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authorAdrian Kummerlaender2019-06-24 14:43:36 +0200
committerAdrian Kummerlaender2019-06-24 14:43:36 +0200
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treec1a6894679563e271f5c6ea7a17fa3462f7212a3 /src/dynamics/mrtLatticeDescriptors.h
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Initialize at openlb-1-3
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+/* This file is part of the OpenLB library
+ *
+ * Copyright (C) 2019 Adrian Kummerlaender
+ * E-mail contact: info@openlb.net
+ * The most recent release of OpenLB can be downloaded at
+ * <http://www.openlb.net/>
+ *
+ * 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
+ * DESCRIPTORBASE 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 "latticeDescriptors.h"
+
+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 {
+
+namespace tag {
+
+struct MRT : public CATEGORY, public DESCRIPTOR_TAG { };
+
+}
+
+using MRTD2Q5Descriptor = D2Q5<tag::MRT>;
+
+/// Advection Diffusion MRT D2Q5
+/**
+ * Based on: Liu, Q., & He, Y. L. (2015). Double multiple-relaxation-time lattice Boltzmann model
+ * for solid–liquid phase change with natural convection in porous media.
+ * Physica A: Statistical Mechanics and its Applications, 438, 94-106.
+ **/
+using AdvectionDiffusionMRTD2Q5Descriptor = D2Q5<tag::MRT,VELOCITY>;
+
+/// 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
+using MRTD2Q9Descriptor = D2Q9<tag::MRT>;
+
+using ForcedMRTD2Q9Descriptor = D2Q9<tag::MRT,FORCE>;
+
+using MRTD3Q7Descriptor = D3Q7<tag::MRT>;
+
+/// Advection Diffusion MRT D3Q7
+/**
+ * Based on: Wu, H., Wang, J., & Tao, Z. (2011). Passive heat transfer in a turbulent
+ * channel flow simulation using large eddy simulation based on the lattice
+ * Boltzmann method framework.
+ * International Journal of Heat and Fluid Flow, 32(6), 1111-1119.
+ *
+ * There are some differences in respect to the order of the columns based on the lattice directions
+ **/
+using AdvectionDiffusionMRTD3Q7Descriptor = D3Q7<tag::MRT,VELOCITY>;
+
+/// 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
+using MRTD3Q19Descriptor = D3Q19<tag::MRT>;
+
+using ForcedMRTD3Q19Descriptor = D3Q19<tag::MRT,FORCE>;
+
+
+namespace mrt_data {
+
+using utilities::Fraction;
+
+// Matrix of base change between f and moments : moments=M.f
+template <unsigned D, unsigned Q>
+constexpr Fraction M[Q][Q] = {};
+
+// inverse of base change matrix : f=invM.moments
