Infrared Spectra and Hydrogen-Bond Configurations of Water Molecules at the Interface of Water-Insoluble Polymers under Humidified Conditions
Elucidating the state of interfacial water, especially the hydrogen-bond configurations, is considered to be key for a better understanding of the functions of polymers that are exhibited in the presence of water. Here, an analysis in this direction is conducted for two water-insoluble biocompatible...
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creator | Ikemoto, Yuka Harada, Yoshihisa Tanaka, Masaru Nishimura, Shin-nosuke Murakami, Daiki Kurahashi, Naoya Moriwaki, Taro Yamazoe, Kosuke Washizu, Hitoshi Ishii, Yoshiki Torii, Hajime |
description | Elucidating the state of interfacial water, especially the hydrogen-bond configurations, is considered to be key for a better understanding of the functions of polymers that are exhibited in the presence of water. Here, an analysis in this direction is conducted for two water-insoluble biocompatible polymers, poly(2-methoxyethyl acrylate) and cyclic(poly(2-methoxyethyl acrylate)), and a non-biocompatible polymer, poly(n-butyl acrylate), by measuring their IR spectra under humidified conditions and by carrying out theoretical calculations on model complex systems. It is found that the OH stretching bands of water are decomposed into four components, and while the higher-frequency components (with peaks at ∼3610 and ∼3540 cm–1) behave in parallel with the CO and C–O–C stretching and CH deformation bands of the polymers, the lower-frequency components (with peaks at ∼3430 and ∼3260 cm–1) become pronounced to a greater extent with increasing humidity. From the theoretical calculations, it is shown that the OH stretching frequency that is distributed from ∼3650 to ∼3200 cm–1 is correlated to the hydrogen-bond configurations and is mainly controlled by the electric field that is sensed by the vibrating H atom. By combining these observed and calculated results, the configurations of water at the interface of the polymers are discussed. |
doi_str_mv | 10.1021/acs.jpcb.2c01702 |
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Here, an analysis in this direction is conducted for two water-insoluble biocompatible polymers, poly(2-methoxyethyl acrylate) and cyclic(poly(2-methoxyethyl acrylate)), and a non-biocompatible polymer, poly(n-butyl acrylate), by measuring their IR spectra under humidified conditions and by carrying out theoretical calculations on model complex systems. It is found that the OH stretching bands of water are decomposed into four components, and while the higher-frequency components (with peaks at ∼3610 and ∼3540 cm–1) behave in parallel with the CO and C–O–C stretching and CH deformation bands of the polymers, the lower-frequency components (with peaks at ∼3430 and ∼3260 cm–1) become pronounced to a greater extent with increasing humidity. From the theoretical calculations, it is shown that the OH stretching frequency that is distributed from ∼3650 to ∼3200 cm–1 is correlated to the hydrogen-bond configurations and is mainly controlled by the electric field that is sensed by the vibrating H atom. By combining these observed and calculated results, the configurations of water at the interface of the polymers are discussed.</description><identifier>ISSN: 1520-6106</identifier><identifier>EISSN: 1520-5207</identifier><identifier>DOI: 10.1021/acs.jpcb.2c01702</identifier><identifier>PMID: 35639685</identifier><language>eng</language><publisher>United States: American Chemical Society</publisher><subject>B: Soft Matter, Fluid Interfaces, Colloids, Polymers, and Glassy Materials ; Hydrogen ; Hydrogen Bonding ; Polymers - chemistry ; Spectrophotometry, Infrared - methods ; Water - chemistry</subject><ispartof>The journal of physical chemistry. B, 2022-06, Vol.126 (22), p.4143-4151</ispartof><rights>2022 The Authors. 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It is found that the OH stretching bands of water are decomposed into four components, and while the higher-frequency components (with peaks at ∼3610 and ∼3540 cm–1) behave in parallel with the CO and C–O–C stretching and CH deformation bands of the polymers, the lower-frequency components (with peaks at ∼3430 and ∼3260 cm–1) become pronounced to a greater extent with increasing humidity. From the theoretical calculations, it is shown that the OH stretching frequency that is distributed from ∼3650 to ∼3200 cm–1 is correlated to the hydrogen-bond configurations and is mainly controlled by the electric field that is sensed by the vibrating H atom. By combining these observed and calculated results, the configurations of water at the interface of the polymers are discussed.