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低密度聚乙烯/乙丙烯三元共聚(LDPE/EPO)共混体系的结晶动力学 总被引:2,自引:0,他引:2
用DSC方法研究了LDPE/EPO共混体系的等温及非等温结晶动力学,对LDPE/EPO共混体系的等温结晶动力学研究表明,共混物是三维生长的异相成核,共混物在各个结晶温度下的结晶过程都是以方式K_g(Ⅱ)进行的.采用联系Avrami方程和Ozawa方程导出的新非等温结晶动力学方程,处理了LDPE/EPO共混体系,得到了非等温结晶过程的一些基本参数,新方程很好地描述了此共混体系的非等温结晶动力学过程. 相似文献
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用DSC法研究了苯乙烯-丙烯等规立构嵌段共聚物的非等温结晶动力学。结果表明:冷却速率在5~20℃/min范围内,共聚物的非等温结晶动力学参数能很好地符合Avrami动力学方程,非等温结晶速率常数与冷却速率有关,动力学结晶能力则同时受到冷却速率和共聚物组成比的影响。文中还讨论了在非等温结晶条件下共聚物的结晶成核和生长方式与共聚物组成和结构的关系。联合Avrami方程和Ozawa方程推导的非等温结晶动力学方程较好地描述了iPS-b-iPP嵌段共聚物的非等温结晶动力学过程。 相似文献
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采用DSC方法研究了聚对苯二甲酸乙二酯 (PET)和热致性液晶共聚酯 6 0PHB PET (LCP)体系在少量扩链剂双 (2 唑啉 ) (BOZ)存在下形成的反应性共混物的非等温结晶动力学 .结果表明反应性共混物的Avrami指数均在 3 0~ 4 5之间 ,BOZ的加入使反应共混物中PET组分的结晶速率降低 ;表明BOZ对酯交换的促进作用 ,使所生成的共聚酯中PET嵌段的数均序列长度变短 ,而使结晶在某种程度上较为困难 ,但对体系的成核和结晶生长机理无明显影响 .结果还表明 ,随冷却速率的增大结晶峰向低温方向移动 相似文献
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以聚对苯二甲酸乙二醇酯-1,4-环己烷二甲醇酯(PETG)作为丙烯腈-丁二烯-苯乙烯(ABS)/聚对苯二甲酸乙二醇酯(PET)合金的增容剂,探讨了PETG用量对合金力学性能的影响,并通过差示扫描量热(DSC)仪研究了PET,ABS/PET和ABS/PET/PETG的非等温结晶动力学过程,使用Jeziorny法对合金的非等温动力学数据进行分析,计算得到相应动力学参数.研究结果表明,随着PETG加入量的增多,合金的冲击性能和断裂伸长率明显增加,拉伸强度和弯曲强度稍有降低,结晶度降低,结晶速率稍有降低. 相似文献
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PET/PEN/DBS共混体系结构与形貌的研究 总被引:2,自引:0,他引:2
共混是改善聚合物性能的一种简单而又行之有效的方法,PET和PEN均为结晶性聚酯,由于PEN合成原料的影响,致使PEN的价格较高,但性能比PET优良,通过二者的共混,既可以提高PET的性能,又可以降低PEN成本,有关PET/PEN共混体系的研究已引起人们的关注,而对于共混体系结晶形态和结晶条件的研究较少,由于成核剂能够提高结晶速率,减小球晶尺寸,因此本文对PET/PEN/DBS共混体系中,组分组成的影响及不同结晶条件下共混物的结晶形貌进行研究。 相似文献
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采用差示扫描量热(DSC)法对反式-/顺式-1,4-聚异戊二烯共混体系的等温及非等温结晶动力学进行了研究,分别采用Avrami方程和莫志深法对其动力学参数进行了解析.研究结果表明,在反式-/顺式-1,4-聚异戊二烯共混体系的等温及非等温结晶过程中,顺式-1,4-聚异戊二烯(CPI)组分的存在会降低反式-1,4-聚异戊二烯(TPI)组分的结晶速率;在等温结晶过程中,CPI组分会提高TPI组分自身的结晶度;而非等温结晶过程中,CPI则提高了共混物中β晶型的相对含量. 相似文献
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用Mandelkern和Ziabicki理论方法求得PVA及PVA/PVP共混物结晶动力学参数Z_C和动力学结晶能力G_C值,并进行了讨论。得到的Avrami指数n不随冷却速度变化,但随非晶组分PVP的加入有所减小,加入量达百分之四十以后n由3降到2;G_C值则随非晶组分的加入而增大,当PVP加入量大于百分之三十时,G_C值不再发生明显变化。同时实验表明该高聚物及其共混体系不适合于Ozawa非等温结晶动力学方程。 相似文献
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间规1,2-聚丁二烯的非等温结晶动力学 总被引:8,自引:1,他引:7
结合Avrami和Ozawa方程,构筑了一个新的聚合物非等温结晶动力学方程.以铁催化体系间规1,2聚丁二烯(st- 1,2PB)为例,将新方法与其他常用的Jeziony和Ozawa方法的处理结果进行比较.发现由Jeziony方法分析得到的表观Avrami指数不能直接用于预测st -1,2PB的非等温结晶机理.由Ozawa方法分析实验数据,得到的线性关系很差,因此也很难得到可靠的动力学参数.而采用新方法可得到一系列线性关系较好的直线.根据新参数a与表观Avrami指数n和Ozawa指数m的关系,st -1,2PB的结晶机理可以预测且与等温方法获得的结果有可比性.这种新方法已应用于聚醚酮、聚酰胺、聚烯烃、烷基取代聚噻吩、聚(β-羟基丁酸酯)及其共混物等多种聚合物体系中. 相似文献
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Nonisothermal crystallization kinetics and melting behavior of bimodal-medium-density- polyethylene (BMDPE) and the blends of BMDPE/LDPE were studied using differential scanning calorimetry (DSC) at various scanning rates. The Avrami analysis modified by Jeziorny and a method developed by Mo were employed to describe the nonisothermal crystallization process of BMDPE. The BMDPE DSC data were analyzed by the theory of Ozawa. Kinetic parameters such as the Avrami exponent (n), the kinetic crystallization rate constant (Zc), the peak temperatures (Tp) and the half-time of crystallization (t1/2) etc. were determined at various scanning rates. The appearance of double melting peaks and the double crystallization peaks in the heating and cooling DSC curves of BMDPE/LDPE blends indicated that the BMDPE and LDPE could crystallize respectively. 相似文献
