四氟乙烯-全氟4-甲基-3,6-二氧杂△~7辛基磺酰氟共聚物的分子运动

本工作用振簧仪,在-150—80℃范围内,测试了四氟乙烯-全氟4-甲基-3,6-二氧杂△~7辛基磺酰氟共聚物的动态力学性能。样品是含有不同侧基数目的部分结晶共聚物。观察到四个松弛过程,按温度下降次序记为α、γ_1-、γ_2-、γ_3-。α峰(室温附近)系玻璃化转变。γ_1峰(-50℃,～215Hz)为主链有阻碍的短链段分子运动。γ_2-峰(-60℃,～230Hz)为侧基的分子运动。γ_3-峰(-77℃,～260Hz)为的链段运动,并且γ_3-峰的强度随结晶度增加而增强。     

高速纺PET纤维结构第三态的初步探讨

本文应用计算分峰的原理,用系数不同的不对称高斯函数去分别表征PET纤维的中介态和无取向非晶态的X衍射,并在实验上设法把这两种衍射区分开来,从而建立了能够测算纤维中晶态、中介态和无取向非晶态的相对含量的方法。用这方法研究了高速纺PET拉伸丝在各温度下热处理时的结构,结果表明,纤维的结晶度随热处理温度升高而相应增加,但中介态含量、无取向非晶态含量及许多性质在130—160℃之间出现转折。作者从中介态在热理处时可能发生解取向松驰和发生结晶的综合变化加以解释,DSC的研究结果符合上述观点。     

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。     

一些有机铁硫原子簇配合物紫外光谱浓度效应的研究

在二氯甲烷溶剂中对有机铁硫原子簇配合物进行了紫外光谱(190～400 nm)研究发现,π-π~*跃迁紫外吸收峰的λ_(max)随溶液浓度的增加明显红移,而对含孤立C—S键或C—O键化合物未见明显移动。本文还研究了一些含n-π、π-π共轭化合物的紫外光谱,发现除π-π跃迁λ_(max)随溶液浓度增加红移外,π-π~*跃迁λ_(max)还随溶液浓度增加发生蓝移。     

最快结晶速率温度与结晶参数的关系

以经典的结晶速率与温度的关系为基础,对T_(c,max)与结晶参数的关系进行了研究.结果表明,T_(c,max)同平衡熔融温度(T_m)的比值仅与成核参数(φ)同扩散活化能(E_d)之比有关.高聚物的结晶过程可用二次成核模型近似.当结晶速率与温度的关系采用下式时 G=G_0exp[-E_d/RT-φT_m~2/T~2(T_m-T)]T_(c,max)与结晶参数的关系为 T_(c,max)=2/3T_m[1-(1+9α)~(1/2)cos(1/3)arccos1/(1+9α)~(3/2)+240°]或 α=φR/E_d=T_(c,max)(T_m-T_(c,max)~2/T_m?2(3T_(c,max)-2T_m)     

小麦条锈病对小麦产量影响的研究——Ⅱ.病害对小麦叶片光合作用的影响初探

利用红外线气体分析仪测定了冬小麦燕大1817和东方红3号在受到条锈菌(Puccinia striiformis West)侵染后叶片光合作用的变化。证明严重度S越高,残余健部光合作用极大值P′_(max)越低,其关系为P′_(max)=P′_(max)(1-0.826*S)。根据试验数据推导建立了条锈病导致的光合产物降低率预测模型:L_(光合)=1-(P_(max)+I_(1α))/(P′_(max)+I_(1α))(1-bS)(1-S),和理论模型L_(光合)=aS~n,n=f(P′_(max)/P_(max))。最后讨论了L_(光合)与验经产量损失模型的关系。     

