聚醚醚酮酮等温结晶动力学的研究

聚醚醚酮酮等温结晶动力学的研究陈艳，王军佐，曹俊奎，那辉，吴忠文（吉林大学化学系，长春，１３００２３）关键词聚醚醚酮酮，等温结晶动力学，差示扫描量热法聚醚醚酮酮（ＰＥＥＫＫ）是在聚醚醚酮（ＰＥＥＫ）基础上开发成功的一种耐热高分子材料。它保持了ＰＥＥＫ...     

PA13N的合成和非等温结晶动力学研究

采用DSC方法研究了PA13N在不同降温速率下的结晶过程,并利用Avrami方程研究了其非等温结晶动力学。在非等温结晶过程中,随着降温速率的增大,结晶温度向低温偏移。综合利用Avrami方程得到Avrami指数为1.35~1.88和结晶速率常数Zc≈1;并求得其结晶活化能为-58.42kJ/mol。结果表明,PA13N的结晶能力小于其他脂肪族尼龙。     

半芳香尼龙6T/66的合成和非等温结晶动力学的研究

采用成盐、预聚合、固相聚合三步法制备高分子量的PA6T/66,用差示扫描量热法(DSC)研究了PA6T/66的非等温结晶动力学,结果表明:结晶温度随着降温速率的增大而降低;半结晶期T1/2随降温速率Ф的增大呈指数下降,表明结晶速率随降温速率的增大而提高;由用R-T法可以得到在不同结晶度下lgΦ对lgT有较好的线性关系。用Kissinger方法计算得到PA6T/66(55/45)非等温结晶活化能分别为ΔE=-61.51kJ/mol。     

高聚物非等温结晶动力学

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。     

己内酯和2,2-二羟甲基丁酸共聚酯的非等温结晶动力学研究

采用示差扫描量热仪(DSC) 研究了具有生物相容性及可降解性P(BHB-CL)超支化共聚酯的非等温熔融结晶过程, 分别采用Avrami 方程、Ozawa 方程和Mo方程对P(BHB-CL)共聚酯的非等温动力学数据进行比较分析, 计算了相关的非等温结晶动力学参数, 并利用Kissinger方程计算其非等温结晶活化能. 结果表明, Mo方程更适合描述P(BHB-CL)共聚酯的非等温结晶过程.     

高岭土相转变的非等温动力学

<正>高岭土为三斜晶系,一般为无色至白色的细小鳞片,单晶呈假六方板状或书册状,平行连生的集合体往往呈蠕虫状或手风琴状,是造纸、陶瓷、化工、涂料、医药和国防等几十个行业中必须的矿物     

超支化聚酯对聚乙二醇非等温结晶行为的影响

利用差示扫描量热法(DSC)、偏光显微镜(POM)以及傅里叶变换红外(FTIR)光谱研究了一种超支化聚酯(HBP)对聚乙二醇(PEG)非等温结晶行为的影响,用Ozawa法、Jeziorny法和莫志深法对非等温结晶动力学进行了分析.结果表明:PEG和HBP/PEG的非等温结晶过程可用Ozawa和莫志深动力学方程描述,与Jeziorny动力学方程不符;超支化聚酯的加入改变了PEG的结晶成核和生长机理,对PEG的结晶有一定的延缓作用.超支化聚酯中的羰基与PEG的端羟基形成的氢键以及超支化聚酯自身较大的分子体积和高度支化的结构所导致的位阻效应是超支化聚酯延缓PEG结晶的主要原因.     

非共价键合杂化体系中聚己内酯的非等温结晶动力学

非共价键合杂化体系中聚己内酯的非等温结晶动力学;聚己内酯;有机-无机杂化材料;差示扫描量热法;非等温结晶动力学     

测定高聚物结晶动力学参数的非等温理论和方法

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。     

Studies on Kinetics of Crystallization of PA6／UFAPR Composites

The influence of Ultrafine Full-Vulcanized Acrylate Powdered Rubber(UFAPR) on the isothermal crys-tallization kinetics and nonisothermal crystallization behavior of PA8 has been studied by means of DSC. The results show that with the introduction of a small amount of UFAPR, the crystallization rate of PA8 can be increased obviously, and the crystallization temperature range can be augmented and the crystallite size distri-bution of the crystal can be narrowed down. The change of free energy perpendicular to the crystal nucleus, which has been calculated according to the Hoffman theory, is consistent with the result of Avrami′s equa-tion. The unit surface free energy of the radial-developing crystal spherulite decreases while the crystalliza-tion rate of PA8 increases with the introduction of UFAPR. Meanwhile, it is shown by means of the polariz-ing microscope(PLM) that the crystal size drops down and the number of the crystal grains augments with the addition of UFAPR, which shows that UFAPR can function as a nucleating agent.     

