{"title":"硅冷却速率对正构烷烃结晶和玻璃化转变的影响","authors":"Santanu Santra and Noam Agmon","doi":"10.1039/D4CP02581D","DOIUrl":null,"url":null,"abstract":"<p >\r\n <em>n</em>-Alkanes (C<small><sub><em>n</em></sub></small>H<small><sub>2<em>n</em>+2</sub></small>) are linear chain compounds spanning length-scales from small molecules to polymers. Intermediate length alkanes (say, <em>n</em> = 10–20) have attracted much interest as organic phase change materials (PCM) for storing energy as latent heat. The cooling rate (<em>γ</em>) determines both the latent heat and temperature of crystallization. While slow cooling of the liquid leads to the crystalline state, rapid cooling leads to a glassy state (glass transition temperature <em>T</em><small><sub>g</sub></small>). Albeit scant theoretical investigations concerning the vitrification processes, the role of molecular conformations therein remains completely unexplored. Our work presents an all-atom molecular dynamics study of (a) cooling intermediate length alkanes (<em>n</em> = 12 and 16) at seven different rates, and (b) rapidly cooling 14 <em>n</em>-alkanes (4 ≤ <em>n</em> ≤ 50) for determining <em>T</em><small><sub>g</sub></small>(<em>n</em>). We find that for linear molecules the end-to-end distance (<em>R</em><small><sub>ee</sub></small>) is of special relevance: the crystal is composed solely of fully stretched molecules (maximal <em>R</em><small><sub>ee</sub></small>). Hence one may define the “degree of crystallization” as the area under the maximal <em>R</em><small><sub>ee</sub></small> peak in the <em>R</em><small><sub>ee</sub></small> distribution. Other peaks in the distribution represent conformations that existed in the supercooled liquid just before vitrification. A peak for the shortest, hairpin rotamer appears only for <em>n</em> ≥ <em>n</em><small><sub>0</sub></small> = 18, and is also manifested in the minimum of <em>R</em><small><sub>g</sub></small>/<em>R</em><small><sub>ee</sub></small>(<em>n</em>) for liquid <em>n</em>-alkanes. The dependence of <em>T</em><small><sub>g</sub></small> on <em>n</em> is represented as two intersecting Ueberreiter and Kanig equations, intersecting near <em>n</em><small><sub>0</sub></small> = 18. Extrapolation gives the asymptotic <em>n</em> → ∞ limit of <em>T</em><small><sub>g</sub></small>, <em>T</em><small><sup>∞</sup></small><small><sub>g</sub></small> = 250 K, which is probably its most accurate estimate obtained theoretically todate.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":" 17","pages":" 8731-8745"},"PeriodicalIF":2.9000,"publicationDate":"2025-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2025/cp/d4cp02581d?page=search","citationCount":"0","resultStr":"{\"title\":\"In silico cooling rate dependent crystallization and glass transition in n-alkanes†\",\"authors\":\"Santanu Santra and Noam Agmon\",\"doi\":\"10.1039/D4CP02581D\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >\\r\\n <em>n</em>-Alkanes (C<small><sub><em>n</em></sub></small>H<small><sub>2<em>n</em>+2</sub></small>) are linear chain compounds spanning length-scales from small molecules to polymers. Intermediate length alkanes (say, <em>n</em> = 10–20) have attracted much interest as organic phase change materials (PCM) for storing energy as latent heat. The cooling rate (<em>γ</em>) determines both the latent heat and temperature of crystallization. While slow cooling of the liquid leads to the crystalline state, rapid cooling leads to a glassy state (glass transition temperature <em>T</em><small><sub>g</sub></small>). Albeit scant theoretical investigations concerning the vitrification processes, the role of molecular conformations therein remains completely unexplored. Our work presents an all-atom molecular dynamics study of (a) cooling intermediate length alkanes (<em>n</em> = 12 and 16) at seven different rates, and (b) rapidly cooling 14 <em>n</em>-alkanes (4 ≤ <em>n</em> ≤ 50) for determining <em>T</em><small><sub>g</sub></small>(<em>n</em>). We find that for linear molecules the end-to-end distance (<em>R</em><small><sub>ee</sub></small>) is of special relevance: the crystal is composed solely of fully stretched molecules (maximal <em>R</em><small><sub>ee</sub></small>). Hence one may define the “degree of crystallization” as the area under the maximal <em>R</em><small><sub>ee</sub></small> peak in the <em>R</em><small><sub>ee</sub></small> distribution. Other peaks in the distribution represent conformations that existed in the supercooled liquid just before vitrification. A peak for the shortest, hairpin rotamer appears only for <em>n</em> ≥ <em>n</em><small><sub>0</sub></small> = 18, and is also manifested in the minimum of <em>R</em><small><sub>g</sub></small>/<em>R</em><small><sub>ee</sub></small>(<em>n</em>) for liquid <em>n</em>-alkanes. The dependence of <em>T</em><small><sub>g</sub></small> on <em>n</em> is represented as two intersecting Ueberreiter and Kanig equations, intersecting near <em>n</em><small><sub>0</sub></small> = 18. Extrapolation gives the asymptotic <em>n</em> → ∞ limit of <em>T</em><small><sub>g</sub></small>, <em>T</em><small><sup>∞</sup></small><small><sub>g</sub></small> = 250 K, which is probably its most accurate estimate obtained theoretically todate.</p>\",\"PeriodicalId\":99,\"journal\":{\"name\":\"Physical Chemistry Chemical Physics\",\"volume\":\" 17\",\"pages\":\" 8731-8745\"},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2025-03-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://pubs.rsc.org/en/content/articlepdf/2025/cp/d4cp02581d?page=search\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Chemistry Chemical Physics\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2025/cp/d4cp02581d\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Chemistry Chemical Physics","FirstCategoryId":"92","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/cp/d4cp02581d","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
In silico cooling rate dependent crystallization and glass transition in n-alkanes†
n-Alkanes (CnH2n+2) are linear chain compounds spanning length-scales from small molecules to polymers. Intermediate length alkanes (say, n = 10–20) have attracted much interest as organic phase change materials (PCM) for storing energy as latent heat. The cooling rate (γ) determines both the latent heat and temperature of crystallization. While slow cooling of the liquid leads to the crystalline state, rapid cooling leads to a glassy state (glass transition temperature Tg). Albeit scant theoretical investigations concerning the vitrification processes, the role of molecular conformations therein remains completely unexplored. Our work presents an all-atom molecular dynamics study of (a) cooling intermediate length alkanes (n = 12 and 16) at seven different rates, and (b) rapidly cooling 14 n-alkanes (4 ≤ n ≤ 50) for determining Tg(n). We find that for linear molecules the end-to-end distance (Ree) is of special relevance: the crystal is composed solely of fully stretched molecules (maximal Ree). Hence one may define the “degree of crystallization” as the area under the maximal Ree peak in the Ree distribution. Other peaks in the distribution represent conformations that existed in the supercooled liquid just before vitrification. A peak for the shortest, hairpin rotamer appears only for n ≥ n0 = 18, and is also manifested in the minimum of Rg/Ree(n) for liquid n-alkanes. The dependence of Tg on n is represented as two intersecting Ueberreiter and Kanig equations, intersecting near n0 = 18. Extrapolation gives the asymptotic n → ∞ limit of Tg, T∞g = 250 K, which is probably its most accurate estimate obtained theoretically todate.
期刊介绍:
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