PET/EN-MFMB增韧体系非等温结晶及熔融行为

用差热分析法研究了PET／EN-MFMB增韧体系逐渐升温和逐渐降温的结晶行为以及逐渐升温的熔融行为。结果表明:PET／EN-MFMB增韧体系中PET冷、热结晶开始结晶温度均比原料PET的有所降低,热结晶成核速率均比原料PET的有明显提高。HDPE的结晶过程受到了PET的阻隔、约束作用。PET结晶开始熔融温度一般都比原料PET 有所提高;HDPE结晶熔融峰顶温度比原料HDPE以及EN-MFMB中的HDPE的明显降低。     

PET/PEN共混体系的结晶及动态力学性能

通过熔融共混法制备了PET/PEN复合材料,利用差示扫描量热法(DSC)和动态热机械分析(DMA)研究了共混比例对复合材料结晶性能和动态力学性能的影响,结果表明:随PEN含量的增加,PET/PEN复合材料的结晶温度向低温方向移动,结晶能力变差,结晶度减小,当PEN用量大于50份时,共混物为非晶共聚物。PEN的加入可以显著提高PET的储能模量,随PEN含量的增加,复合材料的储能模量逐渐减小。tanδ-温度曲线表明:复合材料存在1个θg和1个冷结晶峰温度。随PEN含量的增加,共混物的θg和冷结晶峰逐渐增强,且冷结晶峰温度逐渐向高温方向移动,冷结晶倾向增强。     

PET/凹凸棒土复合材料的结晶行为研究

通过双螺杆熔融共混法制备PET/凹凸棒土(AT)复合材料,用示差扫描量热计(DSC)研究了PET、PET/AT复合材料的结晶行为.非等温分析结果表明:在PET中引入AT提高了PET基体结晶温度和PET结晶速率.PET及PET/AT复合材料的结晶温度随降温速率的增大而移向低温.半结晶时间及结晶度随降温速率的增大而减小.基于Avrami方程的动力学分析表明:PET/AT复合材料的非等温结晶过程是带有异相成核的三维增长过程.     

PEN非等温冷结晶动力学的研究

采用差示扫描量热(DSC)法对聚萘二甲酸乙二醇酯(PEN)的非等温冷结晶动力学进行研究;通过改变升温速率,讨论了PEN冷结晶起始温度与峰顶温度之间存在差值的原因;对比了两种不同的冷结晶起始点的确定方法对冷结晶动力学常数的影响。结果表明:以DSC曲线偏离基线作为PEN冷结晶的起始点,得到的表观Avrami指数很大;用基线延长线与DSC曲线的切线的交点作为冷结晶的起始点和结束点,得到的表观Avrami指数为2.55,且不随升温速率的变化而变化,与等温熔融热结晶方法得到的结果接近,具有相似的结晶生长方式。     

中低粘度PET非等温结晶性能研究

运用差示扫描量热仪研究了不同特性粘数(0.55~0.70 d L/g)的PET非等温冷结晶和熔融结晶过程。结果表明,随着特性粘数降低,PET样品消除热历史后的冷结晶起始温度θo和峰温θp向低温区偏移,半结晶时间t1/2延长,特性粘数在0.617 d L/g以下,易形成完善的大尺寸结晶;PET熔融结晶温度呈上升趋势,熔融结晶t1/2降低,结晶速率增加,当特性粘数大于0.657 d L/g时,t1/2和Avrami指数n明显增加,不利于拉膜时铸片的均匀性。     

PET/HMFNC-MB复合材料的非等温结晶及熔融行为

将H型多功能纳米碳酸钙母料(HMFNC-MB)与PET热机械反应性共混,制得了HMFNC-MB含量不同的PET/HMFNC-MB复合材料,采用DSC法研究了复合材料中PET的玻璃化转变,非等温冷、热结晶和熔融行为以及HDPE的非等温热结晶行为.结果表明,与原料PEF相比,PET/HMFNC-MB系列复合材料中PET的玻璃化转变温度Tg都有不同程度提高,最大提高幅度为6.7 ℃;冷结晶峰温(Tccp)均有不同程度下降,最大下降幅度达到10.2℃,结晶速率明显加快,过热度减小;熔融峰起始温度(Tmo)和峰温(Tmp)均有不同程度提高,最大提高幅度分别为9.0℃和3.5℃;热结晶峰起始温度和峰顶温虽均略有下降,但结晶速率明显加快.与原料HDPE的相比,PET/HMFNC-MB复合材料中HDPE的热结晶峰温降低了大约21℃,结晶过程很弥散.     

