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.     

用模型拟合法研究1,2-聚丁二烯分子运动

本文采用Cole-Cole,Fuoss-Kirkwood经验相关时间分布模型和构象跳跃,高聚物局部主链运动阻尼取向扩散分子模型,对1,2-聚丁二烯在溶液中的~(13)C-NMR自旋-晶格弛豫时间nT_1和核Overhauser效应(NOE)值进行了数值拟合。用拟合所得分子运动参数讨论了1,2-聚丁二烯微观分子运动对链结构和温度的依赖性。     

聚合物链构象的研究 II: 1,2-聚丁二烯的构象特征和链分子的特征比

基于Flory的链分子统计理论, 用MM2分子力学程序改进了1,2-聚丁二烯构象分析,同时讨论了温度的影响. 着重考查了全同1,2-聚丁二烯特征比随能量的变化规律, 并且注意到聚苯乙烯, 聚丙烯酸甲酯等全同链的特征比按相似规律变化, 从而表现了聚烯烃全同链的共同特征.     

裂解色谱法(PGC)分析聚丁二烯分子链结构

近年来热裂解色谱法(PGC)发展不断完善,已成为高分子结构分析的有力手段。利用PGC法对聚丁二烯分子链结构的研究已有很多报导。庄野曾提出用VCH/BD(克分子比)表征聚丁二烯分子链中1,4-结构的含量;Perry通过对1,2-和1,4-结构的聚丁二烯热裂解反应研究,建议用C_2/BD表征聚丁二烯分子链中1,2/1,4结构克分子比。但由于方法的     

聚合物链构象的研究 Ⅱ.1,2-聚丁二烯的构象特征和链分子的特征比

基于Flory的链分子统计理论,用MM2分子力学程序改进了1,2-聚丁二烯构象分析,所得能量E_η和E_(ω″)更加合理,表征聚合物构象特征的统计权重矩阵中各项参数是:η=1.0exp(-E_η/RT),τ=0.8exp(-3340/RT),ω=1.4exp(-7320/RT),ω′=-1.1exp(-4390/RT)和ω″=-1.0exp(-E_(ω″)/RT).同时讨论了温度对这些参数的影响.着重考查了全同1,2-聚丁二烯特征比随能量E(E_η+E_(ω″))的变化规律,并且注意到聚苯乙烯,聚丙烯酸甲酯等全同链的特征比按相似规律变化,从而表现了聚烯烃全同链的共同特征.     

分子结构对1,2-聚丁二烯橡胶性能的影响

本文研究了分子链结构、分子量及其分布对钼催化聚合1,2-聚丁二烯(1,2-PB)的加工工艺性能及硫化胶性能的影响.实验发现,1,2-PB的加工工艺行为随分子量降低和分子量分布加宽而得以改善,其抗湿滑性能随分子链中1,2-结构含量增加而提高,而1,2-结构的空间规整性—间同含量的增加则导致1,2-PB应变诱导结晶、降低硫化胶的弹性和增加生热值。     

1,2-聚丁二烯分子链的结构和内旋转运动

实验订定了1,2-链节含量分别为8％,30％和90％的1,2-聚丁二烯在30℃甲苯溶液中的Mark-Houwink方程[η]=KM~(?)。发现不同样品的α值基本相同,而K值确实随1,2-链节含量的增加而减小,说明溶液中分子链线团变得紧密了。用线膨胀法和Stockmayer-Fixman方程及分子链的统计力学方法,分别得到了样品的玻璃化温度T_g,和它们的分子链内旋转空间位阻因子σ。它们二者符合T_g=A(σ—b),其中A=174(K),b=0.68。反映了1,2-链节对分子链内旋转的阻碍作用。进一步的研究表明,低1,2-链节含量对应着较低的分子链内旋转势垒和内旋转异构化能。     

聚合物分子链的横截面积与分子链的运动

本文把单个分子链的横截面积与聚合物的玻璃化转变温度联系起来,发现对于所讨论的聚合物,考虑了分子链间的相互作用以后,上面二者之间有一一对应的关系。认为单个分子链的横截面积与聚合物分子链柔顺性有关。同时采用文献[17]的方法,得到了1,2-聚丁二烯的分子链的内旋转异构化能,比较所得结果,证实了上面的看法。     