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Yiping Huang Guangmei Chen Zhen Yao Hongwu Li Yong Wu 《European Polymer Journal》2005,41(11):2753-2760
The non-isothermal crystallization kinetics of isotactic polypropylene (iPP) and nucleated iPP was investigated by DSC. The crystalline morphology of iPP was observed by polarized light microscopy. It was found that the crystallization rate increased with the addition of nanometer-scale calcium carbonate (nm-CaCO3) particles. The addition of dibenzylidene sorbitol (DBS) could greatly reduce the spherulite size of iPP. The crystallization temperature for the iPP with DBS was higher than for non-nucleated iPP. DBS was an effective nucleating agent for iPP. The results of measurements suggested that there was a coordinated action to the crystallization of iPP when the organic nucleating agents (DBS) and nm-CaCO3 were added to iPP together. Comparison to the modified Avrami equation and Ozawa equation, another method—Mo’s method can describe the non-isothermal crystallization behavior of iPP and nucleated iPP more satisfactorily. 相似文献
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In this work, the effects of amorphous poly(styrene-co-acrylonitrile) (SAN) chains and hydrophilic and hydrophobic nanosilica at different loadings on the non-isothermal crystallization kinetics of PCL phase have been evaluated using different theoretical models including Avrami, modified Avrami, Ozawa and Mo equations. Using microscopic observations, the interrelations among the changes in the kinetics parameters and the morphology and phase behavior of PCL/SAN and PCL/SAN/nanosilica mixtures have been thoroughly investigated. Microscopic observations on the nanocomposites showed differences in the nanofiller dispersion and distribution state as well as preferential migration and localization state. These differences lead to contradictory trends in the effects of hydrophilic and hydrophobic nanosilica on the crystallization kinetics of pure PCL and PCL/SAN blends. The nanoparticle migration during non-isothermal DSC tests in PCL/SAN blends, the formation of nanoparticle agglomerates at higher loadings, the restrictions imposed on the molecular movements in the crystallization growth stage and slower phase separation and dissolution of PCL/SAN/silica mixtures result in the cooling rate dependence of the kinetics parameters. 相似文献
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Fan Zhang Xiaochun Peng Wenbin Yan Zhiyuan Peng Yongqiang Shen 《Journal of Polymer Science.Polymer Physics》2011,49(19):1381-1388
