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1 | // -*- mode: C++; tab-width: 4; indent-tabs-mode: nil; c-basic-offset: 4 -*- | ||
2 | // vi: set et ts=4 sw=4 sts=4: | ||
3 | // | ||
4 | // SPDX-FileCopyrightInfo: Copyright © DuMux Project contributors, see AUTHORS.md in root folder | ||
5 | // SPDX-License-Identifier: GPL-3.0-or-later | ||
6 | // | ||
7 | |||
8 | // ## The main file (`main.cc`) | ||
9 | // [[content]] | ||
10 | // | ||
11 | // ### Included header files | ||
12 | // [[details]] includes | ||
13 | // [[exclude]] | ||
14 | // Some generic includes. | ||
15 | #include <config.h> | ||
16 | #include <iostream> | ||
17 | #include <dune/common/timer.hh> | ||
18 | #include <dumux/common/dumuxmessage.hh> | ||
19 | // [[/exclude]] | ||
20 | |||
21 | // These is DUNE helper class related to parallel computation | ||
22 | #include <dune/common/parallel/mpihelper.hh> | ||
23 | |||
24 | // The following headers include functionality related to property definition or retrieval, as well as | ||
25 | // the retrieval of input parameters specified in the input file or via the command line. | ||
26 | #include <dumux/common/parameters.hh> | ||
27 | #include <dumux/common/properties.hh> | ||
28 | #include <dumux/common/initialize.hh> | ||
29 | |||
30 | // The following files contain the multi-domain Newton solver, the available linear solver backends and the assembler for the linear | ||
31 | // systems arising from the staggered-grid discretization. | ||
32 | #include <dumux/linear/istlsolvers.hh> | ||
33 | #include <dumux/linear/linearalgebratraits.hh> | ||
34 | #include <dumux/linear/linearsolvertraits.hh> | ||
35 | #include <dumux/multidomain/fvassembler.hh> | ||
36 | #include <dumux/multidomain/traits.hh> | ||
37 | #include <dumux/multidomain/newtonsolver.hh> | ||
38 | |||
39 | // The gridmanager constructs a grid from the information in the input or grid file. | ||
40 | // Many different Dune grid implementations are supported, of which a list can be found | ||
41 | // in `gridmanager.hh`. | ||
42 | #include <dumux/io/grid/gridmanager_yasp.hh> | ||
43 | |||
44 | // This class contains functionality for VTK output for models using the staggered finite volume scheme. | ||
45 | #include <dumux/io/vtkoutputmodule.hh> | ||
46 | #include <dumux/freeflow/navierstokes/velocityoutput.hh> | ||
47 | |||
48 | // We include the problem header used for this simulation. | ||
49 | #include "properties.hh" | ||
50 | // [[/details]] | ||
51 | |||
52 | // The following function writes the velocities and coordinates at x = 0.5 and y = 0.5 into a log file. | ||
53 | // [[codeblock]] | ||
54 | template<class Problem, class SolutionVector> | ||
55 | 2 | void writeSteadyVelocityAndCoordinates(const Problem& problem, const SolutionVector& sol) | |
56 | { | ||
57 | 2 | const auto& gridGeometry = problem.gridGeometry(); | |
58 |
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8 | std::ofstream logFilevx(problem.name() + "_vx.log"), logFilevy(problem.name() + "_vy.log"); |
59 |
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2 | logFilevx << "y vx\n"; |
60 |
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2 | logFilevy << "x vy\n"; |
61 | |||
62 | static constexpr double eps_ = 1.0e-7; | ||
63 |
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6 | std::vector<int> dofHandled(gridGeometry.numDofs(), false); |
64 |
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16390 | for (const auto& element : elements(gridGeometry.gridView())) |
65 | { | ||
66 | 8192 | auto fvGeometry = localView(gridGeometry); | |
67 | 8192 | fvGeometry.bind(element); | |
68 |
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40960 | for (const auto& scv : scvs(fvGeometry)) |
69 | { | ||
70 |
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65536 | if (dofHandled[scv.dofIndex()]) |
71 | continue; | ||
72 | |||
73 |
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16640 | if (!scv.boundary()) |
74 | { | ||
75 |
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16128 | const auto& globalPos = scv.dofPosition(); |
76 |
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16128 | const auto velocity = sol[scv.dofIndex()][0]; |
77 | 16128 | dofHandled[scv.dofIndex()] = true; | |
