4.8 Article

Patience is a virtue: self-assembly and physico-chemical properties of cellulose nanocrystal allomorphs

Journal

NANOSCALE
Volume 12, Issue 33, Pages 17480-17493

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/d0nr04491a

Keywords

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Funding

  1. Swiss National Science Foundation (SNSF) [PZ00P2_167900]
  2. Adolphe Merkle Foundation
  3. KU Leuven [C14/18/061, IDN/19/014]
  4. Research Foundation Flanders [G.0C60.13N]
  5. European Union's European Fund for Regional Development
  6. Flanders Innovation & Entrepreneurship
  7. NSF [DMR-0520547]
  8. European Union's Horizon 2020 research and innovation program under the SINE2020 project [654000]
  9. Provincie West-Vlaanderen (Accelerate3 project, Interreg Vlaanderen-Nederland program)

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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 zeta-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.

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