code is now included using \snippet. Apparently this looks better with the new Doxygen version. The HTML_EXTRA_STYLESHEET is now used rather then the HTML_STYLESHEET in order to include used-defined styles for the same reason
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@@ -24,7 +24,7 @@
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/// \f${\bf u}\f$ denotes the velocity and \f$p\f$ the pressure. The permeability tensor is
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/// given by \f$K\f$ and \f$\mu\f$ denotes the viscosity.
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///
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/// We solve the flow equations for a cartesian grid and we set the source term
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/// We solve the flow equations for a Cartesian grid and we set the source term
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/// \f$q\f$ be zero except at the left-lower and right-upper corner, where it is equal
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/// with opposite sign (inflow equal to outflow).
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@@ -49,28 +49,33 @@
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#include <opm/core/simulator/WellState.hpp>
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/// \page tutorial2
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/// \section commentedcode2 Program walkthrough.
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/// \code
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/// \section commentedcode2 Program walk-through.
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///
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int main()
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{
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/// \endcode
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/// \page tutorial2
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/// We construct a cartesian grid
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/// \code
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/// We construct a Cartesian grid
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/// \snippet tutorial2.cpp cartesian grid
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/// \internal [cartesian grid]
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int dim = 3;
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int nx = 40;
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int ny = 40;
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int nz = 1;
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Opm::GridManager grid(nx, ny, nz);
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/// \endcode
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/// \internal [cartesian grid]
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/// \endinternal
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/// \page tutorial2
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/// \details We access the unstructured grid through
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/// the pointer given by \c grid.c_grid(). For more details on the
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/// UnstructuredGrid data structure, see grid.h.
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/// \code
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/// \snippet tutorial2.cpp access grid
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/// \internal [access grid]
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int num_cells = grid.c_grid()->number_of_cells;
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int num_faces = grid.c_grid()->number_of_faces;
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/// \endcode
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/// \internal [access grid]
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/// endinternal
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/// \page tutorial2
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@@ -80,90 +85,107 @@ int main()
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/// The <opm/core/utility/Units.hpp> header contains support
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/// for common units and prefixes, in the namespaces Opm::unit
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/// and Opm::prefix.
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/// \code
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/// \snippet tutorial2.cpp fluid
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/// \internal [fluid]
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using namespace Opm::unit;
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using namespace Opm::prefix;
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int num_phases = 1;
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std::vector<double> mu(num_phases, 1.0*centi*Poise);
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std::vector<double> rho(num_phases, 1000.0*kilogram/cubic(meter));
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/// \endcode
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/// \internal [fluid]
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/// \endinternal
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/// \page tutorial2
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/// \details
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/// We define a permeability equal to 100 mD.
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/// \code
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/// \snippet tutorial2.cpp perm
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/// \internal [perm]
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double k = 100.0*milli*darcy;
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/// \endcode
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/// \page tutorial2
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/// \details
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/// \internal [perm]
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/// \endinternal
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/// \page tutorial2
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/// \details
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/// We set up a simple property object for a single-phase situation.
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/// \code
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/// \snippet tutorial2.cpp single-phase property
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/// \internal [single-phase property]
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Opm::IncompPropertiesBasic props(1, Opm::SaturationPropsBasic::Constant, rho,
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mu, 1.0, k, dim, num_cells);
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/// \endcode
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/// \internal [single-phase property]
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/// /endinternal
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/// \page tutorial2
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/// \details
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/// We take UMFPACK as the linear solver for the pressure solver
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/// (this library has therefore to be installed).
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/// \code
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/// \snippet tutorial2.cpp linsolver
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/// \internal [linsolver]
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Opm::LinearSolverUmfpack linsolver;
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/// \endcode
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/// \page tutorial2
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/// \internal [linsolver]
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/// \endinternal
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/// \endcode
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/// \page tutorial2
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/// We define the source term.
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/// \code
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/// \snippet tutorial2.cpp source
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/// \internal [source]
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std::vector<double> src(num_cells, 0.0);
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src[0] = 100.;
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src[num_cells-1] = -100.;
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/// \endcode
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/// \internal [source]
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/// \endinternal
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/// \page tutorial2
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/// \details We set up the boundary conditions.
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/// By default, we obtain no-flow boundary conditions.
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/// \code
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/// \snippet tutorial2.cpp boundary
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/// \internal [boundary]
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Opm::FlowBCManager bcs;
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/// \endcode
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/// \internal [boundary]
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/// \endinternal
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/// We set up a pressure solver for the incompressible problem,
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/// using the two-point flux approximation discretization. The
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/// null pointers correspond to arguments for gravity, wells and
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/// boundary conditions, which are all defaulted (to zero gravity,
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/// no wells, and no-flow boundaries).
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/// \code
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/// \snippet tutorial2.cpp tpfa
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/// \internal [tpfa]
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Opm::IncompTpfa psolver(*grid.c_grid(), props, linsolver, NULL, NULL, src, NULL);
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/// \internal [tpfa]
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/// \endinternal
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/// \page tutorial2
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/// We declare the state object, that will contain the pressure and face
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/// flux vectors we are going to compute. The well state
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/// object is needed for interface compatibility with the
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/// <CODE>solve()</CODE> method of class
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/// <CODE>Opm::IncompTPFA</CODE>.
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/// \code
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/// \snippet tutorial2.cpp state
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/// \internal [state]
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Opm::TwophaseState state;
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state.pressure().resize(num_cells, 0.0);
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state.faceflux().resize(num_faces, 0.0);
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state.saturation().resize(num_cells, 1.0);
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Opm::WellState well_state;
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/// \endcode
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/// \internal [state]
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/// \endinternal
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/// \page tutorial2
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/// We call the pressure solver.
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/// The first (timestep) argument does not matter for this
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/// incompressible case.
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/// \code
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/// \snippet tutorial2.cpp pressure solver
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/// \internal [pressure solver]
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psolver.solve(1.0*day, state, well_state);
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/// \endcode
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/// \internal [pressure solver]
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/// \endinternal
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/// \page tutorial2
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/// We write the results to a file in VTK format.
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/// The data vectors added to the Opm::DataMap must
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/// contain cell data. They may be a scalar per cell
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/// (pressure) or a vector per cell (cell_velocity).
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/// \code
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/// \snippet tutorial2.cpp write output
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/// \internal [write output]
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std::ofstream vtkfile("tutorial2.vtu");
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Opm::DataMap dm;
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dm["pressure"] = &state.pressure();
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@@ -171,8 +193,10 @@ int main()
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Opm::estimateCellVelocity(*grid.c_grid(), state.faceflux(), cell_velocity);
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dm["velocity"] = &cell_velocity;
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Opm::writeVtkData(*grid.c_grid(), dm, vtkfile);
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/// \internal [write output]
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/// \endinternal
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}
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/// \endcode
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/// \page tutorial2
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/// We read the vtu output file in \a Paraview and obtain the following pressure
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/// distribution. \image html tutorial2.png
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@@ -181,3 +205,8 @@ int main()
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/// \page tutorial2
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/// \section completecode2 Complete source code:
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/// \include tutorial2.cpp
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/// \page tutorial2
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/// \details
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/// \section pythonscript2 python script to generate figures:
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/// \snippet generate_doc_figures.py tutorial2
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