GCC Code Coverage Report


Directory: ../../../builds/dumux-repositories/
File: /builds/dumux-repositories/dumux/examples/cahn_hilliard/main.cc
Date: 2024-05-04 19:09:25
Exec Total Coverage
Lines: 74 82 90.2%
Functions: 4 10 40.0%
Branches: 136 324 42.0%

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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 // # Cahn-Hilliard equation main program
9 //
10 // The file [`main.cc`](main.cc) contains the problem class `CahnHilliardTestProblem`,
11 // properties and traits specific to the test case as well as the `main` function.
12 // The setup consists of four steps:
13 // 1. Define the problem setting boundary conditions and the diffusion coefficient
14 // 2. Configure the property system reusing the model defined in Part 1
15 // 3. Define a function for setting the random initial condition
16 // 4. The main program defining all steps of the program
17 //
18 // __Table of contents__
19 //
20 // [TOC]
21 //
22 // We start in `main.cc` with the necessary header includes:
23 // [[details]] includes
24 #include <config.h>
25 #include <type_traits>
26 #include <random>
27
28 #include <dumux/common/initialize.hh>
29 #include <dumux/common/properties.hh>
30 #include <dumux/common/parameters.hh>
31 #include <dumux/common/numeqvector.hh>
32 #include <dumux/common/boundarytypes.hh>
33 #include <dumux/common/fvproblem.hh>
34
35 #include <dumux/discretization/box.hh>
36 #include <dumux/linear/linearsolvertraits.hh>
37 #include <dumux/linear/linearalgebratraits.hh>
38 #include <dumux/linear/istlsolvers.hh>
39 #include <dumux/nonlinear/newtonsolver.hh>
40 #include <dumux/assembly/fvassembler.hh>
41
42 #include <dune/grid/yaspgrid.hh>
43 #include <dumux/io/chrono.hh>
44 #include <dumux/io/vtkoutputmodule.hh>
45 #include <dumux/io/grid/gridmanager_yasp.hh>
46
47 #include "model.hh"
48 // [[/details]]
49
50 //
51 // ## 1. The problem class
52 //
53 // The problem class implements boundary conditions and the source term.
54 // It also provides an interface that is used by the local residual (see Part 1) to obtain
55 // the mobility and surface tension. The values are read from the parameter configuration tree.
56 // [[content]]
57 namespace Dumux {
58 template<class TypeTag>
59 3 class CahnHilliardTestProblem : public FVProblem<TypeTag>
60 {
61 // [[details]] boilerplate code
62 using ParentType = FVProblem<TypeTag>;
63 using GridGeometry = GetPropType<TypeTag, Properties::GridGeometry>;
64 using FVElementGeometry = typename GridGeometry::LocalView;
65 using SubControlVolume = typename GridGeometry::SubControlVolume;
66 using GridView = typename GetPropType<TypeTag, Properties::GridGeometry>::GridView;
67 using Element = typename GridView::template Codim<0>::Entity;
68 using GlobalPosition = typename Element::Geometry::GlobalCoordinate;
69
70 using Scalar = GetPropType<TypeTag, Properties::Scalar>;
71 using PrimaryVariables = GetPropType<TypeTag, Properties::PrimaryVariables>;
72 using NumEqVector = Dumux::NumEqVector<PrimaryVariables>;
73 using BoundaryTypes = Dumux::BoundaryTypes<GetPropType<TypeTag, Properties::ModelTraits>::numEq()>;
74 using Indices = typename GetPropType<TypeTag, Properties::ModelTraits>::Indices;
75 // [[/details]]
76 // In the constructor, we read the parameter constants from the
77 // parameter tree (which is initialized with the content of `params.input`).
78 public:
79 3 CahnHilliardTestProblem(std::shared_ptr<const GridGeometry> gridGeometry)
80
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9 : ParentType(gridGeometry)
81 {
82
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3 mobility_ = getParam<Scalar>("Problem.Mobility");
83
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3 surfaceTension_ = getParam<Scalar>("Problem.SurfaceTension");
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3 energyScale_ = getParam<Scalar>("Problem.EnergyScale");
85 3 }
86
87 // In the `source` function, we implement the derivative of the free energy.
88 // This demonstrates how parts of the local residual can be split into model specific
89 // parts (see `CahnHilliardModelLocalResidual`) and parts that might change from scenario to scenario.
90 template<class ElementVolumeVariables>
91 3672800 NumEqVector source(const Element &element,
92 const FVElementGeometry& fvGeometry,
93 const ElementVolumeVariables& elemVolVars,
94 const SubControlVolume &scv) const
95 {
96 3672800 NumEqVector values(0.0);
97 11018400 const auto& c = elemVolVars[scv].concentration();
98 7345600 values[Indices::chemicalPotentialEqIdx] = -energyScale_*2.0*c*(2.0*c*c - 3*c + 1);
99 3672800 return values;
100 }
101
102 // We choose boundary flux (or Neumann) conditions for all equations on the entire boundary,
103 // while specifying zero flux for both equations.
