构象概论——甾体构象与其化学反应的关系(四)

Ⅴ.甾体的构象与其化性及稳定性的关系甾体骨架系属于菲烷并环戊烷 Cyclopentano-perhydrophenanthrene的四圜统系,除得第四圜是五碳圜其他之圜都是环己烷互相骈联起来的,既然环己烷已公认为椅形,故Barton将甾体的两种构型(A/B反式及A/B顺式)按照椅形列式如下(Ⅰ及Ⅱ),     

α-环糊精包合物中环己烷构象平衡的PM3研究

用PM3分子轨道方法研究了α-环糊精的包合作用对环己烷构象平衡的影响。发现α-环糊精的包合作用可以改变环己烷的构象平衡。计算结果表明,虽然环己烷的椅式构象比船式构象稳定18.5 kJ*mol-1, 但在α-环糊精的包合物中,船式环己烷包合物比椅式环己烷包合物稳定4.4 kJ*mol-1。因此,超分子体系中客体分子的构象平衡不能简单地从其游离态的构象平衡外推得到,而应该考虑在超分子体系中分子间相互作用对构象的影响。     

构象概论(一)——甾体构象与其化学反应的关系

1.环己烷及其衍生物的构象近年来有机化合物,除构造(constitution)、构型(configuration)的研究工作外,尚有所谓“con-formation”或德文命名constellation(暂译为构象)的研究工作或说明常常见诸文献。近来在甾体化学上已经证明若干甾体的化学反应与其分子各基团各部位的构象有密切的关系,因此我们逐渐地可以根据物质的构象,能深刻的了解若干化学反应,并且往往可以推定或预料反应的过程。欲述及此种构象与化性的关系,先须约略述及它的最基本的组成体环己烷的构象。环己烷一类物质,或者说含有环己烷的有机物为数极夥,其中若干物质例如碳水化合物、甾体、有机鹼、维生素等等,都是在生物上占重要的位     

[3,3]σ迁移反应过渡态立体化学过程的新观点

结合环己烷的构象与能量关系,讨论[3,3]σ迁移反应的立体化学过程。[3,3]σ迁移反应生成的主产物经过的是椅式过渡态,生成的次要产物经过的是扭船式过渡态,而不是以前认为的船式过渡态。     

扭船式——不应被忽视的环己烷构象

一、问题的提出环己烷有多少种构象异构体?它们的比例是多少?这个问题在国内目前的教科书中,不尽一致.在一些教材中,仍仅着眼于键角张力的影响.认为仅有两种极限构象,一种叫“椅式”,另一种叫“船式”.它不仅忽略了扭船式(twist),而且“极端”的提法也不准确,因为在能量-构象转变座标图上,它们并不处于两个极端,扭船式也不应看做是船式和椅式之间的过渡状态.关于各种构象在室温下的比例,说法有:船式:椅式=1∶1000,扭船式:椅式=1∶1000,扭船式:椅式=1∶10000等.本文想就究竟环己烷有几种异构体,在室温下,它们的比     

气相VO（∑＋）与CH3OH（1^A′）分子自旋禁阻反应C—H，O—H键活化机理的理论研究

采用密度泛函理论（DFT）B3LYP与cCsD方法研究了二重态和四重态势能面自旋禁阻反应VO（∑’）活化cH30H（1^A′）分子c—H,0—H键的微观机理．通过自旋一轨道耦合的计算讨论了势能面交叉点和可能的自旋翻转过程．在MEcP处,四重态和二重态问的旋轨耦合常数为131．14cm^-1．自旋多重度发生改变,从四重态系间穿越到二重态势能面形成中间体2^IM1,导致反应势能面的势垒明显降低．     

关于环己烷构象教学的探索

本文介绍了在有机化学教学中，从乙烷交叉式构象的锯马式及纽曼投影式出发，推导出环己烷的椅式和船式构象的准确书写方法，并外推到十氢萘，氢化菲的各构象式的准确表达形式，在教学中取得预期的效果。     

