热历史对聚醚醚酮及其碳纤维复合材料——Ⅱ.熔融行为的影响

本文利用差示扫描量热仪(DSC)研究了聚醚醚酮(PEEK)和以PEEK为基体的碳纤维复合材料(APC-2)的热历史对它们熔融行为的影响。在200—315℃结晶并退火热处理后,试样的DSC曲线上出现了两个吸热峰。低温吸热峰(峰温T′_m)较小,并与结晶和退火温度(T_c)有关;高温吸热峰(峰温T_m)较大,几乎不受T_n的影响。T′_m的出现与在不同T_c下生成的不完整晶体的熔融和重结晶过程有关,而T_m的出现则与完整晶体的熔融过程有关。实验结果表明,T′_m与T_c之间呈线性关系。按文献报道的方法,将T′_m与T_c的直线外推至与T′_m=T_c直线相交,其交点温度即为平衡熔点.结果表明,PEEK和APC-2试样的“平衡熔点”受不同热历史条件下生成晶体的完整程度的影响。当结晶并退火时间越长,求出的“平衡熔点”值越低,并与理论值接近。实验结果还表明,碳纤维表面具有促进PEEK树脂基体晶体完整化的作用,因而导致APC-2试样中PEEK树脂基体的熔点高于纯PEEK树脂。     

热历史对聚醚醚酮及其碳纤维复合材料——Ⅱ.熔融行为的影响

 本文利用差示扫描量热仪(DSC)研究了聚醚醚酮(PEEK)和以PEEK为基体的碳纤维复合材料(APC-2)的热历史对它们熔融行为的影响。在200—315℃结晶并退火热处理后,试样的DSC曲线上出现了两个吸热峰。低温吸热峰(峰温T′_m)较小,并与结晶和退火温度(T_c与在不同T_c下生成的不完整晶体的熔融和重结晶过程有关,而T_m的出现则与完整晶体的熔融过程有关。实验结果表明,T′_m与T_c之间呈线性关系。按文献报道的方法,将T′_m与T_c的直线外推至与T′_m=T_c直线相交,其交点温度即为平衡熔点.结果表明,PEEK和APC-2试样的“平衡熔点”受不同热历史条件下生成晶体的完整程度的影响。当结晶并退火时间越长,求出的“平衡熔点”值越低,并与理论值接近。实验结果还表明,碳纤维表面具有促进PEEK树脂基体晶体完整化的作用,因而导致APC-2试样中PEEK树脂基体的熔点高于纯PEEK树脂。     

聚醚醚酮/碳纤维复合材料的界面结构以及结晶形态的研究

本文采用扫描电子显微镜观察经氩等离子刻蚀后PEEK/碳纤维复合材料的界面层结构和PEEK树脂的结晶形态。无论是从熔体还是从橡胶体结晶,PEEK树脂的结晶都是从碳纤维表面诱导开始,最后形成横穿晶体结构。在高碳纤维含量的复合材料中,PEEK的球晶尺寸主要由碳纤维之间的距离控制,受温度的影响较小。在PEEK/碳纤维复合材料的结晶过程中,第一片晶片在碳纤维表面取向生长方式为:晶体的ā轴(厚度方向)平行于维纤径 向。b轴(晶片生长方向)与纤维最小圆截面的切线重合,(?)轴(垂直晶片平面的方向)平行于纤维轴向。由于球晶成核过程是取向生长,因而生成的球晶也按一定的方式取向。     

不同初始条件下聚乳酸的等温结晶动力学

用差示扫描量热法(DSC)研究聚乳酸(PLA)从熔体及玻璃态两种初始状态下的等温结晶行为,考查结晶动力学参数与结晶温度(Tc)及初始状态的关系.实验结果表明:从玻璃态结晶活化能(359 kJ/mol)较从熔体结晶活化能(103 kJ/mol)高;相应的Avrami指数n(2.3～2.7)小于从熔体的(2.5～3.1);所测得的平衡熔点是一致的,分别为155.7℃(玻璃态)、156.4℃(熔体);从玻璃态结晶诱导时间(ti)随着Tc升高而逐渐减小,从熔体结晶Tc=95℃时,出现最小ti为9.47min;在整个Tc区间,从玻璃态结晶速率(G)都受生长控制,从熔体低温时G受生长过程控制,高温时受成核过程控制.     