纳米氧化物作为成核剂对PET结晶速率的影响

研究了成核剂纳米氧化镁和纳米氧化硅对聚对苯二甲酸乙二醇酯(PET)结晶速率的影响。通过等温结晶差热分析(DSC)研究了纳米氧化镁在不同含量、不同温度下对PET等温结晶行为的影响。用纳米氧化镁和纳米氧化硅填充PET体系的非等温结晶DSC,由所得冷结晶峰温度值和热结晶峰温度值的对比,探索纳米成核剂对PET结晶速率的影响及其规律。研究结果表明:纳米成核剂均能明显提高PET的结晶速率,而纳米氧化镁比纳米氧化硅对促进PET的结晶效果更好;添加不同含量的纳米氧化镁对PET在不同温度下的等温结晶影响不同,在所研究的范围内,1.0%的添加量较有利于PET的结晶。     

回收PET玻纤复合材料的结晶性能研究

制备了成核回收PET及其玻璃纤维复合材料，研究了成核回收PET及其玻璃纤维复合材料的结晶与熔融行为、力学性能和加工性能。结果表明，无论是有机羧酸盐成核剂还是无机成核剂都使回收PET的冷结晶温度逐渐降低，热结晶温度逐渐提高。PBT作为PET结晶促进剂，降低回收PET的冷结晶温度，提高热结晶温度。成核回收PET复合材料的力学性能提高，加工性能改善，成型周期缩短。     

间苯二甲酸改性PET的结晶行为研究

应用 DSC研究了间苯二甲酸 (IPA)改性 PET的结晶行为。结果表明 :由于第三单体破坏了 PET大分子结构的规整性 ,导致改性聚酯熔点下降 ,冷结晶温度上升 ,热结晶温度下降 ;与常规 PET相比 ,较慢的冷却速度就可使熔融状态的改性 PET保持无定形状态。     

PET/滑石粉复合材料结晶性能、热性能和力学性能研究

采用差示扫描量热仪、热重分析仪等研究了滑石粉作为成核剂对聚对苯二甲酸乙二醇酯（PET）结晶性能、热性能以及力学性能的影响。结果表明,滑石粉的添加量为0.5 %（质量分数,下同）时,可有效改善PET的结晶性能,结晶温度（Tc）比经历相同热历程的PET空白试样提高11.36 ℃,且结晶完善程度随降温速率的减小而提高;非等温结晶动力学研究发现,Jeziorny法和莫志深法更符合复合材料的非等温结晶过程,而二次结晶的存在使Ozawa法并不适用;由于滑石粉与基体树脂相容性好并可均匀分散,从而很好地保持了原树脂的热性能,且所得复合材料的力学性能均有所提高,其中拉伸性能提高12 %。     

无机粒子含量对聚酯切片结晶性能的影响

运用差示扫描量热法(DSC)对含A种无机粒子聚酯(PET)的结晶性能进行表征。研究表明:不同A含量的聚酯在所研究的含量范围内,随A含量升高,聚酯的玻璃化转变温度Tg无明显变化,冷结晶温度Tc呈升高趋势,熔点Tm呈升高趋势,熔融结晶Tmc呈降低趋势,过冷度△Tmc呈增大趋势,半结晶周期t1/2呈增加趋势。     

PET/PTT合金非等温结晶行为的研究

采用差示扫描量热仪对熔融共混制备的聚对苯二甲酸乙二醇酯（PET）/聚对苯二甲酸丙二醇酯（PTT）合金的非等温结晶行为进行研究。结果表明,在相同的降温速率时, 随着PTT含量的增加,PET/PTT合金结晶峰温度向低温方向移动,而且当合金中PET与PTT含量接近时,合金样品出现了双重结晶峰;在降温结晶的过程中,随着降温速率的增大,各合金样品结晶峰温度均降低,其结晶峰均宽化;采用Jeziorny法对上述非等温结晶过程进行了分析,分析结果表明,随着降温速率的增大,各合金样品非等温结晶速率常数增加,其Avrami指数在1~5之间,并且逐渐减小。     

PET/粘土纳米复合材料加工条件下结晶行为的研究

采用DSC手段测试了PET、PET／粘土纳米复合材料熔体降温时的结晶行为。结果表明，在PET中引入纳米粘土可提高PET基体的降温结晶峰峰温，并使结晶速率提高1倍以上。PET及PET／粘土纳米复合材料的结晶峰峰温随降温速率的增大而移向低温，半结晶时间及结晶度随降温速率的增大而减小。基于Avrami方程的动力学分析表明，PET／粘土纳米复合材料的非等温结晶过程是带有异相成核的三维增长过程。     

PET/PTT共混体系的非等温结晶动力学研究

采用DSC方法研究了PET/PTT共混体系的非等温结晶动力学,研究发现:PET/PTT共混体系各样品的结晶峰温度和半结晶时间t1/2随着冷却速率的提高而下降;结晶动力学常数Zc随着冷却速率的提高而增加,表明共混体系的结晶速率随着冷却速率的提高而增大;Zc随着PTT含量的增加而逐渐减小,在其含量达40%￣50%时出现了最小值。     

Nonisothermal melt crystallization kinetics of poly(ethylene terephthalate)/Barite nanocomposites