78 | |||
79 |
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48384 | if (std::abs(globalPos[0]-0.5) < eps_) |
80 |
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384 | logFilevx << globalPos[1] << " " << velocity << "\n"; |
81 |
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48000 | else if (std::abs(globalPos[1]-0.5) < eps_) |
82 |
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384 | logFilevy << globalPos[0] << " " << velocity << "\n"; |
83 | } | ||
84 | } | ||
85 | } | ||
86 | 2 | } | |
87 | // [[/codeblock]] | ||
88 | |||
89 | // ### The main function | ||
90 | // We will now discuss the main program flow implemented within the `main` function. | ||
91 | // At the beginning of each program using Dune, an instance of `Dune::MPIHelper` has to | ||
92 | // be created. Moreover, we parse the run-time arguments from the command line and the | ||
93 | // input file: | ||
94 | // [[codeblock]] | ||
95 | 2 | int main(int argc, char** argv) | |
96 | { | ||
97 | 2 | using namespace Dumux; | |
98 | |||
99 | // maybe initialize MPI and/or multithreading backend | ||
100 | 2 | Dumux::initialize(argc, argv); | |
101 | 2 | const auto& mpiHelper = Dune::MPIHelper::instance(); | |
102 | |||
103 | // parse command line arguments and input file | ||
104 |
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12 | Parameters::init(argc, argv); |
105 | // [[/codeblock]] | ||
106 | |||
107 | // We define a convenience alias for the type tags of the problems. The type | ||
108 | // tag contains all the properties that are needed to define the model and the problem | ||
109 | // setup. Throughout the main file, we will obtain types defined each type tag | ||
110 | // using the property system, i.e. with `GetPropType`. | ||
111 | 2 | using MomentumTypeTag = Properties::TTag::LidDrivenCavityExampleMomentum; | |
112 | 2 | using MassTypeTag = Properties::TTag::LidDrivenCavityExampleMass; | |
113 | |||
114 | // #### Step 1: Create the grid | ||
115 | // The `GridManager` class creates the grid from information given in the input file. | ||
116 | // This can either be a grid file, or in the case of structured grids, one can specify the coordinates | ||
117 | // of the corners of the grid and the number of cells to be used to discretize each spatial direction. | ||
118 | // [[codeblock]] | ||
119 | 4 | GridManager<GetPropType<MomentumTypeTag, Properties::Grid>> gridManager; | |
120 |
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4 | gridManager.init(); |
121 | |||
122 | // We compute on the leaf grid view. | ||
123 |
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2 | const auto& leafGridView = gridManager.grid().leafGridView(); |
124 | // [[/codeblock]] | ||
125 | |||
126 | // #### Step 2: Setting up and solving the problem | ||
127 | // First, a finite volume grid geometry is constructed from the grid that was created above. | ||
128 | // This builds the sub-control volumes (scv) and sub-control volume faces (scvf) for each element | ||
129 | // of the grid partition. | ||
130 | // This is done for both the momentum and mass grid geometries | ||
131 | 2 | using MomentumGridGeometry = GetPropType<MomentumTypeTag, Properties::GridGeometry>; | |
132 |
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4 | auto momentumGridGeometry = std::make_shared<MomentumGridGeometry>(leafGridView); |
133 | 2 | using MassGridGeometry = GetPropType<MassTypeTag, Properties::GridGeometry>; | |
134 |
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4 | auto massGridGeometry = std::make_shared<MassGridGeometry>(leafGridView); |
135 | |||
136 | // We introduce the multidomain coupling manager, which will couple the mass and the momentum problems | ||
137 | // We can obtain the type from either the `MomentumTypeTag` or the `MassTypeTag` because they are mutually coupled with the same manager | ||
138 | 2 | using CouplingManager = GetPropType<MomentumTypeTag, Properties::CouplingManager>; | |
139 |
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4 | auto couplingManager = std::make_shared<CouplingManager>(); |
140 | |||
141 | // We now instantiate the problems, in which we define the boundary and initial conditions. | ||
142 | 2 | using MomentumProblem = GetPropType<MomentumTypeTag, Properties::Problem>; | |
