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Betts 10 144 145 #267

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"""
Van der Pol Oscillator
======================

https://en.wikipedia.org/wiki/Van_der_Pol_oscillator

These are example 10.144 / 145 from Betts' book "Practical Methods for Optimal Control
Using NonlinearProgramming", 3rd edition, Chapter 10: Test Problems.
It is described in more detail in section 4.14. example 4.11 of the book.

"""
import numpy as np
import sympy as sm
import sympy.physics.mechanics as me
from opty.direct_collocation import Problem
from opty.utils import create_objective_function
import matplotlib.pyplot as plt

# %%
# First version of the problem (10.144).
# --------------------------------------
# **States**
# :math:`y_1, y_2` : state variables
#
# **Controls**
# :math:`u` : control variables
#
# Equations of Motion.
# --------------------
t = me.dynamicsymbols._t

y1, y2 = me.dynamicsymbols('y1, y2')
u = me.dynamicsymbols('u')

eom = sm.Matrix([
-y1.diff() + y2,
-y2.diff(t) + (1 - y1**2)*y2 - y1 + u,
])
sm.pprint(eom)

# %%
# Define and Solve the Optimization Problem.
# ------------------------------------------
num_nodes = 2001
iterations = 1000

t0, tf = 0.0, 5.0
interval_value = (tf - t0)/(num_nodes - 1)

state_symbols = (y1, y2)
unkonwn_input_trajectories = (u, )

objective = sm.integrate(u**2 + y1**2 + y2**2, t)
obj, obj_grad = create_objective_function(objective,
state_symbols,
unkonwn_input_trajectories,
tuple(),
num_nodes,
interval_value
)

instance_constraints = (
y1.func(t0) - 1.0,
y2.func(t0),
)

bounds = {
y2: (-0.4, np.inf),
}

prob = Problem(
obj,
obj_grad,
eom,
state_symbols,
num_nodes,
interval_value,
instance_constraints= instance_constraints,
bounds=bounds,
)

# %%
# Solve the optimization problem.
# Give some rough estimates for the trajectories.

initial_guess = np.ones(prob.num_free)

# Find the optimal solution.
for i in range(1):
solution, info = prob.solve(initial_guess)
initial_guess = solution
print(info['status_msg'])
print(f'Objectve is: {info['obj_val']:.8f}, ' +
f'as per the book it is {2.95369916}, so the deviation is: ' +
f'{(info['obj_val'] -2.95369916) /2.95369916*100 :.5e} %')
solution1 = solution
# %%
# Plot the optimal state and input trajectories.
prob.plot_trajectories(solution)

# %%
# Plot the constraint violations.
prob.plot_constraint_violations(solution)

# %%
# Plot the objective function as a function of optimizer iteration.
prob.plot_objective_value()

# %%
# Second version of the problem (10.145).
# ---------------------------------------
# This is example 10.145 from Betts' book "Practical Methods for Optimal Control
# Using NonlinearProgramming", 3rd edition, Chapter 10: Test Problems.
# It is same as problem 10.144 but a bit reformulated.
# It has two control variables and one additional algebraic equation of motion.
# As opty needs as many state variables as equations of motion, I simply call
# the additional control variable v a state variable.
# It is described in more detail in section 4.14, example 4.11 of the book.
#
# This formulation seems to be more accurate compared to the above, when
# considering the violations of the constraints.
#
# **States**
# :math:`y_1, y_2, v` : state variables
#
# **Controls**
# :math:`u` : control variables
#
# Equations of Motion.
# --------------------
y1, y2, v = me.dynamicsymbols('y1, y2, v')
u = me.dynamicsymbols('u')

eom = sm.Matrix([
-y1.diff() + y2,
-y2.diff(t) + v - y1 + u,
v - (1-y1**2)*y2,
])
sm.pprint(eom)

# %%
# Define and Solve the Optimization Problem.
# ------------------------------------------
state_symbols = (y1, y2, v)
unkonwn_input_trajectories = (u,)

objective = sm.integrate(u**2 + y1**2 + y2**2, t)
obj, obj_grad = create_objective_function(objective,
state_symbols,
unkonwn_input_trajectories,
tuple(),
num_nodes,
interval_value
)

instance_constraints = (
y1.func(t0) - 1.0,
y2.func(t0),
)

bounds = {
y2: (-0.4, np.inf),
}

prob = Problem(
obj,
obj_grad,
eom,
state_symbols,
num_nodes,
interval_value,
instance_constraints= instance_constraints,
bounds=bounds,
)

# %%
# Solve the optimization problem.
# Give some rough estimates for the trajectories.

initial_guess = np.ones(prob.num_free)

# Find the optimal solution.
for i in range(1):
solution, info = prob.solve(initial_guess)
initial_guess = solution
print(info['status_msg'])
print(f'Objectve is: {info['obj_val']:.8f}, ' +
f'as per the book it is {2.95369916}, so the deviation is: ' +
f'{(info['obj_val'] -2.95369916) /2.95369916*100 :.5e} %')
# %%
# Plot the optimal state and input trajectories.
prob.plot_trajectories(solution)

# %%
# Plot the constraint violations.
prob.plot_constraint_violations(solution)

# %%
# Plot the objective function as a function of optimizer iteration.
prob.plot_objective_value()

# %%
# Plot the Difference between the two Solutions.
# ----------------------------------------------
diffy1 = solution1[: num_nodes] - solution[: num_nodes]
diffy2 = solution1[num_nodes: 2*num_nodes] - solution[num_nodes: 2*num_nodes]
diffu = solution1[2*num_nodes:] - solution[3*num_nodes:]
times = np.linspace(t0, tf, num_nodes)

fig, ax = plt.subplots(3, 1, figsize=(7, 4), sharex=True, constrained_layout=True)
ax[0].plot(times, diffy1, label='Delta y1')
ax[0].legend()
ax[1].plot(times, diffy2, label='Delta y2')
ax[1].legend()
ax[2].plot(times, diffu, label='Delta u')
ax[2].legend()
ax[2].set_xlabel('Time')
ax[0].set_title('Differences between the two solutions')
avoid_printing = True
# sphinx_gallery_thumbnail_number = 2
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