尼龙1010的流变性能研究

用XLY-Ⅱ重型毛细管流变仪研究了尼龙1010的流变特性。实验结果表明,尼龙1010为假塑性流体;在210～250℃范围内,其非牛顿指数π为0.63～0.71;恒γw＇下的粘流活化能随γw＇的增大而减小。     

Structural change in the Brill transition of Nylon m/n (1) Nylon 10/10 and its model compounds

Structural changes in the Brill transitions of Nylon 10/10 and its model compounds have been investigated by carrying out the temperature-dependent measurements of X-ray diffraction and infrared spectra along with the DSC measurement. The crystal structure at room temperature was found to be the so-called α form with the all-trans zigzag methylene segments. When the samples were heated, the infrared progression bands of the methylene segments, which are sensitive to the length of all-trans segmental parts, were found to change their spectral patterns in the transition temperature region: the progression bands decreased in intensity and disappeared above the transition region. At the same time several new bands were observed to appear, which were found to correspond to the progression bands of (CH₂)₇-(CH₂)₅trans-zigzag segments. These spectral changes indicate that the methylene segments were conformationally disordered by an invasion of some gauche bonds and as a result the effective length of trans-zigzag segments became shorter. This conformational disordering was found to occur more remarkably in the methylene segment of NH-(CH₂)₁₀-NH part than the CO-(CH₂)₈-CO part. At the same time the infrared bands of amide groups, in particular the bands sensitive to the twisting angles about the CH₂-amide bonds were found to show the remarkable change, indicating the local conformational change from planar-zigzag to twisted form in the CH₂-amide moiety. The frequency shift of amide A band (NH stretching mode) indicated a weakening of intermolecular hydrogen bonds, which however, did not disappear up to the melting region. From these data combined with the X-ray diffraction data, the structural disordering in the Brill transition phenomena was deduced concretely.     

Dispersion characterization in layered double hydroxide/Nylon 66 nanocomposites using FIB imaging

Layered double hydroxides (LDHs), a newly emerging 2D host material, consist of cationic brucite-like layers and exchangeable interlayer anions. In this work, the morphology and dispersion of LDH particles in LDH/Nylon 66 (salt) nanocomposites has been investigated using focused ion beam (FIB) techniques, transmission electron microscopy (TEM) and X-ray diffraction (XRD). The FIB images show that LDHs are present in the polymer phase dispersed to different degrees, with partial intercalation, exfoliation, and aggregation all being observed. The most even dispersion was achieved in nanocomposites with the lowest loading (0.5 wt % LDH). Residual tactoids and agglomerates were most common in the samples made with the highest concentration of LDHs studied here (5 wt %). The dispersion observed using FIB was consistent with TEM and XRD analysis, yet this technique had significant benefits in terms of time and simplicity over these “conventional” technologies. © 2008 Wiley Periodicals, Inc. J Appl Polym Sci, 2008     

尼龙6表面金属(Ni)化膜材料的制备及性能研究

用化学还原法制得了尼龙６表面金属（Ｎｉ）化膜材料。研究了还原条件，金属盐浓度对膜材料电性能的影响，以及膜材料的电发热性能，用光电子能谱和扫描电子显微镜对其表面及形貌进行了表征。     

玻纤增强石油发酵尼龙的热稳定性研究

利用热重动力学方法研究了玻纤增强ＰＦ尼龙（即石油发酵尼龙）的热稳定性能。玻纤和偶联剂均对ＰＦ尼龙具有热稳定化作用，且硅烷Ａ１１００对ＰＦ尼龙的热稳定化作用最为显著。     

锦纶66浸胶帘子布生产中的张力与控制

分析了帘子布生产中张力的作用及各区段的张力情况。张力应根据生产品种及浸胶帘子布的内在质量要求来选择，一般张力设定依据为拉伸区张力是干燥区张力的１倍，定型区张力是拉伸区张力的０．６５倍。同时应控制好各区段的温度，降低拉伸应力使锦纶６６帘子布拉伸均匀，提高帘子布的物理性能。     

氧化钕填充尼龙6的结晶行为

利用示差扫描量热仪（ＤＳＣ）研究了氧化钕（Ｎｄ２Ｏ３）对尼龙６（ＰＡ６）等温结晶行为的影响。结果表明，Ｎｄ２Ｏ３在ＰＡ６体系中起到了异相成核作用，提高了ＰＡ６的晶体增长速率。     

PC／PA1010共混物的热行为

利用热失重、微分热失重和显示扫描量热法研究了聚碳酸酯／尼龙１０１０共混物的热行为和解降解过程。结果表明：共混物在６００℃以下分两步降解，降解温度随尼龙１０１０用量增加有下降趋势；共混物的熔点随尼龙１０１０用量增加而升高。     

聚丙烯的官能化及其与尼龙66相容性研究

对聚丙烯（PP）进行官能化，并研究了接枝单体含量，引发剂含量，螺杆转速对接枝率和熔体流动速率的影响。再将不同接枝率的PP与尼龙66共混，研究了接枝率对共混物力学性能及相容性的影响；用扫描电子显微镜观察了共混物的形态，与未增容共混体系相比，增容后共混体系分散相尺寸明显减小，增容共混物的形态依赖于增容剂在共混物中的含量，增容剂的分子量及官能化基团的含量。     

尼龙1212/EPDM-g-MAH共混体系的制备及性能研究

制备了尼龙（PA）1212／EPDM－g-MAH共混物，并对其力学性能、热性能及共混形态进行了研究，结果表明，增韧剂的加入使共混物的缺口冲击强度显著增大，当增韧剂含量为20％时，缺口冲击强度为74．98kJ/m^3，是纯PA1212的13．5倍；用二甲苯处理过的共混物试样断面很不平坦，有很多孔洞和类纤维体，说明弹性体粒子以球状分散于基体树脂中。