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The density of a path P="〈v1,…2,vkvk〉 is defined as ∑i= 1kvali/∑i= 1kwi.
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To overcome these shortcomings, the premium-penalty strategy has been introduced, and the pheromone diversity of the good paths and the ordinary ones is increased to polarize pheromone density of all paths.
We demonstrate this by obtaining a non-trivial lower bound on the path density of an arbitrary set of trajectories that contain a sampling set with explicitly specified stability bounds.
To compensate for this effect, it is necessary to compute the relative density of tool-path points across the surface, and use this information to moderate the feed rate of the polishing spot along the tool path.
This change is achieved by pre-mechanical working that induces a high density of rapid diffusional paths.
Average shortest path refers to the average density of the shortest paths between all pairs of nodes 29, 30.
Map of ray path density counted in each 0.2° × 0.2° cell showing the coverage and density of the ray paths in the study area.
For these limb-scanning spectrometers, the retrieved metal density is averaged over a path of about 100 km around the tangent point.
Since the mean shift vector always points towards the direction of the maximum increase in the density, it can define a path leading to a local density maximum, ie, to a mode of the density.
Since the mean shift vector always points towards the direction of the maximum increase in the density, it can define a path leading to a local density maximum; that is, to a mode of the density (see Figure 1).
For workpieces of same size, the path spacing changes the density degree of path.
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