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Merge pull request #161 from taiga-project/feature-157
Feature 157
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import numpy | ||
import matplotlib.pyplot | ||
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class SolverData: | ||
directory = "bin/example" | ||
reference_velocity = 400000 | ||
number_of_steps = 20000000 | ||
frequency_of_export = 100000 | ||
timestep = 1e-9 | ||
field_scenario = 'B = 1' | ||
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def __init__(self, solver_id, scenario='default'): | ||
self.solver_file = solver_id | ||
self.solver_name = self.get_solver_name(solver_id) | ||
self.solver_file += '_' + scenario | ||
self.set_scenario(scenario) | ||
self.data = self.get_data() | ||
self.x = self.get_field(0) | ||
self.y = self.get_field(1) | ||
self.v = numpy.sqrt(self.get_field(3)**2 + self.get_field(4)**2 + self.get_field(5)**2) | ||
self.v_relative = self.v / self.reference_velocity | ||
self.x_axis = numpy.arange(0, self.number_of_steps, self.frequency_of_export) | ||
self.line_style = self.get_line_style(solver_id) | ||
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def set_scenario(self, scenario): | ||
if scenario == 'start10': | ||
self.timestep = 1e-10 | ||
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if scenario in {'start8', 'gradb_start8', 'b__r_start8'}: | ||
self.timestep = 1e-8 | ||
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if scenario in {'gradb', 'gradb_start'}: | ||
self.field_scenario = 'B_z = 1 + 0.01 y' | ||
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if scenario in {'eparb', 'eparb_start'}: | ||
self.field_scenario = 'B_z = 1, E_z = 0.01' | ||
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if scenario in {'b__r', 'b__r_start', 'b__r_start8'}: | ||
self.field_scenario = '$B_z = \sqrt{x^2+y^2}$' | ||
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if scenario in {'start', 'gradb_start', 'b__r_start', 'eparb_start'}: | ||
self.number_of_steps = 100000 | ||
self.frequency_of_export = 10 | ||
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if scenario in {'start8', 'gradb_start8', 'b__r_start8'}: | ||
self.number_of_steps = 10000 | ||
self.frequency_of_export = 1 | ||
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@staticmethod | ||
def get_solver_name(solver_id): | ||
if solver_id == 'rk4': | ||
return 'linearised Runge--Kutta' | ||
elif solver_id == 'rkn': | ||
return 'Runge--Kutta--Nyström' | ||
elif solver_id == 'verlet': | ||
return 'Verlet--Boris' | ||
elif solver_id == 'yoshida': | ||
return 'Yoshida--Boris' | ||
else: | ||
return 'unknown' | ||
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@staticmethod | ||
def get_line_style(solver_id): | ||
if solver_id == 'rk4': | ||
return '-' | ||
elif solver_id == 'rkn': | ||
return '--' | ||
elif solver_id == 'verlet': | ||
return '-' | ||
elif solver_id == 'yoshida': | ||
return '--' | ||
else: | ||
return ':' | ||
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def get_data(self): | ||
return numpy.loadtxt(self.directory + '/' + self.solver_file + '.dat') | ||
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def get_field(self, identifier): | ||
return self.data[:, identifier] | ||
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def get_timestep(self): | ||
exponent = numpy.floor(numpy.log10(self.timestep)) | ||
mantissa = self.timestep / 10 ** exponent | ||
return '$' + (str(mantissa) + ' \cdot ' if (mantissa != 1.0) else '') + '10^{' + str(int(exponent)) + '}$ s' | ||
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def plot_xy(self): | ||
matplotlib.pyplot.plot(self.x, self.y, '.', markersize=1.5, label=self.solver_name) | ||
matplotlib.pyplot.title('timestep: ' + self.get_timestep() + ', ' + self.field_scenario) | ||
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def plot_v(self): | ||
