{"title":"块体聚甲基丙烯酸正己酯在玻璃化转变附近的光子相关光谱","authors":"Y. Hwang, G. Patterson, J. R. Stevens","doi":"10.1002/(SICI)1099-0488(199610)34:14<2291::AID-POLB1>3.0.CO;2-#","DOIUrl":null,"url":null,"abstract":"Slowly relaxing longitudinal density fluctuations in an optically perfect sample of bulk poly(n-hexyl methacrylate) (PHMA) have been studied by photon correlation spectroscopy in the temperature range 10-36°C. The glass transition temperature for this sample was in the temperature range 10-36°C. The glass transition temperature for this sample was measured to be T g = -3°C by differential scanning calorimetry. The optical purity of the sample was verified by Rayleigh Brillouin spectroscopy and the Landau Placzek ratio was observed to be 2.3 at 25°C. Light-scattering relaxation functions were obtained over the time range 10 6 -l s. The shape of the relaxation functions broadened as the temperature was lowered towards the glass transition. Quantitative analysis of the results was carried out using the Kohlrausch-Williams-Watts (KWW) function to obtain average relaxation times , and width parameters, β. The width parameter decreased from 0.43 to 0.21 over the temperature interval, as suggested by visual inspection. Average relaxation times shifted with temperature in a manner consistent with previous mechanical studies of the primary glass-rubber relaxation in PHMA. The relaxation functions were also analyzed in terms of a distribution of relaxation rates, G(T). The calculated distributions were unimodal at all temperatures. The average relaxation times obtained from G(T) were in agreement with the KWW analysis, and the shape of the distribution broadened as the sample was cooled. The rate at which G(T) displayed a maximum correlated well with the corresponding frequency of maximum dielectric loss for PHMA. The temperature dependence of these two quantities could be reproduced with an Arrhenius activation energy of 21 Kcal/mol. A consistent picture of the molecular dynamics of PHMA near the glass transition requires a strong secondary relaxation process with a different temperature dependence from the primary glass-rubber relaxation. The present results suggest that the behavior of PHMA is similar to the other poly(alkyl methacrylates).","PeriodicalId":16853,"journal":{"name":"Journal of Polymer Science. Part B, Polymer Physics","volume":"1 1","pages":"2291-2305"},"PeriodicalIF":0.0000,"publicationDate":"1996-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":"{\"title\":\"Photon correlation spectroscopy of bulk poly(n‐hexyl methacrylate) near the glass transition\",\"authors\":\"Y. Hwang, G. Patterson, J. R. Stevens\",\"doi\":\"10.1002/(SICI)1099-0488(199610)34:14<2291::AID-POLB1>3.0.CO;2-#\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Slowly relaxing longitudinal density fluctuations in an optically perfect sample of bulk poly(n-hexyl methacrylate) (PHMA) have been studied by photon correlation spectroscopy in the temperature range 10-36°C. The glass transition temperature for this sample was in the temperature range 10-36°C. The glass transition temperature for this sample was measured to be T g = -3°C by differential scanning calorimetry. The optical purity of the sample was verified by Rayleigh Brillouin spectroscopy and the Landau Placzek ratio was observed to be 2.3 at 25°C. Light-scattering relaxation functions were obtained over the time range 10 6 -l s. The shape of the relaxation functions broadened as the temperature was lowered towards the glass transition. Quantitative analysis of the results was carried out using the Kohlrausch-Williams-Watts (KWW) function to obtain average relaxation times , and width parameters, β. The width parameter decreased from 0.43 to 0.21 over the temperature interval, as suggested by visual inspection. Average relaxation times shifted with temperature in a manner consistent with previous mechanical studies of the primary glass-rubber relaxation in PHMA. The relaxation functions were also analyzed in terms of a distribution of relaxation rates, G(T). The calculated distributions were unimodal at all temperatures. The average relaxation times obtained from G(T) were in agreement with the KWW analysis, and the shape of the distribution broadened as the sample was cooled. The rate at which G(T) displayed a maximum correlated well with the corresponding frequency of maximum dielectric loss for PHMA. The temperature dependence of these two quantities could be reproduced with an Arrhenius activation energy of 21 Kcal/mol. A consistent picture of the molecular dynamics of PHMA near the glass transition requires a strong secondary relaxation process with a different temperature dependence from the primary glass-rubber relaxation. The present results suggest that the behavior of PHMA is similar to the other poly(alkyl methacrylates).