2020
DOI: 10.1016/j.cam.2019.05.028
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Solving second order non-linear hyperbolic PDEs using generalized finite difference method (GFDM)

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Cited by 20 publications
(7 citation statements)
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“…Therefore, the finite difference method [ 19 , 20 ]] is used as the discrete differential operator to solve Eq (10) , and the discrete expression of image enhancement is obtained as shown in Eq (11) : Where, ∇ N ( I t ) = I x,y−1 − I x,y , ∇ S ( I t ) = I x,y+1 − I x,y , ∇ E ( I t ) = I x−1,y+1 − I x,y , ∇ W ( I t ) = I x+1,y − I x,y is four divergence formulas, whose values are the partial derivatives of the current pixel in the directions of southeast, northwest, and northwest, respectively. cN x,y = exp(−‖∇ N ( I t )‖ 2 / k 2 ), cS x,y = exp(−‖∇ S ( I t )‖ 2 / k 2 ), cE x,y = exp(−‖∇ E ( I t )‖ 2 / k 2 ), cW x,y = exp(−‖∇ W ( I t )‖ 2 / k 2 ) is the thermal conductivity in the four directions of southeast, northwest, I is the current image.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Therefore, the finite difference method [ 19 , 20 ]] is used as the discrete differential operator to solve Eq (10) , and the discrete expression of image enhancement is obtained as shown in Eq (11) : Where, ∇ N ( I t ) = I x,y−1 − I x,y , ∇ S ( I t ) = I x,y+1 − I x,y , ∇ E ( I t ) = I x−1,y+1 − I x,y , ∇ W ( I t ) = I x+1,y − I x,y is four divergence formulas, whose values are the partial derivatives of the current pixel in the directions of southeast, northwest, and northwest, respectively. cN x,y = exp(−‖∇ N ( I t )‖ 2 / k 2 ), cS x,y = exp(−‖∇ S ( I t )‖ 2 / k 2 ), cE x,y = exp(−‖∇ E ( I t )‖ 2 / k 2 ), cW x,y = exp(−‖∇ W ( I t )‖ 2 / k 2 ) is the thermal conductivity in the four directions of southeast, northwest, I is the current image.…”
Section: Methodsmentioning
confidence: 99%
“…Where div is the divergence operator, r is the gradient operator, t represents the iteration time, and ρ is the diffusion coefficient function of the image at time t, which is used to control the anisotropic characteristics of the diffusion process. Therefore, the finite difference method [19,20]] is used as the discrete differential operator to solve Eq (10), and the discrete expression of image enhancement is obtained as shown in Eq (11):…”
Section: Plos Onementioning
confidence: 99%
“…Many works have been devoted to the numerical solutions of semilinear elliptic problems such as finite element method (FEM) [2,3], finite difference method [4], finite volume element method [5] and discontinuous Galerkin method [6]. Recently, some collocation meshless (or meshfree) methods [7,8], Galerkintype meshless method [8] and generalized finite difference method [9,10] have been developed to solve the semilinear PDEs. Unlike mesh-based numerical methods, the shape functions used in the meshless methods [11][12][13][14] are linkage with nodes (or particles) scattered in the underlying computational domain, which reduces the dependence on the mesh.…”
Section: Introductionmentioning
confidence: 99%
“…The use of second-order approximations with the GFDM has received attention in the last two decades and has been successfully consolidated. Its applications vary among many types of problems, such us: seismic wave propagation, 7 hyperbolic nonlinear equations, 8 transient heat flow in anisotropic composites, 9 mathematical models of tumor growth, 10 inverse heat conduction problem, 11 discontinuous crack-faces, 12 plate bending problems, 13 etc.…”
Section: Introductionmentioning
confidence: 99%