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📄 mrtlatticedescriptors.h

📁 open lattice boltzmann project www.openlb.org
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/*  This file is part of the OpenLB library * *  Copyright (C) 2006, 2007 Jonas Latt *  Address: Rue General Dufour 24,  1211 Geneva 4, Switzerland  *  E-mail: jonas.latt@gmail.com * *  This program is free software; you can redistribute it and/or *  modify it under the terms of the GNU General Public License *  as published by the Free Software Foundation; either version 2 *  of the License, or (at your option) any later version. * *  This program is distributed in the hope that it will be useful, *  but WITHOUT ANY WARRANTY; without even the implied warranty of *  MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the *  GNU General Public License for more details. * *  You should have received a copy of the GNU General Public  *  License along with this program; if not, write to the Free  *  Software Foundation, Inc., 51 Franklin Street, Fifth Floor, *  Boston, MA  02110-1301, USA.*//** \file * Descriptor for all types of 2D and 3D lattices. In principle, thanks * to the fact that the OpenLB code is generic, it is sufficient to * write a new descriptor when a new type of lattice is to be used. *  -- header file */#ifndef MRT_LATTICE_DESCRIPTORS_H#define MRT_LATTICE_DESCRIPTORS_H#include "core/latticeDescriptors.h"#include <vector>namespace olb {/// Descriptors for the 2D and 3D lattices./** \warning Attention: The lattice directions must always be ordered in * such a way that c[i] = -c[i+(q-1)/2] for i=1..(q-1)/2, and c[0] = 0 must * be the rest velocity. Furthermore, the velocities c[i] for i=1..(q-1)/2 * must verify *  - in 2D: (c[i][0]<0) || (c[i][0]==0 && c[i][1]<0) *  - in 3D: (c[i][0]<0) || (c[i][0]==0 && c[i][1]<0) *                       || (c[i][0]==0 && c[i][1]==0 && c[i][2]<0) * Otherwise some of the code will work erroneously, because the * aformentioned relations are taken as given to enable a few * optimizations.*/namespace descriptors {    /// MRT D2Q9 lattice. The numbering follows the one in "Viscous flow computations    /// with the method of lattice Boltzmann equation", D. Yu, L.-S. Luo, W. Shi,    /// Progress in Aerospace Sciences 39, (2003), p. 329-367    template <typename T>    struct MRTD2Q9DescriptorBase : public D2Q9DescriptorBase<T>    {        enum { d_ = 2, q_ = 9 };     ///< number of dimensions/distr. functions        static const T M[q_][q_];    // Matrix of base change between f and moments : moments=M.f        static const T invM[q_][q_]; // inverse of base change matrix : f=invM.moments        static const T S[q_];       // relaxation times        enum {shearIndexes = 2};        static const int shearViscIndexes[shearIndexes]; // relevant indexes of r. t. for shear viscosity        static const int bulkViscIndex  = 2; // relevant index of r. t. for bulk viscosity    };        /// MRT D3Q19 lattice. The numbering follows the one in "Multiple-relaxation-    /// time lattice Boltzmann models in three dimensions", D. D'Humières,     /// I. Ginzburg, M. Krafzcyk, P. Lallemand, L.-S. Luo,    /// Phil. Trans. R. Soc. Lond. A (2002) 660, p. 437-451    template <typename T>    struct MRTD3Q19DescriptorBase : public D3Q19DescriptorBase<T>    {        enum { d_ = 3, q_ = 19 };     ///< number of dimensions/distr. functions        static const T M[q_][q_];    // Matrix of base change between f and moments : moments=M.f        static const T invM[q_][q_]; // inverse of base change matrix : f=invM.moments        static const T S[q_];       // relaxation times        enum {shearIndexes = 5};        static const int shearViscIndexes[shearIndexes]; // relevant indexes of r. t. for shear viscosity        static const int bulkViscIndex  = 1; // relevant index of r. t. for bulk viscosity    };    template <typename T>    struct MRTD2Q9Descriptor        : public MRTD2Q9DescriptorBase<T>, public NoExternalFieldBase    { };    template <typename T>    struct MRTD3Q19Descriptor        : public MRTD3Q19DescriptorBase<T>, public NoExternalFieldBase    { };}  // namespace descriptors}  // namespace olb#endif

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