热拉伸的超高分子量聚乙烯的晶体结构和力学性能

讨论了超高分子量聚乙烯（ＵＨＭＷ－ＰＥ）的熔融一次拉伸和二次拉伸的晶体结构和力学性能．利用ＷＡＸＤ和ＳＡＸＤ测定了拉伸片的晶体取向因子和极图，晶粒尺寸，晶体畸变，长周期等晶体结构．用ＤＳＣ和ＶＥＳ测定热性能和动态力学性能．应力－应变实验测定拉伸片的杨氏模量，断裂强度和伸长．这些实验结果说明ＵＨＭＷ－ＰＥ经二次拉伸能产生正交晶系的伸直链晶体．二次拉伸片由折叠链片晶和伸直链晶体两元结构组成．二次拉伸片的杨氏模量比一次拉伸片有大幅度提高．二次拉伸片的晶体结构和力学性能是在一次拉伸的基础上形成的．     

超高分子量聚乙烯凝胶膜超高取向过程的几个不同阶段

通过Ｘ射线衍射、平板照相、扫描电镜等方法观测超高分子量聚乙烯凝胶／结晶膜取向过程中的结构形态变化，并根据ＰＥ片晶分子动力学模拟结果，提出ＵＨＭＷＰＥ凝胶膜在热拉伸取向过程中明显存在３个不同阶段，即：初期片晶转动或滑移，ｂ轴优先垂直于拉伸方向取向；随着拉伸比增大，片晶的ｃ轴平等于伸方向，同时，分子链的解折叠开始，部分非晶链也进入伸直链区取向，当拉伸比达到极限倍率时，分子链已经接近完全伸展成为比较刚直     

离子自组装超分子荧光材料及其光致各向异性特性

采用离子自组装的方法,制备了侧链含有肉桂酸光敏基元和二苯乙烯荧光基元的新型超分子复合物PCAMSTIL.通过核磁共振(NMR)和红外光谱(FT-IR)表征了该超分子复合物的结构,并用热重分析(TGA)、紫外可见光谱(UV-Vis)和荧光光谱(FL)研究了其热稳定性和光学性能.将PCAMSTIL旋涂成膜,薄膜经过266 nm偏振脉冲激光辐照后,肉桂酸发生轴向选择的[2+2]加成,薄膜垂直于激光偏振方向的紫外可见吸收明显大于平行方向的吸收,证实薄膜具有取向性.取向薄膜的最大吸收二向色性取向值最大可达0.103,优于一般肉桂酸材料的取向性,肉桂酸分子的取向也引起二苯乙烯荧光分子的协同取向,荧光偏振发射比可达1.73.     

预热处理对超高分子量聚乙烯层积状片晶凝胶膜结构的影响

由准稀溶液速冷制备的超高分子量聚乙烯（ＵＨＭＷＰＥ）凝胶膜，具有片晶（Ｌａｍｅｌｌａ）取向平行于膜面的层积状结构，在１２９—１３４℃的温度范围内拉伸，可获得超高拉伸比（λ＞２００）．通过ＩＲ及Ｘ－ｒａｙ衍射等方法研究发现，拉伸前用不同温度退火处理后，凝胶膜的片晶微结构产生明显变化，在对应于超高拉伸温度范围内，其结晶度增加，微晶的ｃ和ｂ轴方向尺寸变大，而ａ轴方向的尺寸减小，从理论上对这一变化过程作了考察，并讨论了超高拉伸取向性与这些结构变化的关系以及可超拉伸取向性的最佳温度范围．     

超延伸高分子量聚乙烯力学性能的研究

超延伸高分子量聚乙烯力学性能的研究王维泮，张凤英（北京化工大学高分子系北京１０００２９）关键词超高分子量聚乙烯，冷拉伸，超延伸，延伸比随着高科技的发展，对材料性能的要求越来越高．目前一些发达国家正在致力于高机能、超强力的塑料．使高分子高度取向是获得高...     

Effect of Drawing Temperature on Structure and Properties of a＇-Phase of Poly（lactic acid）

a＇-晶型聚乳酸（PLA）膜被制备和单轴拉伸．通过凝胶渗透色谱仪（GPC）、全反射红外光谱（ATR-IR）、差示扫描量热仪（DSC）,X射线衍射（XRD）及Raman光谱等测试技术研究了拉伸温度梯度变化对a＇-晶型PLA膜的分子量及其分布、分子链构象、结晶度、晶型转变和取向行为的影响．在恒定拉伸速度与应变下,拉伸温度对PLA膜的应力．应变曲线,特别是屈服强度、拉伸模量产生了较大的影响,其值随拉伸温度的增加而降低．GPC测试结果表明,在不同的温度下拉伸后,PLA会发生一定程度的降解,分子量降低;ATR-IR,XRD,DSC和Raman光谱测试结果表明,在不同的温度下拉伸后a’-型PLA没有发生晶型的转变,即没有由a＇-晶体转变为a-或β-晶体．结果表明PLA的结晶度、分子链取向程度强烈依赖于拉伸温度：当拉伸温度低于100℃时,a’-型PLA膜 的结晶度与沿着拉伸方向的变形程度随拉伸温度的增加而增加,分子链的高度取向诱导了PLA结晶;当拉伸温度超过100℃后,PLA的分子链沿着拉伸方向上的有序度与结晶度将降低．     