聚丙烯/凹凸棒土纳米复合材料的非等温结晶动力学

聚丙烯/凹凸棒土纳米复合材料的非等温结晶动力学     

聚甲醛/蒙脱土纳米复合材料非等温结晶动力学研究

聚甲醛/蒙脱土纳米复合材料非等温结晶动力学研究     

聚丙烯/聚(丙烯-g-马来酸酐)/蒙脱土纳米复合材料结晶动力学研究

非等温结晶动力学;聚丙烯/聚(丙烯-g-马来酸酐)/蒙脱土纳米复合材料结晶动力学研究     

Kinetics of Nonisothermal and Isothermal Crystallization of Metallocene Polyethylene

Thedevelopmentofmetallocenecatalystsundoubtedlyrepresentsarevolutioninthepolyolefinbusiness.MetallocenePE(MPE)coverspolyethyleneswhichareproducedbymetallocenecatalysttechnology.EXXONChemicalCo.developedanewmeta-llocenepolyethylene-EXCEED'"PEin1991.Nowmoreandmoreeffortsarespentonthisinterestingproject.Uniformmolecularstructureandnarrowmoleculardistribution,makeMPEbetterphysicalpropertiesthanthoseofconventionalPE,andalsomakeitlowmeltstrengthandbadprocessability.Sotherelationshipbetween…     

反式1,4-聚丁二烯的非等温结晶动力学研究

采用Nd(P5O7),-LiBu-AlEt3和AlEt3-VCI3两种催化剂体系分别合成了两种分子量与反式1,4单元结构含量不同的反式1,4-聚丁二烯样品(TPBD)。用DSC方法不仅研究了两样品六方相晶体的非等温结晶过程,同时还对单斜相结晶的非等温动力学过程进行了研究。Avrami方程分析显示,在低结晶度下TPBD六方相和单斜相的结晶生长过程呈现热成核的三维球晶生长。研究表明：虽然Ozawa方程在较低温度下能描述TPBD的六方相结构的实验数据,但不能完全描述在较高温度下六方相及单斜相非等温结晶过程,而用莫志深等建议的方程则能很好地描述TPBD六方相和单斜相非等温结晶过程。由Kissinger方程得到TPBD六方相和单斜相结晶的平均结晶活化能分别为-165．8kJ／mol和-220.5kJ／mol。     

Nonisothermal crystallization kinetics of in situ nylon 6/graphene composites by differential scanning calorimetry

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     

聚2-吡咯烷酮的非等温结晶动力学

用差示量热扫描热分析仪(DSC)测试了不同降温速率下聚2-吡咯烷酮(PPD)样品的温度-热焓曲线,样品黏均分子量为2.2×10~4,熔点为272℃。采用Jeziorny法、Ozawa法和莫志深法分析了PPD的非等温结晶动力学。结果表明,在给定降温速率范围内,Ozawa法不适用于描述PPD的非等温结晶动力学过程,Jeziorny法只适用于描述PPD的主结晶阶段,而莫志深法能很好地描述整个结晶过程。Jeziorny法处理结果表明,PPD主结晶阶段的Avrami指数(n)为1.68~1.78,晶体生长为准二维生长。莫志深法处理结果表明,在单位结晶时间里达到某一相对结晶度所需的降温速率随相对结晶度的增加而增大。用Kissinger方程求得PPD的非等温结晶活化能为-31.9kJ/mol。     

O-(4-喹唑啉)羟肟酸硫代酯(酰胺)类化合物的合成及生物活性

用差示扫描量热分析研究了间规聚苯乙烯（ｓＰＳ）的非等温结晶及其动力学，并分别用Ｏｚａｗａ和Ｊｅｚｉｏｒｎｙ两种方法来处理ｓＰＳ的非等温结晶数据．结果表明，在２５～４０℃／ｍｉｎ的冷却速率范围内，ｓＰＳ的半结晶时间随冷却速率增大而呈指数式下降，ｓＰＳ非等温结晶过程遵循Ｏｚａｗａ动力学方程，但不符合Ｊｅｚｉｏｒｎｙ方法中的Ａｖｒａｍｉ动力学方程．所得到的ｓＰＳ非等温结晶Ａｖｒａｍｉ指数ｎ在３６～４１之间，高于等温结晶时的ｎ值