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4 Commits
Author SHA1 Message Date
ParkSuMin e90d5ebc49 Refactoring 2026-09-23 18:10:38 +03:00
ParkSuMin 57b01edebd Create results.py 2026-09-23 18:10:21 +03:00
ParkSuMin ce1a12056d Update optimize.py 2026-09-23 14:02:56 +03:00
ParkSuMin 7a854184a3 New API version 2026-09-23 14:02:51 +03:00
5 changed files with 142 additions and 76 deletions

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-1
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@@ -97,4 +97,3 @@ add_mmps_plugin(
# ПРИМЕР ЗАПУСКА ИЗ КАТАЛОГА build
# bin/Release/mmps_host.exe (Visual Studio)
# bin/mmps_host (Linux/Makefiles)
# Каталог плагинов и значения k1, k2, h программа запросит через std::cin.
+1 -2
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@@ -30,7 +30,7 @@ struct OutputParameters{
size_t point_count;
};
inline constexpr std::uint32_t PLUGIN_API_VERSION = 2;
inline constexpr std::uint32_t PLUGIN_API_VERSION = 3;
#if defined(_WIN32) && defined(PLUGIN_BUILD)
#define PLUGIN_EXPORT extern "C" __declspec(dllexport)
@@ -56,4 +56,3 @@ inline constexpr const char* SYMBOL_NAME = "plugin_name";
inline constexpr const char* SYMBOL_DESCRIPTION = "plugin_description";
inline constexpr const char* SYMBOL_SOLVER = "solver";
inline constexpr const char* SYMBOL_WRITE_OUTPUT = "write_output";
+1 -2
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@@ -28,8 +28,7 @@ inline State derivative(const State& state,
};
}
inline State runge_kutta_step(const State& state,
const SolverParameters& parameters){
inline State runge_kutta_step(const State& state, const SolverParameters& parameters){
double h = parameters.step;
State k1 = derivative(state, parameters);
+90 -71
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@@ -1,20 +1,32 @@
import numpy as np
from scipy.optimize import least_squares
# Эталонные значения параметров
K1_REFERENCE = 0.577
K2_REFERENCE = 0.422
REFERENCE_K1 = 0.577
REFERENCE_K2 = 0.422
TIMES = np.linspace(0.0, 10.0, 101)
SUBSTEPS = 10
K1_BOUNDS = (1e-5, 1e2)
K2_BOUNDS = (1e-2, 1.0)
T_BEGIN = 0.0
T_END = 10.0
H = 0.1
def analytical_solution(t, k1, k2):
"""
Аналитическое решение задачи Коши.
"""
t = np.asarray(t, dtype=float)
def analytical(t, k1, k2):
x1 = np.exp(-k1 * t)
if k1 == k2:
if np.isclose(k1, k2):
x2 = k1 * t * np.exp(-k1 * t)
else:
x2 = k1 / (k2 - k1) * (
np.exp(-k1 * t) - np.exp(-k2 * t)
x2 = (
k1 / (k2 - k1)
* (np.exp(-k1 * t) - np.exp(-k2 * t))
)
x3 = 1.0 - x1 - x2
@@ -22,90 +34,97 @@ def analytical(t, k1, k2):
return np.column_stack((x1, x2, x3))
def solve_rk4(k1, k2):
def derivative(state, k1, k2):
"""
Правая часть системы дифференциальных уравнений.
"""
x1, x2, x3 = state
def rhs(x):
x1, x2, x3 = x
return np.array([
-k1 * x1,
k1 * x1 - k2 * x2,
k2 * x2
])
return np.array([
-k1 * x1,
k1 * x1 - k2 * x2,
k2 * x2,
])
state = np.array([1.0, 0.0, 0.0])
def rk4_step(state, h, k1, k2):
"""
Один шаг метода Рунге--Кутты четвёртого порядка.
"""
q1 = derivative(state, k1, k2)
q2 = derivative(state + h * q1 / 2.0, k1, k2)
q3 = derivative(state + h * q2 / 2.0, k1, k2)
q4 = derivative(state + h * q3, k1, k2)
solution = np.empty((len(TIMES), 3))
solution[0] = state
return state + h / 6.0 * (q1 + 2.0 * q2 + 2.0 * q3 + q4)
for j in range(1, len(TIMES)):
h = (TIMES[j] - TIMES[j - 1]) / SUBSTEPS
for _ in range(SUBSTEPS):
q1 = rhs(state)
q2 = rhs(state + h * q1 / 2.0)
q3 = rhs(state + h * q2 / 2.0)
q4 = rhs(state + h * q3)
def rk4_solution(t, k1, k2):
"""
Решение задачи Коши методом RK4.
"""
solution = np.zeros((len(t), 3), dtype=float)
solution[0] = [1.0, 0.0, 0.0]
state = state + h / 6.0 * (
q1 + 2.0 * q2 + 2.0 * q3 + q4
)
for index in range(1, len(t)):
h = t[index] - t[index - 1]
solution[j] = state
solution[index] = rk4_step(
solution[index - 1],
h,
k1,
k2
)
return solution
time = np.linspace(T_BEGIN, T_END, 101)
def residuals(parameters, reference):
# Эталонные данные
reference_solution = analytical_solution(time, K1_REFERENCE, K2_REFERENCE)
def residuals(parameters):
"""
Вектор невязок между моделью и эталонными данными.
