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1.
用傅里叶变换红外光谱法,将一系列不同温度下退火的PET光谱与熔融淬火的PET光谱进行数字吸光度相减,得到不同结晶状态的“反式构象光谱”。进一步将不同温度退火的“反式构象光谱”(240℃和120℃)彼此相减,可得到“纯晶区的光谱”和“非晶区的反式构象光谱”。通过差示光谱的比较,发现一些新的谱带和谱带的变化。可用PET 的晶区和非晶区中其分子链的内旋转构象的变化解释。  相似文献   

2.
对高聚物的声发射做了进一步的实验观察。玻璃态高聚物在拉伸屈服以前的声发射有Kaiser效应,但在高弹态则不然。非晶态高聚物从玻璃态到高弹态的转变,玻璃态拉伸时在屈服附近出现声发射,高弹态时声发射要少而弱得多,只在高弹拉伸的断裂前出现声发射。非晶态、晶态高聚物或共混高聚物在突然升温到100℃时有声发射,但在突然降温到-60℃时却不出现声发射,这可能也说明声发射与高聚物试样内形成空洞有关。一种聚丙烯树脂在不同注射成形工艺条件下所得试件,在拉伸时的声发射行为可反映加工成形的好坏,成形好的声发射少得多。  相似文献   

3.
用DSC和溶剂诱导结晶(SINC)的方法对比研究了(GOLR)态和未取向聚对苯二甲酸乙二酯(PET)纤维样品的结晶行为.实验结果表明,样品的大尺度取向可有效地降低样品的冷结晶温度(Tcc),证明大尺度取向对样品的结晶行为可起到促进作用.  相似文献   

4.
用小角光散射、电子显微镜等方法研究了熔体温度对熔融结晶的PTFE结晶形态的影响。结果表明,当熔体温度超过400℃时,PTFE的结晶形态从棒晶逐步向球晶转化,力学性能也随之变坏。DSC的研究阐明,形态与力学性能的变化是由于大分子的降解,而不是因为熔体中发生了物理转变所致。  相似文献   

5.
由乙烯高效催化聚合而得的超高分子量聚乙烯的研究   总被引:1,自引:1,他引:0  
本工作系研究以高效催化聚合获得的超高分子量聚乙烯的结构和性能。用扫描电子显微镜观察了高效催化剂及初生聚乙烯的形态。透射电子显微镜观察了初生聚乙烯粉未,发现毛遂边缘的超分子原纤维状织态结构。用偏光显微镜观察了不同分子量聚乙烯粉末的熔融和冷却结晶过程,生成的球晶随分子量增大而增大。用X-射线衍射、差热分析、倒换气相色谱测定了初生聚乙烯的结晶度随分子量而增大;用X-射线衍射、差热分析及密度梯度法测定经退火或热压制的聚乙烯样品的结晶度均随分子量增大而下降。X-射线衍射测定其晶粒尺寸亦随分子量增大而减小。差热分析和倒换气相色谱测定超高分子量聚乙烯粉末的结晶熔点温度(Tm)要比普通分子量聚乙烯高8-12℃。不同分子量聚乙烯的热形变曲线表明,超高分子量聚乙烯在熔融温度后出现明显的橡胶态。此外,还用差热与热重分析研究了超高分子量聚乙烯的热老化行为。测定了超高分子量聚乙烯的优异抗冲强度和沙浆磨耗量。并用扫描电镜对比观察了常规分子量和超高分子量聚乙烯试样的冲击断面的织态结构。  相似文献   

6.
重(三硝基乙基)乙二硝胺(以下简称BTNE)是一种在固态下受热即分解的化合物。我们曾报导过由不同重结晶方法制备的BTNE热分解动力学的初步研究。在本文中,我们对由各种重结晶方法得到的十种BTNE晶体进行了较为深入的非等温热分解动力学的研究。将实验室得到的合成粗品BTNE分别以冰醋酸、无水乙醇、硝基甲烷、二氯乙烷、丙酮、乙酸乙酯、丁酮等溶剂处理、重结晶,控制不同的重结晶条件,得到了十种BTNE晶体。使用理学株式会社的TG-2000型热分析仪对这些晶体进行了非等温反应动力学研究。将实验得到的各种升温速度(线性升温,升温速度分  相似文献   