+template <unsigned D, unsigned Q>
+constexpr Fraction invM[Q][Q] = {};
+
+// relaxation times
+template <unsigned D, unsigned Q>
+constexpr Fraction s[Q] = {};
+
+// relaxation times
+template <unsigned D, unsigned Q>
+constexpr Fraction s_2[Q] = {};
+
+template <unsigned D, unsigned Q>
+constexpr int shearIndexes = {};
+
+// relevant indexes of r. t. for shear viscosity
+template <unsigned D, unsigned Q>
+constexpr int shearViscIndexes[shearIndexes<D,Q>] = {};
+
+// relevant index of r. t. for bulk viscosity
+template <unsigned D, unsigned Q>
+constexpr int bulkViscIndex = {};
+
+template <>
+constexpr Fraction M<2,5>[5][5] = {
+ { 1, 1, 1, 1, 1},
+ { 0,-1, 0, 1, 0},
+ { 0, 0,-1, 0, 1},
+ {-4, 1, 1, 1, 1},
+ { 0, 1,-1, 1,-1}
+};
+
+template <>
+constexpr Fraction M<2,9>[9][9] = {
+ { 1, 1, 1, 1, 1, 1, 1, 1, 1},
+ {-4, 2, -1, 2, -1, 2, -1, 2, -1},
+ { 4, 1, -2, 1, -2, 1, -2, 1, -2},
+ { 0, -1, -1, -1, 0, 1, 1, 1, 0},
+ { 0, -1, 2, -1, 0, 1, -2, 1, 0},
+ { 0, 1, 0, -1, -1, -1, 0, 1, 1},
+ { 0, 1, 0, -1, 2, -1, 0, 1, -2},
+ { 0, 0, 1, 0, -1, 0, 1, 0, -1},
+ { 0, -1, 0, 1, 0, -1, 0, 1, 0}
+};
+
+template <>
+constexpr Fraction M<3,7>[7][7] = {
+ // Li, Yang et al 2016: The directions are modified for the OpenLB definition
+ {1, 1, 1, 1, 1, 1, 1},
+ {0, 1, 0, -1, 0, 0, 0},
+ {0, 0, -1, 0, 0, 1, 0},
+ {0, 0, 0, 0, 1, 0, -1},
+ {6, -1, -1, -1, -1, -1, -1},
+ {0, 2, -1, 2, -1, -1, -1},
+ {0, 0, 1, 0, -1, 1, -1}
+};
+
+template <>
+constexpr Fraction M<3,19>[19][19] = {
+ { 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1},
+ {-30,-11,-11,-11, 8, 8, 8, 8, 8, 8,-11,-11,-11, 8, 8, 8, 8, 8, 8},
+ { 12, -4, -4, -4, 1, 1, 1, 1, 1, 1, -4, -4, -4, 1, 1, 1, 1, 1, 1},
+ { 0, -1, 0, 0, -1, -1, -1, -1, 0, 0, 1, 0, 0, 1, 1, 1, 1, 0, 0},
+ { 0, 4, 0, 0, -1, -1, -1, -1, 0, 0, -4, 0, 0, 1, 1, 1, 1, 0, 0},
+ { 0, 0, -1, 0, -1, 1, 0, 0, -1, -1, 0, 1, 0, 1, -1, 0, 0, 1, 1},
+ { 0, 0, 4, 0, -1, 1, 0, 0, -1, -1, 0, -4, 0, 1, -1, 0, 0, 1, 1},
+ { 0, 0, 0, -1, 0, 0, -1, 1, -1, 1, 0, 0, 1, 0, 0, 1, -1, 1, -1},
+ { 0, 0, 0, 4, 0, 0, -1, 1, -1, 1, 0, 0, -4, 0, 0, 1, -1, 1, -1},
+ { 0, 2, -1, -1, 1, 1, 1, 1, -2, -2, 2, -1, -1, 1, 1, 1, 1, -2, -2},
+ { 0, -4, 2, 2, 1, 1, 1, 1, -2, -2, -4, 2, 2, 1, 1, 1, 1, -2, -2},
+ { 0, 0, 1, -1, 1, 1, -1, -1, 0, 0, 0, 1, -1, 1, 1, -1, -1, 0, 0},
+ { 0, 0, -2, 2, 1, 1, -1, -1, 0, 0, 0, -2, 2, 1, 1, -1, -1, 0, 0},
+ { 0, 0, 0, 0, 1, -1, 0, 0, 0, 0, 0, 0, 0, 1, -1, 0, 0, 0, 0},
