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• W2022276595 startingPage "2747" @default.
• W2022276595 abstract "Nonequilibrium molecular dynamics (NEMD) simulations are used to investigate the behavior of a fluid of dipolar Lennard-Jones (LJ) particles under planar Couette flow. Such systems can be viewed as simple models for magnetic ferrofluids. Various issues that arise in such simulations are discussed. These include the importance of the long-range dipolar forces, the influence of different thermostats, and the induction of orientational order. The shear viscosity is found to be somewhat sensitive to the treatment of the dipolar interactions with spherical truncation giving lower values than Ewald sums. The system considered is characterized by a moderate dipole moment, and strong orientational order does not develop at low shear rates. However, the direction of the weak polarization correlates with the shear-induced distortion of the fluid structure. At very high shear rates the fluid behavior depends on the thermostat applied. While the results are not strongly sensitive to details of the rotational thermostat, this is not the case for translational motion. A translationally biased thermostat leads to a string phase, although string formation requires significantly higher shear rates for the dipolar fluid than for the corresponding LJ system. For the dipolar fluid, the string phase is accompanied by strong orientational ordering perpendicular to the flow for Ewald sums and with the flow for the spherically truncated case. In the Ewald systems the order was ferroelectric for conducting boundary conditions, and an antiferroelectric domain structure formed in the vacuum case. For the truncated potential individually polarized chains are randomly oriented with or against the flow. The string phase and the orientational ordering disappears when the translationally unbiased thermostat of Evans and co-workers is employed. Some NEMD simulations with oscillating shear were also performed. These yielded layer structures and again strong orientational order in the dipolar case." @default.
• W2022276595 created "2016-06-24" @default.
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• W2022276595 date "2002-07-24" @default.
• W2022276595 modified "2023-09-26" @default.
• W2022276595 title "Nonequilibrium molecular dynamics simulations of a simple dipolar fluid under shear flow" @default.
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• W2022276595 cites W1975850980 @default.
• W2022276595 cites W1976299125 @default.
• W2022276595 cites W1977210808 @default.
• W2022276595 cites W1977567909 @default.
• W2022276595 cites W1980349041 @default.
• W2022276595 cites W1982001674 @default.
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• W2022276595 cites W2024844228 @default.
• W2022276595 cites W2024987957 @default.
• W2022276595 cites W2028151286 @default.
• W2022276595 cites W2030409039 @default.
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• W2022276595 doi "https://doi.org/10.1063/1.1491874" @default.
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