Results 291 to 300 of about 64,324 (325)
Some of the next articles are maybe not open access.
Computers & Mathematics with Applications, 2021
zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Huanrong Li +3 more
openaire +1 more source
zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Huanrong Li +3 more
openaire +1 more source
2013 IEEE International Conference on Signal Processing, Communication and Computing (ICSPCC 2013), 2013
In this paper, an improved three-dimensional (3D) locally one-dimensional finite-difference time-domain (LOD-FDTD) method is presented. In the proposed method, the time step is divided into three sub-steps. Dispersion control parameters are inducted into X, Y and Z directions.
Min Su, Bo Yi, Pei-Guo Liu
openaire +1 more source
In this paper, an improved three-dimensional (3D) locally one-dimensional finite-difference time-domain (LOD-FDTD) method is presented. In the proposed method, the time step is divided into three sub-steps. Dispersion control parameters are inducted into X, Y and Z directions.
Min Su, Bo Yi, Pei-Guo Liu
openaire +1 more source
Numerical Methods for Partial Differential Equations, 2018
In this paper, a linearized finite difference scheme is proposed for solving the multi‐dimensional Allen–Cahn equation. In the scheme, a modified leap‐frog scheme is used for the time discretization, the nonlinear term is treated in a semi‐implicit way ...
Dongdong He, Kejia Pan
semanticscholar +1 more source
In this paper, a linearized finite difference scheme is proposed for solving the multi‐dimensional Allen–Cahn equation. In the scheme, a modified leap‐frog scheme is used for the time discretization, the nonlinear term is treated in a semi‐implicit way ...
Dongdong He, Kejia Pan
semanticscholar +1 more source
IEEE Transactions on Antennas and Propagation, 2016
In order to get low numerical dispersion in the desired directions, four-step locally one-dimensional finite-difference time-domain (LOD4-FDTD), five-step LOD-FDTD (LOD5-FDTD), and six-step LOD-FDTD (LOD6-FDTD) methods are developed here. These methods are derived from the three-step LOD-FDTD method, and each of their substeps has variation in either ...
Alok Kumar Saxena +1 more
openaire +1 more source
In order to get low numerical dispersion in the desired directions, four-step locally one-dimensional finite-difference time-domain (LOD4-FDTD), five-step LOD-FDTD (LOD5-FDTD), and six-step LOD-FDTD (LOD6-FDTD) methods are developed here. These methods are derived from the three-step LOD-FDTD method, and each of their substeps has variation in either ...
Alok Kumar Saxena +1 more
openaire +1 more source
Numerical analysis for high-order six-stages split-step unconditionally-stable FDTD methods
2012 International Conference on Microwave and Millimeter Wave Technology (ICMMT), 2012High-order six-stages split-step unconditionally-stable finite-difference time-domain (FDTD) methods are presented. Along the positive and negative of the x, y, and z coordinate directions, the Maxwell's matrix is split into six submatrices, and the time step is divided into six sub-steps. In addition, high-order central finite-difference operators are
Yong-Dan Kong, Qing-Xin Chu
openaire +1 more source
Microwave and Optical Technology Letters, 2014
ABSTRACTA compact fourth‐order six‐stages split‐step finite‐difference time‐domain method is developed, which is based on the compact fourth‐order scheme. The proposed method improves the efficiency of computation by reducing the bandwidth of the matrix to be inversed from seven to five for the fourth‐order scheme.
Yong‐Dan Kong +2 more
openaire +1 more source
ABSTRACTA compact fourth‐order six‐stages split‐step finite‐difference time‐domain method is developed, which is based on the compact fourth‐order scheme. The proposed method improves the efficiency of computation by reducing the bandwidth of the matrix to be inversed from seven to five for the fourth‐order scheme.
Yong‐Dan Kong +2 more
openaire +1 more source
Numerical Methods for Partial Differential Equations
AbstractWe develop two totally decoupled, linear and second‐order accurate numerical methods that are unconditionally energy stable for solving the Cahn–Hilliard–Darcy equations for two phase flows in porous media or in a Hele‐Shaw cell. The implicit‐explicit Crank–Nicolson leapfrog method is employed for the discretization of the Cahn–Hiliard equation
Yali Gao, Daozhi Han
openaire +2 more sources
AbstractWe develop two totally decoupled, linear and second‐order accurate numerical methods that are unconditionally energy stable for solving the Cahn–Hilliard–Darcy equations for two phase flows in porous media or in a Hele‐Shaw cell. The implicit‐explicit Crank–Nicolson leapfrog method is employed for the discretization of the Cahn–Hiliard equation
Yali Gao, Daozhi Han
openaire +2 more sources
2006
Developing a stable and efficient numerical method for solving the convective diffusion problems continues to be an active and challenging research area because of its importance in prediction of heat and mass transfer and fluid flow. Tests of the diverse methods of this area in the literature reveal that two types of problems appear quite frequently ...
openaire +1 more source
Developing a stable and efficient numerical method for solving the convective diffusion problems continues to be an active and challenging research area because of its importance in prediction of heat and mass transfer and fluid flow. Tests of the diverse methods of this area in the literature reveal that two types of problems appear quite frequently ...
openaire +1 more source