铁体系催化丁二烯聚合的研究——Ⅲ.聚丁二烯的分子量调节及性能

<正> 顺丁橡胶与丁苯橡胶在性能上的差别,在于其分子主链上缺少象苯基那样的侧基。而中乙烯基聚丁二烯的分子主链上有相当数量的乙烯基侧基,它弥补丁顺丁胶的不足之处。故日益受到人们的注意。目前,已工业化的中乙烯基聚丁二烯所用的催化剂为烷基锂体系,其聚合物除了1,2-结构外,其余部分反-1,4结构占多数。我们在前文曾经报     

含反式-1,4和间规-1,2链节的聚丁二烯X-射线衍射谱分析

<正> 近年来陆续出现在顺式-1,4聚丁二烯分子链中引入室温下可结晶的反式-1,4及间规-1,2聚丁二烯链节,以期改善顺丁橡胶的抗撕裂性和抗弯曲性等。有关这方面的结构表征工作尚很少报道。本工作用广角X-射线衍射(WAXD)方法,对钒、钴催化体系合成的含反式-1,4及钴催化体系合成的含间规-1,2的顺丁橡胶进行了结构表征。     

Conformational properties of methyl vinyl sulfone: Ab initio geometry optimization and vibrational analysis

An ab initio conformational analysis of methyl vinyl sulfone (CH₂CHSO₂CH₃) has been carried out. Molecular geometry optimizations have been performed at the HF and MP2 levels of the theory. Relative energies of the stationary points have been determined by using different approaches, including electron correlation corrections up to the third order. The IR and Raman spectra of the liquid have been measured and a vibrational assignment is proposed. The height of the barrier to the methyl group internal rotation has been estimated. Theoretical calculations and vibrational spectra have shown that the predominant conformation of methyl vinyl sulfone has the C=C bond eclipsed with one of the S=O bonds. Similar eclipsed forms have been found in vinyl fluoro sulfone, vinyl chloro sulfone and divinyl sulfone by ab initio HF calculations.     

Conformational properties of polar polymers. I. Poly(vinyl chloride)

A recently developed method for including polar bonds in conformational energy calculations is applied to poly(vinyl chloride). Inductive effects on dipole moments and the effects of intervening atoms on electrostatic interaction energies are represented by polarizability centers in conjunction with bond centered dipoles. Solvation energies are estimated by means of a continuum dipole–quadrupole electrostatic model. Calculated energies of a number of conformations of meso and racemic 2,4-dichloropentane and the iso, syndio, and hetero forms of 2,4,6-trichloroheptane give satisfactory representations of isomer and conformer populations. Electrostatic effects are found to be quite important. However they appear to be effectively of sufficiently short range that the calculated conformer energies are found to be fit well by a linear combination of interaction parameters (consisting of gauche, skew chlorine, four-bond CH₂…CH₂, CH₂…Cl, and Cl…Cl interactions) conventional to vinyl polymers and a special four-bond interaction that arises when the bond sequence Cl? CH? CH²? CH? Cl is (nearly) coplanar. These interaction parameters when assembled into statistical weight matrices lead to calculated values of both the characteristic ratio and the dipole moment ratio in satisfactory agreement with experiment. Least energy paths for transitions between the most stable conformations are also calculated.     

单嘧磺隆晶体-活性构象转换的分子动力学模拟

应用分子动力学模拟方法对单嘧磺隆在水、正辛醇和正辛烷3种不同溶剂中的构象行为、单嘧磺隆与3种溶剂之间的相互作用能及氢键相互作用进行了计算研究. 计算结果表明, 在3种不同的溶剂中, 单嘧磺隆的优势构象不同; 其构象转换过程, 特别是转换成活性构象的过程主要发生在水溶液中; 与溶剂分子间的相互作用是分子构象行为的决定因素; 单嘧磺隆的脲桥部分可以和含氢键接受体的溶剂形成氢键, 分子间与分子内氢键的竞争可能是从晶体构象转换成活性构象的主要驱动力.     

