2012
DOI: 10.1016/j.enganabound.2011.12.009
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A meshless solution of two-dimensional unsteady flow

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Cited by 22 publications
(11 citation statements)
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“…where Wðr ij Þ is the multiquadric RBF between points i and j (see [31,19]), r ij is the Euclidean distance between these two points and R is the so-called shape factor of the multiquadric function. The formula of Hardy [32] with a slight modification is applied to the local RBFs (see [31]) to find the optimal value of the shape factor, which can be computed in point i as…”
Section: Meshless Local Integral Formulationmentioning
confidence: 99%
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“…where Wðr ij Þ is the multiquadric RBF between points i and j (see [31,19]), r ij is the Euclidean distance between these two points and R is the so-called shape factor of the multiquadric function. The formula of Hardy [32] with a slight modification is applied to the local RBFs (see [31]) to find the optimal value of the shape factor, which can be computed in point i as…”
Section: Meshless Local Integral Formulationmentioning
confidence: 99%
“…A technique described in detail in [19] can be used to obtain a set of RBF shape functions Φ ij , which can be used to express the pressure and its derivatives in the point i as…”
Section: Meshless Local Integral Formulationmentioning
confidence: 99%
See 1 more Smart Citation
“…2). To express the local boundary integral form of the governing equations developed in the previous section in a domain Ω s , we apply the weighting residual principle [7] to equations (10), (11), (12), and (13) to obtain the weak form. If the test function w * is chosen to be the fundamental solution of the Laplace equation, then after integration by parts twice the following integral equations can be obtained (see also [8])…”
Section: Local Boundary Integral Formulationmentioning
confidence: 99%
“…For other implementations of the DRM meshless approach see Kovarik et al [7] and Dehgam and Shirzadi [4]. These three DRM meshless formulations are based on the DRM approximation of the integral representation formula (4) in terms of superposition of single and double layer potentials, with the fundamental solution and its normal derivative as kernels, instead of the integral formula (10) defined by only superposition of double layer potential, with the Dirichlet Green's function as the kernel, as considered in this work.…”
Section: Mathematical Formulation and Boundary Integral Represention mentioning
confidence: 99%