+ { 0, 0, 0, 0, 0, 0, 0, 0, 1, -1, 0, 0, 0, 0, 0, 0, 0, 1, -1},
+ { 0, 0, 0, 0, 0, 0, 1, -1, 0, 0, 0, 0, 0, 0, 0, 1, -1, 0, 0},
+ { 0, 0, 0, 0, -1, -1, 1, 1, 0, 0, 0, 0, 0, 1, 1, -1, -1, 0, 0},
+ { 0, 0, 0, 0, 1, -1, 0, 0, -1, -1, 0, 0, 0, -1, 1, 0, 0, 1, 1},
+ { 0, 0, 0, 0, 0, 0, -1, 1, 1, -1, 0, 0, 0, 0, 0, 1, -1, -1, 1}
+};
+
+template <>
+constexpr Fraction invM<2,5>[5][5] = {
+ {{1, 5}, 0, 0, {-1, 5}, 0},
+ {{1, 5}, {-1, 2}, 0, { 1, 20}, { 1, 4}},
+ {{1, 5}, 0, {-1, 2}, { 1, 20}, {-1, 4}},
+ {{1, 5}, { 1, 2}, 0, { 1, 20}, { 1, 4}},
+ {{1, 5}, 0, { 1, 2}, { 1, 20}, {-1, 4}}
+};
+
+template <>
+constexpr Fraction invM<2,9>[9][9] = {
+ {{1, 9}, {-1, 9}, { 1, 9}, 0, 0, 0, 0, 0, 0},
+ {{1, 9}, { 1, 18}, { 1, 36}, {-1, 6}, {-1, 12}, { 1, 6}, { 1, 12}, 0, {-1, 4}},
+ {{1, 9}, {-1, 36}, {-1, 18}, {-1, 6}, { 1, 6}, 0, 0, { 1, 4}, 0},
+ {{1, 9}, { 1, 18}, { 1, 36}, {-1, 6}, {-1, 12}, {-1, 6}, {-1, 12}, 0, { 1, 4}},
+ {{1, 9}, {-1, 36}, {-1, 18}, 0, 0, {-1, 6}, { 1, 6}, {-1, 4}, 0},
+ {{1, 9}, { 1, 18}, { 1, 36}, { 1, 6}, { 1, 12}, {-1, 6}, {-1, 12}, 0, {-1, 4}},
+ {{1, 9}, {-1, 36}, {-1, 18}, { 1, 6}, {-1, 6}, 0, 0, { 1, 4}, 0},
+ {{1, 9}, { 1, 18}, { 1, 36}, { 1, 6}, { 1, 12}, { 1, 6}, { 1, 12}, 0, { 1, 4}},
+ {{1, 9}, {-1, 36}, {-1, 18}, 0, 0, { 1, 6}, {-1, 6}, {-1, 4}, 0}
+};
+
+template <>
+constexpr Fraction invM<3,7>[7][7] = {
+ // Li, Yang et al 2016: The directions are modified for the OpenLB definition
+ {{1, 7}, 0, 0, 0, { 1, 7}, 0, 0},
+ {{1, 7}, { 1, 2}, 0, 0, {-1, 42}, { 1, 6}, 0},
+ {{1, 7}, 0, {-1, 2}, 0, {-1, 42}, {-1, 12}, { 1, 4}},
+ {{1, 7}, {-1, 2}, 0, 0, {-1, 42}, { 1, 6}, 0},
+ {{1, 7}, 0, 0, { 1, 2}, {-1, 42}, {-1, 12}, {-1, 4}},
+ {{1, 7}, 0, { 1, 2}, 0, {-1, 42}, {-1, 12}, { 1, 4}},
+ {{1, 7}, 0, 0, {-1, 2}, {-1, 42}, {-1, 12}, {-1, 4}}
+};
+
+template <>
+constexpr Fraction invM<3,19>[19][19] = {
+ {{1,19}, { -5, 399}, { 1, 21}, 0, 0, 0, 0,
+ 0, 0, 0, 0, 0, 0,
+ 0, 0, 0, 0, 0, 0},/*0*/
+ {{1,19}, {-11, 2394}, {-1, 63}, {-1, 10}, { 1, 10}, 0, 0,
+ 0, 0, { 1, 18}, {-1, 18}, 0, 0,
+ 0, 0, 0, 0, 0, 0},/*1*/
+ {{1,19}, {-11, 2394}, {-1, 63}, 0, 0, {-1, 10}, { 1, 10},
+ 0, 0, {-1, 36}, { 1, 36}, { 1, 12}, {-1, 12},
+ 0, 0, 0, 0, 0, 0},/*2*/
+ {{1,19}, {-11, 2394}, {-1, 63}, 0, 0, 0, 0,
+ { -1, 10}, { 1, 10}, {-1, 36}, { 1, 36}, {-1, 12}, { 1, 12},
+ 0, 0, 0, 0, 0, 0},/*3*/
+ {{1,19}, { 4, 1197}, { 1, 252}, {-1, 10}, {-1, 40}, {-1, 10}, {-1, 40},
