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1.
尼龙1010非等温结晶动力学与机理研究   总被引:3,自引:0,他引:3  
尼龙1010非等温结晶动力学与机理研究朱诚身,王经武,李卓美(郑州大学材料工程系郑州450052)(中山大学高分子研究所广州510275)关键词尼龙1010,非等温结晶动力学,结晶机理,动力学结晶能力尼龙1010的结晶动力学,无论是等温还是非等温,研...  相似文献   

2.
测定高聚物动力学结晶能力的非等温DSC方法   总被引:5,自引:0,他引:5  
张志英 《应用化学》1997,14(5):32-35
研究了从非等温DSC结晶曲线计算高聚物动力学结晶能力的方法.从高聚物非等温结晶动力学微分方程出发导出了计算高聚物动力学结晶能力的新方程.以含有不同催化剂的聚对苯二甲酸乙二酯为例,对其结晶进行了测试与计算.发现合理地选定最快结晶速率温度是计算动力学结晶能力的关键.本方法所得动力学结晶能力能正确反映高聚物的整体结晶信息  相似文献   

3.
高聚物非等温结晶动力学   总被引:2,自引:0,他引:2  
由于等温DSC法测定结晶动力学参数在实验上存在着一定的局限性,这些缺点可通过非等温DSC法来克服。本文基于上述观点介绍了高聚物非等温结晶动力学的理论和实验方法,并对影响动力学过程的一些因素进行了讨论,对非等温结晶动力学的最新情况及发展倾向,应用情况作了介绍。  相似文献   

4.
聚合物结晶动力学   总被引:23,自引:0,他引:23  
本文介绍了聚合物等温及非等温结晶动力学过程的理论和实验方法,对影响动力学过程的一些因素进行了讨论。  相似文献   

5.
根据等温DSC法,测定结晶动力学参数在实验上存在着一定的局限性,结晶太快或太慢都难于获得可靠的结果,这就限定了能测定的温度区间。可见,等温DSC法测定结晶动力学参数具有获得的信息量少,结晶起始点难以确定,费时等缺点。这些缺点可通过等速变温DSC法来克服。然而,通过等速变温DSC法测定结晶动力学参数的方法至今还不完善。例如Ozawa曾基于Evans理论把Avrami方程推广于非等温结晶,从Ozawa方程通过等速变温DSC曲线可得到表征结晶机理的函数Avrami $数。和冷却结晶函数。Ozawa方法的不足是从其冷却结晶函数不能解析出表征结晶速率的参数。  相似文献   

6.
高聚物结晶后期动力学过程的研究进展   总被引:9,自引:0,他引:9  
回顾了描述高聚物结晶后期动力学过程的各种模型、方程以及数据处理方法,并就影响高聚物结晶后期动力学过程的某些因素进行了讨论。  相似文献   

7.
测定高聚物结晶动力学参数的非等温理论和方法   总被引:18,自引:0,他引:18  
对测定高聚物结晶动力学参数的非等温结晶理论和等速变温DSC方法进行了讨论,文中包含了作者在此领域研究工作的最新进展。  相似文献   

8.
固相缩聚PET等温结晶动力学   总被引:3,自引:1,他引:3  
高聚物等温结晶动力学方面的研究者甚多,由熔融缩聚制备的不同分子量PET的等温结晶动力学及几种不同缩聚催化体系固相缩聚PET的等温结晶动力学已有报道.本文采用一个修正的Avrami方程对固相缩聚PET样品进行系统的等温结晶动力学研究.  相似文献   

9.
尼龙1218的等温及非等温结晶动力学研究   总被引:10,自引:0,他引:10  
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  相似文献   

10.
聚丙烯接枝马来酸酐及其离聚物的非等温结晶动力学   总被引:14,自引:0,他引:14  
余坚  何嘉松 《高分子学报》1999,39(5):513-519
用 D S C 测定了固相接枝法制备的聚丙烯接枝马来酸酐( P P g M A H) 及其3 种5 个离聚物在不同冷却速率的非等温结晶动力学.分析了结晶峰温( Tmax) 、结晶起始温度( T0) 、结晶峰的初始斜率( Si) 及结晶峰的半高宽( Δw ) 等结晶峰参数;用 Avrami 方程和综合了 Avrami Ozawa 方程的方法处理非等温结晶动力学.对于全部样品在所有的冷却速率下, Avrami 指数n 值均在25 ~28 之间,说明聚丙烯结晶行为没有改变;但同时发现接枝及离子化后,成核速率加快,晶粒分布变窄,结晶总速率增大,与等温结晶动力学得到的结论一致.  相似文献   

