热历史对尼龙1212熔融行为的影响

利用DSC方法研究了不同热历史条件对尼龙1212熔融行为的影响.不同的热历史条件下,在DSC曲线上,观察到尼龙1212产生2个或3个熔融峰,依据聚合物结晶理论,对各峰的来源进行了分析.在160℃下不同温度退火120 min的尼龙1212样品DSC曲线上,低温结晶熔融峰主要由低温结晶形成的一些微晶体或者片晶熔融产生,其晶体完善程度较差,熔融峰值较低,峰面积较小;主熔融峰是由样品在淬火过程中形成的晶体和升温过程中低温结晶形成的晶体的熔融重结晶形成较为完善的晶体熔融所产生,熔融峰值较高,峰面积较大.在不同的升温速率条件下,熔融峰温度有所移动,表明不同升温速率条件下产生的熔融峰的结晶晶型是相同的.在不同结晶时间下结晶,延长结晶时间对较高完善程度晶体的生长有利.在不同温度下依次退火处理的样品,熔融产生两个附加峰,这两个附加峰的峰温都比它们相应的退火温度高,而峰高和峰面积随退火温度降低而减小.根据等温结晶结果,由Hoffman方法确定了尼龙1212的平衡熔融温度为202.8℃.     

聚乳酸可降解材料结晶和熔融行为的研究

用DSC和XRD研究了聚乙二醇（PEG）用量、分子量和退火温度对PLA结晶和熔融行为的影响。结果表明PEG的加入有利提高PLA的结晶度和结晶温度;PLA／PEG样品在低于10022退火后均表现出双熔融峰特征,退火温度越高,样品的低熔融峰（Tm1）越高且熔融热焓也越高;PEG分子量越大,其低熔融峰的熔融热焓（△H1）越大...     

热处理对尼龙6及其与聚酰胺嵌段共聚物共混体系晶体熔融行为和结晶结构的影响

采用溶液共混-共沉淀的办法获得尼龙6及聚酰胺嵌段共聚物/尼龙6共混体系粉末,样品在260℃下熔融之后经程序降温的方法得到非淬火样品,然后分别在190℃下高温退火不同时间(0~48 h),采用示差扫描量热仪(DSC)、广角X射线衍射仪(WAXD)、偏光显微镜(POM)等表征手段研究热处理对体系晶体熔融行为和结晶结构的影响.结果表明,(1)在相同的热历史条件下,嵌段共聚物的存在影响了尼龙6的结晶行为及结晶结构;(2)退火处理对两种样品有着不同的影响,对于尼龙6体系,退火处理促进了非晶相向晶相的转变,大大提高样品的结晶完善程度和结晶度;对于共混体系,退火处理同样促进了非晶相向晶相的转变,同时形成新的α型和γ型结晶,体系的结晶完善程度明显提高,退火48 h后,结晶度比原始样品提高约84%.     

非等温结晶对PLLA的热行为和形貌的影响

将聚L-乳酸(PLLA)熔化非等温熔融结晶, 采用DSC、POM、SEM等技术研究了降温速率对PLLA的热行为和形貌的影响. PLLA在低降温速率(2 ℃·min-1)下的结晶在118 ℃伴随有结晶机制的转变. 玻璃化温度和结晶度随着降温速率的降低而增大. 随着降温速率的降低, 球晶尺寸增大, 当降温速率为10 ℃·min-1 时, PLLA 为无定型材料. 采用模压成型的方法并控制降温速率制备了具有球晶结构的条状PLLA 生物材料, 与高降温速率下制备的PLLA相比,低降温速率下获得的具有球晶结构的PLLA材料的断面更光滑和致密, 但脆性增强.     

尼龙1010等温结晶球晶形态与生成条件研究

本文利用偏光显微镜研究了等温结晶时尼龙1010球晶的形态与生成条件,发现在原始样品熔点附近或高于原始熔点以上温度结晶,主要生成暗、亮与带正环的负光性放射状球晶;熔点以下至195℃主要生成正放射状球晶;在较宽的温度范围内可生成混合光性放射状球晶,与少量的六瓣、两瓣、不对称四瓣形三种异常光性球晶;181℃以下主要生成正环状球晶.     

尼龙1010等温结晶球晶形态与生成条件研究

 本文利用偏光显微镜研究了等温结晶时尼龙1010球晶的形态与生成条件,发现在原始样品熔点附近或高于原始熔点以上温度结晶,主要生成暗、亮与带正环的负光性放射状球晶;熔点以下至195℃主要生成正放射状球晶;在较宽的温度范围内可生成混合光性放射状球晶,与少量的六瓣、两瓣、不对称四瓣形三种异常光性球晶;181℃以下主要生成正环状球晶.     