7.
从溶胀平衡研究玻璃态高聚物的凝聚缠结网络   总被引:1,自引:0,他引:1  
在13~15℃室温条件下对聚苯乙烯(PS)颗粒在二氧六环/水混合溶剂中的溶胀情况进行目视观察,可以看到,当减小混合溶剂二氧六环/水中的水含量时,PS颗粒从玻璃态到溶胀的玻璃态、溶胀的高弹态、流体态的转变,与PS颗粒升温时从玻璃态到高弹态、流体态的转变相对应.选定混合溶剂二氧六环/水(水6·8wt%)对一个单分散PS试样(Mw=1·68×105)在30℃进行分相平衡和溶胀平衡的测定.分相平衡是先将PS/二氧六环/水(混合溶剂水含量6·8wt%)体系加热到130℃使PS溶解成一均相溶液,然后在冷却过程中分相,在30℃达分相平衡(30天)时,浓相高分子体积浓度p″=0·304,稀相几乎为纯溶剂.从Flory-Huggins相平衡理论得出此体系的高分子-溶剂相互作用参数χ=0·63.本工作使用的单分散PS试样在选定的混合溶剂,即二氧六环/水(水6·8wt%)中,30℃时不能溶解只能溶胀,单分散PS颗粒淬冷试样(密度ρp=1·0451g/mL)到达溶胀平衡(80天)时浓相高分子体积浓度p″=0·308.而此淬冷试样经在80℃热处理100h后的老化试样(ρp=1·0470g/mL)达溶胀平衡(70天)时p″=0·312.从溶胀过程中浓相体积变化曲线可知试样经在80℃热处理过程中凝聚网络趋向于更均一,更接近热处理温度下的平衡态,试样密度增大,网络产生了新的链间凝聚,物理交联密度增大(凝聚点间分子量减小).从溶胀平衡理论并取χ=0·63(分相平衡)可得到淬冷试样的物理交联点间分子量Mc=11·6×104,老化试样的物理交联点间分子量Mc=6·9×104.实验结果说明溶胀过程及溶胀平衡的测定可以反映玻璃态高聚物中的凝聚网络结构的细节,而且非常敏感.  相似文献   

8.
徐军 《高分子科学》2017,35(12):1552-1560
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 melt-recrystallization phenomenon be observed when melting of preformed lamellar crystals and recrystallization of thicker lamellae have similar free energy barrier.  相似文献   

9.
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   

10.
The polymorphous crystallization and multiple melting behavior of poly(l-lactic acid) (PLLA) with an optical purity of 92 % were investigated after isothermally crystallized from the melt state by wide-angle X-ray diffraction and differential scanning calorimetry. Owing to the low optical purity, it was found that the disordered (α′) and ordered (α) crystalline phases of PLLA were formed in the samples crystallized at lower (<95 °C) and higher (≥95 °C) temperatures, respectively. The melting behavior of PLLA is different in three regions of crystallization temperature (T c) divided into Region I (T c < 95 °C), Region II (95 °C ≤ T c < 120 °C), and Region III (T c ≥ 120 °C). In Region I, an exothermic peak was observed between the low-temperature and high-temperature endothermic peaks, which results from the solid–solid phase transition of α′-form crystal to α one. In Region II, the double-melting peaks can be mainly ascribed to the melting–recrystallization–remelting of less stable α crystals. In Region III, the single endotherm shows that the α crystals formed at higher temperatures are stable enough and melt directly without the recrystallization process during heating.  相似文献   

11.
CRYSTALLIZATION AND MELTING OF NYLON 610   总被引:1,自引:0,他引:1  
Differential scanning calorimetry was used to study the crystallization andmelting of nylon 610. For nylon 610 crystallized from the melt state (260℃), the overall rateof bulk crystallization can be described by a simple Avrami equation with Avrami exponentn ≈ 2, independent of crystallization temperature. With the experimentally obtainedT_m~0 (235℃ ~ 255℃) of nylon 610, the fold surface free energy σ_e was determined to be35 ~38 erg/cm~2. The effects of annealing temperature and time on the melting of quenchednylon 610 were also investigated. For nylon 610 quenched at room temperature there isonly one DSC endotherm peak DSC scans on annealed samples exhibited an endothermpeak at approximately 10℃ above the annealing temperature. The size and position of theendothermic peak is strongly related to annealing temperature and time. An additionalthird melting was observed when quenched nylon 610 was annealed at high temperaturefor a sufficiently long residence time. The existence of the third melting peak suggests thatmore than one kind of distribution of lamella thickness may occur when quenched nylon610 is annealed. The implications of these results in terms of crystal thickening mechanismwere discussed.  相似文献   