+ 0, 0, { 1, 36}, { 1, 72}, { 1, 12}, { 1, 24},
+ { 1, 4}, 0, 0, {-1, 8}, { 1, 8}, 0},/*4*/
+ {{1,19}, { 4, 1197}, { 1, 252}, {-1, 10}, {-1, 40}, { 1, 10}, { 1, 40},
+ 0, 0, { 1, 36}, { 1, 72}, { 1, 12}, { 1, 24},
+ { -1, 4}, 0, 0, {-1, 8}, {-1, 8}, 0},/*5*/
+ {{1,19}, { 4, 1197}, { 1, 252}, {-1, 10}, {-1, 40}, 0, 0,
+ { -1, 10}, {-1, 40}, { 1, 36}, { 1, 72}, {-1, 12}, {-1, 24},
+ 0, 0, { 1, 4}, { 1, 8}, 0, {-1, 8}},/*6*/
+ {{1,19}, { 4, 1197}, { 1, 252}, {-1, 10}, {-1, 40}, 0, 0,
+ { 1, 10}, { 1, 40}, { 1, 36}, { 1, 72}, {-1, 12}, {-1, 24},
+ 0, 0, {-1, 4}, { 1, 8}, 0, { 1, 8}},/*7*/
+ {{1,19}, { 4, 1197}, { 1, 252}, 0, 0, {-1, 10}, {-1, 40},
+ { -1, 10}, {-1, 40}, {-1, 18}, {-1, 36}, 0, 0,
+ 0, { 1, 4}, 0, 0, {-1, 8}, { 1, 8}},/*8*/
+ {{1,19}, { 4, 1197}, { 1, 252}, 0, 0, {-1, 10}, {-1, 40},
+ { 1, 10}, { 1, 40}, {-1, 18}, {-1, 36}, 0, 0,
+ 0, {-1, 4}, 0, 0, {-1, 8}, {-1, 8}},/*9*/
+ {{1,19}, {-11, 2394}, {-1, 63}, { 1, 10}, {-1, 10}, 0, 0,
+ 0, 0, { 1, 18}, {-1, 18}, 0, 0,
+ 0, 0, 0, 0, 0, 0},/*10*/
+ {{1,19}, {-11, 2394}, {-1, 63}, 0, 0, { 1, 10}, {-1, 10},
+ 0, 0, {-1, 36}, { 1, 36}, { 1, 12}, {-1, 12},
+ 0, 0, 0, 0, 0, 0},/*11*/
+ {{1,19}, {-11, 2394}, {-1, 63}, 0, 0, 0, 0,
+ { 1, 10}, {-1, 10}, {-1, 36}, { 1, 36}, {-1, 12}, { 1, 12},
+ 0, 0, 0, 0, 0, 0},/*12*/
+ {{1,19}, { 4, 1197}, { 1, 252}, { 1, 10}, { 1, 40}, { 1, 10}, { 1, 40},
+ 0, 0, { 1, 36}, { 1, 72}, { 1, 12}, { 1, 24},
+ { 1, 4}, 0, 0, { 1, 8}, {-1, 8}, 0},/*13*/
+ {{1,19}, { 4, 1197}, { 1, 252}, { 1, 10}, { 1, 40}, {-1, 10}, {-1, 40},
+ 0, 0, { 1, 36}, { 1, 72}, { 1, 12}, { 1, 24},
+ { -1, 4}, 0, 0, { 1, 8}, { 1, 8}, 0},/*14*/
+ {{1,19}, { 4, 1197}, { 1, 252}, { 1, 10}, { 1, 40}, 0, 0,
+ { 1, 10}, { 1, 40}, { 1, 36}, { 1, 72}, {-1, 12}, {-1, 24},
+ 0, 0, { 1, 4}, {-1, 8}, 0, { 1, 8}},/*15*/
+ {{1,19}, { 4, 1197}, { 1, 252}, { 1, 10}, { 1, 40}, 0, 0,
+ { -1, 10}, {-1, 40}, { 1, 36}, { 1, 72}, {-1, 12}, {-1, 24},
+ 0, 0, {-1, 4}, {-1, 8}, 0, {-1, 8}},/*16*/
+ {{1,19}, { 4, 1197}, { 1, 252}, 0, 0, { 1, 10}, { 1, 40},
+ { 1, 10}, { 1, 40}, {-1, 18}, {-1, 36}, 0, 0,
+ 0, { 1, 4}, 0, 0, { 1, 8}, {-1, 8}},/*17*/
+ {{1,19}, { 4, 1197}, { 1, 252}, 0, 0, { 1, 10}, { 1, 40},
+ { -1, 10}, {-1, 40}, {-1, 18}, {-1, 36}, 0, 0,
+ 0, {-1, 4}, 0, 0, { 1, 8}, { 1, 8}}/*18*/
+};
+
+template <>
+constexpr Fraction s<2,5>[5] = {
+ 0, 0, 0, {3, 2}, {3, 2}
+};
+
+// s7=s8 to have a shear viscosity nu
+// and the bulk viscosity depends on s2.