β晶型成核剂N,N’-二环己基环己对二甲酰胺的合成与应用研究

合成了新型成核剂N,N’-二环己基环己对二甲酰胺(DCHCHDA),用广角X射线衍射仪、差示扫描量热仪和偏光显微镜对其进行了表征,并研究了其对等规聚丙烯(IPP)的力学性能、结晶行为、β晶含量和熔融行为的影响。结果表明,成核剂DCHCHDA主要是改变球晶的形态,可明显改善IPP的抗冲击性能,并可以大幅度提高IPP的结晶度、β晶含量与结晶峰温度。当DCHCHDA添加量为0.05(wt)%时,IPP的悬臂梁缺口抗冲击强度可以提高137%,结晶度提高47%,β晶含量提高3.3倍。当降温速率为10℃/min时,添加DCHCHDA的IPP的结晶峰温度可从空白样的115.6℃提高到127.5℃。DCHCHDA的成核性能优于传统的芳香酰胺型β晶型成核剂DC26NDCA。     

原位聚合聚乙烯/蒙脱土纳米复合材料的结晶行为

用DSC研究了HDPE与MMT负载的催化剂熔融共混和原位聚合得到的两种纳米复合材料的熔融、 结晶行为和等温结晶动力学.  结果表明, HDPE与熔融共混样品的结晶度、 平衡熔点、 球晶生长速率和结晶能力大体相同; 原位聚合得到的HDPE/MMT纳米复合材料的结晶度和平衡熔点高于纯HDPE; 在相同过冷度条件下熔融结晶速率和结晶能力低于纯HDPE, 而在相同结晶温度Tc下, 熔融结晶速率和结晶能力则高于纯HDPE.  纯HDPE的晶体生长侧向单位面积表面自由能最小, 其次是熔融共混样品, 原位聚合样品最大, 且随ＭＭＴ含量的增加逐渐升高.     

聚丙烯β相结晶的研究

本文研究了冷却速率、结晶温度和熔体温度等因素对聚丙烯β相结晶得到的试样的熔融行为的影响。发现β晶型熔融峰的面积随冷却速率的降低或结晶温度的升高而增加。在低于300℃的温度下,熔体温度对聚丙烯的β相结晶无影响。300℃以上的高温破坏了聚丙烯β相结晶的晶核,冷却结晶时不再生成β相晶体。测定了α相及β相球晶在123—140℃的温度范围内线性增长速率,发现在140℃以下,β球晶的增长速率大于α球晶。研究了β相结晶动力学,发现聚丙烯β相结晶不符合Avrami方程,而要用不完全球晶结晶的动力学理论来描述。     

聚对苯二甲酸乙二酯的结晶与取向

为了了解PET球晶的拉伸性能与球晶结构的关系以及无定形PET的取向和结晶,我们采取了两条不同的路线来制备样品:(1)先用溶液浇铸成膜的办法制备具有正球晶、负球晶或非常球晶的薄膜,然后进行单轴拉伸。电子显微图象及电子衍射证明,球晶的拉伸性能与C轴和球晶半径方向的夹角有关,夹角愈大拉伸愈困难;(2)先制备无定形的薄膜,然后在玻璃化温度附近进行单轴拉伸以获得C轴取向,再在215℃退火,使之结晶。电子衍射图证明,这样制备的样品具有高度的C轴取向。DSC结果表明,结晶的完善程度远比球晶的为高。     

尼龙1010球晶的转化

本文利用偏光显微镜研究了尼龙1010球晶的转化。发现在降温过程中放射状球晶多转变成相同光性的环状球晶。升温时正环状转化为正放射状球晶;正、混合放射球晶部分转化为负放射状球晶;黄蓝两瓣球晶在一定温度范围内可与负放射球晶相互转变。多种球晶共存时,混合放射球晶可转变成两瓣、不对称四瓣和六瓣形放射球晶;正、混合坏状分别转变成不对称四瓣和六瓣形环状球晶;最后都以环状球晶熔化。     

聚醚酮酮的合成、表征与结晶行为

聚醚酮酮的合成、表征与结晶行为＊王军佐郑玉斌柯扬船于冬宏＊＊吴忠文（吉林大学化学系长春１３００２３）关键词聚醚酮酮，结晶结构，低温熔融峰，热处理聚醚醚酮８０年代初由英国ＩＣＩ公司商品化，由于其优异的性能，已在宇航、军工、核能等领域得到了广泛的应用，聚...     

