尼龙66-盐与碳纤维复合-固态缩聚的研究

本工作借助偏光显微镜,扫描电子显微镜和热分析方法(DSC,TGA)研究了尼龙66盐与碳纤维复合-固态缩聚反应历程及纤维-树脂之间的界面效应。发现对尼龙66盐的“原位固态缩聚”存有如碳纤维表面的成核结晶和催化效应之类的界面效应。讨论了碳纤维的界面效应对尼龙66基体的外延结晶和熔融行为及其热氧化稳定作用的影响。     

固态缩聚尼龙1010的熔化行为

本工作借助示差扫描量热法和X-射线衍射分析法(WAXD)首次研究了固态缩聚反应所得初生态尼龙1010的结晶特征和熔化行为。实验结果表明:固态缩聚反应的温度和时间以及产物分子量对初生态尼龙1010的熔化行为有着明显的影响。初生态尼龙1010结晶熔融双峰的显隐与其X-射线衍射峰特征没有明显的依赖关系,但随着尼龙大分子结晶的完善化而出现表观体积收缩观象。     

尼龙1010盐固态缩聚反应的研究

采用测定转化率和分子量、红外光谱、X-射线衍射分析、元素分析、偏光显微镜和扫描电镜等方法研究了结晶尼龙1010盐的特性、尼龙1010盐固态缩聚反应的动力学及其相应的晶体结构形态,用DSC法探讨了其反应机理。     

半结晶聚合物的多重熔化行为

<正> 半结晶聚合物双重熔化行为研究历史经过拉伸取向、退火、或沉淀的半结晶聚合物常常在具差热分析(DTA)、差示扫描量热(DSC)曲线上出现双重熔化峰。从五十年代以来不断出现有关双重熔化峰产生原因的研究报导。1955年White在拉伸取向的尼龙66、尼龙6、尼龙11、聚胺酯的DTA曲线上,首次观察到双重熔化峰,他将低温峰归因于取向晶体的解取向吸热,将高温峰归因于晶区的熔化。Bell在早期研究拉伸的退火的尼龙66、聚对苯二甲酸乙二酯(PET)     

尼龙1010结构的研究

本工作通过X-光衍射、红外光谱、示差扫描量热、偏光显微镜、粘弹谱及密度观测,考察了尼龙1010样品,分别从玻璃态结晶与从熔融态结晶后的聚集态结构,发现它的结晶结构与尼龙66相似,但从熔融态结晶的晶格有很大畸变,对所涉及的问题进行了讨论,提出了氢键面畸变的模型。     

尼龙1010在加热扫描中结构重组的研究

用DSC观察了经不同热处理的尼龙1010的热历史和结构重组的再现过程。合理地解释了DSC曲线上吸热和放热峰的性质,提出预熔结晶峰表征再结晶集合的观点。确定了对结晶完善敏感的热处理温度范围。为尼龙1010的加工和应用提供了部分理论依据。     

尼龙1218的等温及非等温结晶动力学研究

采用示差扫描量热计DSC考察了一种新型长烷基链偶偶尼龙 尼龙 12 18 自熔体的结晶过程 ,分别利用Avrami方程和Ozawa方程对等温及非等温结晶动力学进行了描述与研究 ,计算了相关的结晶动力学参数 ,得出相应的结晶机理 .最后计算了等温结晶活化能和非等温结晶活化能 ,依此得到烷基链段长度与尼龙结晶过程有密切关系     

蒙脱土对尼龙66熔融与结晶行为的影响

通过DSC方法研究了蒙脱土对尼龙66熔融与结晶行为的影响,探讨了蒙脱土对尼龙66结晶的成核作用。发现有机蒙脱土使尼龙66的熔融峰温度Tm提高5.3℃,使结晶峰温度提高13－24℃,二次熔融多产生双重熔融峰,蒙脱土的加入有利于生成低温峰。     

热处理对尼龙1010固态结晶和玻璃态热松驰的影响

本文用DSC首先论证淬火尼龙1010试样在DSC曲线上出现的放热峰是冷结晶峰,然后研究淬火尼龙1010在不同热处理条件下,冷结晶峰和玻璃态热松驰峰的变化规律。实验结果表明,等温结晶时间较短,试样的固态结晶速率较快;等温结晶时间较长,固态结晶速率较慢,这可能与在Tg区域等温所形成的新氢键有关。当升高等温温度时,固态结晶速率加快。在低于Tg的不同温度退火,玻璃态热松弛峰的峰高及热焓在281K达最大值,进而确定对玻璃态热松驰影响最敏感的温度区间是277～284K。     

