分级聚丙烯的取向结晶过程

聚丙烯熔体在剪切或应变应力作用下 ,分子链发生取向形成伸直链纤维晶 ,这些先取向形成的纤维晶成为其后结晶的晶核 .这种线形排列的特殊自晶核被称作排核 ( Row nuclei) [1] .排核诱导的结晶温度高于异相核和均相核 .折叠链片晶在排核上附生生长 ,形成具有柱状对称性的超分子结构 ,称为柱状晶 ( Cylindrite) [2 ,3] .聚合物的分子量 ,剪切温度和剪切速度等因素对柱状晶的生成有很大影响 [4 ,5] .本文选用不同级分的聚丙烯样品 ,利用高分子 (特别是取向结晶 )的记忆效应 [6,7] ,研究了剪切后薄膜试样在熔融重结晶过程中柱状晶的形成和发展…     

甲壳型液晶聚合物纤维的形状记忆效应

采用TA-Q800动态热机械分析仪(DMA)研究了聚乙烯基对苯二甲酸二(对丁氧基苯)酯(PBPCS)纤维的形变回复性能,发现PBPCS纤维具有非常好的形状记忆效应,在145℃及以上温度,形状回复速率最好,9min左右可以从400%的伸长回复到原来的尺寸,于145℃,重复实验5次,结果说明形变回复重复性好.二维X衍射(2DX-Ray)研究显示形变前后PBPCS柱状分子直径d由2.54nm变为2.42nm,表明拉伸后PBPCS螺旋状的大分子主链处于更为伸直的构象,因此分子主链产生一定的内应力,即形变回复应力.由此可见,PBPCS相对柔性的聚乙烯主链使纤维具有良好的形变回复性能,而侧基的甲壳效应使得纤维能够保持初始尺寸,即PBPCS所具有的类似弹簧的特殊螺旋状分子结构是其纤维具有形状记忆效应的内在原因.     

聚对苯二甲酸乙二酯非晶态膜片单轴热——拉伸中的结晶与松弛

用动态力学损耗温度谱作为测试手段,研究了非晶态PET膜片在78—112℃温度范围内的单轴拉伸。实验结果说明,在较低温度下所得结晶的拉伸试样,完全由于应变诱发结晶,发生在应力-应变曲线的屈服后应力开始上升的阶段。在较高温度下(90℃或更高)拉伸可得非晶态而且光学各向同性的试样,是由于分子链的小尺度取向在拉伸过程中已完全热松弛所致,而分子链的大尺度取向要通过高弹态流动而松弛,其速率较慢,用拉伸后试样两端固定时的应力松弛进行了观察。在较低温度下应力松弛后仍为非晶态,在较高温度下应力松弛到起始应力的1O％下才开始结晶。FTIR研究表明在这种状态下的结晶有一结晶诱导期,其时间尺度与应力松弛阶段相当。     

关于超高分子量聚丙烯超拉伸膜的结构性能的研究——Ⅰ.拉伸取向过程的表征

用超高分子量聚丙烯的对二甲苯溶液中冷却析出的结晶沉积压制成的结晶垫,经热拉伸制备了不同拉伸倍数的薄膜.与用低分子量聚丙烯制备的结晶垫或熔融结晶物不同,超高分子量聚丙烯的结晶垫显示出极高的拉伸变形性能,因而制得了高达69倍的拉伸样品.WAXD照片表明在未拉伸的结晶垫中,微晶的c轴沿结晶垫法线方向择优取向,但仅经2-4倍的拉伸,微晶即发生破裂,且产生的较小的折叠链微晶已转向沿拉伸轴方向取向;晶区取向因子在拉伸过程中迅速增加并在较低拉伸倍数下即接近于理想取向.但非晶区取向因子在整个拉伸领域中增加缓慢.随拉伸倍数的增大,晶粒尺寸D_(110)及D_(040)逐渐减小;而长周期L逐渐增加.这表明在高倍拉伸样品中存在着折叠链被从片晶中拉出并部分形成伸直链结晶的转变.     