自增强高性能聚合物的成型工艺同力学性能间相关性研究——1.超高分子量聚乙烯的应力诱导结晶理论和其自增强作用

本文发展了一种高分子量聚合物熔融体的应力诱导结晶结构形态模型,它是由微晶聚集体(以下简称微区)-高分子链组网和缠结网的网络结构组成。基于上述模型,把二种网中的单个链组作为独立的统计单元和形变单元,计算了二种网中单个链组的末端距分布函数,进一步计算了二种网和总网的形变自由能。在此基础上,讨论了诱导结晶结晶机理和自增强聚合物网络自由能的依赖性,并着重地研究了超拉伸高聚物的起始熔点拉伸比间的关系。用超高分子量聚乙烯膜和超取向高密度聚乙烯纤维的起始熔点和拉伸比的实验数据进行处理,得到理论予期的近似直线关系,初步验证了聚合物网应力诱导结晶理论。     

超高分子量PE凝胶膜的超拉伸性与旁式构象关系研究

通过ＩＲ方法，观测并讨论了在不同条件下制备的超高分子量ＰＥ（ＷＨＭＰＥ）凝胶膜中旁式（Ｇ构象）构象与超拉伸性的关系，提出了Ｇ构象浓度及分布对ＵＨＭＰＥ凝胶膜超拉伸性影响的新概念，同时也讨论了它与链缠结之间的联系，发现：反映Ｇ构象的相对浓度的比值σ＝Ｉ１３０３Ｉ１３５２随制膜浓度的增大而增加，在临界浓度Ｃ０（０．４～０．５ｇ＠１００ｍｌ）附近所形成的膜，具有超高拉伸性（λ＝２００），其Ｇ构象的变化与Ｍａｔｓｕｏ由比浓粘度提出的缠结链改变相对应；热处理温度比热处理时间对σ值的影响更显著，在一定温度下约４分钟后σ值基本不变；在σ值最低的温度范围拉伸，凝胶膜具有良好的超高拉伸性．     

聚乙烯串晶在单轴拉伸形变过程中的微结构变化和机理

本文采用电子显微镜和小角Ｘ－射线散射（ＳＡＸＳ）技术研究了含有串晶结构（Ｓｈｉｓｈ—ｋｅｂａｂ）的高密度聚乙烯（ＨＤＰＥ）／超高分子量聚乙烯（ＵＨＭＷＰＥ）共混物高取向膜在单轴拉伸过程中的微结构变化．深入探讨了拉伸温度对聚乙烯在形变过程中微结构变化的影响．室温拉伸时，聚乙烯串晶结构主要发生了解结晶过程；高温（１１５℃）形变时，主要表现为折叠链片晶直接转变为伸展链纤维晶的应变诱导结晶过程．     

在激光辐照下拉伸的聚对苯二甲酸乙二酯纤维的结构与性能

要提高聚对苯二甲酸乙二酯 (ＰＥＴ)纤维的力学性能 ,不仅要求分子链形成伸直链结晶 ,更主要的是增加晶区之间以及微原纤之间连接分子 (Ｔｉｅｍｏｌｅｃｕｌｅｓ)的数目及其取向程度[1,2 ] .研究表明 ,通过将拉伸工艺中的加热区域降低至 2ｍｍ ,可以使非晶态分子链更为伸展且规整排列[3 ] ,这样的非晶态结构可以更快地向结晶转化[3 ,4] ,容易形成伸直链结晶并增加连接分子的数目 .这种区域拉伸的实质是通过减小形变 (细颈 )区域而使形变速率显著提高 .采用ＣＯ2 激光辐照可以达到更高的形变速率 .这是由于ＣＯ2 激光的波长为 1 0 6μｍ ,…     

