多分散性和浓度对稀聚合物溶液弹性毛细管减薄的影响

IF 15.7 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY
Vincenzo Calabrese, Amy Q. Shen, Simon J. Haward
{"title":"多分散性和浓度对稀聚合物溶液弹性毛细管减薄的影响","authors":"Vincenzo Calabrese, Amy Q. Shen, Simon J. Haward","doi":"10.1103/physrevx.15.021025","DOIUrl":null,"url":null,"abstract":"The self-thinning of liquid bridges under the action of capillarity occurs in widespread processes like jetting, dripping, and spraying and gives rise to a strong extensional flow capable of stretching dissolved polymers. If the resulting elastic stress exceeds the viscous stress, an exponential “elastocapillary” (EC) thinning regime arises, yielding a timescale τ</a:mi>EC</a:mi></a:mrow></a:msub></a:math> that is commonly considered equivalent to the longest relaxation time of the polymer <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mi>λ</c:mi></c:math>. A long-standing question is why <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:msub><e:mi>τ</e:mi><e:mrow><e:mi>EC</e:mi></e:mrow></e:msub></e:math> depends strongly on the polymer concentration, even at high dilutions where <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>λ</g:mi></g:math> should be constant in theory. To date, this is understood in terms of intermolecular interactions that arise due to “self-concentration” effects as polymers stretch. However, <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mi>λ</i:mi></i:math> depends on the polymer molecular weight <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mi>M</k:mi></k:math>, and we show how the concentration dependence of <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:msub><m:mi>τ</m:mi><m:mrow><m:mi>EC</m:mi></m:mrow></m:msub></m:math> can be explained by considering the molecular weight distribution (MWD) inherent in real polymer samples, without the need to invoke self-concentration. We demonstrate this by blending low-<o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:mi>M</o:mi></o:math> and high-<q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:mi>M</q:mi></q:math> polymer samples with narrow MWDs at dilute concentrations and in different proportions and by measuring <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:msub><s:mi>τ</s:mi><s:mrow><s:mi>EC</s:mi></s:mrow></s:msub></s:math> for each blend in capillary thinning experiments. Through a simple model that qualitatively reproduces the experimental results, we show how elastic stresses generated by the polymer build up prior to the EC regime due to the sequential stretching of progressively decreasing molecular weight species in the MWD. Since the elastic stress generated by each species depends on its concentration, the fraction of the MWD that is required to stretch in order to induce the EC regime depends on the total polymer concentration <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:mi>c</u:mi></u:math> in the solution. For higher <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:mi>c</w:mi></w:math>, the EC regime is induced by stretching of a higher-<y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mi>M</y:mi></y:math> (longer λ</ab:mi></ab:math>) fraction of the MWD and results in a longer measurement of <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:msub><cb:mi>τ</cb:mi><cb:mrow><cb:mi>EC</cb:mi></cb:mrow></cb:msub></cb:math>. Our results have significant implications for the application of capillary thinning measurements to extensional rheometry, for the interpretation of such measurements, and for the understanding of elastocapillary thinning dynamics in general. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20161,"journal":{"name":"Physical Review X","volume":"13 1","pages":""},"PeriodicalIF":15.7000,"publicationDate":"2025-04-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Effects of Polydispersity and Concentration on Elastocapillary Thinning of Dilute Polymer Solutions\",\"authors\":\"Vincenzo Calabrese, Amy Q. Shen, Simon J. Haward\",\"doi\":\"10.1103/physrevx.15.021025\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The self-thinning of liquid bridges under the action of capillarity occurs in widespread processes like jetting, dripping, and spraying and gives rise to a strong extensional flow capable of stretching dissolved polymers. If the resulting elastic stress exceeds the viscous stress, an exponential “elastocapillary” (EC) thinning regime arises, yielding a timescale τ</a:mi>EC</a:mi></a:mrow></a:msub></a:math> that is commonly considered equivalent to the longest relaxation time of the polymer <c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><c:mi>λ</c:mi></c:math>. A long-standing question is why <e:math xmlns:e=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><e:msub><e:mi>τ</e:mi><e:mrow><e:mi>EC</e:mi></e:mrow></e:msub></e:math> depends strongly on the polymer concentration, even at high dilutions where <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:mi>λ</g:mi></g:math> should be constant in theory. To date, this is understood in terms of intermolecular interactions that arise due to “self-concentration” effects as polymers stretch. However, <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:mi>λ</i:mi></i:math> depends on the polymer molecular weight <k:math xmlns:k=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><k:mi>M</k:mi></k:math>, and we show how the concentration dependence of <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><m:msub><m:mi>τ</m:mi><m:mrow><m:mi>EC</m:mi></m:mrow></m:msub></m:math> can be explained by considering the molecular weight distribution (MWD) inherent in real polymer samples, without the need to invoke self-concentration. We demonstrate this by blending low-<o:math xmlns:o=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><o:mi>M</o:mi></o:math> and high-<q:math xmlns:q=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><q:mi>M</q:mi></q:math> polymer samples with narrow MWDs at dilute concentrations and in different proportions and by measuring <s:math xmlns:s=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><s:msub><s:mi>τ</s:mi><s:mrow><s:mi>EC</s:mi></s:mrow></s:msub></s:math> for each blend in capillary thinning experiments. Through a simple model that qualitatively reproduces the experimental results, we show how elastic stresses generated by the polymer build up prior to the EC regime due to the sequential stretching of progressively decreasing molecular weight species in the MWD. Since the elastic stress generated by each species depends on its concentration, the fraction of the MWD that is required to stretch in order to induce the EC regime depends on the total polymer concentration <u:math xmlns:u=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><u:mi>c</u:mi></u:math> in the solution. For higher <w:math xmlns:w=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><w:mi>c</w:mi></w:math>, the EC regime is induced by stretching of a higher-<y:math xmlns:y=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><y:mi>M</y:mi></y:math> (longer λ</ab:mi></ab:math>) fraction of the MWD and results in a longer measurement of <cb:math xmlns:cb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cb:msub><cb:mi>τ</cb:mi><cb:mrow><cb:mi>EC</cb:mi></cb:mrow></cb:msub></cb:math>. Our results have significant implications for the application of capillary thinning measurements to extensional rheometry, for the interpretation of such measurements, and for the understanding of elastocapillary thinning dynamics in general. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>\",\"PeriodicalId\":20161,\"journal\":{\"name\":\"Physical Review X\",\"volume\":\"13 1\",\"pages\":\"\"},\"PeriodicalIF\":15.7000,\"publicationDate\":\"2025-04-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review X\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevx.15.021025\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review X","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevx.15.021025","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0