热塑性聚酰亚胺与聚醚醚酮共混物的等温结晶动力学

采用熔融共混方法制备了热塑性聚酰亚胺(TPI)与聚醚醚酮(PEEK)的共混物; 用示差扫描量热分析(DSC)研究了共混物的等温结晶动力学. 分别采用Avrami方程和Hoffman-Lauritzen方程分析共混物的等温结晶动力学、端表面自由能(σe)和分子链折叠功(q). 结果表明, 加入TPI后PEEK的结晶速率降低, 结晶活化能、σe和q均增加. 但这些数值的变化与TPI含量不呈线性关系, 并从共混物的相容性和表面形貌给出了可能的解释.     

PEEK复合材料的降解动力学

石墨、碳纤维和聚四氟乙烯(PTFE)填充的聚醚醚酮(PEEK)具有自润滑作用,是高性能的复合材料。采用热失重分析仪研究了聚醚醚酮及其复合材料的热降解行为,用Kissinger方法和Ozawa方法计算了复合材料的反应活化能(Ea)。与PEEK相比较,自润滑PEEK复合材料具有更高的降解反应活化能和更低的反应速率常数(K)。     

乙烯含量对抗冲丙烯共聚物等温结晶行为的影响

利用DSC研究了乙烯含量不同的4种抗冲丙烯共聚物的等温结晶动力学.结果表明4种样品在考察的温度范围内(126~130℃)的等温结晶动力学完全符合Avrami方程,并得到了不同结晶温度下Avrami方程的结晶动力学参数k,n和t1/2,随着样品中乙烯含量的增加,Avrami指数(n)随温度变化不大,样品的结晶过程可能属于三维扩散控制的成核增长,4种样品的结晶活化能ΔE在279.5~343.1 kJ/mol范围内,且随乙烯含量增加,结晶活化能增大,充分说明样品中的乙烯含量是影响其结晶活化能的主要因素.结晶分级分析测试结果显示,随着乙烯含量的增加,聚丙烯均聚物部分链结构规整性提高,结构规整、可结晶的长序列含量在减少,可见乙烯含量的变化规律直接决定上述参数的变化规律.     

新型聚芳醚酮与热致性液晶高聚物共混物流变性能和力学性能的研究

本文研究了新型聚芳醚酮与热致性液晶高聚物(PEK-C/LCP)共混物的流变性能及力学性能。结果表明:由于LCP的加入,PEK-C的熔体粘度降低;随着剪切速率的增加,共混物熔体流动活化能从223.5KJ/mol降为102.2KJ/mol。共混物的玻璃化转变温度从纯PEK-C的218℃降为199℃;除模量增加外,其它力学性能均有所下降。同时利用SEM观察了共混物冲击断面形貌,未发现有LCP微纤维生成。     

新型聚芳醚酮与热致性液晶高聚物共混物流变性能和力学性能的研究

 本文研究了新型聚芳醚酮与热致性液晶高聚物(PEK-C/LCP)共混物的流变性能及力学性能。结果表明:由于LCP的加入,PEK-C的熔体粘度降低;随着剪切速率的增加,共混物熔体流动活化能从223.5KJ/mol降为102.2KJ/mol。共混物的玻璃化转变温度从纯PEK-C的218℃降为199℃;除模量增加外,其它力学性能均有所下降。同时利用SEM观察了共混物冲击断面形貌,未发现有LCP微纤维生成。     

左旋聚乳酸的结晶行为研究

用DSC, WAXD和POM对Zn催化剂制备的左旋聚乳酸(PLLA)的熔体结晶行为进行了研究. 在95~125 ℃范围内, PLLA熔体结晶生成厚度约(14±1) nm的片晶, 该片晶不易发生熔体等温增厚. 对实验数据分别用Avrami方程和Arrhenius方程进行了计算, Avrami指数n=3±0.3, 表明PLLA以球晶形式生长, 其最大结晶速率温度为(105.0±0.5) ℃, t1/2约为5.2 min. 利用Lauritzen-Hoffmann（LH）理论对PLLA结晶机理进行了分析, 发现PLLA结晶的Regime Ⅱ和Regime Ⅲ的转变温度为107 ℃. Kg(Ⅱ)和Kg(Ⅲ)分别为4.57×105 K2和1.115×106 K2, 且Kg(Ⅲ)/Kg(Ⅱ)=2.4, 与LH理论值一致.     

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...     

