PP/纳米Dy_2O_3复合材料的非等温结晶

用溶液法制备了聚丙烯(PP)/纳米三氧化二镝(Dy_2O_3)复合材料,用差示扫描量热法研究了PP/纳米Dy_2O_3复合材料的非等温结晶行为,采用Caze法和莫志深法对其结晶动力学进行了分析,研究了纳米粒子的成核效率和成核活性。结果表明:纳米Dy_2O_3提高了PP的结晶峰温和结晶速率,使结晶活化能增大;w(Dy_2O_3)为2%的纳米粒子成核效率最高,w(Dy_2O_3)为5%的纳米粒子成核活性最低。     

纳米Al_2O_3改性聚丙烯的非等温结晶动力学

采用差示扫描量热法研究了聚丙烯(PP)及PP/纳米Al_2O_3复合材料的非等温结晶动力学。结果表明:纳米Al_2O_3有异相成核的作用,使PP的结晶峰温升高;PP的半结晶时间随纳米Al_2O_3含量增大而减小;纳米粒子的填充使PP的结晶活化能(△E)增大,含纳米Al_2O_3质量分数为2%的PP的△E最大。     

纳米SiO_2/MC尼龙6原位复合材料等温结晶行为的研究

将纳米SiO2均匀分散在己内酰胺单体熔体中,采用阴离子开环聚合法制备了纳米SiO2/单体浇铸(MC)尼龙6原位复合材料。通过差示扫描量热仪(DSC)、Avrami方程、Lauritizen-Hoffmann方程对复合材料的等温结晶行为进行了研究。结果表明:纳米SiO2的引入改变了基体MC尼龙6的成核机理和生长方式;低含量的纳米SiO2阻碍了MC尼龙6的结晶行为,高含量的纳米SiO2降低了MC尼龙6的结晶活化能,提高了其球晶生长速率,并促进了其结晶行为。     

MC尼龙6/TiO2原位纳米复合材料等温结晶动力学的研究

采用差示扫描量热法(DSC)研究了阴离子原位聚合法制备的铸型尼龙6(MC尼龙6)/TiO2纳米复合材料的等温结晶行为,并应用Avrami方程分析了MC尼龙6的等温结晶动力学过程.结果表明纳米TiO2对MC尼龙6基体具有异相成核作用,使其原位纳米复合材料结晶速率常数变大,半结晶时间变小.Hoffman成核结晶理论计算结果表明,原位纳米复合材料的Kg(与结晶温度无关而与成核方式有关的参数)大于MC尼龙6且随着纳米含量的增加而增加,说明纳米TiO2阻碍了MC尼龙6分子链的运动,同时尼龙6由晶核生长占主导地位逐渐向成核机制占主导地位转变.     

MC尼龙/稀土纳米复合材料制备的反应动力学研究

测定了MC尼龙和MC尼龙/稀土纳米复合材料制备的温度与时间关系曲线,用非等温反应动力学方法对数据进行处理,用多元回归法确定其表观动力学参数。结果表明:MC尼龙和MC尼龙/稀土纳米复合材料制备过程的动力学特征基本相似,是一个并行的聚合/结晶过程;稀土纳米氧化物对MC尼龙制备的阴离子聚合反应有促进作用;MC尼龙和MC尼龙/稀土纳米复合材料制备过程的表观活化能在92~145kJ/mol之间,反应级数在0.9~1之间,频率因子在108~1014之间,MC尼龙和MC尼龙/稀土纳米复合材料制备过程由化学反应步骤控制。     

纳米二氧化硅/MC尼龙6原位复合材料非等温结晶动力学的研究

通过阴离子开环聚合法制备了纳米二氧化硅(SiO2)／MC尼龙6原位复合材料。采用差示扫描量热法研究了MC尼龙6及其原位纳米复合材料的非等温结晶行为；并利用修正Avrami方程的Jeziomy和Liu法进一步处理原位纳米复合材料的非等温结晶动力学。结果表明，在纳米SiO2／MC尼龙6原位复合材料中，纳米SiO2对基体MC尼龙6的结晶有一定的成核作用，并提高了其结晶速率。     

MC尼龙／Sm2O3纳米复合材料的制备及性能研究

用原位分散聚合法制备了一系列MC尼龙/Sm2O3纳米复合材料,并对其结构和力学性能进行了表征.结果表明,纳米Sm2O3使MC尼龙晶格尺寸发生了一定程度的改变;纳米Sm2O3的加入可以明显改善MC尼龙的力学性能,对MC尼龙同时具有增强和增韧双重效果;MC尼龙/Sm2O3纳米复合材料的力学性能随着纳米Sm2O3用量的增加呈先升高后降低的趋势.当纳米Sm2O3的质量分数为0.5%时,复合材料的拉伸强度和断裂伸长率达到最大值,分别比MC尼龙提高了18.8%和91.5%,当纳米Sm2O3的质量分数为1.0%时,复合材料的缺口冲击强度、穹曲强度和弯曲弹性模量达到最大值,分别比MC尼龙基体提高了36.6%、11.2%和11.5%.     