12.
热分析法研究超高分子量聚乙烯的热熔性质   总被引:2,自引:1,他引:1  
本文采用差热分析(DTA)、差示扫描量热法(DSC)研究了一系列以高效催化聚合而得的初生态超高分子量(Mw=70-315×104)聚乙烯粉的热熔行为,还研究了在接近熔化或部分熔化的温度下恒温热处理对晶体性质的影响.  相似文献   

13.
报道分子量为5000的聚氧化乙烯(PEO)从熔融态淬火到液氮温度后形成的两次链折叠(2-FC)片晶增厚过程的研究结果.在升温和恒温条件下,采用小角X射线散射(SAXS)在位地跟踪了2-FC片晶增厚成一次链折叠(1-FC)和进一步成为伸直链(EC)片晶的增厚过程.通过对SAXS数据以及它们的一维相关函数的数据的分析,发现在52℃以下,2-FC片晶主要增厚为1-FC片晶;在52℃以上,2-FC片晶则主要增厚为EC片晶;在58℃到EC片晶的熔点的温度区域里,已经形成的1-FC片晶还会熔融,完全转化为EC片晶.利用偏光显微镜(PLM)和扫描电子显微镜(SEM)观察晶体的形貌,比如球晶,获得的研究结果表明,没有发生大范围的晶体破坏后再形成的变化,也就是说片晶的增厚过程是一个发生在球晶内部的薄片晶熔融后转化为厚片晶的过程.  相似文献   

14.
合成了一系列基于4,4-′ODPA,3,4-′ODPA以及3,3-′ODPA 3种异构二苯醚二酐单体的异构聚酰亚胺,以苯酐(PA)作为封端剂来控制分子量.用DSC和WAXD为主要手段研究了这几种异构聚酰亚胺的结晶行为.研究发现聚酰亚胺4,4-′ODPA/ODA(二苯醚二胺)在分子量较低的情况下能够在热处理,退火或剪切作用下结晶.并且升高热处理温度和延长热处理时间有利于结晶的完善,在玻璃化温度以上施加剪切能够加速聚酰亚胺的结晶.而对于其他的两种异构体3,4-′ODPA/ODA以及3,3-′ODPA/ODA无论是经过热处理还是施加外力剪切都未能使其结晶.  相似文献   

15.
淬火温度对聚偏氟乙烯形态结构的影响   总被引:8,自引:0,他引:8  
用透射电子显微镜(TEM)和傅里叶交换红外光谱(FTIR)等方法研究了结晶温度对聚偏氟乙烯(PVF2)晶相结构的影响.结果表明,从PVF2熔体高速淬火到较低温度等温结晶可直接生成β相结晶,临界淬火温度为30℃.淬火温度在40—70℃时,α和β相共存.当淬火温度较高时(80—150℃),生成α相结晶.在淬火温度高于165℃时,则得到PVF2的γ相结晶.在临界温度以下淬火的PVF2薄膜含有β相微晶,而高于临界淬火温度时则生成α相或γ相的片晶或球晶结构.  相似文献   