11.
聚丙烯/蒙脱土纳米复合材料非等温结晶动力学的研究   总被引:22,自引:0,他引:22  
用熔融插层法制备聚丙烯 蒙脱土纳米复合材料 ,用DSC手段研究了其非等温结晶行为 ,并与聚丙烯进行了对比 .对所得数据分别用修正Avrami方程的Jeziorny法、Ozawa法和Mo法进行处理 .结果表明 ,用Jeziorny法和Mo法处理非等温结晶过程比较理想 ,而用Ozawa法处理则不太适用 .用Jeziorny法求出的参数Zc和n随冷却速率的增加而增加 ,但复合材料的Zc 和n略大于聚丙烯的Zc 和n ,用Mo法求出的参数F(T)随结晶度的增加而略有增加 ,a几乎未变 ,复合材料的F(T)略小于聚丙烯的F(T) ,复合材料的a约为 1.40略大于聚丙烯的a(其值约为 1.0 4) .按Kissinger方法计算出聚丙烯及聚丙烯 蒙脱土纳米复合材料的结晶活化能分别为 189.37kJ mol,15 5 .6 9kJ mol,说明有机蒙脱土的加入 ,降低了聚丙烯的结晶活化能 ,起到了异相成核的作用  相似文献   

12.
The melt-direct intercalation method was employed to prepare polypropylene (PP)/maleic anhydride grafted polypropylene (PP-g-MAH)/organic-montmorillonite (Org-MMT), X-ray diffractometer was used to investigate the intercalation effect and crystallite size in composites and TEM micrograph to observe the dispersion of Org-MMT interlayers in polypropylene. The results showed that by introducing maleated polypropylene in PP/Org-MMT composite, macromolecule segments had intercalated into interlayer space of Org-MMT. As a result, Org-MMT interlayers were dispersed evenly in polypropylene and PP/PP-g-MAH/Org-MMT nanocomposite was synthesized. The crystallite size of nanocomposite perpendicular to the crystalline plane such as (0 4 0), (1 3 0), (1 1 1), (0 4 1) is smaller than that of pristine PP, which indicated that the crystallite size of PP in nanocomposite can be diminished by adding PP-g-MAH and Org-MMT in PP. Moreover, the nonisothermal crystallization kinetics of PP and PP/PP-g-MAH/Org-MMT nanocomposite was investigated by differential scanning calorimetry (DSC) with various cooling rates. The Avrami analysis modified by Jeziorny, Ozawa method and a method developed by Liu were employed to describe the nonisothermal crystallization process of these samples. The difference in the exponent n between PP and nanocomposite, indicated that nonisothermal kinetic crystallization corresponded to tridimensional growth with heterogeneous nucleation. The values of half-time, Zc, F(T) and K(T) showed that the crystallization rate of composites was faster than that of PP at a given cooling rate.  相似文献   

13.
聚丙烯/凹凸棒土纳米复合材料的非等温结晶动力学   总被引:2,自引:0,他引:2  
聚丙烯/凹凸棒土纳米复合材料的非等温结晶动力学  相似文献   

14.
PP/PP-g-MAH/PA6共混物结构与可纺性研究   总被引:3,自引:0,他引:3  
运用DSC、SEM、纺丝成形等手段研究了增容剂聚丙烯接枝马来酸酐 (PP g MAH)对聚丙烯 聚酰胺 6(PP PA6 )共混物结构和性能的影响 .结果表明 ,共混物呈典型海岛型两相结构 ;增容剂PP g MAH与PA6之间的在位反应改善了PP PA6共混体系的相容性 ,使共混物中PA6的热结晶峰消失 ,PP的结晶生长速率和成核速率降低 ,可纺性提高  相似文献   

15.
GMA/苯乙烯多组分单体接枝聚丙烯结晶行为研究   总被引:8,自引:0,他引:8  
使用差示扫描量热计 (DSC)研究了甲基丙烯酸缩水甘油酯 苯乙烯 (GMA St)多单体熔融接枝聚丙烯[PP g (GMA co St) ]的等温和非等温结晶行为 ,用偏光显微镜观察了结晶的形态 ,并利用Avrami方程对其结晶动力学进行了分析 .研究发现接枝聚丙烯的结晶模式与PP相似 ,属于异相成核控制的球晶三维生长 ;但接枝聚丙烯的结晶温度 (Tc)显著提高 ,幅度高达 16~ 19℃ ,总结晶速率与纯PP相比明显加快 .接枝聚丙烯上GMA co St支链的存在 ,降低了成核界面自由能 ,促进了聚丙烯结晶的异相成核 .在接枝率不太高的情况下 ,随着接枝率的提高 ,接枝聚丙烯的结晶温度升高 ,总结晶速率加快 .在高接枝率范围内 ,随着接枝率的提高 ,接枝PP的Tc 不再升高 ,且由于接枝链的增长严重阻碍了球晶生长 ,导致接枝PP的总结晶速率反而随接枝率的升高而下降  相似文献   

16.
聚丙烯/蒙脱土纳米复合材料的等温结晶研究   总被引:19,自引:0,他引:19  
采用差示扫描量热法 (DSC)对插层聚合法制备的聚丙烯 /蒙脱土纳米复合材料 (PP MMT)的等温结晶过程进行了研究 .引入蒙脱土 (MMT)后 ,PP MMT的结晶速率大幅度提高 ,相对结晶度略有下降 .采用Avrami方程对结晶动力学进行研究 ,Avrami指数n≈ 3 .0 ,半结晶时间t1 2 大幅度降低 .采用Hoffman理论计算了PP MMT的球晶生长的单位面积表面自由能σe,结果表明σe 随MMT含量的增加逐渐降低  相似文献   

