2021
DOI: 10.1007/s12039-021-01973-8
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Dielectric relaxations of molten acetamide: dependence on the model interaction potentials and the effects of system size

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Cited by 7 publications
(6 citation statements)
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“…to overestimate the experimental DR times by a factor of ~2. 39 The simulated slower than experimental relaxation times fails to correctly describe the viscosity coupling of the diffusive dynamics, and as a result, the simulated DR activation energies show an anion dependence reverse of that found in measurements. An additional support to this view comes from a previous simulation study 105 which reported a much weaker decoupling between the centre-ofmass diffusion and viscosity than reported in experiments.…”
Section: Frequency-dependent Dielctric Function: Connection To Experi...mentioning
confidence: 86%
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“…to overestimate the experimental DR times by a factor of ~2. 39 The simulated slower than experimental relaxation times fails to correctly describe the viscosity coupling of the diffusive dynamics, and as a result, the simulated DR activation energies show an anion dependence reverse of that found in measurements. An additional support to this view comes from a previous simulation study 105 which reported a much weaker decoupling between the centre-ofmass diffusion and viscosity than reported in experiments.…”
Section: Frequency-dependent Dielctric Function: Connection To Experi...mentioning
confidence: 86%
“…OPLS (optimized potentials for liquid simulations) type model force field were used 81 . Since the functional forms and notations associated with different pieces of the OPLS model potential were discussed earlier 39 , these are provided in the Appendix A1 (supplementary material). Interaction parameters developed 82 for correctly reproducing the experimental 83 šœ€ š‘  of neat molten acetamide were employed to represent the acetamide molecules.…”
Section: Simulation Details and Validationmentioning
confidence: 99%
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“…The simulated frequency-dependent dielectric function, Īµ(Ļ‰) can be obtained from the normalized total dipole moment autocorrelation function, Ļ•( t ), which is given by , Ļ• false( t false) = āŸØ M false( 0 false) Ā· M false( t false) āŸ© āŸØ false| M false( 0 false) false| 2 āŸ© where total dipole moment, M ( t ) = āˆ‘ i Ī¼ i ( t ), where Ī¼ i is the dipole moment of the individual dipolar molecules.…”
Section: Theory and Computational Detailsmentioning
confidence: 99%
“…27 This is because this force field describes well the experimental densities 15 (deviation being ā‰¤3%) and reproduces the experimental static dielectric constant 12 and other liquid properties for molten acetamide, 27 although dielectric relaxation time constants and translational diffusion constants were found to be considerably slower than those predicted by its OPLS-AA counterpart. 42,43 A comparison between the simulated (by using the OPLS-UA model potential) and experimental densities is shown in Figure 1 for these two DESs at different temperatures.…”
Section: Validation Of the Simulation Force Fieldmentioning
confidence: 99%