摘要

在毛细作用下,液体桥的自减薄在喷射、滴下和喷射等广泛的过程中发生,并产生能够拉伸溶解聚合物的强拉伸流动。如果产生的弹性应力超过粘性应力,则会出现指数“弹性毛细管”(EC)变薄的情况,产生通常被认为相当于聚合物最长松弛时间λ的时间标度τEC。一个长期存在的问题是,为什么τEC强烈依赖于聚合物浓度,即使在理论上λ应该是恒定的高稀释度下。迄今为止,这被理解为在聚合物拉伸时由于“自集中”效应而产生的分子间相互作用。然而,λ取决于聚合物分子量M,我们展示了τEC的浓度依赖性如何可以通过考虑真实聚合物样品中固有的分子量分布(MWD)来解释,而无需调用自浓度。我们通过在稀释浓度和不同比例下混合具有窄MWDs的低m和高m聚合物样品,并通过在毛细管稀释实验中测量每种混合物的τEC来证明这一点。通过一个定性再现实验结果的简单模型,我们展示了聚合物产生的弹性应力是如何在EC制度之前建立的,这是由于MWD中分子量逐渐减少的物质的顺序拉伸。由于每种物质产生的弹性应力取决于其浓度,因此为了诱导EC状态而拉伸的MWD的比例取决于溶液中聚合物的总浓度c。对于较高的c, EC区是由MWD的高m(更长的λ)部分的拉伸引起的,从而导致τEC的测量时间更长。我们的研究结果对毛细管变薄测量在拉伸流变学中的应用、对这些测量的解释以及对弹性毛细管变薄动力学的理解具有重要意义。2025年由美国物理学会出版
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effects of Polydispersity and Concentration on Elastocapillary Thinning of Dilute Polymer Solutions
The self-thinning of liquid bridges under the action of capillarity occurs in widespread processes like jetting, dripping, and spraying and gives rise to a strong extensional flow capable of stretching dissolved polymers. If the resulting elastic stress exceeds the viscous stress, an exponential “elastocapillary” (EC) thinning regime arises, yielding a timescale τEC that is commonly considered equivalent to the longest relaxation time of the polymer λ. A long-standing question is why τEC depends strongly on the polymer concentration, even at high dilutions where λ should be constant in theory. To date, this is understood in terms of intermolecular interactions that arise due to “self-concentration” effects as polymers stretch. However, λ depends on the polymer molecular weight M, and we show how the concentration dependence of τEC can be explained by considering the molecular weight distribution (MWD) inherent in real polymer samples, without the need to invoke self-concentration. We demonstrate this by blending low-M and high-M polymer samples with narrow MWDs at dilute concentrations and in different proportions and by measuring τEC for each blend in capillary thinning experiments. Through a simple model that qualitatively reproduces the experimental results, we show how elastic stresses generated by the polymer build up prior to the EC regime due to the sequential stretching of progressively decreasing molecular weight species in the MWD. Since the elastic stress generated by each species depends on its concentration, the fraction of the MWD that is required to stretch in order to induce the EC regime depends on the total polymer concentration c in the solution. For higher c, the EC regime is induced by stretching of a higher-M (longer λ) fraction of the MWD and results in a longer measurement of τEC. Our results have significant implications for the application of capillary thinning measurements to extensional rheometry, for the interpretation of such measurements, and for the understanding of elastocapillary thinning dynamics in general. Published by the American Physical Society 2025
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
Physical Review X
Physical Review X PHYSICS, MULTIDISCIPLINARY-
CiteScore
24.60
自引率
1.60%
发文量
197
审稿时长
3 months
期刊介绍: Physical Review X (PRX) stands as an exclusively online, fully open-access journal, emphasizing innovation, quality, and enduring impact in the scientific content it disseminates. Devoted to showcasing a curated selection of papers from pure, applied, and interdisciplinary physics, PRX aims to feature work with the potential to shape current and future research while leaving a lasting and profound impact in their respective fields. Encompassing the entire spectrum of physics subject areas, PRX places a special focus on groundbreaking interdisciplinary research with broad-reaching influence.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信