17.
朱德钦  生瑜  童庆松  王真 《应用化学》2014,31(8):885-891
在转矩流变仪中用熔融接枝法制备马来酸酐(MAH)和苯乙烯(St)接枝聚丙烯(PP)-PP-g-(MAH/St)和PP-g-MAH,将其作为聚丙烯/木粉复合材料的相容剂。 FTIR证实MAH和St单体与PP发生接枝反应。 用SEM和DSC等手段考察两种相容剂对PP/木粉复合材料微观形貌和结晶性能的影响,探索了各种PP/木粉复合材料加工和力学性能不同的内在原因。 SEM显示,PP-g-(MAH/St)改性木粉比PP-g-MAH改性木粉在PP基体中分散性更佳,木粉与PP的界面更加模糊,相容性进一步改善。 DSC结果表明,PP-g-(MAH/St)改性体系可增强木粉对PP的异相成核作用,提高结晶温度和结晶度。 复合材料的加工和力学性能测试结果表明,PP-g-(MAH/St)改性效果明显优于PP-g-MAH。 复合材料的熔体质量流动速率随相容剂用量的增加而逐步下降,PP-g-(MAH/St)改性体系拉伸强度和弯曲强度却逐步上升,并在相容剂用量为4.8 g/100 g PP时达到极值。 此时其拉伸强度达40.62 MPa,分别是未改性体系和PP-g-MAH改性体系的1.29和1.17倍;其弯曲强度达45.72 MPa,分别是未改性体系和PP-g-MAH改性体系的1.23和1.59倍;而无缺口冲击强度却在相容剂用量为3.6 g/100 g PP时达到极值13.35 kJ/m2,分别是未改性体系和PP-g-MAH改性体系的1.62倍和1.42倍。  相似文献   

18.
The nonisothermal crystallization kinetics of poly(propylene) (PP) and poly(propylene)/organic‐montmorillonite (PP/Mont) nanocomposite were investigated by differential scanning calorimetry (DSC) with various cooling rates. The Avrami analysis modified by previous research was used to describe the nonisothermal crystallization process of PP and PP/Mont nanocomposite very well. The values of half‐time and Zc showed that the crystallization rate increased with increasing cooling rates for both PP and PP/Mont nanocomposite, but the crystallization rate of PP/Mont nanocomposite was faster than that of PP at a given cooling rate. The activation energies were estimated by the Kissinger method, and the values were 189.4 and 155.7 kJ/mol for PP and PP/Mont nanocomposite, respectively. PP/Mont nanocomposite could be easily fabricated as original PP, although the addition of organomontmorillonite might accelerate the overall nonisothermal crystallization process. © 2002 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 40: 408–414, 2002; DOI 10.1002/polb.10101  相似文献   

19.
The crystallization kinetics of polypropylene (PP) with hyperbranched polyurethane acrylate (HUA) being used as a toughening agent was studied by isothermal and nonisothermal differential scanning calorimetry (DSC). The presence of a small amount of HUA (2-7%) remarkably influences the crystallizability of PP. An addition of HUA leads to an increase in the number of effective nuclei, thus resulting in an increase of crystallization rate and a stronger trend of instantaneous three-dimensional growth. For isothermal crystallization, Avrami exponents were determined to be about 2.97 for pure PP and 3.51 for the HUA/PP blend containing 5% HUA (HUA-PP). The half crystallization time (t1/2) of pure PP was measured to be 8.43 min, while being 3.28 min for HUA-PP at the crystallization temperature of 132 °C. The nonisothermal crystallization kinetics of HUA/PP blends was analyzed by Avrami, Ozawa and Kissinger methods. It has also been proved that an addition of HUA could increase the crystallization rate of PP. Moreover, the crystallization activation energies of pure PP and HUA-PP were estimated by Kissinger and Friedman methods.  相似文献   

20.
Crystalline structures, nonisothermal crystallization behavior and surface folding free energy of polypropylene (PP)/poly(ethylene‐co‐vinyl acetate) (EVA) blend‐based organically modified montmorillonite (OMMT) nanocomposites were investigated by use of wide angle X‐ray scattering (WAXS) and differential scanning calorimetry (DSC) techniques. Nonisothermal crystallization kinetic analysis was performed using Avrami equation modified by Jeziorny as well as combined Avrami‐Ozawa method. Surface folding free energy and activation energy for PP and nanocomposite samples were also determined employing Hoffman‐Lauritzen's and Vyazovkins's approaches, respectively. The results obtained from transmission electron microscopy (TEM) showed that presence of EVA, which attracts most of the layered silicates, reduces number density of heterogeneous nuclei in the matrix and as a consequence, decreases the nucleation rate. Incorporation of EVA, PP‐g‐MA and OMMT results in a decrease of the chain surface folding free energy level. It was shown that although, OMMT acts as a barrier against the PP macromolecular motion but interestingly, it increases the overall crystallization rate. © 2009 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 47: 674–684, 2009  相似文献   

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