Longitudinal dynamics in a Lennard-Jones binary liquid: Crossover from hydrodynamics to the molecular regime
Longitudinal collective dynamics of an equimolar Lennard-Jones KrAr mixture is studied in detail in a wide range of spatial and time scales. Combining both the molecular dynamics simulations and analytical generalized collective mode approach, we calculated the spectrum of generalized collective...
Збережено в:
| Дата: | 2004 |
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| Автори: | , |
| Формат: | Стаття |
| Мова: | English |
| Опубліковано: |
Інститут фізики конденсованих систем НАН України
2004
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| Назва видання: | Condensed Matter Physics |
| Онлайн доступ: | https://nasplib.isofts.kiev.ua/handle/123456789/118715 |
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| Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Цитувати: | Longitudinal dynamics in a Lennard-Jones binary liquid: Crossover from hydrodynamics to the molecular regime / T. Bryk, I. Mryglod // Condensed Matter Physics. — 2004. — Т. 7, № 1(37). — С. 15-34. — Бібліогр.: 20 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of Ukraine| Резюме: | Longitudinal collective dynamics of an equimolar Lennard-Jones KrAr mixture
is studied in detail in a wide range of spatial and time scales. Combining
both the molecular dynamics simulations and analytical generalized collective
mode approach, we calculated the spectrum of generalized collective
excitations and analyzed the dominant dynamic processes that determine
the main contributions to time correlation functions in different regions
– starting from the hydrodynamic limit and up to the range of the so-called
molecular regime. The origin of collective propagating modes as well as the
specific features of their dispersion laws within and beyond the hydrodynamic
region are established. It is shown that the structural relaxation and
processes, connected with mutual diffusion of particles, determine mainly
the central peak of total dynamic structure factor beyond the hydrodynamic
region. The dispersion laws, obtained for the propagating modes in our analytical
approach, are compared with the dispersion curves, estimated from
the maxima positions of partial current spectral functions. The difference in
these two sets of numerical results is discussed. |
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