143 |
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4 | auto momentumProblem = std::make_shared<MomentumProblem>(momentumGridGeometry, couplingManager); |
144 | 2 | using MassProblem = GetPropType<MassTypeTag, Properties::Problem>; | |
145 |
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4 | auto massProblem = std::make_shared<MassProblem>(massGridGeometry, couplingManager); |
146 | |||
147 | // We set a solution vector which consist of two parts: one part (indexed by `massIdx`) | ||
148 | // is for the pressure degrees of freedom (`dofs`) living in grid cell centers. Another part | ||
149 | // (indexed by `momentumIdx`) is for degrees of freedom defining the normal velocities on grid cell faces. | ||
150 | // We initialize the solution vector by what was defined as the initial solution of the the problem. | ||
151 | 2 | constexpr auto momentumIdx = CouplingManager::freeFlowMomentumIndex; | |
152 | 2 | constexpr auto massIdx = CouplingManager::freeFlowMassIndex; | |
153 | 2 | using Traits = MultiDomainTraits<MomentumTypeTag, MassTypeTag>; | |
154 | 2 | using SolutionVector = typename Traits::SolutionVector; | |
155 |
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4 | SolutionVector x; |
156 |
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6 | momentumProblem->applyInitialSolution(x[momentumIdx]); |
157 |
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6 | massProblem->applyInitialSolution(x[massIdx]); |
158 |
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4 | auto xOld = x; |
159 | |||
160 | // We use the initial solution vector to create the `gridVariables`. | ||
161 | // The grid variables are used store variables (primary and secondary variables) on sub-control volumes and faces (volume and flux variables). | ||
162 | 2 | using MomentumGridVariables = GetPropType<MomentumTypeTag, Properties::GridVariables>; | |
163 |
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4 | auto momentumGridVariables = std::make_shared<MomentumGridVariables>(momentumProblem, momentumGridGeometry); |
164 | 2 | using MassGridVariables = GetPropType<MassTypeTag, Properties::GridVariables>; | |
165 |
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4 | auto massGridVariables = std::make_shared<MassGridVariables>(massProblem, massGridGeometry); |
166 | |||
167 | // using the problems and the grid variables, the coupling manager and the grid variables are initialized with the initial solution. | ||
168 | // The grid variables have to be initialized _after_ the coupling manager. | ||
169 | // This is because they require the correct coupling context between the mass and momentum model to be initialized. | ||
170 |
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10 | couplingManager->init(momentumProblem, massProblem, std::make_tuple(momentumGridVariables, massGridVariables), x, xOld); |
171 |
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6 | momentumGridVariables->init(x[momentumIdx]); |
172 |
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6 | massGridVariables->init(x[massIdx]); |
173 | |||
174 | // We get some time loop parameters from the input file | ||
175 | // and instantiate the time loop | ||
176 | 2 | using Scalar = typename Traits::Scalar; | |
177 |
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2 | const auto tEnd = getParam<Scalar>("TimeLoop.TEnd"); |
178 |
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2 | const auto maxDt = getParam<Scalar>("TimeLoop.MaxTimeStepSize"); |
179 |
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2 | const auto dt = getParam<Scalar>("TimeLoop.DtInitial"); |
180 | |||
181 |
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4 | auto timeLoop = std::make_shared<TimeLoop<Scalar>>(0, dt, tEnd); |
182 |
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4 | timeLoop->setMaxTimeStepSize(maxDt); |
183 | |||
184 | // We then initialize the predefined model-specific output vtk output. | ||
185 | 2 | using IOFields = GetPropType<MassTypeTag, Properties::IOFields>; | |
186 |
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8 | VtkOutputModule vtkWriter(*massGridVariables, x[massIdx], massProblem->name()); |
187 |