Elastic modulus and thermal conductivity of ultradrawn polyethylene

The axial and transverse Young's modulus and thermal conductivity of gel and single crystal mat polyethylene with draw ratios λ = 1–350 have been measured from 160 to 360 K. The axial Young's modulus increases sharply with increasing λ, whereas the transverse modulus shows a slight decrease. The thermal conductivity exhibits a similar behavior. At λ = 350, the axial Young's modulus and thermal conductivity are, respectively, 20% and three times higher than those of steel. For this ultradrawn material both the magnitude and the temperature dependence of the axial Young's modulus are close to those of polyethylene crystal. The high values of the axial Young's modulus and thermal conductivity arise from the presence of a large percentage (∼85%) of long needle crystals. © 1999 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 37: 3359–3367, 1999     

Thermal conductivity and thermal expansivity of thermotropic liquid crystalline polymers

The thermal conductivity and thermal expansivity of a thermotropic liquid crystalline copolyesteramide with draw ratio λ from 1.3 to 15 have been measured parallel and perpendicular to the draw direction from 120 to 430 K. The sharp rise in the axial thermal conductivity K_par; and the drastic drop in the axial expansivity α_∥ at low λ, and the saturation of these two quantities at λ > 4 arise from the corresponding increase in the degree of chain orientation revealed by wide-angle x-ray diffraction. In the transverse direction, the thermal conductivity and expansivity exhibit the opposite trends but the changes are relatively small. The draw ratio dependences of the thermal conductivity and expansivity agree reasonably with the predictions of the aggregate model. At high orientation, K_par; of the copolyesteramide is slightly higher than that of polypropylene but one order of magnitude lower than that of polyethylene. In common with other highly oriented polymers such as the lyotropic liquid crystalline polymer, Kevlar 49, and flexible chain polymer, polyethylene, α_par; of the copolyesteramide is negative, with a room temperature value differing from those of Kevlar 49 and polyethylene by less than 50%. Both the axial and transverse expansivity show transitions at about 390 and 270 K, which are associated with large-scale segmental motions of the chains and local motions of the naphthalene units, respectively. ©1995 John Wiley & Sons, Inc.     

Thermal conductivity of poly(ether ether ketone) and its short-fiber composites

The effects of crystallinity, orientation, and short-fiber filler on the thermal diffusivity D and thermal conductivity K of poly (ether ether ketone) (PEEK) have been studied. Below the glass transition, D increases by less than 10% as the crystallinity increases from 0 to 0.3. For amorphous PEEK, there is an abrupt drop in D at the glass transition (T_g ? 420 K). The drop is less prominent for the 30% crystalline sample and occurs at 20 K higher. At a draw ratio of 2.5, the axial thermal conductivity is 2.3 times higher while the transverse thermal conductivity is 30% lower than that of the unoriented material. For an injection-molded bar of carbon fiber reinforced PEEK, the variation of D with position along the width or thickness direction is found to correlate well with the fiber orientation. By regarding the injection-molded bar as a multidirectional laminate comprising a large number of unidirectional plies, the thermal conductivities along the longitudinal and transverse direction are calculated and found to agree closely with the experimental data. © 1994 John Wiley & Sons, Inc.     

Thermal conductivity of gel-spun polyethylene fibers

The thermal conductivities of unidirectional gel-spun polyethylene fiber-reinforced composites have been measured parallel (K∥?) and perpendicular (K⊥) to the fiber axis from 15 to 300K. The axial thermal conductivity K∥? varies linearly with volume fraction v_f of fiber, while the transverse thermal conductivity K⊥ follows the Halpin-Tsai equation. Extrapolation to v_f = 1 gives the thermal conductivity of gel-spun polyethylene fiber which, at 300K, has values of 380 and 3.3 mW cm^?1K^?1 along and perpendicular to the fiber axis, respectively. The axial thermal conductivity is exceptionally high for polymers, and is more than twice the thermal conductivity of stainless steel. This high value arises from the presence of a large fraction of long (> 50 nm) extended chain crystals in the fiber. Further improvement of up to a factor of 10 is possible if the length and volume fraction of the extended chain crystals can be increased. © 1993 John Wiley & Sons, Inc.     

Elastic moduli of ultradrawn polyethylene

The five independent elastic moduli C₁₁, C₁₂, C₁₃, C₃₃, and C₄₄ of oriented high-density polyethylene with draw ratio λ from 1 to 27 have been determined from ?60 to 100°C by an ultrasonic method at 10 MHz. At low temperature the sharp rise in the axial extensional modulus C₃₃ with increasing λ and the slight changes in the other moduli result from chain alignment and the increase in the number of intercrystalline bridges connecting the crystalline blocks. At high temperature (say, 100°C) the transverse extensional modulus C₁₁, as well as the axial (C₄₄) and transverse (C₆₆) shear moduli, also show substantial increases, reflecting the prominent reinforcing effect of stiff crystalline bridges in this temperature region where the amorphous matrix is rubbery. If the crystalline bridges are regarded as the fiber phase, the mechanical behavior can be understood in terms of the Halpin–Tsai equation for aligned short-fiber composites.     

