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               <dc:title>Patience is a virtue: self-assembly and physico-chemical properties of cellulose nanocrystal allomorphs</dc:title>
               <dc:creator>Delepierre, Gwendoline</dc:creator>
               <dc:creator>Eyley, Samuel</dc:creator>
               <dc:creator>Thielemans, Wim</dc:creator>
               <dc:creator>Weder, Christoph</dc:creator>
               <dc:creator>Cranston, Emily</dc:creator>
               <dc:creator>Zoppe, Justin Orazio</dc:creator>
               <dc:subject>Àrees temàtiques de la UPC::Matemàtiques i estadística</dc:subject>
               <dc:subject>Cellulose nanocrystals</dc:subject>
               <dc:subject>Cel·lulosa</dc:subject>
               <dc:subject>Nanocristalls</dc:subject>
               <dc:description>Cellulose nanocrystals (CNCs) are bio-based rod-like nanoparticles with a quickly expanding market. Despite the fact that a variety of production routes and starting cellulose sources are employed, all industrially produced CNCs consist of cellulose I (CNC-I), the native crystalline allomorph of cellulose. Here a comparative study of the physico-chemical properties and liquid crystalline behavior of CNCs produced from cellulose II (CNC-II) and typical CNC-I is reported. CNC-I and CNC-II are isolated by sulfuric acid hydrolysis of cotton and mercerized cotton, respectively. The two allomorphs display similar surface charge densities and ¿-potentials and both have a right-handed twist, but CNC-II have a slightly smaller average length and aspect ratio, and are less hygroscopic. Interestingly, the self-assembly behavior of CNC-I and CNC-II in water is different. Whilst CNC-I forms a chiral nematic phase, CNC-II initially phase separates into an upper isotropic and a lower nematic liquid crystalline phase, before a slow reorganization into a large-pitch chiral nematic texture occurs. This is potentially caused by a combination of factors, including the inferred faster rotational diffusion of CNC-II and the different crystal structures of CNC-I and CNC-II, which are responsible for the presence and absence of a giant dipole moment, respectively.</dc:description>
               <dc:description>Peer Reviewed</dc:description>
               <dc:description>Postprint (published version)</dc:description>
               <dc:date>2020</dc:date>
               <dc:type>Article</dc:type>
               <dc:relation>https://pubs.rsc.org/en/content/articlelanding/2020/NR/D0NR04491A#!divAbstract</dc:relation>
               <dc:rights>http://creativecommons.org/licenses/by-nc-nd/3.0/es/</dc:rights>
               <dc:rights>Restricted access - publisher's policy</dc:rights>
               <dc:rights>Attribution-NonCommercial-NoDerivs 3.0 Spain</dc:rights>
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