CRYSTALLIZATION AND MELTING OF NYLON 610

Differential scanning calorimetry was used to study the crystallization andmelting of nylon 610. For nylon 610 crystallized from the melt state (260℃), the overall rateof bulk crystallization can be described by a simple Avrami equation with Avrami exponentn ≈ 2, independent of crystallization temperature. With the experimentally obtainedT_m~0 (235℃ ～ 255℃) of nylon 610, the fold surface free energy σ_e was determined to be35 ～38 erg/cm~2. The effects of annealing temperature and time on the melting of quenchednylon 610 were also investigated. For nylon 610 quenched at room temperature there isonly one DSC endotherm peak DSC scans on annealed samples exhibited an endothermpeak at approximately 10℃ above the annealing temperature. The size and position of theendothermic peak is strongly related to annealing temperature and time. An additionalthird melting was observed when quenched nylon 610 was annealed at high temperaturefor a sufficiently long residence time. The existence of the third melting peak suggests thatmore than one kind of distribution of lamella thickness may occur when quenched nylon610 is annealed. The implications of these results in terms of crystal thickening mechanismwere discussed.     

PC/PET/EPDM共混体系的结晶与熔融行为

本文用解偏振光法与DSC法分别测定并研究了PC/PET/EPDM共混体系的结晶速度、结晶度、Avrami指数(n)和熔融温度及其影响因素,共混物中PET的结晶速度、结晶度均随PC含量增加而下降;EPDM用量不超过10%时,可提高PET的结晶速度,但不影响结晶度和成核与增长方式,n值不变。当EPDM为5%时,结晶速度呈现极大值。经退火处理的共混物呈现熔融双峰,PC量增加,高温熔融峰略移向高温方向;热处理温度升高或时间延长,则低温熔融峰移向高温方向。     

Partial melting and recrystallization of isotactic polypropylene

<正>A relatively high predetermined crystallization temperature(135℃) was chosen to grow well developed iPP spherulites,then the partial melting was carried out at a temperature of 165℃,where the preformed spherulites were seen to only decrease their size but not completely melted.The crystallization behavior of partially melted isotactic polypropylene (iPP) has been carefully examined by different scanning calorimetry(DSC) and polarized light microscopy(PLM).The experimental results show that at a special annealing temperature(165℃) the melting behavior of iPP includes two parts with different mechanism,one part is the melting of iPP spherulite outside,another is the partial lamellae perfection during longer annealing time in the unmelted spherulite.The conformational orders of the iPP melt decrease with the increase of the annealing temperature.     

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。     

The double melting behavior of a liquid crystalline polyimide derived from PMDA and 1,3‐bis[4‐(4′‐aminophenoxyl) cumyl] benzene

The double melting behavior of a thermotropic liquid crystalline polyimide was studied by means of differential scanning calorimetry (DSC), polarized light microscopy (PLM), transmission electron microscopy (TEM), wide‐angle X‐ray diffraction (WAXD), and small‐angle X‐ray scattering (SAXS). This liquid crystalline polyimide exhibited a normal melting peak around 278 °C and transformed into a smectic A phase. The smectic A phase changed to nematic phase upon heating to 298 °C, then became isotropic melt around 345 °C. The samples annealed or isothermally crystallized at lower temperature showed double melting endotherms during heating scan. The annealing‐induced melting endotherm was highly dependent on annealing conditions, whereas the normal melting endotherm was almost not influenced by annealing when the annealing temperature was low. Various possibilities for the lower melting endotherm are discussed. The equilibrium melting points of both melting peaks were extrapolated to be 283.2 °C. Combined analytical results showed that the double melting peaks were from the melting of the two types of crystallites generated from two crystallization processes: a slow and a fast one. Fast crystallization may start from the well‐aligned liquid crystal domains, whereas the slow one may be from the fringed or amorphous regions. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 3018–3031, 2000     

THE DOUBLE MELTING PEAKS OF POLY(ETHYLENE TEREPHTHALATE)

Three sets of PET samples, comprising original (undrawn), uniaxially drawn and biaxially ones, after annealed at 230°, 240°and 250℃respectively, were subjected to DSC thermal analysis, X-ray diffraction analysis and IR analysis. The results indicate that the phenomenon of double melting peaks during DSC analysis is due to the partial melting and recrystallization of the crystallite at the moment of thermal scanning. The lower temperature peak, which varies slightly according to annealing condition, corresponds to the melting of imperfect crystallite, and the higher temperature peak corresponds to the melting of better organized crystallite. In the course of temperature scanning, the unit cell parameters of PET remains unchanged while the crystals turn to better crystal lattice, greater crystal size and more regular folding.We also found that there is a slight reduction in crystal size between the two melting peaks, and an explanation is suggested for this phenomenon.     

聚对苯二甲酸乙二酯的熔融双峰

未拉伸聚对苯二甲酸乙二酯(PET)、单轴拉伸PET、双轴拉伸PET在不同条件下热处理,并进行了DSC热分析、X-射线衍射分析、红外分析。结果表明:熔融双峰现象起因于DSC等速升温过程中PET的部分熔融和重结晶;低温峰是等温热处理过程中形成的不完善微晶的熔融峰,高温峰是重结晶后较完善的微晶的熔融峰;在等速升温过程中,PET晶胞参数不变、晶格完善、晶粒增大,并且规则折迭链增加,但晶粒随温度增大的过程中出现低谷。