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A nonuniform grid lattice Boltzmann technique previously described by He et al. [1] has been extended to simulate three-dimensional flows in complex geometries.
The number of prototypes K is defined by the dimensions of the grid (lattice size), i.e, (width times height).
Watts Strogatz networks (1998) (small-world networks) are in a regime between a fully regular grid (lattice) and a random network (Erdös Rényi).
First, we used a lower focusing grid resolution (1 Å/grid instead of 0.5 Å/grid) to perform the same interaction energy calculations.[18] Second, we doubled the grid lattice size to >14 times the dimension of the model for macromolecule complexes in all axes.
Here, force application points were chosen on a regular hexagonal grid (lattice constant 5 µm) covering the whole cell area.
The quadrats were placed at the left edge of intersections of the PV or nuclear membrane with a randomly placed grid lattice (grid spacing 22.12 μm, n = 2 to 5 measurements per nucleus or PV).
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They also showed the completeness and reversibility of the pull move set for rectangular grid lattices.
These facts raise great interest in the plausibility of extending the GPUs' use to non-graphics applications, in particular numerical simulations on structured grids (lattice).
Provided that the density of nodes is high, each distance to the nearest transmitting node becomes D and the location of the transmitting nodes is a honey-grid lattice, as shown in Figure 1.
For decades network systems have been modeled either as chains, grids, lattices and fully-connected graphs which are completely regular or as random Erdős-Rényi network whose node degrees follow a Poisson distribution [ 3].
Lattice QCD calculations use a four-dimensional grid, or lattice, of points to represent the three dimensions of space and one of time.
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