Structure and thermodynamics of mixed polymeric micelles with crystalline cores: tuning properties via co-assembly
We investigate micelles formed by mixtures of n-alkyl-poly(ethylene oxide) block copolymers, Cn-PEO, with different alkyl block lengths in aqueous solution. This model system has previously been used to shed light on the interplay between exchange kinetics and crystallinity in self-assembling system...
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Veröffentlicht in: | Soft matter 2019, Vol.15 (39), p.7777-7786 |
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description | We investigate micelles formed by mixtures of n-alkyl-poly(ethylene oxide) block copolymers, Cn-PEO, with different alkyl block lengths in aqueous solution. This model system has previously been used to shed light on the interplay between exchange kinetics and crystallinity in self-assembling systems [König et al., Phys. Rev. Lett., 2019, 122, 078001]. Now we report on the structure and thermodynamics of these micelles by combining results from small-angle X-ray scattering, differential scanning calorimetry and volumetric measurements. We show that mixed micelles are formed despite the fact that length-mismatched n-alkanes of similar weights in bulk tend to demix below the crystallization temperature. Instead, the system exhibits similar properties as single-component micelles but with a modulated melting region. Interestingly, the melting point depression due to self-confinement within the micellar core can be approximately described by a generalized Gibbs-Thomson equation, similar to single-component micelles [Zinn et al. Phys. Rev. Lett., 2014, 113, 238305]. Furthermore, we find a novel scaling law for these micelles where, at least for larger n, the aggregation number scales with the third power of the length of the hydrophobic block, Nagg ∝ n3. Possibly, there might be a cross-over from the conventional Nagg ∝ n2 behaviour around n ≈ 19. However, the reason for such a transition as well as the strong n dependence remains a challenge and requires more theoretical work. |
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This model system has previously been used to shed light on the interplay between exchange kinetics and crystallinity in self-assembling systems [König et al., Phys. Rev. Lett., 2019, 122, 078001]. Now we report on the structure and thermodynamics of these micelles by combining results from small-angle X-ray scattering, differential scanning calorimetry and volumetric measurements. We show that mixed micelles are formed despite the fact that length-mismatched n-alkanes of similar weights in bulk tend to demix below the crystallization temperature. Instead, the system exhibits similar properties as single-component micelles but with a modulated melting region. Interestingly, the melting point depression due to self-confinement within the micellar core can be approximately described by a generalized Gibbs-Thomson equation, similar to single-component micelles [Zinn et al. Phys. Rev. Lett., 2014, 113, 238305]. Furthermore, we find a novel scaling law for these micelles where, at least for larger n, the aggregation number scales with the third power of the length of the hydrophobic block, Nagg ∝ n3. Possibly, there might be a cross-over from the conventional Nagg ∝ n2 behaviour around n ≈ 19. However, the reason for such a transition as well as the strong n dependence remains a challenge and requires more theoretical work.</description><identifier>ISSN: 1744-683X</identifier><identifier>EISSN: 1744-6848</identifier><identifier>DOI: 10.1039/c9sm01452g</identifier><identifier>PMID: 31482169</identifier><language>eng</language><publisher>England: Royal Society of Chemistry</publisher><subject>Alkanes ; Aqueous solutions ; Assembling ; Block copolymers ; Calorimetry ; Crossovers ; Crystal structure ; Crystallinity ; Crystallization ; Dependence ; Differential scanning calorimetry ; Ethylene oxide ; Hydrophobicity ; Melting ; Melting point ; Melting points ; Micelles ; Polyethylene oxide ; Scaling laws ; Small angle X ray scattering ; Thermodynamics ; X-ray scattering</subject><ispartof>Soft matter, 2019, Vol.15 (39), p.7777-7786</ispartof><rights>Copyright Royal Society of Chemistry 2019</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c352t-ac612fa5bc1f680bae86434171a63d202abbf0c99b04f8b4aa20f4c6c442bd993</citedby><cites>FETCH-LOGICAL-c352t-ac612fa5bc1f680bae86434171a63d202abbf0c99b04f8b4aa20f4c6c442bd993</cites><orcidid>0000-0001-8017-6396 ; 0000-0003-3319-5708 ; 0000-0001-6482-7937</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,4010,27904,27905,27906</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/31482169$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>König, Nico</creatorcontrib><creatorcontrib>Willner, Lutz</creatorcontrib><creatorcontrib>Lund, Reidar</creatorcontrib><title>Structure and thermodynamics of mixed polymeric micelles with crystalline cores: tuning properties via co-assembly</title><title>Soft matter</title><addtitle>Soft Matter</addtitle><description>We investigate micelles formed by mixtures of n-alkyl-poly(ethylene oxide) block copolymers, Cn-PEO, with different alkyl block lengths in aqueous solution. This model system has previously been used to shed light on the interplay between exchange kinetics and crystallinity in self-assembling systems [König et al., Phys. Rev. Lett., 2019, 122, 078001]. Now we report on the structure and thermodynamics of these micelles by combining results from small-angle X-ray scattering, differential