2—（4—氨酰基—2—噻唑基）—1,4—脱水—L—木糖醇及其氟代衍 …

用计算机分析模拟方法研究了２－（４－氨酰基－２－噻唑基）－１，４－脱水－Ｌ－木糖醇及其氟代衍生物的糖基构象，计算结果显示，６个碳核苷类似物的糖基构象均为Ｓ型。核磁共振谱和晶体Ｘ射线衍射结果与计算结果相吻合。     

聚合物链构象的研究I: 1,2-聚丁二烯的构象分析

本文应用Flory的链分子统计理论研究1,2-聚丁二烯的链构象,选择固定键长和键角的分子模型,计算构象能,构成势能面图,并由势能面的构型积分,得到了表征1,2-聚丁二烯链构象特征的统计权重矩阵.     

胃泌素有关肽溶液构象的2D-NMR研究

用2D NMR深入研究了五肽、四肽胃泌素在 DMSO 中的构象。利用 COSY 谱、Relayed-COSY 谱、DQF-J 分解谱和 NOESY 谱归属了全部共振峰。计算了肽键平面的Φ角、旋转异构体分布和旋转异构体之间自由能差。根据 NOESY 谱得到了距离约束条件。结合Φ角及旋转异构体分布, 推导出五肽胃泌素分子的构象膜型。结果表明, 五肽、四肽胃泌素在 DMSO 中以半角构象存在, 在其主要的旋转异构体中 Trp 的吲哚环和 Met 的 S 原子具有类似5,1-benzothiazocine 三维结构, 可能是具有生物活性的原因。     

Determination of the enthalpy of fusion of K<Subscript>3</Subscript>TaO<Subscript>2</Subscript>F<Subscript>4</Subscript> and KTaF<Subscript>6</Subscript>

Areas of fusion and crystallization peaks of K₃TaO₂F₄ and KTaF₆ were measured using the DSC mode of a high-temperature calorimeter (SETARAM 1800 K). On the basis of these quantities, considering the temperature dependence of the calorimeter sensitivity, values of the fusion enthalpy of K₃TaO₂F₄ at the fusion temperature of 1181 K of (43 ± 4) kJ mol⁻¹ and of KTaF₆ at the fusion temperature of 760 K of (8 ± 1) kJ mol⁻¹ were determined.     

Physicochemical foundations of synthesis of new ferromagnets from chalcopyrites A<Superscript>II</Superscript>B<Superscript>IV</Superscript>C<Stack><Subscript>2</Subscript><Superscript>V</Superscript></Stack>

The results of studying phase equilibria of ternary A^IIB^IVC^V systems have been reported. Physicochemical foundations have been developed for the synthesis of new ferromagnets with Curie temperatures above room temperature structurally compatible with basic semiconducting materials. Methods of synthesis and physicochemical properties of manganese-doped A^IIB^IVC₂^V ferromagnets have been described. The results of theoretical simulation of magnetic properties have been considered and basic approaches to the explanation of the emergence of ferromagnetism in A^IIB^IVC₂^V doped with 3d metals have been surveyed. The most promising ways to produce and study dilute magnetic semiconductors as spintronics materials have been presented.     

Determination of the enthalpy of fusion of K<Subscript>3</Subscript>NbO<Subscript>2</Subscript>F<Subscript>4</Subscript>

Areas of fusion and crystallization peaks of K₃NbO₂F₄ were measured using the DCS mode of a high-temperature calorimeter (SETARAM 1800 K). On the basis of these quantities, considering the temperature dependence of the calorimeter sensitivity, the value of the fusion enthalpy of K₃NbO₂F₄ of (98 ± 6) kJ mol⁻¹ was determined at the fusion temperature of 1257 K.     