反应性增容对PP/纳米SiO2中填料成核活性的影响

采用示差扫描量热法研究PP/纳米二氧化硅(SiO2)复合材料的非等温结晶动力学.研究结果表明:纳米SiO2起到异相成核的作用,使PP的结晶峰温升高;反应性增容增强了纳米SiO2的威核活性;添加纳米SiO2使PP的结晶活化能增大,反应性增容使复合材料的结晶活化能减小,与纯PP的结晶活化能相近;但反应性增容使PP的结晶总速率小于未增容填充体系.     

MC尼龙6/TiO2原位纳米复合材料的制备及表征

利用阴离子原位聚合法制备了铸型尼龙6(MC尼龙6)／TiO2原位纳米复合材料,并对其结构与性能进行了表征。透射电子显微镜观察表明,TiO2以纳米级均匀分散于MC尼龙6中,其含量小于1份时近乎单分散,大于1份时则开始团聚。差示扫描量热法和X射线衍射法分析结果表明,纳米TiO2对MC尼龙6的结晶起到了异相成核作用,提高了MC尼龙6的结晶温度,但不改变MC尼龙6的α晶型结构;退火处理结果表明,高温退火或加入纳米TiO2,都有利于MC尼龙6基体中α晶型的生成,加快γ晶向α晶的转变。热重分析和力学性能测试表明,纳米TiO2提高了复合材料的热稳定性,其拉伸强度、冲击强度等也得到了不同程度的提高。     

纳米二氧化硅／MC尼龙6原位复合材料非等温结晶动力学

通过阴离子开环聚合法制各纳米二氧化硅／MC尼龙6原位复合材料,采用差示扫描量热法研究MC尼龙6及其原位纳米复合材料非等温结品行为,并利用修正Avrami方程的Jeziomy和Liu的方法进一步处理原位纳米复合材料的非等温结晶动力学,结果表明在纳米二氧化硅／MC尼龙6原位复合材料中,纳米二氧化硅对基体MC尼龙6的结晶有一定的成核作用,并提高了其结品速率。     

Isothermal and nonisothermal crystallization kinetics of MC nylon and polyazomethine/MC nylon composites

Crystallization kinetics of MC nylon (PA6) and polyazomethine (PAM)/MC nylon (PAM/PA6) both have been isothermally and nonisothermally investigated by different scanning calorimetry (DSC). Two stages of crystallization are observed, including primary crystallization and secondary crystallization. The Avrami equation and Mo's modified method can describe the primary stage of isothermal and nonisothermal crystallization of PA6 and PAM/PA6 composite, respectively. In the isothermal crystallization process, the values of the Avrami exponent are obtained, which range from 1.70 to 3.28, indicating an average contribution of simultaneous occurrence of various types of nucleation and growth of crystallization. The equilibrium melting point of PA6 is enhanced with the addition of a small amount of rigid rod polymer chains (PAM). In the nonisothermal crystallization process, we obtain a convenient method to analyze the nonisothermal crystallization kinetics of PA6 and PAM/PA6 composites by using Mo's method combined with the Avrami and Ozawa equations. In the meanwhile, the activation energies are determined to be ?306.62 and ?414.81 KJ/mol for PA6 and PAM/PA6 (5 wt %) composite in nonisothermal crystallization process from the Kissinger method. Analyzing the crystallization half‐time of isothermal and nonisothermal conditions, the over rate of crystallization is increased significantly in samples with a small content of PAM, which seems to result from the increased nucleation density due to the presence of PAM rigid rod chain polymer. © 2004 Wiley Periodicals, Inc. J Appl Polym Sci 93: 2844–2855, 2004     

PPES/MC尼龙6中相互作用对MC尼龙6的结晶及熔融行为影响

采用原位共混与溶液共沉淀两种不同的方法制得了PPES/MC尼龙6共混物。通过对共混物的DSC非等温结晶与熔融行为表征,推出共混物之间的相互作用。结果表明两种共混物中PPES对MC尼龙6的结晶都起阻碍作用,溶液共混物中熔融峰温(Tm)相对于MC尼龙6变化不大,而其在原位共混物中的影响很大,使得MC尼龙6的熔融峰温(Tm)向高温移动。更值得注意的是,原位共混物中MC尼龙6的结晶与熔融峰温相对于溶液共沉淀样品中偏移纯MC尼龙6的峰温更明显,说明原位共混物中PPES与MC尼龙6之间的相互作用大于溶液共沉淀共混物中的PPES与MC尼龙6的相互作用。在溶液共沉淀中MC尼龙6的结晶和熔融峰温均比在原位共混物中的高。     