Temperature-induced dynamical conformational disorder in 4-vinyl benzoic acid molecular crystals: a molecular simulation study

Extensive molecular simulations are carried out as a function of temperature to understand and quantify the conformational disorder in molecular crystals of 4-vinyl benzoic acid. The conformational disorder is found to be dynamic and associated with a flip-flop motion of vinyl groups. The population of minor conformer is less than 3% up to 300 K and is 13.2% at 350 K and these results are consistent with the experimental observations. At still higher temperatures, the population of minor conformer increases up to 25%. The evolution of structure at both molecular and unit-cell level of the molecular crystal as a function of temperature has been characterized by various quantities such as radial distribution functions, average cell parameters, volume, and interaction energies. The van't Hoff plot shows a nonlinear behavior at lower temperatures as it has been reported recently by Ogawa and co-workers in the case of stilbene, azobenzene, and N-(4-methylbenzylidene)-4-methylaniline molecular crystals. A set of rigid body simulations were also carried out to quantify the effect of conformational disorder on structural quantities such as unit-cell volume and interaction energy. The anomalous shrinkage of vinyl C=C bond length as a function of temperature has been explained by combining the results of simulations and a set of constrained optimizations using ab initio electronic structure calculations for various molecular structures differing in torsional angle.     

4‐Vinyl­benzoic acid and 9‐vinyl­anthracene

The crystal structures of two styrene analogues, 4‐vinyl­benzoic acid, C₉H₈O₂, (I), and 9‐vinyl­anthracene, C₁₆H₁₂, (II), were determined by X‐ray analyses at 108 and 293 K for (I) and at 123 and 293 K for (II). In (I), a pair of mol­ecules around an inversion center form a dimer connected by two carboxyl groups. The anthracene planes of two mol­ecules in (II) are antiparallel to each other around an inversion center. The vinyl group of (I) is almost coplanar with the phenyl ring, whereas the vinyl group of (II) is nearly perpendicular to the anthracene plane. In (I), the bond length of the vinyl group at 293 K is significantly shorter than that at 108 K [1.288 (2) versus 1.3248 (14) Å] suggesting a bias of the thermal motion, whereas the bond lengths are not so different between the two temperatures in (II) [1.3266 (15) versus 1.310 (2) Å].     

Effect of fluorination: gas-phase structures of N,N-dimethylvinylamine and perfluoro-N,N-dimethylvinylamine.

The gas-phase structures of N,N-dimethylvinylamine, (CH(3))(2)NC(H)=CH(2) (1), and perfluoro-N,N-dimethylvinylamine, (CF(3))(2)NC(F)=CF(2) (2), were determined by gas electron diffraction and quantum chemical methods (B3LYP and MP2 with 6-31G basis sets). The configuration around nitrogen is slightly pyramidal in both compounds, with the sum of the nitrogen bond angles 351.2(12) degrees and 354.8(6) degrees in 1 and 2, respectively. In the parent compound 1, the (CH(3))(2)N group lies nearly in the plane of the vinyl group, and the nitrogen lone pair (lp) is almost perpendicular to this plane (Phi(C=C-N-lp) = 98(6) degrees). In the perfluorinated species 2, however, the (CF(3))(2)N group is oriented perpendicular to the vinyl plane, and the lone pair is parallel to the C=C bond (Phi(C=C-N-lp) = 2(5) degrees). A natural bond orbital analysis provides a qualitative explanation for this conformational change upon fluorination. The sterically unfavorable in-plane orientation of the dimethylamino group in 1 is stabilized by conjugation between the nitrogen lone pair and the C=C pi-bond. The anomeric effect between the lone pair and the C(alpha)-F sigma-bond in addition to steric effects favors the perpendicular orientation of the (CF(3))(2)N group in 2. Both quantum chemical methods reproduce the experimental structures satisfactorily.     

