2009
DOI: 10.1016/j.compstruc.2008.09.004
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Integrated radial-basis-function networks for computing Newtonian and non-Newtonian fluid flows

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Cited by 8 publications
(6 citation statements)
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“…It can be seen that (24) is a special case of (29), where f is simply set to null. By substituting Equation (29)…”
Section: One-dimensional Integrated Radial Basis Function Networkmentioning
confidence: 99%
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“…It can be seen that (24) is a special case of (29), where f is simply set to null. By substituting Equation (29)…”
Section: One-dimensional Integrated Radial Basis Function Networkmentioning
confidence: 99%
“…The orders of convergence are 2.42, 2.61 and 2.92 for the minimum horizontal velocity u min , the maximum vertical velocity v max and the minimum vertical velocity v min along the center lines, respectively. The present results for a grid of 101 × 101 are more accurate than those of FDMs with more refined grids [1,28], but less than those of 1D-IRBFN [29]. Table 7 describes comparisons of the number of nonzero elements per row of the system matrix (N nzpr ), number of iterations (N iteration ) and total CPU time (T total ) required to obtain the converged solution with T OL = 10 −12 .…”
Section: Example 3: Lid-driven Cavity Flowmentioning
confidence: 99%
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“…Due to the approximation process based on integration technique rather than conventional differentiation, it does not require the basis function to be differentiable or continuous. So far, many basis functions are available to incorporate into the present formulation, such as Haar wavelet, [11][12][13] Chebyshev polynomials, [14][15][16] radial basis function, 17,18 and so on. Moreover, in order to investigate the strain and stress fields of structures, the approximation of multi-order derivatives of displacements needs a considerably smooth quality.…”
Section: Introductionmentioning
confidence: 99%