Structure of Zn<Subscript>3</Subscript>P<Subscript>2</Subscript>

The structure of Z_n3P₂ (P 4₂/nmc, a = b = 8. 0785 Å, c = 11. 3966 Å) was solved and refined to R = 3. 2% in a precision X-ray diffraction experiment (λ-MoK _a, graphite monochromator on a primary beam, 27,496 reflections) . Interatomic distances and bond angles have been determined. The fcc lattice of the structure is built from phosphorus atoms, and the zinc atoms occupy 3/4 of all tetrahedral voids; the structure is described by two equivalent models where 1/4 occupied (by zinc atoms) and 1/4 vacant voids change places. The zinc atoms that occupy the voids following the diamond principle do not change places.Original Russian Text Copyright © 2004 by I. E. Zanin, K. B. Aleinikova, M. M. Afanasiev, and M. Yu. Antipin__________Translated from Zhurnal Strukturnoi Khimii, Vol. 45, No. 5, pp. 889–892, September–October, 2004.     

Coefficients of thermal expansion of KPb<Subscript>2</Subscript>Cl<Subscript>5</Subscript> and RbPb<Subscript>2</Subscript>Br<Subscript>5</Subscript> crystals

The temperature dependence of unit cell parameters for monoclinic KPb₂Cl₅ and tetragonal RbPb₂Br₅ crystals was studied in the range of 100–298 K. Linear and volume thermal expansion coefficients were determined.     

Effect of SO<Subscript>2</Subscript> on chlorination of Bi<Subscript>2</Subscript>O<Subscript>3</Subscript> + Fe<Subscript>2</Subscript>O<Subscript>3</Subscript> mixtures

The reaction of Bi₂O₃ + Fe₂O₃ mixtures with chlorine and SO₂ at 250–700°C is studied. At 300–500°C, the degree of bismuth chloride sublimation from the oxide mixture increases in the presence of SO₂. Chemical sublimation of FeCl₃ occurs after BiCl₃ is virtually completely recovered from the solid phase.     

2,4‐Di­nitro­phenyl­hydrazones of 2,4‐di­hydroxy­benz­aldehyde, 2,4‐di­hydroxy­aceto­phenone and 2,4‐di­hydroxy­benzo­phenone

In 2,4‐di­hydroxy­benz­aldehyde 2,4‐di­nitro­phenyl­hydrazone N,N‐di­methyl­form­amide solvate {or 4‐[(2,4‐di­nitro­phenyl)­hydrazono­methyl]­benzene‐1,3‐diol N,N‐di­methyl­form­amide solvate}, C₁₃H₁₀N₄O₆·C₃H₇NO, (X), 2,4‐di­hydroxy­aceto­phenone 2,4‐di­nitro­phenyl­hydrazone N,N‐di­methyl­form­am­ide solvate (or 4‐{1‐[(2,4‐di­nitro­phenyl)hydrazono]ethyl}benzene‐1,3‐diol N,N‐di­methyl­form­amide solvate), C₁₄H₁₂N₄O₆·C₃H₇NO, (XI), and 2,4‐di­hydroxy­benzo­phenone 2,4‐di­nitro­phenyl­hydrazone N,N‐di­methyl­acet­amide solvate (or 4‐­{[(2,4‐di­nitro­phenyl)hydrazono]phenyl­methyl}benzene‐1,3‐diol N,N‐di­methyl­acet­amide solvate), C₁₉H₁₄N₄O₆·C₄H₉NO, (XII), the molecules all lack a center of symmetry, crystallize in centrosymmetric space groups and have been observed to exhibit non‐linear optical activity. In each case, the hydrazone skeleton is fairly planar, facilitated by the presence of two intramolecular hydrogen bonds and some partial N—N double‐bond character. Each molecule is hydrogen bonded to one solvent mol­ecule.     

Phase diagram of V<Subscript>2</Subscript>O<Subscript>5</Subscript>-MoO<Subscript>3</Subscript>-Ag<Subscript>2</Subscript>O system

The results concerning the synthesis, structure and thermal properties of V₂O₅-MoO₃-Ag₂O samples in the vanadium rich region of ternary system are presented in the form of quasi-binary phase diagrams in which at constant V₂O₅/MoO₃ molar ratios, equal 9:1, 7:3 and 1:1, the content of Ag₂O was variable. A new ternary phase isostructural with NaVMoO₆ has been detected in the investigated system.