"""
k1, k2 = parameters
calculated = solve_rk4(k1, k2)
numerical_solution = rk4_solution(time, k1, k2)
return (calculated - reference).ravel()
# Получается вектор из 101 * 3 = 303 невязок
return (numerical_solution - reference_solution).ravel()
def main():
reference = analytical(TIMES, REFERENCE_K1, REFERENCE_K2)
# Начальное приближение
initial_parameters = np.array([0.3, 0.7])
result = least_squares(
fun=residuals,
x0=[0.3, 0.7],
args=(reference,),
bounds=(
[1e-5, 0.01],
[100.0, 1.0],
),
method="trf",
max_nfev=200,
verbose=1,
result = least_squares(
residuals,
initial_parameters,
bounds=(
[K1_BOUNDS[0], K2_BOUNDS[0]],
[K1_BOUNDS[1], K2_BOUNDS[1]]
)
)
k1_found, k2_found = result.x
# result.x - solution
found_k1, found_k2 = result.x
absolute_error_k1 = abs(k1_found - REFERENCE_K1)
absolute_error_k2 = abs(k2_found - REFERENCE_K2)
absolute_error_k1 = abs(found_k1 - K1_REFERENCE)
absolute_error_k2 = abs(found_k2 - K2_REFERENCE)
relative_error_k1 = absolute_error_k1 / REFERENCE_K1 * 100
relative_error_k2 = absolute_error_k2 / REFERENCE_K2 * 100
relative_error_k1 = absolute_error_k1 / K1_REFERENCE * 100.0
relative_error_k2 = absolute_error_k2 / K2_REFERENCE * 100.0
sum_squared_errors = np.sum(result.fun ** 2)
rmse = np.sqrt(np.mean(result.fun ** 2))
print("Results")
print(f"Found k1:{found_k1:.4f}")
print(f"Theoretical k1:{K1_REFERENCE:.4f}")
print(f"Absolute error of k1:{absolute_error_k1:.5e}")
print(f"Relative error of k1:{relative_error_k1:.5e} %")
print()
print(f"\nk1 = {k1_found:.4f}")
print(f"k2 = {k2_found:.4f}")
print(f"\nАбсолютное отклонение k1: {absolute_error_k1:.6e}")
print(f"Абсолютное отклонение k2: {absolute_error_k2:.6e}")
print(f"\nОтносительное отклонение k1: {relative_error_k1:.6e}%")
print(f"Относительное отклонение k2: {relative_error_k2:.6e}%")
print(f"\nСумма квадратов отклонений: {sum_squared_errors:.6e}")
print(f"RMSE: {rmse:.6e}")
if not result.success:
print("\nПоиск завершён без подтверждённой сходимости.")
if __name__ == "__main__":
main()
print(f"Found k2:{found_k2:.5f}")
print(f"Theoretical k2:{K2_REFERENCE:.5f}")
print(f"Absolute error of k2:{absolute_error_k2:.5e}")
print(f"Relative error of k2:{relative_error_k2:.5e} %")
print()
+50
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@@ -0,0 +1,50 @@
import pandas as pd
import matplotlib.pyplot as plt
def export_component_comparison(
rk4_path: str,
ab2_path: str,
component: str,
ylabel: str,
out_name: str,
):
"""
Строит график зависимости одной компоненты x_i(t) от времени,
на котором результаты метода Рунге--Кутты и метода Адамса--Башфорта
представлены на общей координатной плоскости (п.4 базовой части задания).
"""
df_rk4 = pd.read_csv(rk4_path)
df_ab2 = pd.read_csv(ab2_path)
t_rk4, y_rk4 = df_rk4["t"].values, df_rk4[component].values
t_ab2, y_ab2 = df_ab2["t"].values, df_ab2[component].values
plt.figure(figsize=(10, 6))
plt.plot(t_rk4, y_rk4, label="Рунге--Кутты 4-го порядка",
linewidth=2.2, color="#1f77b4")
plt.plot(t_ab2, y_ab2, label="Адамса--Башфорта 2-го порядка",
linewidth=1.8, color="#ff7f0e", linestyle="--")
plt.xlabel("t", fontsize=12)
plt.ylabel(ylabel, fontsize=12)
plt.grid(True, which="both", linestyle="--", alpha=0.6)
plt.legend(fontsize=11, loc="best", framealpha=0.9)
t_min = min(t_rk4.min(), t_ab2.min())
t_max = max(t_rk4.max(), t_ab2.max())
plt.xlim(t_min - 0.1, t_max + 0.1)
plt.ylim(-0.02, 1.05)
plt.tight_layout()
plt.savefig(f"figures/{out_name}.png", dpi=300)
plt.close()
RK4_CSV = "../build/bin/results/runge_kutta_plugin.csv"
AB2_CSV = "../build/bin/results/adams_bashforth_plugin.csv"
export_component_comparison(RK4_CSV, AB2_CSV, "x1", r"$x_1(t)$", "x1_comparison")
export_component_comparison(RK4_CSV, AB2_CSV, "x2", r"$x_2(t)$", "x2_comparison")
export_component_comparison(RK4_CSV, AB2_CSV, "x3", r"$x_3(t)$", "x3_comparison")