Poly(ethylene terephthalate) (PET)/Barite nanocomposites were prepared by direct melt compounding. The nonisothermal melt crystallization kinetics of pure PET and PET/Barite nanocomposites, containing unmodified Barite and surface‐modified Barite (SABarite), was investigated by differential scanning calorimetry (DSC) under different cooling rates. With the addition of barite nanoparticles, the crystallization peak became wider and shifted to higher temperature and the crystallization rate increased. Several analysis methods were used to describe the nonisothermal crystallization behavior of pure PET and its nanocomposites. The Jeziorny modification of the Avrami analysis was only valid for describing the early stage of crystallization but was not able to describe the later stage of PET crystallization. Also, the Ozawa method failed to describe the nonisothermal crystallization behavior of PET. A combined Avrami and Ozawa equation, developed by Liu, was used to more accurately model the nonisothermal crystallization kinetics of PET. The crystallization activation energies calculated by Kissinger, Takhor, and Augis‐Bennett models were comparable. The results reveal that the different interfacial interactions between matrix and nanoparticles are responsible for the disparate effect on the crystallization ability of PET. POLYM. COMPOS., 31:1504–1514, 2010. © 2009 Society of Plastics Engineers     

TiO_2含量对聚酯切片结晶性能的影响

TiO2粒子作为消光剂存在于聚酯的非晶区中,对聚酯结晶过程有显著影响。在聚酯切片的冷结晶过程中,由于吸附及空间位阻作用,对结晶起阻碍作用;在聚酯熔融结晶过程中,作为晶核,对结晶起促进作用。w(TiO2)DSC参数表明:玻璃化转变温度tg、冷结晶峰温tc、熔融结晶峰温tmc随w(TiO2)降低而下降。     

Effect of molecular weight on crystallization and melting of poly(trimethylene terephthalate). 1: Isothermal and dynamic crystallization

The crystallization behavior of poly(trimethylene terephthalate) as a function of molecular weight was investigated under isothermal and dynamic cooling conditions using a differential scanning calorimeter (DSC) and polarized light optical microscopy (POM). THe overall rate of bulk crystallization increased with molecular weight. An Avrami analysis of the isothermal crystallization kinetics indicated that the crystallization rate constant increased with increasing molecular weight. The Avrami exponent, n, approached 2 and was nearly independent of both molecular weight and temperature. The modified Avrami analysis developed by Jeziorny and Ozawa was applied to the dynamic crystallization data. At the same cooling rate, higher molecular weight resulted in a narrower crystallization peak, higher onset crystallization temperature, and larger rate constant (Z_t)^1/n. Higher molecular weight resulted in larger cooling function of dynamic crystallization K(T) and lower Ozawa exponent m. For dynamic crystallization, the average value of the Avrami exponent varied from 3.4 to 3.8 and the average value of the Ozawa exponent changed from 2.3 to 2.6 as the number‐average molecular weight changed from 13,000 to 67,000. Morphology studies indicated that both the isothermal crystallization and the dynamic crystallization of PTT from the melt were thermal nucleation processes, and for a fixed temperature between 190°C and 210°C, the nucleation density increased with increasing the molecular weight.     

改性PET非等温结晶行为的研究

用差示扫描量热法研究了ＰＥＴ及改性ＰＥＴ的非等温结晶动力学,结果表明：ＰＥＴ及改性ＰＥＴ均随冷却速率的增加,结晶峰峰温向低温方向移动。经改性后的ＰＥＴ,其结晶能力和结晶速率均有所下降,且随改性剂的不同,其结晶能力和速率也不同     

Nonisothermal crystallization kinetics of biodegradable poly(butylene succinate)/poly(vinyl phenol) blend

Nonisothermal melt crystallization kinetics of biodegradable PBSU/PVPh blend was investigated with differential scanning calorimetry (DSC) from the viewpoint of practical application. PBSU/PVPh blends were cooled from the melt at various cooling rates ranging from 2.5 to 40°C/min. The crystallization peak temperature decreased with increasing the cooling rate for both neat and blended PBSU. Furthermore, the crystallization peak temperature of PBSU in the blend was lower than that of neat PBSU at a given cooling rate. Two methods, namely the Avrami equation and the Tobin method, were used to describe the nonisothermal crystallization of PBSU/PVPh blend. It was found that the Avrami equation was more suitable to predict the nonisothermal crystallization of PBSU/PVPh blend than the Tobin method. The effects of cooling rate and blend composition on the crystallization behavior of PBSU were studied in detail. It was found that the crystallization rate decreased with decreasing the cooling rate for both neat and blended PBSU. However, the crystallization of PBSU blended with PVPh was retarded compared with that of neat PBSU at the same cooling rate. © 2007 Wiley Periodicals, Inc. J Appl Polym Sci 104: 972–978, 2007     

PA6／PET共混物的非等温结晶动力学研究

采用等速升温和等速降温ＤＳＣ法对ＰＡ６／ＰＥＴ共混物的非等温结晶动力学进行了研究。在升温和降温ＤＳＣ相变曲线上，ＰＡ６／ＰＥＴ共混物具有双重熔融峰和双重结晶峰，表明ＰＡ６和ＰＥＴ组分可形成各自的结晶体。给出了各组分的结晶峰温度、结晶峰的半高宽、结晶半时间等表征结晶行为的参数，并讨论了影响结晶的因素。