Catalyzed intramolecular olefin insertion into a carbon-carbon single bond

Intramolecular insertion of a C-C double bond into a C-C single bond was achieved by treatment of cyclobutanone bearing an o-styryl group at the 3-position with a catalytic amount of a cationic rhodium(I)-dppp complex. Initially, rhodium is inserted between the carbonyl carbon and the alpha-carbon of the cyclobutanone. Intramolecular coordination of the vinyl group results in its migratory insertion into the C-Rh linkage. Reductive elimination affords benzobicyclo[3.2.1]octan-3-one. Notably, a ring-opened alpha,beta-unsaturated ketone was obtained when dppe was used instead of dppp. In this reaction, rhodium cleaved the bond between the alpha sp3 carbon and the beta sp3 carbon of the cyclobutanone. The coordinating vinyl group directs this new regioselectivity of cleavage observed with the dppe ligand.     

Rhodium‐Catalyzed Cascade Reaction of 1,6‐Enynes Involving Addition,Cyclization, and β‐Oxygen Elimination

The reaction of arylboronic acids with 1,6‐enynes that contain an allylic ether moiety is catalyzed by a rhodium(I) complex to produce cyclopentanes with a tetrasubstituted exo olefin and a pendant vinyl group. The reaction is initiated by the regioselective addition of an arylrhodium(I) species to the carbon–carbon triple bond of the 1,6‐enyne. The resulting alkenylrhodium(I) compound subsequently undergoes intramolecular carborhodation of the allylic double bond in a 5‐exo‐trig mode. β Elimination of the methoxy group affords the cyclization product and the catalytically active methoxorhodium(I) species. The use of alkyl Grignard reagents instead of arylboronic acids as organometallic nucleophiles was also examined.     

Dynamics of proton exchange in a model phosphonic acid‐functionalized polymer

The dynamics and mechanism of proton exchange in phosphonic acid‐functionalized polymers were studied using poly(vinyl‐phosphonic acid) (PVPA) as a model system along with quantum chemical calculations and Born–Oppenheimer molecular dynamics (BOMD) simulations at the B3LYP/TZVP level as model calculations. This theoretical study began with searching for the smallest, most active polymer segments and their intermediate conformations which could be involved in the local proton‐exchange process. The B3LYP/TZVP results confirmed that a low local dielectric environment and excess proton conditions are required to generate the intermediate conformations, and the shapes of the potential energy curves of the proton exchange between the two phosphonic acid functional groups are sensitive to the local conformational changes. In contrast, a high local dielectric environment increases the energy barriers, thereby preventing the proton from returning to the original functional group. Based on the static results, a mechanism for the proton exchange between the two functional groups involving fluctuations in the local dielectric environment and a local conformational change was proposed. The BOMD results confirmed the proposed mechanism by showing that the activation energies for the proton exchange in the hydrogen bond between two immobilized phosphonic acid moieties, obtained from the exponential relaxation behaviors of the envelopes of the velocity autocorrelation functions and the ¹H Nuclear Magnetic Resonance (NMR) line‐shape analyses, are too low to be the rate‐determining process. Instead, coupled librational motion in the backbone which leads to the interconversion between the two intermediate conformations possesses higher activation energy, and therefore represents one of the most important rate‐determining processes. These findings suggested that the rate of the proton exchange in the model phosphonic acid‐functionalized polymer is determined by the polymer mobility which, in this case, is the large‐amplitude librational motion of the vinyl backbone. © 2015 Wiley Periodicals, Inc.     

Cycloalkane and cycloalkene C-H bond dissociation energies

Both C-H bond dissociation energies for cyclobutene were measured in the gas phase (BDE = 91.2 +/- 2.3 (allyl) and 112.5 +/- 2.5 (vinyl) kcal mol-1) via a thermodynamic cycle by carrying out proton affinity and electron-binding energy measurements on 1- and 3-cyclobutenyl anions. The results were compared to those for an acyclic model compound, cis-2-butene, and provide the needed information to experimentally establish the heat of formation of cyclobutadiene. Chemically accurate G3 and W1 calculations also were carried out on cycloalkanes, cycloalkenes, and selected reference compounds. It appears that commonly cited bond energies for cyclopropane, cyclobutane, and cyclohexane are 3 to 4 kcal mol-1 too small and their pi bond strengths, as given by BDE1 - BDE2, are in error by up to 8 kcal mol-1.