聚苯基单醚喹噁啉薄膜的形变机理

非晶聚合物塑性变形机理主要包括银纹化和剪切屈服[1 ,2 ] .银纹化是链段局部排列疏松区域或缺陷在膨胀应力作用下成为银纹核 ,引发银纹 ,银纹 本体界面应变软化 ,银纹微纤拉伸的应变硬化过程 ,使得聚合物银纹微纤沿拉伸方向取向 ,伴随这一过程聚合物的体积增大[3] .剪切屈服是分子链沿拉伸方向的流动以及分子链间的滑移过程 ,这一过程使聚合物形状改变而体积不变 .聚合物的形变机理与聚合物的内在性质如临界缠结分子量 ,缠结密度或硬度等有关[4] .聚苯基单醚喹啉是一种高性能的芳杂环聚合物 ,它的玻璃化转变温度是 2 98℃ ,它具有耐高温…     

高剪切速率对PCL/RGO附生结晶行为影响的原位研究

以聚己内酯(PCL)/还原氧化石墨烯(RGO)复合材料为研究对象, 利用同步辐射小角X射线散射(SAXS)和广角X射线衍射(WAXD)原位分析了75 s^?1的高速率剪切作用前后的附生晶体结构演变及其对本体晶体形成的影响. 研究结果表明, 在剪切后降温160 s后, PCL分子链开始在RGO表面附生, 形成表面结晶层, 同时形成部分PCL本体晶体; 在200~480 s的等温结晶阶段, 大量PCL本体片晶生成并形成规整的周期结构. 较高的剪切速率使体系的黏度降低, 因此在较高的剪切温度下PCL分子链更容易由伸直链转变为无规线团, 不利于PCL分子链在RGO表面形成表面结晶层. 在剪切速率为75 s^?1时, 70 ℃的剪切温度更有利于PCL分子链在RGO表面附生形成表面结晶层.     

分子链大尺度高取向而小尺度接近无规取向态的非晶态聚对苯二甲酸乙二酯膜片

对非晶态聚对苯二甲酸乙二酯膜片经在Ｔｇ以上单轴拉伸然后淬冷至室温的试样，其物理性质的各向同性或各向异性进行了研究．实验结果说明这种分子链大尺度高度取向而小尺度接近无规取向的非晶态（ＧＯＬＲ态）其折光指数和小形变的拉伸模量是接近各向同性的，而热导率和微波介电常数很可能是各向异性的．     

分子链大尺度高取向而小尺度接近无规取向态的非晶态聚对苯二甲酸…

对非晶态聚对苯二甲酸乙二酯膜片经在Ｔｇ以上单轴拉伸然后淬冷至室温的试样，其物理性质的各向同性或各向异性进行了研究。实验结果说明这种分子链大尺度高度取向而小尺度接近无规取向的非晶态（ＧＯＬＲ态）其折光指数和小形变的拉伸模量是接近各向同性的，而热导率和微波介电常数很可能是各向异性的。     

运用静电势图像分割方法预测超分子结合能

[2]-轮烷是由大环与分子链组成的两组分超分子体系,计算评估大环和链之间的结合强度,对于理解超分子识别和超分子体系可控设计尤为重要.本文借鉴计算机图像处理技术,通过全局阈值分割方法将大环和链的静电势图像分成两个片段,两者的静电势差值近似为[2]-轮烷体系的结合能.该计算方法可以直观简便地预测超分子体系的结合能.基于静电势的图像阈值分割方法计算的结合能定性符合实验测定的结合常数和密度泛函理论(DFT)计算的结合能.对于不同分子链和大环分子组成的多种[2]-轮烷体系的对比研究表明,大环与链的结合强度与结合位点的给质子能力、形成氢键的数目、大环的尺寸以及大环与链之间?-?堆积作用相关.     

乙烯共聚单体对双轴拉伸聚丙烯薄膜用树脂的结晶及拉伸性能的影响

采用热分析、光学显微镜、拉伸测试与广角X-射线衍射等方法研究了双轴拉伸聚丙烯薄膜用均聚聚丙烯(h-BOPP)与含有少量乙烯单体的共聚聚丙烯(c-BOPP)材料的熔融、结晶特性和拉伸性能.研究发现,与均聚样品相比,共聚样品的等规度低,结晶速率慢,在相同的结晶温度条件下,其半结晶时间较长.退火处理后,结晶完善程度增加,均聚和共聚样品的断裂伸长率均比其未退火处理的低.但共聚样品的结晶速率慢,经过退火处理后其结晶完善性稍低于均聚样品,所以其断裂伸长率略大于均聚样品.经过拉伸形变后,样品的结晶结构被部分破坏,取向的非晶的分子链在后续的升温过程中很容易重构为更加完善的结晶结构,由于分子链结构的差异,均聚样品的结晶重构能力更强.阐释了由于链结构的不同导致的BOPP拉伸性能和结晶性能差异的机理.     

