About: Finite difference method is a research topic. Over the lifetime, 21603 publications have been published within this topic receiving 468852 citations. The topic is also known as: Finite-difference methods & FDM.
TL;DR: In this paper, a multiscale finite element method for the incompressible Navier-Stokes equations is proposed, which is based on a decomposition of the velocity field into coarse/resolved scales and fine/unsolved scales.
TL;DR: A high order difference scheme and Galerkin spectral technique is applied for the numerical solution of multi-term time fractional partial differential equations and it is proved the unconditional stability of the compact procedure by coefficient matrix property is proved.
TL;DR: In this article, new explicit methods for the finite difference solution of a parabolic PDE are derived using stable asymmetric approximations to the partial differential equation which when coupled in groups of 2 adjacent points on the grid result in implicit equations which can be easily converted to explicit form which in turn offer many advantages.
Abstract: In this paper, new explicit methods for the finite difference solution of a parabolic partial differential equation are derived. The new methods use stable asymmetric approximations to the partial differential equation which when coupled in groups of 2 adjacent points on the grid result in implicit equations which can be easily converted to explicit form which in turn offer many advantages. By judicious use of alternating this strategy on the grid points of the domain results in an algorithm which possesses unconditional stability. The merit of this approach results in more accurate solutions because of truncation error cancellations. The stability, consistency, convergence and truncation error of the new method is discussed and the results of numerical experiments presented.
TL;DR: In this article, the numerical solution of partial differential equations is used to solve the boundary value problem in partial differential form (PDP) and the numerical optimization problem is used for the coupling of field and circuit equations.
Abstract: 1 Introduction: 1.1 Numerical solution process. 2 Computer aided design in magnetics: 2.1 Finite element based CAD systems 2.2 Design strategies. 3 Electromagnetic fields: 3.1 Quasi stationary fields 3.2 Boundary value problem 3.3 Field equations in partial differential form. 4 Potentials and formulations: 4.1 Magnetic vector potential 4.2 Electric vector potential for conducting current 4.3 Electro-static scalar potential 4.4 Magnetic scalar potential 4.5 A? -formulation 4.6 AV-formulation 4.7 In-plane formulation 4.8 AV-formulation with v?B motion term 4.9 Gauge conditions 4.10 Subsequent treatment of the Maxwell equations. 5 Field computation and numerical techniques: 5.1 Magnetic equivalent circuit 5.2 Point mirroring method 5.3 The numerical solution of partial differential equations 5.4 Finite difference method 5.5 Finite element method 5.6 Material modelling 5.7 Numerical implementation of the FEM 5.8 Adaptive refinement for 2D triangular meshes 5.9 Coupling of field and circuit equations 5.10 Post-processing. 6 Coupled field problems: 6.1 Coupled fields 6.2 Strong and weak coupling 6.3 Coupled problems 6.4 Classification of coupled field problems. 7 Numerical optimisation: 7.1 Electromagnetic optimisation problems 7.2 Optimisation problem definition 7.3 Methods. 8 Linear system equation solvers: 8.1 Methods 8.2 Computational costs. 9 Modelling of electrostatic and magnetic devices: 9.1 Modelling with respect to the time 9.2 Geometry modelling 9.3 Boundary conditions 9.4 Transformations. 10 Examples of computed models: 10.1 Electromagnetic and electrostatic devices 10.2 Coupled thermo-electromagnetic problems 10.3 Numerical optimisation
TL;DR: A novel, linear, second order semi-discrete scheme in time to solve the governing system of equations in the hydrodynamic Q -tensor model, developed following the novel ‘ energy quadratization ’ strategy so that it is linear and unconditionally energy stable at the semi- Discrete level.