16.
选择 3种不同丙烯酸含量的乙烯 丙烯酸共聚物 (EAA)为原材料 ,二苯醚 (DPE)为稀释剂 ,研究了淬冷温度、粗化时间等影响液滴生长的动力学因素对热诱导相分离法 (TIPS)制备EAA DPE亲水性高分子微孔膜结构的影响 .淬冷温度的高低决定了EAA DPE体系是发生液 液相分离还是固 液相分离 ,而产生相分离的机理不同将影响稀释剂液滴的生长 ,最终影响微孔膜的孔径 .实验结果表明 ,在相同粗化时间的条件下 ,随着EAA1 41 0 DPE、EAA3 0 0 2 DPE、EAA3 0 0 3 DPE三体系冷却温度的逐渐升高 ,孔径逐渐变大 .在结晶温度以下 ( 0℃、3 0℃、60℃ )粗化时间相同时 ,温度对微孔膜的孔径影响较小 ,例如 0℃和 3 0℃的恒温条件粗化 1 0min,微孔膜的孔径在 1~ 3 μm之间 ;在 60℃的恒温条件粗化 1 0min ,微孔膜的孔径在 3~ 5 μm之间 .而在 90℃的恒温条件粗化相同的时间 ,由于体系始终处于结晶温度线以上 ,体系始终处在液 液相分离区域 ,最终得到微孔膜的孔径达到了 6~8μm .在结晶温度以下 ( 3 0℃ )进行恒温粗化 ,由于体系的过冷程度很大 ,液滴相的粗化过程被抑制住 ,所以粗化时间对微孔膜的孔径影响不大 ;而在结晶温度以上 ( 90℃ )进行恒温粗化时 ,则是随着粗化时间的延长 ,微孔膜的孔径逐渐变大  相似文献   

17.
The effects of grinding and the excipients used on the solid state stability of warfarin in ground mixtures with β-cyclodextrin or microcrystalline cellulose have been investigated by using x-ray powder diffractometry, IR spectrophotometry and differential scanning calorimetry. The grinding process did not result in warfarin-excipient interaction, but caused a crystalline form of warfarin to transfer to an amorphous state in the presence of β-cyclodextrin. The stability of this amorphous state of warfarin in tablets made from the ground mixtures stored at 37°C and 75% RH (relative humidity) was also studied. There was only a small amount of amorphous warfarin in tablets that recrystallized under storage conditions. The recrystallization of amorphous warfarin might be due to moisture adsorption. β-cyclodextrin possesses an ability to prevent the recrystallization of large amounts of amorphous warfarin in tablets stored at 37°C and 75% RH.  相似文献   

18.
杂质对六氯环三聚磷腈热聚合的影响   总被引:1,自引:0,他引:1  
利用红外光谱、磷核磁共振谱、广角X射线衍射、差示扫描量热、凝胶色谱等分析手段,研究了六氯环三聚磷腈(HCCP)在存放过程中产生的杂质,以及不同纯化方法对这些杂质的去除效果,探讨了这些杂质对HCCP单体真空热开环聚合反应的影响.HCCP在存放过程中接触空气中的水汽在环上氯基团处易被水解,产生Trimer-1、Gem-2、Dimmer-3等杂质,重结晶能去除Gem-2、Dimmer-3和少量的Trimer-1,升华能较好地去除Trimer-1.杂质Gem-2、Dimmer-3中的羟基引发聚二氯磷腈交联,生成不可溶的交联态聚二氯磷腈,而Trimer-1则会降低聚合速度,并在聚合物中引入磷氧基和亚胺基杂链,从而影响后续聚磷腈取代产物的性质,表现为聚合物中晶态发生变异,结晶度降低,玻璃化温度、晶态转化温度和熔融温度出现差别.用重结晶结合升华的方法对HCCP单体进行纯化后,应用FTIR或31P-NMR分析来验证纯化效果,以确保能控制聚合速度和时间,使聚合顺利进行.  相似文献   

19.
The nature of the transition in molten FEP copolymer was examined in relation to the enthalpy change, mechanical damping and melt viscosity. For a pre-heat-treated FEP copolymer sample a small endothermic peak appeared at 309—312 ℃in DSC trace with enthalpy change 0.03—0.05 cal/g. A peak was also detected in damping versus temperature curve at the same temperature range. The theological property of FEP copolymer melt was similar to that of liquid crystal, but no birefrigence was viewed in the melt. Therefore the transition was explained as the melting of small crystallites which persist in typical copolymer beyond its melting temperature. These crystallites can act as nuclei for crystallization upon cooling.  相似文献   

20.
WAXD研究表明,在结晶温度T_c≤196℃时,尼龙1010等温熔体结晶样品的结晶度X_c和微晶尺寸L_(100)随T_c升高近乎线性增大,而氢键面上的相对衍射强度R却降低;T_c>196℃后三者与T_c关系发生相反变化。结晶速率快时有利于分子链在垂直于氢键平面方向上堆砌,反之有利于在平行于氢键平面方向上生长。  相似文献   

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