铝酸钠溶液的紫外吸收峰

分别用量子化学MNDO和DV-X_α方法计算了二聚铝酸离子[Al_2O(OH)_6]~(2-)和Al(OH)_4~-。结果表明前者旋转势垒很低, 只有10.08 kJ·mol~(-1), 最稳定平衡构型为C_s。用X_α过渡态理论计算获得这两个离子紫外吸收峰的理论值分别为266.6 nm和234.4 nm, 与实验值270.0 nm和230.0 nm相当接近。因此可以认为, 紫外吸收峰270.0 nm和230.0 nm分别为[Al_2O(OH)_6]~(2-)和Al(OH)_4~-离子的最高占有轨道电子向最低空轨道跃迁时产生的吸收峰。计算结果支持铝酸钠溶液中存在二聚铝酸离子的观点。     

论文选摘

理论塔片高度(H.E.T.P.)与溫度的关系气相色谱学中理论塔片数n=t_R~2(σ_1~2+σ_2~2)~(-1),其中σ_1~2=2D_gLu~(-3),σ_2~2=2β~2F_1~2L(αF_gK~2u)~(-1)。(t_R为校正保留时间,D_g气相扩散常数,L色谱柱长,u载气线速,α气相溶入液相的速率常数或吸附速率常数,F_l,     

单轴取向PET薄膜的α松弛与力学行为的相关性

本文用动态力学方法研究了在不同温度和速度下单轴自由辐拉伸的聚对苯二甲酸乙二酯薄膜的非晶区状态,表明从熔体骤冷的非晶态试片在不同热拉伸条件下拉伸,可以得到非晶状态有显著差别的单轴取向薄膜。它们的非晶状态可以用动态力学温度谱的α峰的高度,形状和位置来表征。具有不同非晶状态的试样的储能模量E′(25℃)、屈服应力、负荷-伸长曲线与α松弛的参数以及其他结构参数间有很好的相关性。在一定的条件下热拉伸温度和速度存在Arrhenius型的速度-温度变换关系。     

α-和β-[SiW_9O_(37)M_3(H_2O)_3]~(7-)(M=A1~(3+),Ga~(3+),In~(3+))的合成和钨-183核磁共振研究

本文报道了α和β-[SiW_9O_(37)M_3(H_2O)_3]~((?))(M=Al~(3+),Ga~(3+),In~(3+))钾、铯盐的合成和性质。6种化合物的钨-183核磁共振谱都含有2个峰,相对强度为2∶1,表明其阴离子分别具有Aα和Aβ型Keggin结构,即3个MO_6八面体是角顶共用。     

Mechanical loss processes in polysaccharides

Dynamic mechanical properties of cellophane, amylose, and dextran have been obtained over the temperature range 100–520°K and frequency range 10^?2 to 10⁺² Hz on specimens containing various amounts of water. Four mechanical transitions have been characterized. At about 180°K, there is a γ transition that has been assigned to rotation of methylol groups; no comparable transition was found to exist in dextran. At about 240°K, there is a β transition that has been assigned to rotation of methylol–water complexes, but the β transition in dextran appears to be due to some other kind of motion. In cellophane at about 450°K there is an α₂ transition which appears to have contributions from motion of chain segments in disordered regions. The α₁ transition for cellophane occurs at temperatures too high to measure and may be due to segmental motions in chains within crystalline regions. Dextran and amylose were found to have at these same temperatures α loss processes that probably correspond to glass–rubber transitions in amorphous material. The changes in these mechanical loss mechanisms due to moisture uptake suggest that sorbed water associates with glucose repeat units in ways ranging from those which stiffen molecular structure to those which allow greater freedom for other types of motion to occur.     

Comparative study of dielectric,mechanical, and nuclear magnetic relaxations in linear polyethylene. II. Relaxation spectroscopy of the α, β, and γ loss bands with special emphasis on fine structure

Dielectric, mechanical, and NMR retardation (correlation) spectra for relaxations in linear polyethylene were calculated in normalized form and intercompared. For each of the two local-mode relaxations in the γ region, called γ₁ and γ₂, these spectra are found to be in excellent agreement. For the α region, the spectra for two mechanical processes, called α₁ and α₂, two NMR processes, called α′ and α, and one dielectric process α were calculated. Excellent agreement is found between the spectra for the dielectric α and NMR α′ processes and also spectra for the mechanical α₂ and NMR α processes, due to molecular motion in the interior of crystals. However, the spectrum for the mechanical α₁ process is different from that for the dielectric α and NMR α′ processes, though the activation energy for the first process is almost the same as for the other two. This behavior is interpreted on the assumption that the dielectric α and NMR α′ processes are caused by molecular motion in lamellar surface layers while the mechanical α₁ process is due to grain-boundary slip with viscous resistance of the surface layers in the boundaries. The shapes of the spectra, including the spectrum for the β process, are not affected by diluent.     