+template <>
+constexpr Fraction s<2,9>[9] = {
+ 0, {11, 10}, {11, 10}, 0, {11, 10}, 0, {11, 10}, 0, 0
+};
+
+template <>
+constexpr Fraction s<3,7>[7] = {
+ // Original MRT Relaxation times
+ /*s0*/ 0, // rho (conserved)
+ /*s1*/ 0, // Function of the thermal diffusivity: S_a = 1/t_a = 1/(4*a + 1/2)
+ /*s2*/ 0, // Function of the thermal diffusivity: S_a = 1/t_a = 1/(4*a + 1/2)
+ /*s3*/ 0, // Function of the thermal diffusivity: S_a = 1/t_a = 1/(4*a + 1/2)
+ /*s4*/ {19, 10},
+ /*s5*/ {19, 10},
+ /*s6*/ {19, 10}
+};
+
+// Original MRT Relaxation times
+template <>
+constexpr Fraction s<3,19>[19] = {
+ /*s0*/ 0, // rho (conserved)
+ /*s1*/ { 119, 100},
+ /*s2*/ { 7, 5},
+ /*s3*/ 0, // rho*ux (conserved)
+ /*s4*/ { 6, 5},
+ /*s5*/ 0, // rho*uy (conserved)
+ /*s6*/ { 6, 5}, // = s4
+ /*s7*/ 0, // rho*uz (conserved)
+ /*s8*/ { 6, 5}, // = s4
+ /*s9*/ 0, //should be equal to s13, used to define nu
+ /*s10*/ { 7, 5},
+ /*s11*/ 0, // = s9,
+ /*s12*/ { 7, 5},
+ /*s13*/ 0, //should be equal to s9, used to define nu
+ /*s14*/ 0, // = s13,
+ /*s15*/ 0, // = s13,
+ /*s16*/ { 99, 50},
+ /*s17*/ { 99, 50}, // = s16,
+ /*s18*/ { 99, 50} // = s16,
+};
+
+// Use these relaxation time for higher stability
+template <>
+constexpr Fraction s_2<3,19>[19] = {
+ /*s0*/ 0, // rho (conserved)
+ /*s1*/ 1,
+ /*s2*/ 1,
+ /*s3*/ 0, // rho*ux (conserved)
+ /*s4*/ 1,
+ /*s5*/ 0, // rho*uy (conserved)
+ /*s6*/ 1, // = s4
+ /*s7*/ 0, // rho*uz (conserved)
+ /*s8*/ 1, // = s4
+ /*s9*/ 0, //should be equal to s13, used to define nu
+ /*s10*/ 1,
+ /*s11*/ 0, // = s9,
+ /*s12*/ 1,
+ /*s13*/ 0, //should be equal to s9, used to define nu
+ /*s14*/ 0, // = s13,
+ /*s15*/ 0, // = s13,
+ /*s16*/ 1,
+ /*s17*/ 1, // = s16,
+ /*s18*/ 1 // = s16,
+};
+
+template <>
+constexpr int shearIndexes<2,5> = 2;
+
+template <>
+constexpr int shearIndexes<2,9> = 2;
+
+template <>
+constexpr int shearIndexes<3,7> = 3;
+
+template <>
+constexpr int shearIndexes<3,19> = 5;
+
+template <>
+constexpr int shearViscIndexes<2,5>[shearIndexes<2,5>] = { 1, 2 };
+
+template <>
+constexpr int shearViscIndexes<2,9>[shearIndexes<2,9>] = { 7, 8 };
+
+template <>
+constexpr int shearViscIndexes<3,7>[shearIndexes<3,7>] = { 1, 2, 3 };
+
+template <>
+constexpr int shearViscIndexes<3,19>[shearIndexes<3,19>] = { 9, 11, 13, 14, 15 };
+
+template <>
+constexpr int bulkViscIndex<2,9> = 2;
+
+template <>
+constexpr int bulkViscIndex<3,19> = 1;
+
+} // mrt_data
+
