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Elucidating the Role of Interfacial Hydrogen Bonds on Glass Transition Temperature Change in a Poly(Vinyl Alcohol)/SiO 2 Polymer‐Nanocomposite by Noncovalent Interaction Characterization and Atomistic Molecular Dynamics Simulations
Author(s) -
Panigrahi Ritwik,
Chakraborty Souvik,
Ye Jun,
Lim Geraldine S.,
Lim Freda C. H.,
Yam Joachim Khin Hun,
Wu Linda Yongling,
Chng Shuyun,
Prawirasatya Melissa,
Herk Alexander M.,
Thoniyot Praveen
Publication year - 2020
Publication title -
macromolecular rapid communications
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.348
H-Index - 154
eISSN - 1521-3927
pISSN - 1022-1336
DOI - 10.1002/marc.202000240
Subject(s) - vinyl alcohol , materials science , fourier transform infrared spectroscopy , nanocomposite , polymer , hydrogen bond , glass transition , chemical engineering , dynamic mechanical analysis , composite number , composite material , molecular dynamics , polymer chemistry , contact angle , differential scanning calorimetry , molecule , chemistry , thermodynamics , organic chemistry , computational chemistry , physics , engineering
A thorough experimental investigation of polymer‐glass transition temperature ( T g ) is performed on poly(vinyl alcohol) (PVA) and fumed silica nanoparticle (SiNP) composite. This is done together with atomistic molecular dynamics simulations of PVA systems in contact with bare and fully hydroxylated silica. Experimentally, PVA‐SiNP composites are prepared by simple solution casting from aqueous solutions followed by its characterization using Fourier‐transform infrared spectroscopy (FTIR), dynamic mechanical analysis (DMA), and dynamic scanning calorimetry (DSC). Both theoretical and experimentally deduced T g are correlated with the presence of hydrogen bonding interactions involving OH functionality present on the surface of SiNP and along PVA polymer backbone. Further deconvolution of FTIR data show that inter‐molecular hydrogen bonding present between PVA and SiNP surface is directly responsible for the increase in T g . SiNP filler and PVA matrix ratio is also optimized for a desired T g increase. An optimal loading of SiNP exists, in order to yield the maximum T g increase arising from the competition between hydrogen bonding and crowding effect of SiNP.