Comparative study of dielectric,mechanical, and nuclear magnetic relaxations of linear polyethylene. I. Broad-line NMR investigation of the fine structure of the α and γ loss bands observed by dielectric and mechanical measurements

Detailed investigation of the linewidth, second moment, and mobile fraction by straightline decomposition of NMR spectra of linear polyethylene from ca. ?160 to ca. 100°C reveals five molecular processes denoted γ₁, γ₂, β, α′, and α. Relaxation maps show that the γ₁, γ₂, and β processes correspond to the dielectric and mechanical relaxations given the same names, while the α and α′ processes correspond respectively to the mechanical α₂ process due to molecular motion in the interior of crystals and to the dielectric α process. Close relations are found between the mass fractions of protons for the γ₁ and β processes and also between those for the γ₂ and α′ processes. From the effects of diluent on these processes and the annealing-time dependence of mass fractions of protons, the γ₁, and β processes are attributed to two modes of molecular motion in an interlamellar amorphous region, while the γ₂ and α′ processes are attributed to motions in the lamellar surface layers. The surface-layer thickness obtained by applying the two-phase model for the data on mobile fraction agrees quite well with that reported in the literature. The Bergmann–Nawotki three-component analysis of NMR spectra and symmetric-line decomposition for determining mobile fraction are shown to be unsuitable for studying the fine structure of the α and γ loss bands.     

分子量分布对等规聚丙烯卷绕丝织构形成的影响

本文研究了分子量分布对聚丙烯卷绕丝结构和性能的影响。结果表明,聚丙烯树脂中的高分子量尾端对卷绕丝的结构有明显影响。在通常的纺丝条件下,用控制降解的聚丙烯树脂纺得的卷绕丝具有低取向的次晶结构;而在相同的粘均分子量和纺丝条件下,高分子量尾端的存在使聚丙烯易于在纺丝线上生成结晶性较高的α-晶型,卷绕丝的取向也随高分子量尾端而显著增大。高分子量尾端对卷绕丝结构的影响,导致卷绕丝牵伸性能和成品纤维力学性能变差。     

以催化油浆为增孔剂的MCM-41介孔分子筛的合成

采用阳离子表面活性剂十六烷基三甲基溴化铵为模板剂、正硅酸乙酯为硅源、硫酸铝为铝源，水热合成了以甲苯溶解的催化油浆为添加剂的MCM-41介孔分子筛，通过XRD、N2吸附脱附、TG-DTA、SEM等测试手段对合成样品进行了表征，重点研究了在甲苯/催化油浆=1∶1和2∶1（质量比）两个剂油比下分子筛结晶度、晶胞参数、BET表面积、平均孔径以及孔容等结构性质随催化油浆添加量的变化规律，并对合成机理进行了解释。结果表明，当剂油比为1∶1时，分子筛的结晶度和晶胞参数随催化油浆添加量的变化呈现先增加后减小趋势，当noil/nCTMAB=0.34时，其晶胞参数最大可以达到5.95 nm；当剂油比为2∶1时，随添加剂量的增加，分子筛结晶度降低，BET表面积成先增大后减小，而孔容和平均孔径呈逐渐增加趋势。当noil/nCTMAB＝0.15时，MCM-41的BET表面积可达1163.7m2·g-1，孔容可达到1.34cm3·g-1，平均孔径为4.34 nm。     

Development of the mesomorphic phase in isotactic propene/higher α-olefin copolymers at intermediate comonomer content and its effect on properties

Several isotactic propene-α-olefin copolymers using 1-octene, 1-dodecene and 1-tetradecene as comonomers (CiPO, CiPDD and CiPTD, respectively) have been synthesized and their structure and thermal/mechanical/viscoelastic properties have been evaluated. At intermediate comonomer molar content ranged from around 4 to 9, the mesomorphic phase is developed under rather mild quenching conditions and independently of length of the comonomer. Thermal and mechanical parameters diminish as α-olefin content increases and their dependence on composition changes as function of existence of three-dimensional monoclinic crystallites or less ordered entities.     