Thermal diffusivity of polymer films by pulsed photothermal radiometry

We have developed a pulsed photothermal radiometry technique for determining the thermal diffusivity parallel to the surface of a polymer film that involves flashing a line-shaped laser beam on the surface of the sample at right angle to its length, and monitoring the temperature change with time at a distance from the line source using an infrared detector. Combining this with our previous laser-flash radiometry method for thermal diffusivity measurement perpendicular to the film surface, we can now measure the thermal diffusivity of a polymer film along all directions. These two techniques have been used to study uniaxially and biaxially oriented poly(ethylene terephalate) and uniaxially drawn ultrahigh molecular weight polyethylene films. For uniaxially oriented poly(ethylene terephalate), the thermal diffusivity along the draw direction is substantially higher than that in the transverse direction, which in turn, is slightly higher than that in the thickness direction. For a polyethylene film with a draw ratio of 200, the axial thermal diffusivity is extremely high, being about five times that of stainless steel. The anisotropy of the thermal diffusivity of this film exceeds 90. © 1997 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 35 : 1621–1631, 1997     

Thermal conductivity of high strength polyethylene fiber in low temperature

High strength polyethylene fiber (Toyobo, Dyneema® fiber, hereinafter abbreviated to DF) used as reinforcement of fiber‐reinforced plastics for cryogenic use has a high thermal conductivity. To understand the thermal conductivity of DF, the relation between fiber structure and thermal conductivity of several kinds of polyethylene fibers having different modulus from 15 to 134 GPa (hereinafter abbreviated to DFs) was investigated. The mechanical series‐parallel model composed of crystal and amorphous was applied to DFs for thermal conductivity. This mechanical model was obtained by crystallinity and crystal orientation angle measured by solid state NMR and X‐ray. Thermal conductivity of DF in fiber direction was dominated by that of the continuous crystal region. The thermal conductivity of the continuous crystal part estimated by the mechanical model increases from 16 to 900 mw/cmK by the increasing temperature from 10 to 150K, and thermal diffusivity of the continuous crystal part was estimated to about 100 mm²/s, which is almost temperature independent. The phonon mean free path of the continuous crystal region of DF obtained by thermal diffusivity is almost temperature independent and its value about 200 Å. With the aforementioned, the mechanical series‐parallel model composed of crystal and amorphous regions could be applied to DFs for thermal conductivity. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 1495–1503, 2005     

单向纤维增强环氧复合材料的热膨胀系数

本文在123—413K的温度范围内,测量了单向玻璃纤维和碳纤维增强环氧树脂复合材料α_P~C(纤维方向),α_(T1)~C(横截面板厚度方向),α_(T2)~2(横截面板宽度方向)三个热膨胀系数.研究了纤维体积分数V_f和纤维表面处理对α_P~C和α_T~C的影响.结果表明,α_P~C在整个温度范围内不受纤维表面处理影响,随V_f的增加而减小,变化规律符合Schapery方程.对于横向热膨胀系数,在T<基体玻璃化温度T_g~m时,有α_(T1)~C α_(T2)~C=α_(T)~C,在V_f 0.3时,有α_T~C>α_m(基体的),而后随V_f的增加而减小,经分析也符合Schapery理论.在T>T_g~m时,α_(T1)~C和α_(T2)~C呈各向异性,特别在纤维表面未处理时更为显著.形态研究表明,其原因是在纤维铺层之间存在片状树脂层.     

Modifying thermal transport in electrically conducting polymers: effects of stretching and combining polymer chains

If their thermal conductivity can be lowered, polyacetylene (PA) and polyaniline (PANI) offer examples of electrically conducting polymers that can have potential use as thermoelectrics. Thermal transport in such polymers is primarily influenced by bonded interactions and chain orientations relative to the direction of heat transfer. We employ molecular dynamics simulations to investigate two mechanisms to control the phonon thermal transport in PANI and PA, namely, (1) mechanical strain and (2) polymer combinations. The molecular configurations of PA and PANI have a significant influence on their thermal transport characteristics. The axial thermal conductivity increases when a polymer is axially stretched but decreases under transverse tension. Since the strain dependence of the thermal conductivity is related to the phonon scattering among neighboring polymer chains, this behavior is examined through Herman's orientation factor that quantifies the degree of chain alignment in a given direction. The conductivity is enhanced as adjacent chains become more aligned along the direction of heat conduction but diminishes when they are orthogonally oriented to it. Physically combining these polymers reduces the thermal conductivity, which reaches a minimum value for a 2:3 PANI/PA chain ratio.