Drawing behavior and characteristics of laser‐drawn polypropylene fibers

Drawing behavior, flow drawing, and neck drawing, was studied for isotacticpolypropylene fibers in CO₂ laser drawing system, and the fiber structure and the mechanical properties of drawn fibers were analyzed. For a certain laser power, flow drawing of polypropylene (PP) was possible up to draw ratio (DR) 19.5. Though the drawing stress was very low, the flow‐drawn PP fiber exhibited oriented crystal structure and improved mechanical properties. On the other hand, neck‐drawing was accomplished from DR 4 to 12, with significant increase in drawing stress that enhanced the development of fiber structure and mechanical properties. Unlike PET, the drawing stress depends not only on the DR, but on irradiated laser power also. The 10–12 times neck‐drawn fibers were highly fibrillated. The fibers having tensile strength 910 MPa, initial modulus 11 GPa, and dynamic modulus 14 GPa were obtained by single‐step laser drawing system. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 44: 398–408, 2006     

La1-xLixMnO3体系的输运特性及EPR研究

利用固相反应法合成了掺杂锂的La_1-xLi_xMnO₃(x=0,0.10,0.15,0.20,0.25,0.30)钙钛矿氧化物.XRD测试表明,所有样品均为菱方结构.除x=0,0.3外,其它样品均随温度的降低在液氮温区可观察到从绝缘态到金属态的转变,其中x=0.15样品的转变温度最高为167K.在H=1T的磁场下,出现了负磁阻现象.EPR谱上的g=2.00信号与Mn³⁺和Mn⁴⁺组成的复合团簇有关.     

Ultra-drawing of high molecular weight polyethylene cast from solution

Summary Hot drawing of high molecular weight polyethylene ( ) was studied. It was found that solutioncast films exhibited a drastically increased drawability in comparison with melt-crystallized material. This phenomenon, which enabled the production of polyethylene structures with a Young's modulus of 108 GPa and a strength of 3.0 GPa, is discussed in terms of a reduced number of entanglements in solution-crystallized material related to melt-crystallized films.With 2 figures and 1 table     

负载型钴二亚胺配合物-TiCl_4复合催化剂制备新型乙烯/1-丁烯共聚产物结构性能研究

合成了三种负载型二亚胺配体钴配合物 TiCl4复合催化剂 (CL1、CL2、CL3催化剂 ) .不用MAO ,以烷基铝为助催化剂 ,用它们催化乙烯 1 丁烯淤浆共聚合制备一系列塑性体和弹性体共聚物 .研究表明 ,复合催化剂性质受二亚胺配体性质影响 ,配体L1制备的复合催化剂具有低聚及原位共聚性能 ,可制得高支化度(36 0～ 6 1 5branchnumber 10 0 0C)低密度和极低密度 (0 885～ 0 910g cm3)塑性体和弹性体共聚物 .在 1 丁烯用量低于 5 %时 ,CL1催化剂制备的共聚产物中 1 丁烯含量超过投料比     

新型可溶性聚芳酰胺及其共聚物的合成与性能研究

采用新型二胺 1,2 二氢 2 (4 氨基苯基 ) 4 [4 (4 氨基苯氧基 ) 苯基 ] 二氮杂萘 1 酮与对苯二甲酸、间苯二甲酸、萘二酸进行均聚或共聚 ,所得聚芳酰胺的Tg 均高于 30 0℃ ,且易溶于非质子极性溶剂中 ,聚合物的特性粘数为 1 2 6～ 1 5 1dL g(2 5℃ ,NMP) ,拉伸强度为 6 2～ 89MPa ,断裂伸长率为 5 %～ 9% ,拉伸模量为 2 2～ 2 9GPa ,电阻系数为 10 1 4 ～ 10 1 6     

Microstructure and mechanical properties of hot‐air drawn poly(ethylene terephthalate) fibers

Hot‐air drawing method has been applied to poly(ethylene terephthalate) (PET) fibers in order to investigate the effect of strain rate on their microstructure and mechanical properties and produce high‐performance PET fibers. The hot‐air drawing was carried out by blowing hot air controlled at a constant temperature against an as‐spun PET fiber connected to a weight. As the hot air blew against the fibers weighted variously at a flow rate of about 90 ℓ/min, the fibers elongated instantaneously at a strain rate in the range of 2.3–18.7 s⁻¹. The strain rate in the hot‐air drawing increased with increasing drawing temperature and applied tension. When the hot‐air drawing was carried out at a drawing temperature of 220°C under an applied tension of 27.6 MPa, the strain rate was the highest value of 18.7 s⁻¹. A draw ratio, birefringence, crystallite orientation factor, and mechanical properties increased as the strain rate increased. The fiber drawn at the highest stain rate had a birefringence of 0.231, degree of crystallinity of 44%, tensile modulus of 18 GPa, and dynamic storage modulus of 19 GPa at 25°C. The mechanical properties of fiber obtained had almost the same values as those of the zone‐annealed PET fiber reported previously. © 1999 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 37: 1703–1713, 1999     

掺稀土多孔硅中稀土光学活化的新方法: 微波热法

首次报道掺稀土多孔硅中稀土光学活化的一种新方法--微波热法.经微波加热处理后,掺稀土多孔硅样品外观均匀;室温下,分别观察到掺铒多孔硅在-1.5μm处、掺钕多孔硅在-1.06μm处强的光致发光.除起加热作用外,微波与样品之间的非热相互作用在稀土的光学活化方面与也起重要作用.     