104 // [[codeblock]]
105 BoundaryTypes boundaryTypesAtPos(const GlobalPosition& globalPos) const
106 {
107 72560 BoundaryTypes values;
108
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72560 values.setAllNeumann();
109 return values;
110 }
111
112 NumEqVector neumannAtPos(const GlobalPosition& globalPos) const
113 1335104 { return { 0.0, 0.0 }; }
114 // [[/codeblock]]
115
116 // The parameters interfaces are used in the local residual (see Part 1).
117 // We can name this interface however we want as long as we adapt the calling site
118 // in the `CahnHilliardModelLocalResidual` class in `model.hh`.
119 // [[codeblock]]
120 Scalar mobility() const
121 { return mobility_; }
122
123 Scalar surfaceTension() const
124 { return surfaceTension_; }
125
126 private:
127 Scalar mobility_;
128 Scalar surfaceTension_;
129 Scalar energyScale_;
130 };
131 } // end namespace Dumux
132 // [[/codeblock]]
133 // [[/content]]
134
135 //
136 // ## 2. Property tag and specializations
137 //
138 // We create a new tag `DiffusionTest` that inherits all properties
139 // specialized for the tag `DiffusionModel` (we created this in Part 1)
140 // and the tag `BoxModel` which provides types relevant for the spatial
141 // discretization scheme (see [dumux/discretization/box.hh](https://git.iws.uni-stuttgart.de/dumux-repositories/dumux/-/blob/master/dumux/discretization/box.hh)).
142 //
143 // [[content]]
144 namespace Dumux::Properties::TTag {
145 struct CahnHilliardTest
146 {
147 using InheritsFrom = std::tuple<CahnHilliardModel, BoxModel>;
148
149 using Grid = Dune::YaspGrid<2>;
150
151 template<class TypeTag>
152 using Problem = CahnHilliardTestProblem<TypeTag>;
153
154 using EnableGridGeometryCache = std::true_type;
155 using EnableGridVolumeVariablesCache = std::true_type;
156 using EnableGridFluxVariablesCache = std::true_type;
157 };
158 } // end namespace Dumux::Properties
159 // [[/content]]
160 //
161 // ## 3. Creating the initial solution
162 //
163 // To initialize with a random field in parallel, where each processor
164 // creates its own random number sequence, we need to communicate the
165 // resulting values on the processor border and overlap.
166 // See [Diffusion equation example](https://git.iws.uni-stuttgart.de/dumux-repositories/dumux/-/blob/master/examples/diffusion/docs/main.md).
167 // for details. Here in addition, we need to provide a custom scatter operation
168 // that handles vector types. We only need to communicate the first entry (concentration).
169 //
170 // [[content]]
171 // [[codeblock]]
172 // functor for data communication with MPI
173 struct MinScatter
174 {
175 template<class A, class B>
176 static void apply(A& a, const B& b)
177 { a[0] = std::min(a[0], b[0]); }
178 };
179
180 // create the random initial solution
181 template<class SolutionVector, class GridGeometry>
182 3 SolutionVector createInitialSolution(const GridGeometry& gg)
183 {
184 6 SolutionVector sol(gg.numDofs());
185
186 // Generate random number and add processor offset
187 // For sequential runs `rank` always returns `0`.
188 3 std::mt19937 gen(0); // seed is 0 for deterministic results
189 3 std::uniform_real_distribution<> dis(0.0, 1.0);
190
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300 for (int n = 0; n < sol.size(); ++n)
191 {
192
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297 sol[n][0] = 0.42 + 0.02*(0.5-dis(gen)) + gg.gridView().comm().rank();
193 594 sol[n][1] = 0.0;
194 }
195
196 // We take the value of the processor with the minimum rank
197 // and subtract the rank offset
198
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6 if (gg.gridView().comm().size() > 1)
199 {
200 Dumux::VectorCommDataHandle<
201 typename GridGeometry::VertexMapper,
202 SolutionVector,
203 GridGeometry::GridView::dimension,
204 MinScatter
205
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4 > minHandle(gg.vertexMapper(), sol);
206
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4 gg.gridView().communicate(minHandle, Dune::All_All_Interface, Dune::ForwardCommunication);
207
208 // Remove processor offset
209
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178 for (int n = 0; n < sol.size(); ++n)
210 704 sol[n][0] -= std::floor(sol[n][0]);
211 }
212 3 return sol;
213 }
214 // [[/codeblock]]
215 // [[/content]]
216 //
217 // ## 4. The main program
218 //
219 // The `main` function sets up the simulation framework, initializes runtime parameters,
220 // creates the grid and storage vectors
221 // for the variables, primary and secondary. It specifies and constructs and assembler, which
222 // assembles the discretized residual and system matrix (Jacobian of the model residual), as well as
223 // a linear solver. A Newton method is used to solve the nonlinear equations where in each Newton iteration
224 // the Jacobian and the residual needs to be reassembled and the resulting linear system is solved.
225 // The time loop controls the time stepping. Here, we let the Newton solver suggest an adaption of
226 // the time step size based on the convergence history of the nonlinear solver.
