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Add Vyasarayani example to the gallery, but left multi option version in examples dir. #199

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83 changes: 0 additions & 83 deletions docs/examples.rst

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1 change: 0 additions & 1 deletion docs/index.rst
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theory
examples/index.rst
examples
api

.. include:: ../README.rst
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153 changes: 153 additions & 0 deletions examples-gallery/plot_vyasarayani.py
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"""
Multi-minimum Parameter Identification
======================================

This example is taken from the following paper:

Vyasarayani, Chandrika P., Thomas Uchida, Ashwin Carvalho, and John McPhee.
"Parameter Identification in Dynamic Systems Using the Homotopy Optimization
Approach". Multibody System Dynamics 26, no. 4 (2011): 411-24.

In Section 3.1 there is a simple example of a single pendulum parameter
identification that has many local minima.

For the following differential equations that describe a single pendulum acting
under the influence of gravity, the goals is to identify the parameter p given
noisy measurements of the angle, y1.

::

-- -- -- --
| y1' | | y2 |
y' = f(y, t) = | | = | |
| y2' | | -p*sin(y1) |
-- -- -- --

"""

import numpy as np
import sympy as sm
from scipy.integrate import odeint
import matplotlib.pyplot as plt
from opty import Problem

# %%
# Specify the symbolic equations of motion.
p, t = sm.symbols('p, t')
y1, y2 = [f(t) for f in sm.symbols('y1, y2', cls=sm.Function)]
y = sm.Matrix([y1, y2])
f = sm.Matrix([y2, -p*sm.sin(y1)])
eom = y.diff(t) - f
sm.pprint(eom)

# %%
# Generate some data by integrating the equations of motion.
duration = 50.0
num_nodes = 5000
interval = duration/(num_nodes - 1)
time = np.linspace(0.0, duration, num=num_nodes)

p_val = 10.0
y0 = [np.pi/6.0, 0.0]


def eval_f(y, t, p):
return np.array([y[1], -p*np.sin(y[0])])


y_meas = odeint(eval_f, y0, time, args=(p_val,))
y1_meas = y_meas[:, 0]
y2_meas = y_meas[:, 1]

# %%
# Add measurement noise.
y1_meas += np.random.normal(scale=0.05, size=y1_meas.shape)
y2_meas += np.random.normal(scale=0.1, size=y2_meas.shape)


# %%
# Setup the optimization problem to minimize the error in the simulated angle
# and the measured angle. The midpoint integration method is preferable to the
# backward Euler method because no artificial damping is introduced.
def obj(free):
"""Minimize the error in the angle, y1."""
return interval*np.sum((y1_meas - free[:num_nodes])**2)


def obj_grad(free):
grad = np.zeros_like(free)
grad[:num_nodes] = 2.0*interval*(free[:num_nodes] - y1_meas)
return grad


prob = Problem(obj, obj_grad, eom, (y1, y2), num_nodes, interval,
time_symbol=t, integration_method='midpoint')

num_states = len(y)

# %%
# Give noisy measurements as the initial state guess and a random positive
# values as the parameter guess.
initial_guess = np.hstack((y1_meas, y2_meas, 100.0*np.random.random(1)))

# %%
# Find the optimal solution.
solution, info = prob.solve(initial_guess)
p_sol = solution[-1]

# %%
# Print the result.
known_msg = "Known value of p = {}".format(p_val)
guess_msg = "Initial guess for p = {}".format(initial_guess[-1])
identified_msg = "Identified value of p = {}".format(p_sol)
divider = '='*max(len(known_msg), len(identified_msg))

print(divider)
print(known_msg)
print(guess_msg)
print(identified_msg)
print(divider)

# %%
# Simulate with the identified parameter.
y_sim = odeint(eval_f, y0, time, args=(p_sol,))
y1_sim = y_sim[:, 0]
y2_sim = y_sim[:, 1]

# %%
# Plot results
fig_y1, axes_y1 = plt.subplots(3, 1, layout='constrained')

legend = ['measured', 'initial guess', 'direct collocation solution',
'identified simulated']

axes_y1[0].plot(time, y1_meas, '.k',
time, initial_guess[:num_nodes], '.b',
time, solution[:num_nodes], '.r',
time, y1_sim, 'g')
axes_y1[0].set_xlabel('Time [s]')
axes_y1[0].set_ylabel('y1 [rad]')
axes_y1[0].legend(legend)

axes_y1[1].set_title('Initial Guess Constraint Violations')
axes_y1[1].plot(prob.con(initial_guess)[:num_nodes - 1])
axes_y1[2].set_title('Solution Constraint Violations')
axes_y1[2].plot(prob.con(solution)[:num_nodes - 1])

# %%
fig_y2, axes_y2 = plt.subplots(3, 1, layout='constrained')

axes_y2[0].plot(time, y2_meas, '.k',
time, initial_guess[num_nodes:-1], '.b',
time, solution[num_nodes:-1], '.r',
time, y2_sim, 'g')
axes_y2[0].set_xlabel('Time [s]')
axes_y2[0].set_ylabel('y2 [rad]')
axes_y2[0].legend(legend)

axes_y2[1].set_title('Initial Guess Constraint Violations')
axes_y2[1].plot(prob.con(initial_guess)[num_nodes - 1:])
axes_y2[2].set_title('Solution Constraint Violations')
axes_y2[2].plot(prob.con(solution)[num_nodes - 1:])

plt.show()
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