树枝状尼龙6的合成与研究

用单羧基封端的尼龙6分别与树枝状聚酰胺-胺(PAMAM)的G1代和G2代外围活泼氨基进行缩聚反应,合成出具有规整结构的由核心向外发散增长的树枝状尼龙6,采用红外光谱、扫描电镜、DSC和TGA对缩聚物进行了分析。     

固态缩聚尼龙66的熔化行为

固态缩聚尼龙６６的熔化行为沈百拴，张喜亮，李新法（郑州大学材料工程系郑州４５００５２）关键词尼龙６６，固态缩聚物，熔化行为，差示扫描量热注关于固态缩聚反应的研究国内外已有报道［１～４］，叵未见固态缩聚尼龙６６（ＳＳＰＰＡ６６）熔化行为的报道。本文用Ｄ...     

Partial miscibility in a nylon‐6/nylon‐66 blend coalesced from their common α‐cyclodextrin inclusion complex

We successfully formed a series of inclusion complexes (ICs) between an α‐cyclodextrin (α‐CD) host and two kinds of guest polymers, nylon‐6 and nylon‐66. An attempt to achieve an intimate blend between nylon‐6 and nylon‐66 through the formation and dissociation of their common α‐CD IC was made. The formation of all nylon ICs was verified with wide‐angle X‐ray diffraction, differential scanning calorimetry (DSC), and Fourier transform infrared (FTIR) and cross‐polarized/magic‐angle‐spinning ¹³C NMR spectroscopy. The experimental results demonstrated that α‐CD could only host single nylon polymer chains in the IC channels, either nylon‐6 or nylon‐66 in their own complexes, and presumably either nylon in neighboring channels of their common IC. The IC‐coalesced blend of nylon‐6 and nylon‐66 was obtained after the removal of the host cyclodextrin from their common IC with dimethyl sulfoxide. The spectroscopic results (FTIR and ¹³C NMR) illustrated that there was a degree of intimate miscibility existing in the IC‐coalesced blend, but not in the solution‐cast physical blend, although X‐ray diffraction patterns showed that the crystal structure of the IC‐coalesced blend was similar to that of the physical blend. DSC thermal profiles suggested that nylon‐66 first formed crystals during coalescence and that the subsequent crystallization of nylon‐6 was greatly affected by the nylon‐66 crystallites because of the close proximity of the two components in portions of the coalesced blend. DSC observations also demonstrated that the melting of the coalesced blend did not lead to complete phase separation of the nylon‐6 and nylon‐66 components. © 2004 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 42: 1369–1378, 2004     

Crystalline stoichiometric adducts of polyamides with phosphoric acid

It is shown the crystalline stoichiometric adducts of phosphoric acid with polyamides such as nylon 6 and poly-p-benzamide, and probably nylon 66, nylon 69, nylon 11, and nylon 12, can be prepared. These adducts are characterized by their unique wide-angle x-ray diffraction patterns and by rather low melting or decomposition temperatures. The thermal behavior and infrared data, indicate that interactions between the acid and the polymeric amide residues are weak.     

THERMAL BEHAVIOUR OF γ-IRRADIATED NYLON 610

The thermal behaviour of γ-irradiated nylon 610 was investigated. In DSC (differential scanning calorimetry) thermograms in addition to general features characteristic of γ-irradiatinn cross-linked crystalline polymers, a typical cold-crystallization phenomenon was observed during the sceond scan for samples that had been subjected to high radiation dose. G-values for cresslinking nylon 610 were estimated from gel fraction measurement and TMA (thermomechanical analysis), From TMA curves it was estimated that the dimensional stability of properly irradiated nylon 610 articles might be raised up to ca. 300℃.     

Crystalline structure and thermal behavior of nylon‐10,14

The structure and morphology of a novel polyamide, nylon‐10,14, and its lamellar crystals from dilute solution were examined by transmission electron microscopy and wide‐angle X‐ray diffraction (WAXD). Both the electron‐diffraction pattern and WAXD data demonstrated that nylon‐10,14 adopts the structure of a triclinic lattice similar to that of the traditional nylon‐66 but with a corresponding increase of the c parameter to 3.23 nm. In addition, the thermal behavior of melt‐crystallized nylon‐10,14 was investigated by dynamic mechanical analysis (DMA) and differential scanning calorimetry (DSC). The glass‐transition temperature of nylon‐10,14 determined by the DMA data was 46.6°C. DSC indicated that the multiple melting behavior of isothermally crystallized nylon‐10,14 probably results from the melt and recrystallization mechanism. © 2003 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 41: 1422–1427, 2003     

