int main()
{
cout << "\n";
cout << "=== Hyperbolic: 1D Euler gasdynamics shocktube =====\n";
cout << "\n";
// define the domain/mesh
const double left = 0.0;
const double right = 1.0;
const unsigned N = 400;
DenseVector<double> faces_x = Utility::uniform_node_vector( left, right, N );
double t = 0.0;
Example::Euler_1d conservative_problem;
OneD_TVDLF_Mesh Euler_mesh( faces_x, &conservative_problem, Example::Q_init );
Euler_mesh.set_limiter( 0 );
double I1 = Euler_mesh.integrate()[0];
int loop_counter( 0 );
int file_counter( 0 );
std::string filename_stub;
filename_stub = "./DATA/HYP_shocktube_sod";
TrackerFile my_file( 10 );
OneD_Node_Mesh<double> soln = Euler_mesh.get_soln();
my_file.push_ptr( &soln, "mesh" );
do
{
if ( loop_counter % 10 == 0 )
{
my_file.set_filename( filename_stub + Utility::stringify( file_counter ) + ".dat" );
soln = Euler_mesh.get_soln( );
my_file.update();
file_counter += 1;
}
t += Euler_mesh.update( 0.499 );
++loop_counter;
}
while ( ( t < 0.2 ) && ( loop_counter < 1000 ) );
double I2 = Euler_mesh.integrate()[0];
// These are clawpack results (to 4dp) with N=400 and minmod for the
// density of the two density steps ...
soln = Euler_mesh.get_soln( );
double E1 = std::abs( soln.get_interpolated_vars( 0.575 )[0] - 0.4264 );
double E2 = std::abs( soln.get_interpolated_vars( 0.75 )[0] - 0.2656 );
// check against the clawpack data, and that the mass is conserved.
if ( ( E1 > 1.e-3 ) || ( E2 > 1.e-3 ) || ( std::abs( I1 - I2 ) > 1.e-8 ) || ( loop_counter >= 1000 ) )
{
cout << "\033[1;31;48m * FAILED \033[0m\n";
cout << E1 << " " << E2 << " " << std::abs( I1 - I2 ) << " " << loop_counter << "\n";
}
else
{
cout << "\033[1;32;48m * PASSED \033[0m\n";
}
} // end of main()
int main()
{
cout << "\n";
cout << "=== Hyperbolic: Shallow water radial dam break ======\n";
cout << "\n";
// There is a singular source_fn at r=0, so we bodge it here (for now).
/// \todo Include a mechanism for avoiding source term computations
/// at the singular point by indicating where edge conditions are specified.
/// For the time being, we'll bodge it by stopping away from x=0.
const double left = 1.e-4;
const double right = 2.5;
const unsigned N = 2001;
DenseVector<double> faces_x = Utility::power_node_vector( left, right, N, 1.0 );
// time
double t = 0;
double t_end = 0.5;
// hyperbolic problem
Example::Shallow_1d_rad conservative_problem;
OneD_TVDLF_Mesh Shallow_mesh( faces_x, &conservative_problem, Example::Q_init );
Shallow_mesh.set_limiter( 0 );
// output
int loop_counter( 0 );
int file_counter( 0 );
std::string dirname("./DATA");
mkdir( dirname.c_str(), S_IRWXU );
std::string filename_stub;
filename_stub = "./DATA/HYP_shallow_rad";
TrackerFile my_file( 5 );
OneD_Node_Mesh<double> soln = Shallow_mesh.get_soln();
my_file.push_ptr( &soln, "mesh" );
do
{
if ( loop_counter % 50 == 0 )
{
my_file.set_filename( filename_stub + Utility::stringify( file_counter ) + ".dat" );
soln = Shallow_mesh.get_soln();
my_file.update();
file_counter += 1;
}
t += Shallow_mesh.update( 0.499, t_end - t );
++loop_counter;
}
while ( ( t < t_end ) && ( loop_counter < 3000 ) );
// we test the result against the Clawpack computational result
soln = Shallow_mesh.get_soln();
double h_clawpack( 1.13466 );
double h_test( soln.get_interpolated_vars( 0.5 )[ h ] );
if ( abs( h_test - h_clawpack ) > 1.e-3 )
{
cout << "\033[1;31;48m * FAILED \033[0m\n";
cout << " deviation from the Clawpack data = " << abs( h_test - h_clawpack ) << "\n";
return 1;
}
else
{
cout << "\033[1;32;48m * PASSED \033[0m\n";
return 0;
}
} // end of main()
int main()
{
cout << "\n";
cout << "=== Hyperbolic: 1D nonlinear advection equation ====\n";
cout << "\n";
// define the domain/mesh
const double left = 0.0;
const double right = 1.0;
const unsigned N = 141;
DenseVector<double> faces_x = Utility::uniform_node_vector( left, right, N );
double t = 0.0;
Example::NlinAdv conservative_problem;
OneD_TVDLF_Mesh NlinAdv_mesh( faces_x, &conservative_problem, Example::Q_init );
NlinAdv_mesh.set_limiter( 0 );
double I1 = NlinAdv_mesh.integrate()[0];
int loop_counter( 5 );
TrackerFile my_file( "./DATA/HYP_NlinAdv.dat" );
// first column of the output will always be the time
my_file.push_ptr( &t, "time" );
OneD_Node_Mesh<double> soln = NlinAdv_mesh.get_soln();
my_file.push_ptr( &soln, "mesh" );
double asym( 0.0 );
do
{
double dt = NlinAdv_mesh.update( 0.475 );
t += dt;
soln = NlinAdv_mesh.get_soln();
if ( loop_counter % 10 == 0 )
{
soln = NlinAdv_mesh.get_soln();
my_file.update();
my_file.newline();
}
++loop_counter;
asym = std::max( asym, std::abs( soln.get_interpolated_vars( 0.75 )[0] + soln.get_interpolated_vars( 0.25 )[0] ) );
}
while ( ( t < 0.4 ) && ( loop_counter < 1000 ) );
double I2 = NlinAdv_mesh.integrate()[0];
soln = NlinAdv_mesh.get_soln();
my_file.update();
my_file.newline();
// problem should be antisymmetric about x = 1/2
if ( ( asym > 1.e-10 ) || ( std::abs( I1 - I2 ) > 1.e-8 ) || ( loop_counter >= 1000 ) )
{
cout << "\033[1;31;48m * FAILED \033[0m\n";
cout << "asymmetry = " << asym << "\n";
cout << "integral difference = " << I1 - I2 << "\n";
cout << "loop counter = " << loop_counter << "\n";
}
else
{
cout << "\033[1;32;48m * PASSED \033[0m\n";
}
} // end of main()