The production and properties of poly(ethylene naphthalate-2,6-dicarboxylate) monofilaments

Experimental spinning and drawing conditions are described for poly(ethylene naphthalate-2,6-dicarboxylate), PEN, which produce good quality 0.5 mm monofilaments with high strength and uniformity. Mechanical properties were measured for a range of draw temperatures and draw ratios and an initial modulus of 22 GPa and a strength of 0.6 GPa were obtained by single stage drawing to a draw ratio of 6.6. The maximum birefringence achieved by single stage drawing was 0.33 compared with a theoretical maximum of 0.332 calculated from the bond polarizabilities and bond angles of the aligned monomer unit. Network parameters relevant to undrawn PEN and to the early stages in the drawing process were derived from simple rubber elasticity theory by making birefringence and shrinkage force measurements on films drawn homogeneously to low draw ratios. These suggest that the PEN network contains relatively stiff chains between entanglements and that the PEN network is modified much more in the drawing process than is the case with poly(ethylene terephthalate). A new method of measuring the birefringence of highly drawn thick filaments is described.     

Specific heat capacity and thermodynamic properties of CuTeO3 and HgTeO3

Tellurites of CuTeO₃ and HgTeO₃ are synthesized and their specific molar heat capacities are experimentally determined for the first time. The tellurites discussed in the present paper are used for preparation of optical glasses with special properties for optoelectronics, nuclear and power industries. The tellurites synthesized are prepared for chemical analysis, differential thermal analysis and X-ray analysis. The use of the tellurites studied is related to knowing their thermodynamic properties like specific molar heat capacity (C _p,m), enthalpy \( \left( {\Delta_{{{\text {T}}^{\prime}}}^{\text{T}} H_{\text{m}}^{0} } \right), \) entropy \( \left( {\Delta_{{{\text {T}}^{\prime}}}^{\text{T}} S_{\text{m}}^{0} } \right) \) and Gibbs energy \( \left( { - \Delta_{{{\text {T}}^{\prime}}}^{\text{T}} G_{\text{m}}^{0} } \right) \) . The temperature dependences of their molar heat capacities are determined using the least squares method. The thermodynamic properties are calculated: entropy, enthalpy and Gibbs function.     

Melt drawing of ultra‐high molecular weight polyethylene: Comparison of Ziegler‐ and metallocene‐catalyzed reactor powders

The drawing behavior of the ultra‐high molecular weight polyethylene (UHMW‐PE) melts has been studied by comparing the stress/strain curves for two types of samples as polymerized using conventional Ziegler and newer metallocene catalyst systems. Two UHMW‐PE samples, having the same viscosity average molecular weight of 3.3 × 10⁶, but different molecular weight distribution, have been drawn from melt at special conditions. The sample films for drawing were prepared by compression molding of reactor powders at 180°C in the melt. Differences in the structural changes during drawing and resultant properties, ascribable to their broad or narrow molecular weight distribution, were estimated from tensile tests, SEM observations, X‐ray measurements and thermal analyses. The metallocene‐catalyzed sample having narrower molecular weight distribution, could be effectively drawn from the melt up to a maximum draw ratio (DR) of 20, significantly lower than that obtained for the Ziegler‐catalyzed sample, ∼ 50. The stress/strain curves on drawing were remarkably influenced by draw conditions, including draw temperature and rate. However, the most effective draw for both was achieved at 150°C and a strain rate of 5 min⁻¹, independent of sample molecular weight distribution. The efficiency of drawing, as evaluated by the resultant tensile properties as a function of DR, was higher for the metallocene‐catalyzed sample having narrower molecular weight distribution. Nevertheless, the maximum achieved tensile modulus and strength for the Ziegler sample, 50–55 and 0.90 GPa, respectively, were significantly higher than those for the metallocene sample, 20 and 0.65 GPa, respectively, reflecting the markedly higher drawability for the former than the latter. The stress/strain behavior indicated that the origin of differences during drawing from the melt could be attributed to the ease of chain relaxation for the lower molecular weight chains in the melt. © 1999 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 37: 1921–1930, 1999