Hydrogen bonding in polyamide 66/clay nanocomposite

Hydrogen bonding in polyamide 66/clay nanocomposite (PA66CN) was first investigated with temperature Fourier transform infrared (FTIR), the results of which were compared with that of pristine polyamide 66 (PA66) with the same thermal history. FTIR spectra at room temperature revealed that there is essentially 100% hydrogen bonding in both PA66CN and PA66, and the difference in hydrogen‐bonding status between them is tiny. Additionally, DSC showed that the crystalline degrees and melting temperatures of PA66CN and PA66 prepared by melt quenching are similar. However, the changes of hydrogen bonding with temperature in PA66CN and PA66 are different. As the temperature rose, the hydrogen bonding in PA66CN attenuated and dissociated considerably at a smaller rate than PA66. According to transmission electron microscopic morphology of PA66CN, we analyzed the effect of nanodispersion clay layers on the motion of a polymer chain and the thermal expansion of crystalline lamella for interpreting the observed phenomenon. © 2003 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 41: 2313–2321, 2003     

STUDY ON THE BLENDS OF NYLON 66 AND LIQUID CRYSTALLINE POLYESTERS

Blends of polyamide (Nylon 66) with two different kinds of liquid crystalline polyesters were studied in all the composition range. Homogeneous samples were obtained by coprccipitation from 2 wt%. solution of blends. The thermal properties, crystallinity and morphology of these blends were studied by using DSC, polarizing microscopy, and scanning electron microscopy. The phase transition and morphology of the blends are markedly-influenced by the composition of liquid crystalline polyesters. The mechanical behaviour of PHB/HNA-Nylon 66 blend was improved. although polyamidc (Nylon 66)with the liquid crystalline polyesters were incompatible, but a rather strong interaction between the polymers did exist.     

Multiple endotherm melting behavior in relation to polymer morphology

The two endotherms found during DSC analysis of annealed or drawn poly(ethylene terephthalate), PET, are discussed in greater. detail. Earlier workers proposed that the endotherms were the result of separate morphologies, i.e., extended-chain and folded-chain crystals, but more recently Roberts and others have presented data on the effect of DSC heating rate on annealed PET endotherm areas which indicate that the higher temperature endotherm is the result of recrystallization in the DSC. The present work explains the reasons for recrystallization, and presents data showing that samples cooled at various rates from the melt also exhibit recrystallization in the DSC, in much the same manner as samples annealed for different lengths of time. Further, by prolonged annealing before analysis, part of the recrystallization exotherm can be observed in the DSC scan. Drawn nylon 66 also exhibits recrystallization in the DSC, in a manner similar to annealed or slowly crystallized PET. The amount of material that recrystallizes is determined by the time and supercooling available between first melting and the ultimate recrystallization temperature, i.e., a temperature at which there is too little time and temperature driving force for further recrystallization to occur. Infrared absorption data show an increase in “regular” fold content during prolonged annealing of PET, while dynamic mechanical data show a marked decrease in a dispersion that is likely associated with the looser fold crystal morphologies. Annealed PET does superheat in the DSC, leaving unanswered the question as to whether any partially extended material is present along with the regular-fold material. For cold-drawn PET, the infrared data indicate disappearance of regular folds and the dynamic mechanical data indicate disappearance of the looser folds. Cold-drawn PET also superheats. These data indicate a likelihood of at least partially extended morphologies in cold-drawn PET; these observations do not apply to PET drawn at high temperatures or to polyethylene.     

Polymer crystalline structure and morphology changes in nylon‐6/ZnO nanocomposites

The influence of ZnO nanoparticles on the crystalline structures of nylon‐6 under different crystallization conditions (annealing at different temperatures from the amorphous solid, isothermal crystallization from the melt at different temperatures, and crystallization from the solution) has been examined with differential scanning calorimetry (DSC), wide‐angle X‐ray diffraction, field emission scanning electron microscopy, and Fourier transform infrared. ZnO nanoparticles can induce the γ‐crystalline form in nylon‐6 when it is cooled from the melted state and annealed from the amorphous solid. This effect of ZnO nanoparticles increases with decreasing particle size and changes under different crystallization conditions. The effects of ZnO nanoparticles on the crystallization kinetics of nylon‐6 have also been studied with DSC. The results show that ZnO nanoparticles have two competing effects on the crystallization of nylon‐6: inducing the nucleation but retarding the mobility of polymer chains. Finally, the melting behavior of the composites has been investigated with DSC, and the multiple melting peaks of composites containing ZnO nanoparticles and pure nylon‐6 are ascribed to the reorganization of imperfect crystals. © 2003 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 41: 1033–1050, 2003