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The physical model of edge water breakthrough is shown in Fig. 1.
These maps emphasize that, globally, raccoons and skunks respond similarly to landscape heterogeneity, and the IBR model of edge effects (no. 7, i.e. the best model in skunks) was the second-best model in all three raccoon analyses (Fig. 2A C), especially in females (see Appendix C also).
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Early models of edge debonding adopted failure criteria based on interfacial stresses.
However, to date, no publications are available on the predictive modeling of edge chipping during RUD of brittle materials.
These are classically analyzed through empirical measurements of linear gradients referenced to the patch border, which yield models of edge effects that: (i) wrongly assume a simple spatial relationship to a single point of the border (the nearest one), (ii) provide flawed predictions on the effect fields generated in ecological patches.
However, no combination of current models of edge surface structure, reactivity and electrostatics can quantitatively predict, without fitted parameters, the experimental titration data over the entire range of pH (4.5 to 9) and ionic strength (0.001 to 0.5 mol dm−3) covered by available data.
These patterns clearly support additive models of edge effects [28], which suggest that the intensity of edge phenomena is compounded by multiple nearby edges.
In the case of a network with highly homogeneous edge weights, the disparity filter will provide an increasingly accurate model of fractional edge weight distributions (see Figure S1).
Based on the analytical model of cutting edge combined with runout parameters, the expression of the rotary surface formed by each cutting edge undergoing general spatial motion is firstly derived.
A 2D Finite Element model of an edge crack has been developed, in which the combined effects of the travelling Hertzian load and the lubricant are accounted for.
A new computational model of the edge plasma in axisymmetric magnetic fusion devices has been developed based on finite element methods.
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