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Finite difference example #635
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############################################################################ | ||
# Copyright (c) 2018-2022 by the Cabana authors # | ||
# All rights reserved. # | ||
# # | ||
# This file is part of the Cabana library. Cabana is distributed under a # | ||
# BSD 3-clause license. For the licensing terms see the LICENSE file in # | ||
# the top-level directory. # | ||
# # | ||
# SPDX-License-Identifier: BSD-3-Clause # | ||
############################################################################ | ||
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add_subdirectory(finite_difference) |
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############################################################################ | ||
# Copyright (c) 2018-2022 by the Cabana authors # | ||
# All rights reserved. # | ||
# # | ||
# This file is part of the Cabana library. Cabana is distributed under a # | ||
# BSD 3-clause license. For the licensing terms see the LICENSE file in # | ||
# the top-level directory. # | ||
# # | ||
# SPDX-License-Identifier: BSD-3-Clause # | ||
############################################################################ | ||
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add_executable(FiniteDifference finite_difference.cpp) | ||
target_link_libraries(FiniteDifference Cajita) |
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example/methods/finite_difference/finite_difference.cpp
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/**************************************************************************** | ||
* Copyright (c) 2018-2023 by the Cabana authors * | ||
* All rights reserved. * | ||
* * | ||
* This file is part of the Cabana library. Cabana is distributed under a * | ||
* BSD 3-clause license. For the licensing terms see the LICENSE file in * | ||
* the top-level directory. * | ||
* * | ||
* SPDX-License-Identifier: BSD-3-Clause * | ||
****************************************************************************/ | ||
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#include <array> | ||
#include <iostream> | ||
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#include <mpi.h> | ||
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#include <Kokkos_Core.hpp> | ||
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#include <Cabana_Grid.hpp> | ||
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// Apply boundary conditions. For simplicity of the code, rebuild the index | ||
// spaces each step even though it's a fixed geometry. Apply all boundaries in | ||
// one kernel for performance. | ||
template <class ExecutionSpace, class LocalGridType, class ArrayType> | ||
void updateBoundaries( ExecutionSpace exec_space, LocalGridType local_grid, | ||
ArrayType& field ) | ||
{ | ||
// Create boundary indices for each plane. | ||
Kokkos::Array<Cabana::Grid::IndexSpace<3>, 6> boundary_spaces; | ||
// Store the boundary details in device-accessible fixed-size arrays. | ||
Kokkos::Array<Kokkos::Array<int, 3>, 6> planes; | ||
// Generate the boundary condition index spaces. | ||
int count = 0; | ||
for ( int d = 0; d < 3; d++ ) | ||
{ | ||
for ( int dir = -1; dir < 2; dir += 2 ) | ||
{ | ||
planes[count] = { 0, 0, 0 }; | ||
planes[count][d] = dir; | ||
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// Get the boundary indices for this plane (each one is a separate, | ||
// contiguous index space). | ||
boundary_spaces[count] = local_grid->boundaryIndexSpace( | ||
Cabana::Grid::Own(), Cabana::Grid::Cell(), planes[count][0], | ||
planes[count][1], planes[count][2] ); | ||
count++; | ||
} | ||
} | ||
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// Update the boundary on each face of the cube. Pass the vector of index | ||
// spaces to avoid launching 6 separate kernels. | ||
Cajita::grid_parallel_for( | ||
"boundary_update", exec_space, boundary_spaces, | ||
KOKKOS_LAMBDA( const int b, const int i, const int j, const int k ) { | ||
// Set boundary cells to the nearest internal value. | ||
field( i, j, k, 0 ) = field( i - planes[b][0], j - planes[b][1], | ||
k - planes[b][2], 0 ); | ||
} ); | ||
} | ||
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/* | ||
This micro-application solves the heat equation using finite differences. | ||
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If not familiar with Cabana, it is recommended to go through the Core and | ||
Grid tutorials prior to this example. | ||
*/ | ||
void finiteDifference() | ||
{ | ||
// Use the default execution (and memory) space - these can instead be | ||
// explicitly chosen. | ||
using exec_space = Kokkos::DefaultExecutionSpace; | ||
using device_type = exec_space::device_type; | ||
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// Define the system and create the global mesh | ||
double cell_size = 1e-5; | ||
std::array<double, 3> global_low_corner = { -2.5e-4, -2.5e-4, -2.5e-4 }; | ||
std::array<double, 3> global_high_corner = { 2.5e-4, 2.5e-4, 0 }; | ||
auto global_mesh = Cabana::Grid::createUniformGlobalMesh( | ||
global_low_corner, global_high_corner, cell_size ); | ||
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// Create the global grid for a non-periodic system. | ||
Cabana::Grid::DimBlockPartitioner<3> partitioner; | ||
std::array<bool, 3> periodic = { false, false, false }; | ||
auto global_grid = | ||
createGlobalGrid( MPI_COMM_WORLD, global_mesh, periodic, partitioner ); | ||
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// Create a local grid and local mesh with halo region. | ||
// Note this halo width needs to be large enough for the stencil used below. | ||
unsigned halo_width = 1; | ||
auto local_grid = Cabana::Grid::createLocalGrid( global_grid, halo_width ); | ||
auto local_mesh = Cabana::Grid::createLocalMesh<device_type>( *local_grid ); | ||