Isothermal and nonisothermal crystallization kinetics of bio-sourced nylon 69☆

Bio-sourced nylon 69,one of promising engineering plastics,has a great potential in developing sustainable technology and various commercial applications.Isothermal and nonisothermal crystallization kinetics of nylon 69 is a base to optimize the process conditions and establish the structure–property correlations for nylon 69,and it is also highly bene ficial for successful applications of nylon products in industry.Isothermal and nonisothermal crystallization kinetics has been investigated by differential scanning calorimetry for nylon 69,bio-sourced even–odd nylon.The isothermal crystallization kinetics has been analyzed by the Avrami equation,the calculated Avrami exponent at various crystallization temperatures falls into the range of 2.28 and 2.86.In addition,the Avrami equation modi fied by Jeziorny and the equation suggested by Mo have been adopted to study the nonisothermal crystallization.The activation energies for isothermal and nonisothermal crystallization have also been determined.The study demonstrates that the crystallization model of nylon 69 might be a twodimensional(circular)growth at both isothermal and nonisothermal crystallization conditions.Furthermore,the value of the crystallization rate parameter(K)decreases signi ficantly but the crystallization half-time(t1/2)increases with the increase of the isothermal crystallization temperature.To nonisothermal crystallization,the crystallization rate increases as the cooling rate increases according to the analysis of Jeziorny's theory.The results of Mo's theory suggest that a faster cooling rate is required to reach a higher relative degree of crystallinity in a unit of time,and crystallization rate decreases when the relative degree of crystallinity increases at nonisothermal crystallization conditions.     

Melting behavior,isothermal and nonisothermal crystallization kinetics of nylon 1111

The isothermal and nonisothermal crystallization kinetics of nylon 1111 was extensively studied using differential scanning calorimetry (DSC). The equilibrium melting temperature of nylon 1111 was determined to be 188°C. In this article, the Avrami equation was used to describe the isothermal crystallization behavior of nylon 1111. On the basis of the DSC results, the Avrami exponent, n, was determined to be around 3 during the isothermal crystallization process. Nonisothermal crystallization was analyzed using both the Avrami equation as modified by Jeziorny and an equation suggested by Mo. The larger value of the Avrami exponent, n, during the nonisothermal crystallization process indicates that the development of nucleation and crystal growth are more complicated during the nonisothermal crystallization for nylon 1111, and that the nucleation mode might simultaneously include both homogeneous and heterogeneous nucleations. The isothermal and nonisothermal crystallization activation energies of nylon 1111 were determined to be ?132 kJ/mol and ?121 kJ/mol using the Arrhenius equation and the Kissinger method, respectively. POLYM. ENG. SCI., 2009. © 2009 Society of Plastics Engineers     

MCPA6/纳米TiO2原位复合材料的熔融行为

采用差示扫描量热法(DSC)研究了铸型尼龙6(MCPA6)及其纳米TiO2原位复合材料的等温结晶与非等温结晶晶体的熔融行为。结果表明：MCPA6／纳米TiO2原位复合材料等温结晶晶体的熔融行为呈现三重熔融峰，非等温结晶晶体的熔融行为呈现二重熔融峰；其高温熔融峰温随等温结晶温度或降温速率的变化基本不变，而低温熔融峰温则随等温结晶温度的升高或降温速率的减小而提高；纳米TiO2的加入对MCPA6有一定的成核作用，使其熔点提高。     

Studies on crystallization kinetics of nylon 6-polyoxypropylene-nylon 6 copolymers

The crystllization kinetics of anionic-prepared nylon6-poly(oxypropylene) 1000-nylon 6 (NPN) block copolymers containing 1.20 to 8.76 wt% poly(oxypropylene)(POP) were studied. The thermograms of isothermal and nonisothermal differential scanning calorimetry of NPN block copolymers obtained were used for the study. The Avrami equation was used to analyze the isothermal crystallization of NPN nylon block copolymers. The Avrami exponent n obtained in the temperature range of 180 to 200 °C was 2.0 to 2.5. It was not similar to that for nylon 6 reported in literature. The activation energies of crystallization for the nylon block copolymers were smaller than that of nylon 6, and showed a minimum with POP content. The equilibrium melting point increased as the POP content decreased. For the nylon block copolymers with lower POP content, the slopes of T_c vs. T_m plots were higher than the values reported elsewhere. The Ozawa plot was used to analyze the data of nonisothermal crystallization. The obvious curvature in the plot indicated that the Ozawa model could not fit our system well, and there was an abrupt change of the slope in the Ozawa plot at a critical cooling rate.     

Isothermal and nonisothermal crystallization kinetics of novel even‐odd nylon 10 11

Isothermal and nonisothermal crystallization kinetics of even‐odd nylon 10 11 were investigated by differential scanning calorimetry (DSC). Equilibrium melting point was determined to be 195.20°C. Avarmi equation was adopted to describe isothermal and nonisothermal crystallization. A new relation suggested by Mo was used to analyze nonisothermal crystallization and gave a good result. The crystallization activation energies have been obtained to be ?583.75 and ?270.06 KJ/mol for isothermal and nonisothermal crystallization, respectively. © 2005 Wiley Periodicals, Inc. J Appl Polym Sci 97: 1637–1643, 2005