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Exact(5)
An efficient method for discretization of Laplacian operators on adaptive meshes is proposed.
We use Nyström's method for discretization, and combine it with special quadrature rules for the singular kernels that appear in the boundary integrals.
Additional file 1 This file contains the method for discretization of the diffusion equation and Figure.
The simplest method for discretization is to determine the minimum and maximum values of the attributes and then divide the range into user defined number of intervals of equal length.
The first order Euler Maruyama method for discretization of these equations is given by (6) X t + Δ t = X t + A (X t ) Δ t + B (X t ) Δ t ζ, where X = { X t, t ⩾ 0 } is the state vector of the system, which is represented in this case by the position of the particle y and the reduced (v 1, v 2 ) velocity phase space.
Similar(55)
There are several known methods for discretization including Equal Information Gain, Maximum Entropy, and Equal Interval Width.
The present paper deals with the numerical solution of the incompressible Navier Stokes equations using high-order discontinuous Galerkin (DG) methods for discretization in space.
In this paper, for a simplified model problem, we give an analysis that explains why known (standard) methods for discretization of the localized force term and for discretization of the pressure variable often yield large spurious velocities.
We have previously described methods for discretization of continuous data and their potential impact on learned networks during structure learning [ 8, 20].
The method allows for discretization of complicated geometries with arbitrary order representations of the B and E fields.
The transport equation is solved using operator splitting, with the discontinuous finite element method (DFE) for discretization of the advective term.
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