matplotlib.pyplot.plot(self.x_axis, self.v_relative, self.line_style, linewidth=2.5, label=self.solver_name) | ||
matplotlib.pyplot.title('timestep: ' + self.get_timestep() + ', ' + self.field_scenario) | ||
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def visualise(): | ||
matplotlib.pyplot.xlabel('steps') | ||
matplotlib.pyplot.ylabel('relative velocity') | ||
matplotlib.pyplot.legend() | ||
matplotlib.pyplot.tight_layout() | ||
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def visualise_trajectory(): | ||
matplotlib.pyplot.xlabel('x [m]') | ||
matplotlib.pyplot.ylabel('y [m]') | ||
matplotlib.pyplot.axis('square') | ||
matplotlib.pyplot.legend() | ||
matplotlib.pyplot.tight_layout() | ||
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def compare_solvers(scenario='default'): | ||
SolverData('rk4', scenario).plot_v() | ||
SolverData('rkn', scenario).plot_v() | ||
SolverData('verlet', scenario).plot_v() | ||
SolverData('yoshida', scenario).plot_v() | ||
visualise() | ||
matplotlib.pyplot.savefig('bin/example/' + scenario + '.pdf') | ||
matplotlib.pyplot.savefig('bin/example/' + scenario + '.png') | ||
matplotlib.pyplot.show() | ||
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def compare_solvers_trajectory(scenario='default'): | ||
SolverData('rk4', scenario).plot_xy() | ||
SolverData('rkn', scenario).plot_xy() | ||
SolverData('verlet', scenario).plot_xy() | ||
SolverData('yoshida', scenario).plot_xy() | ||
visualise_trajectory() | ||
matplotlib.pyplot.savefig('bin/example/' + scenario + '_traj.pdf') | ||
matplotlib.pyplot.savefig('bin/example/' + scenario + '_traj.png') | ||
matplotlib.pyplot.show() | ||
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if __name__ == "__main__": | ||
compare_solvers('b__r') | ||
compare_solvers_trajectory('b__r') | ||
compare_solvers('start8') | ||
compare_solvers_trajectory('start8') | ||
compare_solvers_trajectory('start') | ||
compare_solvers('gradb_start') | ||
compare_solvers_trajectory('gradb_start') |
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#include <stdio.h> | ||
#include <stdlib.h> | ||
#include <stdbool.h> | ||
#include <math.h> | ||
#include <string.h> | ||
#include <sys/stat.h> | ||
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#include "export_solver.h" | ||
#include "test_solver.h" | ||
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#include "utils/taiga_constants.h" | ||
#include "utils/prop.h" | ||
#include "core/maths/maths.cuh" | ||
#include "core/solvers/solvers.cuh" | ||
#include "core/solvers/rk4.cuh" | ||
#include "core/solvers/runge_kutta_nystrom.cuh" | ||
#include "core/solvers/yoshida.cuh" | ||
#include "core/solvers/verlet.cuh" | ||
#include "core/solvers/boris.cuh" | ||
#include "core/physics/lorentz.cuh" | ||
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#include "utils/basic_functions.c" | ||
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#define FOLDER "example" | ||
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void export_coordinate (FILE *f, double *X, long N_half) { | ||
fprintf(f, "%lf\t%lf\t%lf\t%lf\t%lf\t%lf\t%ld\n", X[0], X[1], X[2], X[3], X[4], X[5], N_half); | ||
} | ||
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void generate_R_B_const_field(double *X, double *local_bfield, double *local_efield, | ||
TaigaCommons *c, bool is_electric_field_on, | ||
int *local_spline_indices, | ||
double *local_spline_brad, double *local_spline_bz, double *local_spline_btor, | ||
double *local_spline_erad, double *local_spline_ez, double *local_spline_etor, | ||
double *local_psi_n) { | ||
local_bfield[0] = 0.0; | ||
local_bfield[1] = 0.0; | ||
local_bfield[2] = 1.0 / (X[0] + 1.0); | ||
local_efield[0] = 0.0; | ||
local_efield[1] = 0.0; | ||
local_efield[2] = 0.0; | ||
} | ||
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void generate_B_over_R_field(double *X, double *local_bfield, double *local_efield, | ||
