe₂O₃Y₂O₃ system have been established at 1200°C. The following phases were stable: yttria, hematite, magnetite, wüstite, metallic iron, yttrium-iron perovskite, yttrium-iron garnet, and a new phase YFe₂O₄, belonging to a rhombohedral crystal system. The YFe₂O₄ compound has a solid solution from YFe₂O_3.905 to YFe₂O_4.000. The standard free energies of formation of YFe₂O_3.905, YFeO₃, and Y₃Fe₅O₁₂ have been determined to be ?96 800 ± 200 cal, ?59 800 ± 200 cal, and ?143 700 ± 600 cal, respectively, from metallic iron, Y₂O₃, and oxygen.