2 research outputs found

    Orientational Jumps in (Acetamide + Electrolyte) Deep Eutectics: Anion Dependence

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    All-atom molecular dynamics simulations have been carried out to investigate orientation jumps of acetamide molecules in three different ionic deep eutectics made of acetamide (CH<sub>3</sub>CONH<sub>2</sub>) and lithium salts of bromide (Br<sup>ā€“</sup>), nitrate (NO<sub>3</sub><sup>ā€“</sup>) and perchlorate (ClO<sub>4</sub><sup>ā€“</sup>) at approximately 80:20 mole ratio and 303 K. Orientational jumps have been dissected into acetamideā€“acetamide and acetamideā€“ion catagories. Simulated jump characteristics register a considerable dependence on the anion identity. For example, large angle jumps are relatively less frequent in the presence of NO<sub>3</sub><sup>ā€“</sup> than in the presence of the other two anions. Distribution of jump angles for rotation of acetamide molecules hydrogen bonded (H-bonded) to anions has been found to be bimodal in the presence of Br<sup>ā€“</sup> and is qualitatively different from the other two cases. Estimated energy barrier for orientation jumps of these acetamide molecules (H-bonded to anions) differ by a factor of āˆ¼2 between NO<sub>3</sub><sup>ā€“</sup> and ClO<sub>4</sub><sup>ā€“</sup>, the barrier height for the latter being lower and āˆ¼0.5<i>k</i><sub>B</sub><i>T</i>. Relative radial and angular displacements during jumps describe the sequence ClO<sub>4</sub><sup>ā€“</sup> > NO<sub>3</sub><sup>ā€“</sup> > Br<sup>ā€“</sup> and follow a reverse viscosity trend. Jump barrier for acetamideā€“acetamide pairs reflects weak dependence on anion identity and remains closer to the magnitude (āˆ¼0.7<i>k</i><sub>B</sub><i>T</i>) found for orientation jumps in molten acetamide. Jump time distributions exhibit a power law dependence of the type, <i>P</i>(<i>t</i><sub>jump</sub>) āˆ <i>A</i>(<i>t</i><sub>jump</sub>/Ļ„)<sup>āˆ’Ī²</sup>, with both Ī² and Ļ„ showing substantial anion dependence. The latter suggests the presence of dynamic heterogeneity in these systems and supports earlier conclusions from time-resolved fluorescence measurements

    Derivation of Coarse Grained Models for Multiscale Simulation of Liquid Crystalline Phase Transitions

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    We present a systematic derivation of a coarse grained (CG) model for molecular dynamics (MD) simulations of a liquid crystalline (LC) compound containing an azobenzene mesogen. The model aims at a later use in a multiscale modeling approach to study liquid crystalline phase transitions that are (photo)Ā­induced by the trans/cis photoisomerization of the mesogen. One of the major challenges in the coarse graining process is the development of models that are for a given chemical system structurally consistent with for example an all-atom reference model and reproduce relevant thermodynamic properties such as the LC phase behavior around the state point of interest. The reduction of number of degrees of freedom makes the resulting coarse models by construction state point dependent; that is, they cannot easily be transferred to a range of temperatures, densities, system compositions, etc. These are significant challenges, in particular if one wants to study LC phase transitions (thermally or photoinduced). In the present paper we show how one can systematically derive a CG model for a LC molecule that is highly consistent with an atomistic description by choosing an appropriate state point for the reference simulation. The reference state point is the supercooled liquid just below the smectic-isotropic phase transition which is characterized by a high degree of local nematic order while being overall isotropic. With the resulting CG model it is possible to switch between the atomistic and the CG levels (and vice versa) in a seamless manner maintaining values of all the relevant order parameters which describe the smectic A (smA) state. This model will allow us in the future to link large length scale and long time scale CG simulations of the LC state with chemically accurate QM/MM simulations of the photoisomerization process
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