TaigaCommons *c, bool is_electric_field_on, | ||
int *local_spline_indices, | ||
double *local_spline_brad, double *local_spline_bz, double *local_spline_btor, | ||
double *local_spline_erad, double *local_spline_ez, double *local_spline_etor, | ||
double *local_psi_n) { | ||
local_bfield[0] = 0.0; | ||
local_bfield[1] = 0.0; | ||
local_bfield[2] = sqrt (X[0] * X[0] + X[1] * X[1]); | ||
local_efield[0] = 0.0; | ||
local_efield[1] = 0.0; | ||
local_efield[2] = 0.0; | ||
} | ||
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void run_field_with_solver_and_export(char* scenario_name, double timestep, int field_type, char* solver_name, | ||
long number_of_steps, long frequency_of_export, | ||
double (*solve_diffeq)(double *X, double eperm, double timestep, | ||
TaigaCommons *c, bool is_electric_field_on, | ||
int *local_spline_indices, | ||
double *local_spline_brad, double *local_spline_bz, double *local_spline_btor, | ||
double *local_spline_erad, double *local_spline_ez, double *local_spline_etor, | ||
double *local_psi_n) ) { | ||
switch(field_type){ | ||
case HOMOGENEOUS: | ||
generate_local_field = &generate_homogeneous_magnetic_field; | ||
break; | ||
case GRAD_B: | ||
generate_local_field = &generate_grad_B_field; | ||
break; | ||
case E_PAR_B: | ||
generate_local_field = &generate_E_par_B_field; | ||
break; | ||
case BR_FIELD: | ||
generate_local_field = &generate_R_B_const_field; | ||
break; | ||
case B_OVER_R_FIELD: | ||
generate_local_field = &generate_B_over_R_field; | ||
break; | ||
default: | ||
printf("Error: Illegal field_type\n"); | ||
} | ||
FILE *file; | ||
double X[6] = {0}; | ||
int local_spline_indices[2]; | ||
local_spline_indices[0] = SPLINE_INDEX_ERROR; | ||
local_spline_indices[1] = SPLINE_INDEX_ERROR; | ||
double local_spline_brad[16]; | ||
double local_spline_bz[16]; | ||
double local_spline_btor[16]; | ||
double local_spline_erad[16]; | ||
double local_spline_ez[16]; | ||
double local_spline_etor[16]; | ||
double local_psi_n[16]; | ||
TaigaCommons *c; | ||
double eperm = 4e7; | ||
int is_electric_field_on = true; | ||
long number_of_half_cyclotron_periods = 0; | ||
double v_previous; | ||
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get_acceleration_from_lorentz_force = &get_acceleration_from_lorentz_force_with_electric_field; | ||
X[4] = eperm * LARMOR_RADIUS; | ||
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if (field_type == B_OVER_R_FIELD) X[0] = 1.5; | ||
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mkdir(FOLDER, S_IRWXU | S_IRWXG | S_IRWXO); | ||
const char *path = concat(FOLDER, "/", solver_name, "_", scenario_name, ".dat", NULL); | ||
printf("export to: %s\n", path); | ||
file = fopen(path ,"w"); | ||
for (int i = 0; i < number_of_steps; ++i) { | ||
v_previous = X[4]; | ||
solve_diffeq(X, eperm, timestep, | ||
c, is_electric_field_on, | ||
local_spline_indices, | ||
local_spline_brad, local_spline_bz, local_spline_btor, | ||
local_spline_erad, local_spline_ez, local_spline_etor, | ||
local_psi_n); | ||
if ((X[4] * v_previous) <= 0) ++number_of_half_cyclotron_periods; | ||
if (i % frequency_of_export == 0) export_coordinate(file, X, number_of_half_cyclotron_periods); | ||
} | ||
fclose(file); | ||
} | ||
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void run_scenario(char* scenario_name, double timestep, int field_type, | ||
long number_of_steps, long frequency_of_export){ | ||
run_field_with_solver_and_export(scenario_name, timestep, field_type, "rk4", number_of_steps, frequency_of_export, solve_diffeq_by_rk4); | ||
run_field_with_solver_and_export(scenario_name, timestep, field_type, "rkn", number_of_steps, frequency_of_export, solve_diffeq_by_rkn); | ||
run_field_with_solver_and_export(scenario_name, timestep, field_type, "verlet", number_of_steps, frequency_of_export, solve_diffeq_by_verlet); | ||
