{"title":"对差示扫描量热(DSC)实验研究聚对苯二甲酸乙二醇酯(PET)非晶相的贡献","authors":"M. W. Khemici, B. Rahmani, N. Doulache, S. Derbil","doi":"10.1109/ICSD.2013.6619661","DOIUrl":null,"url":null,"abstract":"In their semi-crystalline form, the polyesters can be studied by a two phases model in which, materials are described without transitional region between crystalline and amorphous domains. However, since 20 years there have been several attempts in order to describe easily such polymers, a three phase model with taking into account the rigid amorphous fraction has been proposed. The third phase of this model is a transitional region located between crystalline and mobile amorphous regions, it is called rigid amorphous fraction and it can be characterized easily by calorimetric measurements, because it does not participate in the glass transition of the amorphous phase (called amorphous phase mobile). PET is one of polymers for which, the three phase model has successfully described its thermal behavior. The aim of this contribution is to study the amorphous phase of this polymer by differential scanning calorimerty (DSC) experiments. The semi-crystalline form of PET can be obtained by quenching it in ice water at various temperatures lower than the melting point Tm or by annealing at temperature higher than its crystallization temperature TC. The thermograms of DSC obtained after annealing the polymer at various temperatures varying between 110°C and 220°C during different times allowed us to estimate the crystalline rate, the mobile and rigid rates of the amorphous phase.","PeriodicalId":437475,"journal":{"name":"2013 IEEE International Conference on Solid Dielectrics (ICSD)","volume":"11 8","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2013-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Contribution to the study of the amorphous phase of polyethylene terephtalate (PET) by the differential scanning calorimerty (DSC) experiments\",\"authors\":\"M. W. Khemici, B. Rahmani, N. Doulache, S. Derbil\",\"doi\":\"10.1109/ICSD.2013.6619661\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In their semi-crystalline form, the polyesters can be studied by a two phases model in which, materials are described without transitional region between crystalline and amorphous domains. However, since 20 years there have been several attempts in order to describe easily such polymers, a three phase model with taking into account the rigid amorphous fraction has been proposed. The third phase of this model is a transitional region located between crystalline and mobile amorphous regions, it is called rigid amorphous fraction and it can be characterized easily by calorimetric measurements, because it does not participate in the glass transition of the amorphous phase (called amorphous phase mobile). PET is one of polymers for which, the three phase model has successfully described its thermal behavior. The aim of this contribution is to study the amorphous phase of this polymer by differential scanning calorimerty (DSC) experiments. The semi-crystalline form of PET can be obtained by quenching it in ice water at various temperatures lower than the melting point Tm or by annealing at temperature higher than its crystallization temperature TC. The thermograms of DSC obtained after annealing the polymer at various temperatures varying between 110°C and 220°C during different times allowed us to estimate the crystalline rate, the mobile and rigid rates of the amorphous phase.\",\"PeriodicalId\":437475,\"journal\":{\"name\":\"2013 IEEE International Conference on Solid Dielectrics (ICSD)\",\"volume\":\"11 8\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2013-10-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2013 IEEE International Conference on Solid Dielectrics (ICSD)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ICSD.2013.6619661\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2013 IEEE International Conference on Solid Dielectrics (ICSD)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICSD.2013.6619661","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Contribution to the study of the amorphous phase of polyethylene terephtalate (PET) by the differential scanning calorimerty (DSC) experiments
In their semi-crystalline form, the polyesters can be studied by a two phases model in which, materials are described without transitional region between crystalline and amorphous domains. However, since 20 years there have been several attempts in order to describe easily such polymers, a three phase model with taking into account the rigid amorphous fraction has been proposed. The third phase of this model is a transitional region located between crystalline and mobile amorphous regions, it is called rigid amorphous fraction and it can be characterized easily by calorimetric measurements, because it does not participate in the glass transition of the amorphous phase (called amorphous phase mobile). PET is one of polymers for which, the three phase model has successfully described its thermal behavior. The aim of this contribution is to study the amorphous phase of this polymer by differential scanning calorimerty (DSC) experiments. The semi-crystalline form of PET can be obtained by quenching it in ice water at various temperatures lower than the melting point Tm or by annealing at temperature higher than its crystallization temperature TC. The thermograms of DSC obtained after annealing the polymer at various temperatures varying between 110°C and 220°C during different times allowed us to estimate the crystalline rate, the mobile and rigid rates of the amorphous phase.