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 共查询到19条相似文献,搜索用时 125 毫秒
1.
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...  相似文献   

2.
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。  相似文献   

3.
聚醚醚酮/聚醚醚酮酮共混体系的熔融和等温结晶行为   总被引:3,自引:0,他引:3  
采用熔融共混方法制备了聚醚醚酮和聚醚醚酮酮的共混物,用DSC对共混物的熔融行为和等温结晶行为进行了研究.结果表明,共混物熔点随聚醚醚酮含量增加而降低,但与聚醚醚酮酮有相同的平衡熔点,二者共混没有改变其结晶的成核与生长机制.  相似文献   

4.
根据Flory热力学统计理论和比容-熔融热作国法,由DSC结果得到了不同联苯含量的聚醚醚酮酮-含联苯聚醚醚酮酮(PEEKK-PEBEKK)共聚物的熔融热,两种方法获得的结果吻合。在此基础上给出了PEEKK-PEBEKK共聚物不同联苯含量的熔点计算表达式。结果还表明,随着联苯含量nB,的变化,明显改变;当nB=0.35时,PEEKKPEBEKK共聚物的值最小。  相似文献   

5.
igh performance crystal/crystal blends of poly (phenylene sulfide) and poly (ether ether ketone) (PPS/PEEK) have ho prepared by dry mixing and melhng at different temperatures. The crystallization and melting behavior of PEEK component in quenched blends have ho investigated by differential scanningcalorimetry (DSC). As melt temperature (Tmelt) increases, the crystalline andmelting behavior of PPS and PEEK is different due to the difference of thermalproperty of PPS and PEEK. The temperature of melhng (Tm) and crystallization (Tc) and crystallinity (Xc) of PEEK component in blends increase as the content of PPS increases up to 50%. However. this action of PPS is suppresed with increasing of Tmelt.  相似文献   

6.
结晶/结晶共混体系聚苯硫酸/聚醚醚酮中聚醚醚酮组分的结晶熔融行为──熔融温度的影响麦堪成,许家瑞,梅震,曾汉民(中山大学材料科学研究所,广州,510275)关键词聚醚醚酮,聚苯硫醚,结晶/结晶共混物,结晶熔融行为近年来,高性能聚合物共混物如聚砜(PS...  相似文献   

7.
超临界CO_2及共溶剂作用下聚碳酸酯的结晶和熔融行为   总被引:8,自引:0,他引:8  
廖霞  李刚  孙兴华  何嘉松 《化学学报》2003,61(10):1697-1699
采用差示扫描量法(DSC)研究了在超临界CO_2以及超临界CO_2+乙醇作用下温 度和压力对聚碳酸酯的结晶和熔融行为的影响。结果表明超临界CO_2能使聚碳酸酯 (PC)在其玻璃化转变温度下结晶。CO2是非极性流体,加入共溶剂能增加超 临界流体的极性,提高流体的溶解能力。与纯CO_2条件比较,少量共溶剂的加入使 PC的结晶更加完善,并能使其在更低的温度下和压力条件下结晶。  相似文献   

8.
9.
结晶/结晶共混体系PPS/PEEK中PPS组分的结晶熔融行为(Ⅱ)──熔融条件对退火样品的影响麦堪成,许家瑞,梅震,曾汉民(广州中山大学材料科学研究所,广州,510275)关键词聚苯硫醚,聚醚醚酮,结晶熔融行为,熔融双峰聚苯硫醚(PPS)的结晶熔融行...  相似文献   

10.
用透射电子显微镜和电子衍射方法研究了含间苯连接的聚醚醚酮酮(PEEKmK)溶液浇铸薄膜的等温结晶过程和形态结构.结果表明,PEEKmK无论从玻璃态结晶还是从熔体结晶均能形成2种不同取向的结晶形态结构,即平放片晶和侧放片晶;前者c轴垂直于膜平面,后者c轴平行于膜平面.其结晶发展过程为先形成平放单晶状片晶,随着时间的增长,在单晶上开始生长侧放片晶,逐渐发展形成球晶,最终形成2种不同取向的单晶和球晶共存的结晶形态结构.  相似文献   

11.
Slow evaporation of toluene from poly(2,6-dimethyl-1,4-phenylene oxide), PPO, at 23°C produced crystals which melt between 185 and 265°C and have a crystallinityof 0.58. About 8 wt% of the crystals appear to melt temperatures below 220°C. The lattertemperature marks the end of the glass transition interval for this polymer.This revised version was published online in November 2005 with corrections to the Cover Date.  相似文献   

12.
A throughout investigation of crystallization and melting behavior of poly(L -lactic acid) is detailed in this contribution. Crystallization analyses, conducted in both isothermal and non-isothermal conditions, revealed the occurrence of a sudden acceleration in phase transition rate in the temperature range between 100 and 118 °C. This unusual increase, due to very high rates of spherulite growth, seems not related to morphological changes of PLLA spherulites, nor to unexpected variations in nucleation rate. DSC analyses disclosed multiple melting behavior of PLLA, depending on crystallization temperature. At low temperatures the very high crystallization rates lead to the achievement of low values of crystalline degree, with formation of small and/or defective crystals, which have a large tendency to reorganize into more stable structures during the heating scan that leads to complete fusion. The multiple melting process of PLLA was also analyzed at different heating rates.  相似文献   