</description><subject>B: Soft Matter, Fluid Interfaces, Colloids, Polymers, and Glassy Materials</subject><subject>Hydrogen</subject><subject>Hydrogen Bonding</subject><subject>Polymers - chemistry</subject><subject>Spectrophotometry, Infrared - methods</subject><subject>Water - chemistry</subject><issn>1520-6106</issn><issn>1520-5207</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp1kUtvEzEUhUeIipbCnhXykgWT-jH2jDdINAISqVWRALG0PJ7r1NWMHewxUn4E_xk3CREsWFj2vT7n8-NU1SuCFwRTcqVNWjxsTb-gBpMW0yfVBeEU12W0T49rQbA4r56n9IAx5bQTz6pzxgWTouMX1a-1t1FHGNCXLZg5aqT9gFa7IYYN-Po6lGoZvHWbHPXsgk8oWPRdzxDRbRjB5BES0jOa7wGtfWlbbeCkqdc-hTH3I6DPYdxNEBPKfijmVZ7c4KyDPX9we_aL6szqMcHL43xZffv44etyVd_cfVov39_UupFyri3uieYWRMMwBU5h4G3DZQ8DkS1tjOwkx23badmwXjZto0XX4tJkgBvLJLus3h2429xPMBjw5eWj2kY36bhTQTv1745392oTfipJOtmxpgDeHAEx_MiQZjW5ZGActYeQk6KipYwKjnmR4oPUxJBSBHs6hmD1mKIqKarHFNUxxWJ5_ff1ToY_sRXB24Ngbw05-vJb_-f9Bk3vq4I</recordid><startdate>20220609</startdate><enddate>20220609</enddate><creator>Ikemoto, Yuka</creator><creator>Harada, Yoshihisa</creator><creator>Tanaka, Masaru</creator><creator>Nishimura, Shin-nosuke</creator><creator>Murakami, Daiki</creator><creator>Kurahashi, Naoya</creator><creator>Moriwaki, Taro</creator><creator>Yamazoe, Kosuke</creator><creator>Washizu, Hitoshi</creator><creator>Ishii, Yoshiki</creator><creator>Torii, Hajime</creator><general>American Chemical Society</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0002-1115-2080</orcidid><orcidid>https://orcid.org/0000-0002-5552-4384</orcidid><orcidid>https://orcid.org/0000-0001-6266-0977</orcidid><orcidid>https://orcid.org/0000-0002-6061-9599</orcidid><orcidid>https://orcid.org/0000-0003-0102-9326</orcidid><orcidid>https://orcid.org/0000-0002-7249-7090</orcidid><orcidid>https://orcid.org/0000-0002-4590-9109</orcidid><orcidid>https://orcid.org/0000-0002-5787-7204</orcidid><orcidid>https://orcid.org/0000-0001-6857-5095</orcidid></search><sort><creationdate>20220609</creationdate><title>Infrared Spectra and Hydrogen-Bond Configurations of Water Molecules at the Interface of Water-Insoluble Polymers under Humidified Conditions</title><author>Ikemoto, Yuka ; Harada, Yoshihisa ; Tanaka, Masaru ; Nishimura, Shin-nosuke ; Murakami, Daiki ; Kurahashi, Naoya ; Moriwaki, Taro ; Yamazoe, Kosuke ; Washizu, Hitoshi ; Ishii, Yoshiki ; Torii, Hajime</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a499t-f0b1a5fe64302e52ed57459bed19724c98950778a943b9474a68708953e04f393</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>B: Soft Matter, Fluid Interfaces, Colloids, Polymers, and Glassy Materials</topic><topic>Hydrogen</topic><topic>Hydrogen Bonding</topic><topic>Polymers - chemistry</topic><topic>Spectrophotometry, Infrared - methods</topic><topic>Water - chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ikemoto, Yuka</creatorcontrib><creatorcontrib>Harada, Yoshihisa</creatorcontrib><creatorcontrib>Tanaka, Masaru</creatorcontrib><creatorcontrib>Nishimura, Shin-nosuke</creatorcontrib><creatorcontrib>Murakami, Daiki</creatorcontrib><creatorcontrib>Kurahashi, Naoya</creatorcontrib><creatorcontrib>Moriwaki, Taro</creatorcontrib><creatorcontrib>Yamazoe, Kosuke</creatorcontrib><creatorcontrib>Washizu, Hitoshi</creatorcontrib><creatorcontrib>Ishii, Yoshiki</creatorcontrib><creatorcontrib>Torii, Hajime</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>The journal of physical chemistry. 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It is found that the OH stretching bands of water are decomposed into four components, and while the higher-frequency components (with peaks at ∼3610 and ∼3540 cm–1) behave in parallel with the CO and C–O–C stretching and CH deformation bands of the polymers, the lower-frequency components (with peaks at ∼3430 and ∼3260 cm–1) become pronounced to a greater extent with increasing humidity. From the theoretical calculations, it is shown that the OH stretching frequency that is distributed from ∼3650 to ∼3200 cm–1 is correlated to the hydrogen-bond configurations and is mainly controlled by the electric field that is sensed by the vibrating H atom. 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subjects | B: Soft Matter, Fluid Interfaces, Colloids, Polymers, and Glassy Materials Hydrogen Hydrogen Bonding Polymers - chemistry Spectrophotometry, Infrared - methods Water - chemistry |
title | Infrared Spectra and Hydrogen-Bond Configurations of Water Molecules at the Interface of Water-Insoluble Polymers under Humidified Conditions |
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