Study of the carbon fiber–Poly(Ether–Ether–Ketone) (PEEK) interfaces, 3: influence and properties of interphases

The aim of this third part is to analyze the structure and properties of the interfacial region between carbon fibers and PEEK as a function of different thermal conditioning treatments. First, it is shown by means of optical microscopy that the interfacial zone is not different from the bulk matrix when standard cooling conditions are used. On the contrary, a transcrystalline interphase is formed near the carbon fiber surface in systems that have been subjected to isothermal treatments. By comparison with previous results concerning the mechanical properties of the fiber–matrix interface, it appears that the interfacial shear strength decreases in the presence of a transcrystalline interphase or when the crystallization rate of PEEK increases. Moreover, it seems that the “constraint state” of the amorphous phase of PEEK near the fiber surface could also play a role in the interfacial shear strength. Secondly, a method is proposed in order to estimate the elastic modulus of crystalline interphases. It seems that this modulus is strongly dependent on the crystallization rate of the polymer. Finally, the determination of the stress-free temperature, defined as the temperature at which a longitudinal compressive stress just appears on the carbon fiber during the processing of the composites, is performed by recording the acoustic events corresponding to the fragmentation process in single-fiber composites. The results confirm that the crystallization rate and the “constraint state” of the amorphous phase of the matrix play an important role in the mechanical behavior of carbon fiber–PEEK interfaces.     

Study of the carbon fiber–poly(ether–ether–ketone) (PEEK) interfaces, 2: relationship between interfacial shear strength and adhesion energy

In the second part of this general study, the carbon fiber–PEEK interfacial shear strength is measured by means of a fragmentation test on single-fiber composites. Different thermal treatments (continuous cooling from the melt, isothermal treatments and long melting temperature time) are applied to these model composites prior to testing. The results are systematically compared with the previously determined reversible work of adhesion between carbon fiber and PEEK. It is shown that physical interactions at the interface determine, to a large extent, the magnitude of the interfacial shear strength between both materials. However, it appears that the magnitude of the stress transfer from the matrix to the fiber is affected either by the existence of an interfacial layer or by a preferential orientation of the polymer chains near the fiber surface. The results obtained on systems that have been subjected to isothermal treatments (isothermal crystallization of PEEK) seem to confirm the existence of a transcrystalline interphase, the properties of which are dependent upon the crystallization rate of the matrix and the interfacial adhesion energy.     

Unified isothermal and non-isothermal modelling of neat PEEK crystallization

A differential generalized Avrami’s law is used to model crystallization kinetic of PEEK in considering that PEEK crystallization results from the contribution of two distinct mechanisms. The form of this equation allows to predict with good accuracy both isothermal and non-isothermal crystallization kinetics. Nevertheless, isothermal model parameters are not entirely satisfactory for predicting non-isothermal crystallization and the identification of kinetic parameters is needed for both isothermal and non-isothermal cases. The results show that the Avrami exponents and Arrhenius activation energies remain constant for both conditions and therefore suggest that these parameters are only material dependent. On the other hand, the other kinetic parameters depend on the crystallization condition and vary with temperature and/or cooling rate.     

固相缩聚PET等温结晶动力学

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.     

联苯聚醚醚酮酮的结晶动力学的研究

通过ｄｓｃ 方法对新型聚芳醚酮联苯聚醚醚酮酮（ＰＥＥＫＤＫ） 的等温及非等温熔融结晶动力学进行了研究,运用Ａｖｒａｍｉ 方程分析了其等温结晶行为,求得了等温结晶活化能,平衡熔点,成核参数,并与其它聚芳醚酮类聚合物进行了比较。同时,对ＰＥＥＫＤＫ的非等温结晶动力学也进行了研究。     

尼龙6,6(PA_(6,6)及其共混物结晶性能的研究

<正> 尼龙6,6(PA_(6,6))是一种典型的结晶性工程塑料,被广泛应用于纺织、机械制造等行业,但其加工温度范围较窄,耐热性差。聚醚砜(PES)具有较高的玻璃化转变温度,是非晶聚合物,可以诱发某些结晶聚合物结晶。PES与PA_(6,6)共混体系的研究报道较少,本文用熔融法将PES与PA_(6,6)制成共混物,企图改善PA_(6,6)的结晶性,以提高其耐热性,取得了较理想的结果。     

Nonisothermal crystallization kinetics of poly(β-hydroxybutyrate)

Kinetics of nonisothermal crystallization of poly(β-hydroxybutyrate) from melt and glassy states were performed by differential scanning calorimetry under various heating and cooling rates. Several different analysis methods were used to describe the process of nonisothermal crystallization. The results showed that both Avrami treatment and a new method developed by combining the Avrami equation and Ozawa equation could describe this system very well. However, Ozawa analysis failed. By using an evaluation method, proposed by Kissinger, activation energies have been evaluated to be 92.6 kJ/mol and 64.6 kJ/mol for crystallization from the glassy and melt state, respectively. © 1998 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 36: 1305–1312, 1998