用~(13)C-NMR研究 1,2-聚丁二烯的分子运动——1,2-聚丁二烯分子运动对微观结构的依赖性

本工作用200兆赫脉冲傅里叶变换 NMR 波谱仪测定了一系列1,2-聚丁二烯样品在溶液中~13C核自旋-晶格弛豫时间(T_1)和核Overhauser效应(NOE)。较系统地研究了1,2-聚丁二烯的分子运动与化学结构、序列结构和大分子链节构成的关系,分析了乙烯基的内旋转运动。实验结果表明,顺1,4-链节中各碳的nT_1值比1,2-链节中相应各碳的nT_1值长1倍左右;对于相同的链节,当其两旁由1,2-链节变为顺1,4-链节时,其各类碳的nT_1值都大大增加;随着1,2-链节增加,各类碳的nT_1值都明显缩短。乙烯基叔碳的nT_1值大于端碳,经计算表明,引起乙烯基叔、端碳的nT_1值不相等的主要因素是乙烯基在垂直于主链的平面上的摆动。     

Molecular aggregation of solid aromatic polymers. II. Mechanical properties of aromatic polyimide film

Molecular aggregation of the aromatic polyimide poly(4,4′-oxydiphenylene-pyromellitimide) is influenced by the initial imidization temperature and by cold drawing. The effect of molecular aggregation in polyimides on their mechanical properties has been investigated. The density of a polyimide in which molecular aggregation gives an amorphous state is increased slightly by cold drawing. On the other hand, if molecular aggregation leads to a heterogeneous two-phase structure, the density is decreased by cold drawing. With increasing initial imidization temperature, the α absorption peak in dynamic tensile measurements becomes broader and smaller, and shifts to a higher temperature. From analysis of correlations between molecular aggregation and mechanical properties, it is concluded that the mode of molecular motion corresponding to the α dispersion in polyimide is a long-range cooperative motion of the main chain which is associated with the glass transition.     

Molecular modeling study on surface,thermal, mechanical and gas diffusion properties of chitosan

The motivation of this work is to provide reliable and accurate modeling studies of the physical (surface, thermal, mechanical and gas diffusion) properties of chitosan (CS) polymer. Our computational efforts have been devoted to make a comparison of the structural bulk properties of CS with similar type of polymers such as chitin and cellulose through cohesive energy density, solubility parameter, hydrogen bonding, and free volume distribution calculations. Atomistic modeling on CS polymer using molecular mechanics (MM) and molecular dynamics (MD) simulations has been carried out in three dimensionally periodic and effective two dimensionally periodic condensed phases. From the equilibrated structures, surface energies were computed. The equilibrium structure of the films shows an interior region of mass density close to the value in the bulk state. Various components of energetic interactions have been examined in detail to acquire a better insight into the interactions between bulk structure and the film surface. MD simulation (NPT ensemble) has also been used to obtain polymer specific volume as a function of temperature. It is demonstrated that these V–T curves can be used to locate the volumetric glass transition temperature (T_g) reliably. The mechanical properties of CS have been obtained using the strain deformation method. Diffusion coefficients of O₂, N₂, and CO₂ gas molecules at 300 K in CS have been estimated. The calculated properties of CS are comparable with the experimental values reported in the literature. © 2007 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 45: 1260–1270, 2007     

β晶型聚丙烯的力学性质

研究了主要含β晶型的聚丙烯在不同温度下的应力-应变性质,并与同一商品牌号得到的α晶型聚丙烯作了对比。发现,β晶型试样的屈服强度低于α晶型,而抗冲击强度则比α晶型试样高1—2倍。结合X射线衍射法对β晶型试样在拉伸过程中发生的晶型转变的研究及形变的分子机制解释了二种晶型试样在力学性质上的差异。