run_field_with_solver_and_export(scenario_name, timestep, field_type, "yoshida", number_of_steps, frequency_of_export, solve_diffeq_by_yoshida); | ||
} | ||
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int main() { | ||
double timestep = 1e-9; | ||
long number_of_steps = 20000000; | ||
long frequency_of_export = 100000; | ||
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run_scenario("default", timestep, HOMOGENEOUS, number_of_steps, frequency_of_export); | ||
run_scenario("gradb", timestep, GRAD_B, number_of_steps, frequency_of_export); | ||
run_scenario("eparb", timestep, E_PAR_B, number_of_steps, frequency_of_export); | ||
run_scenario("br", timestep, BR_FIELD, number_of_steps, frequency_of_export); | ||
run_scenario("b__r", timestep, B_OVER_R_FIELD, number_of_steps, frequency_of_export); | ||
run_scenario("start8", 1e-8, HOMOGENEOUS, 10000, 1); | ||
run_scenario("b__r_start8", 1e-8, B_OVER_R_FIELD, 10000, 1); | ||
run_scenario("start", timestep, HOMOGENEOUS, 100000, 10); | ||
run_scenario("b__r_start", timestep, B_OVER_R_FIELD, 100000, 10); | ||
run_scenario("gradb_start", timestep, GRAD_B, 100000, 10); | ||
run_scenario("eparb_start", timestep, E_PAR_B, 100000, 10); | ||
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return 0; | ||
} |
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#ifndef EXPORT_SOLVER_CUH | ||
#define EXPORT_SOLVER_CUH | ||
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#include <stdbool.h> | ||
#include "utils/taiga_constants.h" | ||
#include "utils/prop.h" | ||
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#define __device__ ; | ||
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#define BR_FIELD 90 | ||
#define B_OVER_R_FIELD 91 | ||
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void export_coordinate (FILE *f, double *X, long N_half); | ||
void generate_R_B_const_field(double *X, double *local_bfield, double *local_efield, | ||
TaigaCommons *c, bool is_electric_field_on, | ||
int *local_spline_indices, | ||
double *local_spline_brad, double *local_spline_bz, double *local_spline_btor, | ||
double *local_spline_erad, double *local_spline_ez, double *local_spline_etor, | ||
double *local_psi_n); | ||
void generate_B_over_R_field(double *X, double *local_bfield, double *local_efield, | ||
TaigaCommons *c, bool is_electric_field_on, | ||
int *local_spline_indices, | ||
double *local_spline_brad, double *local_spline_bz, double *local_spline_btor, | ||
double *local_spline_erad, double *local_spline_ez, double *local_spline_etor, | ||
double *local_psi_n); | ||
void run_field_with_solver_and_export(char* scenario_name, double timestep, int field_type, char* solver_name, | ||
long number_of_steps, long frequency_of_export, | ||
double (*solve_diffeq)(double *X, double eperm, double timestep, | ||
TaigaCommons *c, bool is_electric_field_on, | ||
int *local_spline_indices, | ||
double *local_spline_brad, double *local_spline_bz, double *local_spline_btor, | ||
double *local_spline_erad, double *local_spline_ez, double *local_spline_etor, | ||
double *local_psi_n) ); | ||
void run_scenario(char* scenario_name, double timestep, int field_type, | ||
long number_of_steps, long frequency_of_export); | ||
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#endif //EXPORT_SOLVER_CUH |
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import unittest | ||
from taiga.example.solvers.compare_solvers import SolverData | ||
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class TestCompareSolvers(unittest): | ||
def test_timestep(self): | ||
s = SolverData('rk4') | ||
reference = '$10^{-9}$ s' | ||
self.assertEqual(reference, s.get_timestep()) | ||
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def test_timestep_1p5em10(self): | ||
s = SolverData('rk4') | ||
s.timestep = 1.5e-10 | ||
reference = '$1.5 \cdot 10^{-10}$ s' | ||
self.assertEqual(reference, s.get_timestep()) |
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