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Experimental and Modeling Studies of Local and Nanoscale para-Cresol Behavior: A Comparison of Classical Force Fields

[Image: see text] The dynamics of bulk liquid para-cresol from 340–390 K was probed using a tandem quasielastic neutron scattering (QENS) and molecular dynamics (MD) approach, due to its relevance as a simple model component of lignin pyrolysis oil. QENS experiments observed both translational jump...

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Detalles Bibliográficos
Autores principales: Morton, Katie S. C., Elena, Alin M., Armstrong, Jeff, O’Malley, Alexander J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10123653/
https://www.ncbi.nlm.nih.gov/pubmed/37039426
http://dx.doi.org/10.1021/acs.jpca.2c08022
Descripción
Sumario:[Image: see text] The dynamics of bulk liquid para-cresol from 340–390 K was probed using a tandem quasielastic neutron scattering (QENS) and molecular dynamics (MD) approach, due to its relevance as a simple model component of lignin pyrolysis oil. QENS experiments observed both translational jump diffusion and isotropic rotation, with diffusion coefficients ranging from 10.1 to 28.6 × 10(–10) m(2)s(–1) and rotational rates from 5.7 to 9.2 × 10(10) s(–1). The associated activation energies were 22.7 ± 0.6 and 10.1 ± 1.2 kJmol(–1) for the two different dynamics. MD simulations applying two different force field models (OPLS3 and OPLS2005) gave values close to the experimental diffusion coefficients and rotational rates obtained upon calculating the incoherent dynamic structure factor from the simulations over the same time scale probed by the QENS spectrometer. The simulations gave resulting jump diffusion coefficients that were slower by factors of 2.0 and 3.8 and rates of rotation that were slower by factors of 1.2 and 1.6. Comparing the two force field sets, the OPLS3 model showed slower rates of dynamics likely due to a higher molecular polarity, leading to greater quantities and strengths of hydrogen bonding.