scanning calorimetry and volumetric measurements. We show that mixed micelles are formed despite the fact that length-mismatched n-alkanes of similar weights in bulk tend to demix below the crystallization temperature. Instead, the system exhibits similar properties as single-component micelles but with a modulated melting region. Interestingly, the melting point depression due to self-confinement within the micellar core can be approximately described by a generalized Gibbs-Thomson equation, similar to single-component micelles [Zinn et al. Phys. Rev. Lett., 2014, 113, 238305]. Furthermore, we find a novel scaling law for these micelles where, at least for larger n, the aggregation number scales with the third power of the length of the hydrophobic block, Nagg ∝ n3. Possibly, there might be a cross-over from the conventional Nagg ∝ n2 behaviour around n ≈ 19. However, the reason for such a transition as well as the strong n dependence remains a challenge and requires more theoretical work.</description><subject>Alkanes</subject><subject>Aqueous solutions</subject><subject>Assembling</subject><subject>Block copolymers</subject><subject>Calorimetry</subject><subject>Crossovers</subject><subject>Crystal structure</subject><subject>Crystallinity</subject><subject>Crystallization</subject><subject>Dependence</subject><subject>Differential scanning calorimetry</subject><subject>Ethylene oxide</subject><subject>Hydrophobicity</subject><subject>Melting</subject><subject>Melting point</subject><subject>Melting points</subject><subject>Micelles</subject><subject>Polyethylene oxide</subject><subject>Scaling laws</subject><subject>Small angle X ray scattering</subject><subject>Thermodynamics</subject><subject>X-ray scattering</subject><issn>1744-683X</issn><issn>1744-6848</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNpdkU9LxDAQxYMo_lm9-AEk4EWEaibJxtSbLLoKiodV8FaSNNVI065Jqvbb23XXPXiaGebH4_EeQodAzoCw_Nzk0RPgY_q6gXbhgvNMSC431zt72UF7Mb4TwiQHsY12GHBJQeS7KMxS6EzqgsWqKXF6s8G3Zd8o70zEbYW9-7Ylnrd1721wZriNrWsb8ZdLb9iEPiZV166x2LTBxkucusY1r3ge2rkNyQ3kp1PDM1MxWq_rfh9tVaqO9mA1R-j55vppcpvdP07vJlf3mWFjmjJlBNBKjbWBSkiilZWCMw4XoAQrKaFK64qYPNeEV1JzpSipuBGGc6rLPGcjdLLUHax8dDamwru4MK8a23axoFTysQCgMKDH_9D3tgvN4K6gjDAQQKgcqNMlZUIbY7BVMQ_Oq9AXQIpFE8Uknz38NjEd4KOVZKe9LdfoX_TsBwqzheQ</recordid><startdate>2019</startdate><enddate>2019</enddate><creator>König, Nico</creator><creator>Willner, Lutz</creator><creator>Lund, Reidar</creator><general>Royal Society of Chemistry</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QF</scope><scope>7QO</scope><scope>7QQ</scope><scope>7SC</scope><scope>7SE</scope><scope>7SP</scope><scope>7SR</scope><scope>7TA</scope><scope>7TB</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>H8D</scope><scope>H8G</scope><scope>JG9</scope><scope>JQ2</scope><scope>KR7</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope><scope>P64</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0001-8017-6396</orcidid><orcidid>https://orcid.org/0000-0003-3319-5708</orcidid><orcidid>https://orcid.org/0000-0001-6482-7937</orcidid></search><sort><creationdate>2019</creationdate><title>Structure and thermodynamics of mixed polymeric micelles with crystalline cores: tuning properties via co-assembly</title><author>König, Nico ; 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This model system has previously been used to shed light on the interplay between exchange kinetics and crystallinity in self-assembling systems [König et al., Phys. Rev. Lett., 2019, 122, 078001]. Now we report on the structure and thermodynamics of these micelles by combining results from small-angle X-ray scattering, differential scanning calorimetry and volumetric measurements. We show that mixed micelles are formed despite the fact that length-mismatched n-alkanes of similar weights in bulk tend to demix below the crystallization temperature. Instead, the system exhibits similar properties as single-component micelles but with a modulated melting region. Interestingly, the melting point depression due to self-confinement within the micellar core can be approximately described by a generalized Gibbs-Thomson equation, similar to single-component micelles [Zinn et al. Phys. Rev. Lett., 2014, 113, 238305]. Furthermore, we find a novel scaling law for these micelles where, at least for larger n, the aggregation number scales with the third power of the length of the hydrophobic block, Nagg ∝ n3. Possibly, there might be a cross-over from the conventional Nagg ∝ n2 behaviour around n ≈ 19. However, the reason for such a transition as well as the strong n dependence remains a challenge and requires more theoretical work.</abstract><cop>England</cop><pub>Royal Society of Chemistry</pub><pmid>31482169</pmid><doi>10.1039/c9sm01452g</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0001-8017-6396</orcidid><orcidid>https://orcid.org/0000-0003-3319-5708</orcidid><orcidid>https://orcid.org/0000-0001-6482-7937</orcidid></addata></record> |
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subjects | Alkanes Aqueous solutions Assembling Block copolymers Calorimetry Crossovers Crystal structure Crystallinity Crystallization Dependence Differential scanning calorimetry Ethylene oxide Hydrophobicity Melting Melting point Melting points Micelles Polyethylene oxide Scaling laws Small angle X ray scattering Thermodynamics X-ray scattering |
title | Structure and thermodynamics of mixed polymeric micelles with crystalline cores: tuning properties via co-assembly |
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