The nonisothermal crystallization kinetics was investigated by differential scanning calorimetry for the nylon 6/graphene composites prepared by in situ polymerization. The Avrami theory modified by Jeziorny, Ozawa equation, and Mo equation was used to describe the nonisothermal crystallization kinetics. The analysis based on the Avrami theory modified by Jeziorny shows that, at lower cooling rates (at 5, 10, and 20 K/min), the nylon 6/graphene composites have lower crystallization rate than pure nylon 6. However, at higher cooling rates (at 40 K/min), the nylon 6/graphene composites have higher crystallization rate than pure nylon 6. The values of Avrami exponent m and the cooling crystallization function F(T) from Ozawa plots indicate that the mode of the nucleation and growth at initial stage of the nonisothermal crystallization may be as follows: two‐dimensional (2D), then one‐dimensional (1D) for all samples at 5–10 °C/min; three‐dimensional (3D) or complicated than 3D, then 2D and 1D at 10–20 and 20–40 °C/min. The good linearity of the Mo plots indicated that the combined approach could successfully describe the crystallization processes of the nylon 6 and nylon 6/graphene composites. The activation energies (ΔE) of the nylon 6/graphene composites, determined by Kissinger method, were lower than those of pure nylon 6. © 2011 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 49: 1381–1388, 2011 相似文献
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一种研究聚合物非等温结晶动力学的方法 总被引:19,自引:2,他引:17
作者基于多年对聚合物结晶动力学方面研究的工作积累,联合Avrami方程和Ozawa方程,提出了一种研究聚合物非等温结晶动力学的新方法.该方法既克服了使用Ozawa方程所获得的数据点过少,常常出现非线性,不能获得可靠的动力学参数的缺点,又克服了使用经Jeziorny修正的Avrami方程所获得的表观Avrami指数无法准确预测非等温过程成核生长机理的缺点.该方法已成功用于多种聚合物体系,被国内外学者引用数百次,已成为研究聚合物非等温结晶动力学一种有效方法. 相似文献
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Xu W. B. Zhai H. B. Guo H. Y. Zhou Z. F. Whitely N. Pan W.-P. 《Journal of Thermal Analysis and Calorimetry》2004,78(1):101-112
The non-isothermal crystallization kinetics of polyethylene (PE), PE/organic-montmorillonite (Org-MMT) composites were investigated
by differential scanning calorimetry (DSC) with various cooling rates. The Avrami analysis modified by Jeziorny and a method
developed by Mo were employed to describe the non-isothermal crystallization process of these samples very well. The difference
in the exponent n between PE and PE/Org-MMT nanocomposites, indicated that non-isothermal kinetic crystallization corresponded to tridimensional
growth with heterogeneous nucleation. The values of half-time, Zc and F(T) showed that the crystallization rate increased with the increasing of cooling rates for PE and PE/Org-MMT composites,
but the crystallization rate of PE/Org-MMT composite was faster than that of PE at a given cooling rate. The method developed
by Ozawa did not describe the non-isothermal crystallization process of PE very well. Moreover, the method proposed by Kissinger
was used to evaluate the activation energy of the mentioned samples. The results showed that the activation energy of PE/Org-MMT
was greatly larger than that of PE.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
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用DSC方法对乙烯基甲醚/马来酸酐交替共聚物多缩乙二醇酯(CBP) 聚氧化乙烯(PEO)共混体系的非等温结晶动力学进行了研究,用Mandelkern、Z J(Ziabiki Jeziorny)、Ozawa和对Ozawa方法的一种修正方法对该体系进行了处理.结果表明:得到了一种既没有结晶又有较多EO单元含量的共混物,CBP对PEO的结晶有抑制作用.Avrami指数随冷却速率的加快在38~57之间波动.Mandelkern方法求得的结晶动力学参数Zc随冷却速率的增加而增加,共混物的Gc值不随冷却速率的变化而变化,随PEO含量增加而减少,处理结果表明而Z J理论能较好地解释本体系的非等温结晶过程和机理. 相似文献