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For the system studied here, phase inversion does not occur under no-flow conditions.
The behaviour of the system studied here is compared with that of the corresponding aqueous mixtures, previously by other authors.
However, the graphene system studied here is subject to thermal motion as well as bombardment, and the impinging particle should not be included in Brillouin zone integration.
Unlike in the companion paper where the system was seeded after each avalanche, the system studied here was driven by a continuous external input.
The system studied here is similar in construction to Pancharatnam configuration and behaves as an achromatic half-wave plate over a wide spectral range.
The particular system studied here would have limited use due to energy density and stability but is studied as a model system.
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The systems studied here reveal that the reinforcement increases with decreasing filler size.
We have also noticed that the fluidization of the membrane is a common feature for all systems studied here.
However, the mineralogical complexity of soils [3, 4] and the diversity of soil organic matter [83 86] go well below the variability considered in the model systems studied here.
We verified that collisions with a velocity of 250 m/s are bouncing for all collision systems studied here, while at vanishing velocity, collisions are sticking.
Nevertheless, from a practical point of view, based on the systems studied here, the possibility to design CdS nanocomposites with a predetermined band gaps has been demonstrated.
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