\",\"PeriodicalId\":16853,\"journal\":{\"name\":\"Journal of Polymer Science. Part B, Polymer Physics\",\"volume\":\"1 1\",\"pages\":\"2291-2305\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1996-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"5\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Polymer Science. Part B, Polymer Physics\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://doi.org/10.1002/(SICI)1099-0488(199610)34:14<2291::AID-POLB1>3.0.CO;2-#\",\"RegionNum\":3,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Materials Science\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Polymer Science. Part B, Polymer Physics","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1002/(SICI)1099-0488(199610)34:14<2291::AID-POLB1>3.0.CO;2-#","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Materials Science","Score":null,"Total":0}
引用次数: 5
摘要
在10 ~ 36℃的温度范围内,用光子相关光谱研究了光学完美体聚甲基丙烯酸正己酯(PHMA)样品的缓慢弛豫纵向密度波动。该样品的玻璃化转变温度范围为10-36℃。用差示扫描量热法测得该样品的玻璃化转变温度为tg = -3℃。通过瑞利布里渊光谱法验证了样品的光学纯度,在25°C时观察到朗道普拉西克比为2.3。在10.6 ~ l s的时间范围内得到了光散射弛豫函数,弛豫函数的形状随着温度向玻璃化转变而变宽。利用Kohlrausch-Williams-Watts (KWW)函数对结果进行定量分析,得到平均松弛时间和宽度参数β。根据目测,宽度参数在温度区间内从0.43下降到0.21。平均弛豫时间随温度变化的方式与先前的PHMA中玻璃橡胶初级弛豫的力学研究一致。松弛函数也根据松弛速率G(T)的分布进行了分析。计算出的分布在所有温度下均为单峰分布。由G(T)得到的平均弛豫时间与KWW分析结果一致,随着样品冷却,弛豫时间的分布形状变宽。G(T)达到最大值的速率与相应的PHMA最大介电损耗频率具有良好的相关性。这两个量的温度依赖性可以用21 Kcal/mol的阿伦尼乌斯活化能再现。PHMA在玻璃化转变附近的分子动力学的一致图像需要一个强烈的二次弛豫过程,其温度依赖性与初次玻璃橡胶弛豫不同。本研究结果表明,聚甲基丙烯酸烷基酯的行为与其他聚甲基丙烯酸烷基酯相似。
Photon correlation spectroscopy of bulk poly(n‐hexyl methacrylate) near the glass transition
Slowly relaxing longitudinal density fluctuations in an optically perfect sample of bulk poly(n-hexyl methacrylate) (PHMA) have been studied by photon correlation spectroscopy in the temperature range 10-36°C. The glass transition temperature for this sample was in the temperature range 10-36°C. The glass transition temperature for this sample was measured to be T g = -3°C by differential scanning calorimetry. The optical purity of the sample was verified by Rayleigh Brillouin spectroscopy and the Landau Placzek ratio was observed to be 2.3 at 25°C. Light-scattering relaxation functions were obtained over the time range 10 6 -l s. The shape of the relaxation functions broadened as the temperature was lowered towards the glass transition. Quantitative analysis of the results was carried out using the Kohlrausch-Williams-Watts (KWW) function to obtain average relaxation times , and width parameters, β. The width parameter decreased from 0.43 to 0.21 over the temperature interval, as suggested by visual inspection. Average relaxation times shifted with temperature in a manner consistent with previous mechanical studies of the primary glass-rubber relaxation in PHMA. The relaxation functions were also analyzed in terms of a distribution of relaxation rates, G(T). The calculated distributions were unimodal at all temperatures. The average relaxation times obtained from G(T) were in agreement with the KWW analysis, and the shape of the distribution broadened as the sample was cooled. The rate at which G(T) displayed a maximum correlated well with the corresponding frequency of maximum dielectric loss for PHMA. The temperature dependence of these two quantities could be reproduced with an Arrhenius activation energy of 21 Kcal/mol. A consistent picture of the molecular dynamics of PHMA near the glass transition requires a strong secondary relaxation process with a different temperature dependence from the primary glass-rubber relaxation. The present results suggest that the behavior of PHMA is similar to the other poly(alkyl methacrylates).
期刊介绍:
Since its launch in 1946 by P. M. Doty, H. Mark, and C.C. Price, the Journal of Polymer Science has provided a continuous forum for the dissemination of thoroughly peer-reviewed, fundamental, international research into the preparation and properties of macromolecules.
From January 2020, the Journal of Polymer Science, Part A: Polymer Chemistry and Journal of Polymer Science, Part B: Polymer Physics will be published as one journal, the Journal of Polymer Science. The merged journal will reflect the nature of today''s polymer science research, with physics and chemistry of polymer systems at the heart of the scope.
You can continue looking forward to an exciting mix of comprehensive reviews, visionary insights, high-impact communications, and full papers that represent the rapid multidisciplinary developments in polymer science.
Our editorial team consists of a mix of well-known academic editors and full-time professional editors who ensure fast, professional peer review of your contribution. After publication, our team will work to ensure that your paper receives the recognition it deserves by your peers and the broader scientific community.