+template <typename T, unsigned D, unsigned Q>
+constexpr T t(unsigned iPop, tag::MRT)
+{
+ return data::t<D,Q>[iPop].template as<T>();
+}
+
+template <typename T, unsigned D, unsigned Q>
+constexpr T m(unsigned iPop, unsigned jPop, tag::MRT)
+{
+ return mrt_data::M<D,Q>[iPop][jPop].template as<T>();
+}
+
+template <typename T, typename DESCRIPTOR>
+constexpr T m(unsigned iPop, unsigned jPop)
+{
+ return m<T, DESCRIPTOR::d, DESCRIPTOR::q>(iPop, jPop, typename DESCRIPTOR::category_tag());
+}
+
+template <typename T, unsigned D, unsigned Q>
+constexpr T invM(unsigned iPop, unsigned jPop, tag::MRT)
+{
+ return mrt_data::invM<D,Q>[iPop][jPop].template as<T>();
+}
+
+template <typename T, typename DESCRIPTOR>
+constexpr T invM(unsigned iPop, unsigned jPop)
+{
+ return invM<T, DESCRIPTOR::d, DESCRIPTOR::q>(iPop, jPop, typename DESCRIPTOR::category_tag());
+}
+
+template <typename T, unsigned D, unsigned Q>
+constexpr T s(unsigned iPop, tag::MRT)
+{
+ return mrt_data::s<D,Q>[iPop].template as<T>();
+}
+
+template <typename T, typename DESCRIPTOR>
+constexpr T s(unsigned iPop)
+{
+ return s<T, DESCRIPTOR::d, DESCRIPTOR::q>(iPop, typename DESCRIPTOR::category_tag());
+}
+
+template <typename T, unsigned D, unsigned Q>
+constexpr T s_2(unsigned iPop, tag::MRT)
+{
+ return mrt_data::s_2<D,Q>[iPop].template as<T>();
+}
+
+template <typename T, typename DESCRIPTOR>
+constexpr T s_2(unsigned iPop)
+{
+ return s_2<T, DESCRIPTOR::d, DESCRIPTOR::q>(iPop, typename DESCRIPTOR::category_tag());
+}
+
+template <unsigned D, unsigned Q>
+constexpr int shearIndexes(tag::MRT)
+{
+ return mrt_data::shearIndexes<D,Q>;
+}
+
+template <typename DESCRIPTOR>
+constexpr int shearIndexes()
+{
+ return shearIndexes<DESCRIPTOR::d, DESCRIPTOR::q>(typename DESCRIPTOR::category_tag());
+}
+
+template <unsigned D, unsigned Q>
+constexpr int shearViscIndexes(unsigned iPop, tag::MRT)
+{
+ return mrt_data::shearViscIndexes<D,Q>[iPop];
+}
+
+template <typename DESCRIPTOR>
+constexpr int shearViscIndexes(unsigned iPop)
+{
+ return shearViscIndexes<DESCRIPTOR::d, DESCRIPTOR::q>(iPop, typename DESCRIPTOR::category_tag());
+}
+
+template <unsigned D, unsigned Q>
+constexpr int bulkViscIndex(tag::MRT)
+{
+ return mrt_data::bulkViscIndex<D,Q>;
+}
+
+template <typename DESCRIPTOR>
+constexpr int bulkViscIndex()
+{
+ return bulkViscIndex<DESCRIPTOR::d, DESCRIPTOR::q>(typename DESCRIPTOR::category_tag());
+}
+
+} // namespace descriptors
+
+} // namespace olb
+
+#endif