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2 | IOFields::initOutputModule(vtkWriter); // Add model specific output fields |
188 |
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4 | vtkWriter.addVelocityOutput(std::make_shared<NavierStokesVelocityOutput<MassGridVariables>>()); |
189 |
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2 | vtkWriter.write(0.0); |
190 | |||
191 | // To solve the non-linear problem at hand, we use the `NewtonSolver`, | ||
192 | // which we have to tell how to assemble and solve the system in each | ||
193 | // iteration. Here, we use the direct linear solver UMFPack. | ||
194 | 2 | using Assembler = MultiDomainFVAssembler<Traits, CouplingManager, DiffMethod::numeric>; | |
195 | 2 | auto assembler = std::make_shared<Assembler>(std::make_tuple(momentumProblem, massProblem), | |
196 | 4 | std::make_tuple(momentumGridGeometry, massGridGeometry), | |
197 | 4 | std::make_tuple(momentumGridVariables, massGridVariables), | |
198 |
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4 | couplingManager, timeLoop, xOld); |
199 | // the linear solver | ||
200 | 2 | using LinearSolver = Dumux::UMFPackIstlSolver<SeqLinearSolverTraits, LinearAlgebraTraitsFromAssembler<Assembler>>; | |
201 |
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4 | auto linearSolver = std::make_shared<LinearSolver>(); |
202 | |||
203 | // the non-linear solver | ||
204 | 2 | using NewtonSolver = MultiDomainNewtonSolver<Assembler, LinearSolver, CouplingManager>; | |
205 |
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12 | NewtonSolver nonLinearSolver(assembler, linearSolver, couplingManager); |
206 | |||
207 | // ##### The time loop | ||
208 | // In each time step, we solve the non-linear system of equations, write | ||
209 | // the current solution into VTK files and prepare for the next time step. | ||
210 | // [[codeblock]] | ||
211 |
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4 | timeLoop->start(); do |
212 | { | ||
213 | // We solve the non-linear system with time step control. | ||
214 |
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20 | nonLinearSolver.solve(x, *timeLoop); |
215 | |||
216 | // We make the new solution the old solution. | ||
217 |
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10 | xOld = x; |
218 |
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20 | massGridVariables->advanceTimeStep(); |
219 |
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20 | momentumGridVariables->advanceTimeStep(); |
220 | |||
221 | // We advance to the time loop to the next step. | ||
222 |
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20 | timeLoop->advanceTimeStep(); |
223 | |||
224 | // We write vtk output for each time step. | ||
225 |
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30 | vtkWriter.write(timeLoop->time()); |
226 | |||
227 | // We report statistics of this time step. | ||
228 |
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20 | timeLoop->reportTimeStep(); |
229 | |||
230 | // We set a new dt as suggested by the newton solver for the next time step. | ||
231 |
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50 | timeLoop->setTimeStepSize(nonLinearSolver.suggestTimeStepSize(timeLoop->timeStepSize())); |
232 | |||
233 |
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20 | } while (!timeLoop->finished()); |
234 | // [[/codeblock]] | ||
235 | |||
236 | // We write the velocities and coordinates at x = 0.5 and y = 0.5 into a file. | ||
237 |
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6 | writeSteadyVelocityAndCoordinates(*momentumProblem, x[momentumIdx]); |
238 | |||
239 | // The following piece of code prints a final status report of the time loop | ||
240 | // before the program is terminated. | ||
241 | // [[codeblock]] | ||
242 |
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4 | timeLoop->finalize(leafGridView.comm()); |
243 | |||
244 | // print used and unused parameters | ||
245 |
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4 | if (mpiHelper.rank() == 0) |
246 |
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2 | Parameters::print(); |
247 | |||
248 | 2 | return 0; | |
249 | } // end main | ||
250 | // [[/codeblock]] | ||
251 | // [[/content]] | ||
252 |