227 //
228 // [[content]]
229 3 int main(int argc, char** argv)
230 {
231 3 using namespace Dumux;
232
233 // We initialize MPI and/or multithreading backend. When not running
234 // in parallel the MPI setup is skipped.
235 3 Dumux::initialize(argc, argv);
236
237 // Then we initialize parameter tree.
238
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12 Parameters::init(argc, argv);
239
240 // We create an alias for the type tag for this problem
241 // and extract type information through properties.
242 3 using TypeTag = Properties::TTag::CahnHilliardTest;
243
244 3 using Scalar = GetPropType<TypeTag, Properties::Scalar>;
245 3 using Grid = GetPropType<TypeTag, Properties::Grid>;
246 3 using GridGeometry = GetPropType<TypeTag, Properties::GridGeometry>;
247 3 using Problem = GetPropType<TypeTag, Properties::Problem>;
248 3 using SolutionVector = GetPropType<TypeTag, Properties::SolutionVector>;
249 3 using GridVariables = GetPropType<TypeTag, Properties::GridVariables>;
250
251 // We initialize the grid, grid geometry, problem, solution vector, and grid variables.
252 6 GridManager<Grid> gridManager;
253
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6 gridManager.init();
254
255
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6 auto gridGeometry = std::make_shared<GridGeometry>(gridManager.grid().leafGridView());
256
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6 auto problem = std::make_shared<Problem>(gridGeometry);
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9 auto sol = createInitialSolution<SolutionVector>(*gridGeometry);
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6 auto gridVariables = std::make_shared<GridVariables>(problem, gridGeometry);
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6 gridVariables->init(sol);
260
261 // We initialize the VTK output module and write out the initial concentration and chemical potential
262
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12 VtkOutputModule<GridVariables, SolutionVector> vtkWriter(*gridVariables, sol, problem->name());
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9 vtkWriter.addVolumeVariable([](const auto& vv){ return vv.concentration(); }, "c");
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9 vtkWriter.addVolumeVariable([](const auto& vv){ return vv.chemicalPotential(); }, "mu");
265
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3 vtkWriter.write(0.0);
266
267 // We instantiate time loop using start and end time as well as
268 // the time step size from the parameter tree (`params.input`)
269 3 auto timeLoop = std::make_shared<CheckPointTimeLoop<Scalar>>(
270
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3 Chrono::toSeconds(getParam("TimeLoop.TStart", "0")),
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6 Chrono::toSeconds(getParam("TimeLoop.InitialTimeStepSize")),
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6 Chrono::toSeconds(getParam("TimeLoop.TEnd"))
273
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6 );
274
275 // We set the maximum time step size allowed in the adaptive time stepping scheme.
276
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6 timeLoop->setMaxTimeStepSize(Chrono::toSeconds(getParam("TimeLoop.MaxTimeStepSize")));
277
278 // Next, we choose the type of assembler, linear solver and PDE solver
279 // and construct instances of these classes.
280 3 using Assembler = FVAssembler<TypeTag, DiffMethod::numeric>;
281 3 using LinearSolver = SSORBiCGSTABIstlSolver<LinearSolverTraits<GridGeometry>, LinearAlgebraTraitsFromAssembler<Assembler>>;
282 3 using Solver = Dumux::NewtonSolver<Assembler, LinearSolver>;
283
284
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6 auto oldSol = sol;
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6 auto assembler = std::make_shared<Assembler>(problem, gridGeometry, gridVariables, timeLoop, oldSol);
286
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18 auto linearSolver = std::make_shared<LinearSolver>(gridGeometry->gridView(), gridGeometry->dofMapper());
287
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15 Solver solver(assembler, linearSolver);
288
289 // The time loop is where most of the actual computations happen.
290 // We assemble and solve the linear system of equations, update the solution,
291 // write the solution to a VTK file and continue until the we reach the
292 // final simulation time.
293 //
294 // [[codeblock]]
295
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6 timeLoop->start(); do
296 {
297 // Assemble & solve
298 // Passing the time loop enables the solver to repeat the time step
299 // with a reduced time step size if the Newton solver does not converge.
300
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612 solver.solve(sol, *timeLoop);
301
302 // make the new solution the old solution
303
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306 oldSol = sol;
304
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612 gridVariables->advanceTimeStep();
305
306 // advance to the time loop to the next step
307
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612 timeLoop->advanceTimeStep();
308
309 // write VTK output (concentration field and chemical potential)
310
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918 vtkWriter.write(timeLoop->time());
311
312 // report statistics of this time step
313
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612 timeLoop->reportTimeStep();
314
315 // set new dt as suggested by the Newton solver
316
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1530 timeLoop->setTimeStepSize(solver.suggestTimeStepSize(timeLoop->timeStepSize()));
317
318
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612 } while (!timeLoop->finished());
319
320 // print the final report
321
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12 timeLoop->finalize(gridGeometry->gridView().comm());
322 3 return 0;
323 }
324 // [[/codeblock]]
325 // [[/content]]
326