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// Create temperature array on the cells for finite difference calculations | ||
auto owned_space = local_grid->indexSpace( | ||
Cabana::Grid::Own(), Cabana::Grid::Cell(), Cabana::Grid::Local() ); | ||
auto layout = | ||
createArrayLayout( global_grid, halo_width, 1, Cabana::Grid::Cell() ); | ||
std::string name( "temperature" ); | ||
auto T_array = | ||
Cabana::Grid::createArray<double, device_type>( name, layout ); | ||
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// Set all initial values to room temperature (K). This sets both the owned | ||
// and ghosted cell values. | ||
Cabana::Grid::ArrayOp::assign( *T_array, 300.0, Cabana::Grid::Ghost() ); | ||
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// Create the halo for grid MPI communication. | ||
auto T_halo = | ||
createHalo( Cabana::Grid::NodeHaloPattern<3>(), halo_width, *T_array ); | ||
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// Update initial physical and MPI processor boundaries. | ||
auto T = T_array->view(); | ||
updateBoundaries( exec_space(), local_grid, T ); | ||
T_halo->gather( exec_space(), *T_array ); | ||
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// Create array to store previous temperature for explicit time udpate. | ||
// Note that this should not be created from the original array - this must | ||
// point to different memory. | ||
auto T_prev_array = | ||
Cabana::Grid::createArray<double, device_type>( name, layout ); | ||
auto T_prev = T_prev_array->view(); | ||
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// Time-related inputs. | ||
double dt = 1e-6; | ||
double end_time = 1e-3; | ||
int num_steps = static_cast<int>( end_time / dt ); | ||
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// Material property inputs. | ||
double density = 1000.0; | ||
double specific_heat = 1000.0; | ||
double thermal_conductivity = 10.0; | ||
// Derived inputs. | ||
double alpha = thermal_conductivity / ( density * specific_heat ); | ||
double alpha_dt_dx2 = alpha * dt / ( cell_size * cell_size ); | ||
double dt_rho_cp = dt / ( density * specific_heat ); | ||
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// Gaussian heat source parameters (sigma is the standard deviation of the | ||
// gaussian). | ||
double eta = 0.1; | ||
double power = 200.0; | ||
double sigma[3] = { 50e-6, 50e-6, 25e-6 }; | ||
double sqrt2 = Kokkos::sqrt( 2.0 ); | ||
double r[3] = { sigma[0] / sqrt2, sigma[1] / sqrt2, sigma[2] / sqrt2 }; | ||
// Intensity of the heat source. | ||
double I = 2.0 * eta * power / | ||
( M_PI * Kokkos::sqrt( M_PI ) * r[0] * r[1] * r[2] ); | ||
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// Timestep loop. | ||
int output_freq = 10; | ||
for ( int step = 0; step < num_steps; ++step ) | ||
{ | ||
if ( global_grid->blockId() == 0 && step % output_freq == 0 ) | ||
std::cout << "Step " << step << " / " << num_steps << std::endl; | ||
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// Store previous value for explicit update | ||
Kokkos::deep_copy( T_prev, T ); | ||
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// Solve heat conduction from point source with finite difference. | ||
Cabana::Grid::grid_parallel_for( | ||
"finite_difference", exec_space(), owned_space, | ||
KOKKOS_LAMBDA( const int i, const int j, const int k ) { | ||
double loc[3]; | ||
int idx[3] = { i, j, k }; | ||
local_mesh.coordinates( Cabana::Grid::Cell(), idx, loc ); | ||
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double f = ( loc[0] * loc[0] / r[0] / r[0] ) + | ||
( loc[1] * loc[1] / r[1] / r[1] ) + | ||
( loc[2] * loc[2] / r[2] / r[2] ); | ||
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double Q = I * Kokkos::exp( -f ) * dt_rho_cp; | ||
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double laplacian = | ||
( -6.0 * T_prev( i, j, k, 0 ) + T_prev( i - 1, j, k, 0 ) + | ||
T_prev( i + 1, j, k, 0 ) + T_prev( i, j - 1, k, 0 ) + | ||
T_prev( i, j + 1, k, 0 ) + T_prev( i, j, k - 1, 0 ) + | ||
T_prev( i, j, k + 1, 0 ) ) * | ||
alpha_dt_dx2; | ||
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T( i, j, k, 0 ) += laplacian + Q; | ||
} ); | ||
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// Update the physical system boundary conditions. | ||
updateBoundaries( exec_space(), local_grid, T ); | ||
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// Exchange halo values on MPI boundaries. | ||
T_halo->gather( exec_space(), *T_array ); | ||
} | ||
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// Write the final state to file. | ||
Cabana::Grid::Experimental::BovWriter::writeTimeStep( 0, 0, *T_array ); | ||
} | ||
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// Main function which initializes/finalizes MPI and Kokkos. | ||
int main( int argc, char* argv[] ) | ||
{ | ||
MPI_Init( &argc, &argv ); | ||
Kokkos::initialize( argc, argv ); | ||
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finiteDifference(); | ||
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Kokkos::finalize(); | ||
MPI_Finalize(); | ||
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return 0; | ||
} | ||
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//---------------------------------------------------------------------------// |
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It might be a good idea to add comment about the problem. I think this is about unsteady heat equation problem in 3d.
The governing equstion :$$\rho c_p dT/dt = k \nabla^2{T} + q$$ $$k \nabla{T} \cdot n = f$$
Neumann boundary condition (describing heat flux ) :
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@kwitaechong, you are correct. This boundary conditions is just an adiabatic one. I will correct the description.
Also, it is worth pointing out that I think the left-hand and right-hand sides are swapped...
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@colemanjs can you add a more detailed comment below?