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Ethylene glycol revisited: Molecular dynamics simulations and visualization of the liquid and its hydrogen-bond network

Alexander KaiserInstitute for Ion-Physics and Applied Physics, University of Innsbruck, 6020, Technikerstraße 25/3, AustriaOksana IsmailovaAntti KoskelaInstitute for Mathematics, University of Innsbruck, 6020, Technikerstraße 25/3, AustriaStefan E. HuberInstitute for Ion-Physics and Applied Physics, University of Innsbruck, 6020, Technikerstraße 25/3, AustriaMarcel RitterInstitute for Basic Sciences in Engineering Science, University of Innsbruck, 6020, Technikerstraße 13, AustriaBiagio CosenzaInstitute for Computer Science, University of Innsbruck, 6020, Technikerstraße 25/3, AustriaWerner BengerCenter for Computation and Technology, Louisiana State University, 211 Johnston Hall, Baton Rouge, LA 70803, United StatesRenat R. NazmutdinovKazan National Research Technological University, 420015 Kazan, Republic of Tatarstan, Russian FederationMichael ProbstInstitute for Ion-Physics and Applied Physics, University of Innsbruck, 6020, Technikerstraße 25/3, Austria
2013en
ABI

Annotatsiya

Molecular dynamics simulations of liquid ethylene glycol described by the OPLS-AA force field were performed to gain insight into its hydrogen-bond structure. We use the population correlation function as a statistical measure for the hydrogen-bond lifetime. In an attempt to understand the complicated hydrogen-bonding, we developed new molecular visualization tools within the Vish Visualization shell and used it to visualize the life of each individual hydrogen-bond. With this tool hydrogen-bond formation and breaking as well as clustering and chain formation in hydrogen-bonded liquids can be observed directly. Liquid ethylene glycol at room temperature does not show significant clustering or chain building. The hydrogen-bonds break often due to the rotational and vibrational motions of the molecules leading to an H-bond half-life time of approximately 1.5 ps. However, most of the H-bonds are reformed again so that after 50 ps only 40% of these H-bonds are irreversibly broken due to diffusional motion. This hydrogen-bond half-life time due to diffusional motion is 80.3 ps. The work was preceded by a careful check of various OPLS-based force fields used in the literature. It was found that they lead to quite different angular and H-bond distributions.

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