Exact(4)
As a result, it is only suitable to simulate fluid behaviours at the nanoscale owing to the limitation of computation cost (Zhao et al. 2016).
However, relating the two measures was informative in characterising repellency across materials and at different sites, while preserving temporal differences in fluid behaviours.
The results presented herein encompass the following ranges of conditions: 10≤Gr≤107; 0.72≤Pr≤100 and 0.4≤n≤1.8 thereby covering both shear-thinning and shear-thickening types of fluid behaviours.
All in all, the present results encompass wide ranges of conditions as follows: Reynolds number: 1 500; Peclet number: 1 500; bed voidage: 0.4 0.8 and the flow behaviour index: 0.5 1.8 thereby covering extremely shear-thinning and shear-thickening types of fluid behaviours.
Similar(56)
Differences in fluid behaviour at the macro and micro-scales are discussed.
Pore wetting is significant for understanding fluid behaviour in porous media.
In MD simulations, the fluid behaviour is described by the motion of the individual particles interacting with each other via intermolecular potentials (Koplik and Banavar 1995).
The model set forth herein features: compressible fluid behaviour, nonlinear flow rate-pressure relations, valve mechanical equations and rubber mounts.
Assuming Newtonian fluid behaviour, image analysis permitted computation of local porosity, intra-pore fluid shear, and visualization of flow heterogeneity within the sample.
The dynamic bulk fluid behaviour is characterised in terms of: (i) fluid properties, (ii) governing physics and (iii) microchannel geometric features.
This is because accurate predictions of the fluid behaviour are strongly dependent on the inflow conditions, particularly in turbulent flows at high turbulent Reynolds numbers.
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