13.
官能团化聚丙烯对Mg(OH)2/PP结晶与熔融行为的影响   总被引:6,自引:1,他引:6  
制备了官能团化聚丙烯改性Mg(OH)2/PP复合材料,并用DSC研究了改性PP,Mg(OH)2/PP和改性Mg/(OH)2/PP中PP的结晶与熔融行为,官能团化PP(FPP),丙烯酸(AA)和Mg(OH)2都能提高PP的结晶温度,归结于异相成核作用,AA和FPP加入进一步使Mg(OH)/PP中PP结晶温度提高,但AA用量增加对PP结晶温度无影响。  相似文献   

14.
The melting behavior of isothermally crystallized poly(butylene succinate) (PBS) has been investigated using differential scanning calorimetry (DSC) and wide‐angle X‐ray analysis. The samples crystallized between 80°C to 100°C show middle endotherm at the position just before the high exotherm, while the others under 80°C show two endotherms (low and high). From the results of the melting peak vs. crystallization temperature plot, it was suggested that the middle endotherm corresponds to the melting process of the original crystallites and the high endotherms to the melting process of the recrystallized ones. As the DSC heating rate was increased, the peak temperature of the low and middle endotherms increased and that of the high endotherm decreased, indicating that the low endotherm was due to the original crystallites as well as the middle endotherm. Consequently, in the heating scan of PBS, the existence of two kinds of morphologically different crystallites as well as the process of melting and recrystallization becomes evident. © 1999 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 37: 1357–1366, 1999  相似文献   

15.
The melting behavior of drawn, compression-molded isotactic polypropylene has been ex-amined in terms of the infuence of drawing conditions on the observed properties. Two endothermic peaks were observed on differential scanning calorimetry (DSC) for samples when high draw ratios and high heating rates were used during DSC tests. The peak at lower temperature is influenced by draw ratio, temperature, and rate, and exhibits a strong superheating effect. The species associated with this peak can partially recrystallize into another species associated with the peak at higher temprature during DSC measurements. The position of the peak at higher temperature depends only on draw ratio. It is proposed that the doubel-melting peaks at lower and higher temperature result from extremely thin quasi-amorphous or crystalline layers between microfibrils and the lamellar crystals within microfibrils, repectively. © 1993 John Wiley & Sons, Inc.  相似文献   

16.
The melting behavior and crystallization kinetics of poly(thiodiethylene adipate) (PSDEA) were investigated with differential scanning calorimetry and hot‐stage optical microscopy. The observed multiple endotherms, commonly displayed by polyesters, were influenced by the crystallization temperature (Tc) and ascribed to melting and recrystallization processes. Linear and nonlinear treatments were applied to estimate the equilibrium melting temperature for PSDEA with the corrected values of the melting temperature. The nonlinear estimation yielded a higher value by about 9 °C. Isothermal crystallization kinetics were analyzed according to Avrami's treatment. Values of Avrami's exponent close to 3 were obtained, independently of Tc, in agreement with a crystallization process originating from predetermined nuclei and characterized by three‐dimensional spherulitic growth. As a matter of fact, space‐filling spherulites were observed by optical microscopy at all Tc's. The rate of crystallization became lower as Tc increased, as usual at a low undercooling, the crystallization process being controlled by nucleation. Moreover, the crystal structure of PSDEA was determined from powder X‐ray diffraction data by full profile fitting. A triclinic unit cell containing two polymer chains arranged parallel to the c axis was found. © 2003 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 42: 553–566, 2004  相似文献   

17.
Differential scanning calorimetry (DSC) has been widely applied to study crystallization and melting of materials.However,for polymeric lamellar crystals,the melting thermogram during heating process usually exhibits a broad endothermic peak or even multiple endotherms,which may result from changes of metastability via recrystallization process.Sometimes,the recrystallization exotherm cannot be observed due to its overlapping with the melting endotherm.In this work,we employed a step heating procedure consisting of successive heating and temperature holding stages to measure the metastability of isothermally crystallized poly(butylene succinate) (PBS) crystals.With this approach we could gain the fraction of crystals melted at different temperature ranges and quantitatively detect the melting-recrystallization behavior.The melting-recrystallization behavior depends on the polymer chain structure and the crystallization temperature.For instance,PBS block copolymer hardly shows recrystallization behavior while PBS oligomer and high molecular weight PBS homopolymer demonstrate remarkable melting-recrystallization phenomenon.High molecular weight PBS isothermally crystallized in the low temperature range shows multiple melting-recrystallization while those isothermally crystallized at elevated temperatures do not exhibit observable recrystallization behavior.Furthermore,the melting endotherms were fitted via the melting kinetics equations.The original isothermally crystallized lamellae demonstrate quite different melting kinetics from the recrystallized lamellar crystals that melt at the highest temperature range,which is attributed to the different degrees of stabilization.Finally,the mechanism of melting-recrystallization is briefly discussed.We propose that apparent meltrecrystallization phenomenon be observed when melting of preformed lamellar crystals and recrystallization of thicker lamellae have similar free energy barrier.  相似文献   

18.
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.  相似文献   

19.
A combination of common and low-temperature differential scanning calorimetry (DSC) techniques was used to detect the thermodynamic parameters of heat denaturation and of ice-water phase transitions for native and denaturated DNA, at different low water contents. We suggest that the main contribution to the enthalpy of the process of the heat denaturation of DNA duplex (35±5 kJ/mol bp) is the enthalpy of disruption of the ordered water structure in the hydration shell of the double helix (26±1 kJ/mol bp). It is possible that this part of the energy composes the non-specific general contribution (70%) of the enthalpy of transition of all type of duplexes. For DNA in the condensed state the ratioα=ΔC pS ~2 is smaller than for DNA in diluted aqueous solutions (α≅2–4). This means that there are other sources for the large heat capacity change in diluted solutions of DNA – for example the hydrophobic effects and unstacking(unfolding) of single polynucleotide chains. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

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