def test_brachistochrone_for_docs_radau(self):
from openmdao.api import Problem, Group, ScipyOptimizeDriver, DirectSolver, SqliteRecorder
from openmdao.utils.assert_utils import assert_rel_error
import dymos as dm
from dymos.examples.plotting import plot_results
from dymos.examples.brachistochrone import BrachistochroneODE
#
# Initialize the Problem and the optimization driver
#
p = Problem(model=Group())
p.driver = ScipyOptimizeDriver()
p.driver.options['dynamic_simul_derivs'] = True
#
# Create a trajectory and add a phase to it
#
traj = p.model.add_subsystem('traj', dm.Trajectory())
phase = traj.add_phase(
'phase0',
dm.Phase(ode_class=BrachistochroneODE,
transcription=dm.Radau(num_segments=10)))
#
# Set the variables
#
phase.set_time_options(initial_bounds=(0, 0), duration_bounds=(.5, 10))
phase.set_state_options('x', fix_initial=True, fix_final=True)
phase.set_state_options('y', fix_initial=True, fix_final=True)
phase.set_state_options('v', fix_initial=True)
phase.add_control('theta', units='deg', lower=0.01, upper=179.9)
phase.add_design_parameter('g', units='m/s**2', opt=False, val=9.80665)
#
# Minimize time at the end of the phase
#
phase.add_objective('time', loc='final', scaler=10)
p.model.linear_solver = DirectSolver()
#
# Setup the Problem
#
p.setup()
#
# Set the initial values
#
p['traj.phase0.t_initial'] = 0.0
p['traj.phase0.t_duration'] = 2.0
p['traj.phase0.states:x'] = phase.interpolate(ys=[0, 10],
nodes='state_input')
p['traj.phase0.states:y'] = phase.interpolate(ys=[10, 5],
nodes='state_input')
p['traj.phase0.states:v'] = phase.interpolate(ys=[0, 9.9],
nodes='state_input')
p['traj.phase0.controls:theta'] = phase.interpolate(
ys=[5, 100.5], nodes='control_input')
#
# Solve for the optimal trajectory
#
p.run_driver()
# Test the results
assert_rel_error(self,
p.get_val('traj.phase0.timeseries.time')[-1],
1.8016,
tolerance=1.0E-3)
# Generate the explicitly simulated trajectory
exp_out = traj.simulate()
plot_results(
[('traj.phase0.timeseries.states:x',
'traj.phase0.timeseries.states:y', 'x (m)', 'y (m)'),
('traj.phase0.timeseries.time',
'traj.phase0.timeseries.controls:theta', 'time (s)',
'theta (deg)')],
title='Brachistochrone Solution\nRadau Pseudospectral Method',
p_sol=p,
p_sim=exp_out)
plt.show()
def flying_robot_direct_collocation(transcription='gauss-lobatto',
compressed=True):
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = 'SLSQP'
p.driver.declare_coloring()
if transcription == 'gauss-lobatto':
t = dm.GaussLobatto(num_segments=8, order=5, compressed=compressed)
elif transcription == "radau-ps":
t = dm.Radau(num_segments=8, order=5, compressed=compressed)
else:
raise ValueError('invalid transcription')
traj = p.model.add_subsystem('traj', dm.Trajectory())
phase = traj.add_phase('phase0',
dm.Phase(ode_class=FlyingRobotODE, transcription=t))
phase.set_time_options(fix_initial=True,
fix_duration=False,
duration_bounds=(0.1, 1E4),
units='s')
phase.add_state('x',
shape=(2, ),
fix_initial=True,
fix_final=True,
rate_source='v',
units='m')
phase.add_state('v',
shape=(2, ),
fix_initial=True,
fix_final=True,
rate_source='u',
units='m/s')
phase.add_state('J',
fix_initial=True,
fix_final=False,
rate_source='u_mag2',
units='m**2/s**3')
phase.add_control('u',
units='m/s**2',
shape=(2, ),
scaler=0.01,
continuity=False,
rate_continuity=False,
rate2_continuity=False,
lower=-1,
upper=1)
# Minimize the control effort
phase.add_objective('time', loc='final')
p.model.linear_solver = om.DirectSolver()
p.setup(check=True)
p['traj.phase0.t_initial'] = 0.0
p['traj.phase0.t_duration'] = 1.0
p['traj.phase0.states:x'] = phase.interp('x',
[[0.0, 0.0], [-100.0, 100.0]])
p['traj.phase0.states:v'] = phase.interp('v', [[0.0, 0.0], [0.0, 0.0]])
p['traj.phase0.controls:u'] = phase.interp('u', [[1, 1], [-1, -1]])
p.run_driver()
return p
def test_brachistochrone_for_docs_coloring_demo_solve_segments(self):
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
import dymos as dm
from dymos.examples.plotting import plot_results
from dymos.examples.brachistochrone import BrachistochroneODE
#
# Initialize the Problem and the optimization driver
#
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver(optimizer='IPOPT')
p.driver.opt_settings['print_level'] = 4
# p.driver.declare_coloring()
#
# Create a trajectory and add a phase to it
#
traj = p.model.add_subsystem('traj', dm.Trajectory())
#
# In this case the phase has many segments to demonstrate the impact of coloring.
#
phase = traj.add_phase(
'phase0',
dm.Phase(ode_class=BrachistochroneODE,
transcription=dm.Radau(num_segments=100,
solve_segments='forward')))
#
# Set the variables
#
phase.set_time_options(fix_initial=True, duration_bounds=(.5, 10))
phase.add_state('x', fix_initial=True)
phase.add_state('y', fix_initial=True)
phase.add_state('v', fix_initial=True)
phase.add_control('theta',
continuity=True,
rate_continuity=True,
units='deg',
lower=0.01,
upper=179.9)
phase.add_parameter('g', units='m/s**2', val=9.80665)
#
# Replace state terminal bounds with nonlinear constraints
#
phase.add_boundary_constraint('x', loc='final', equals=10)
phase.add_boundary_constraint('y', loc='final', equals=5)
#
# Minimize time at the end of the phase
#
phase.add_objective('time', loc='final', scaler=10)
p.model.linear_solver = om.DirectSolver()
#
# Setup the Problem
#
p.setup()
#
# Set the initial values
#
p['traj.phase0.t_initial'] = 0.0
p['traj.phase0.t_duration'] = 2.0
p.set_val('traj.phase0.states:x', phase.interp('x', ys=[0, 10]))
p.set_val('traj.phase0.states:y', phase.interp('y', ys=[10, 5]))
p.set_val('traj.phase0.states:v', phase.interp('v', ys=[0, 9.9]))
p.set_val('traj.phase0.controls:theta',
phase.interp('theta', ys=[5, 100.5]))
#
# Solve for the optimal trajectory
#
dm.run_problem(p)
# Test the results
assert_near_equal(p.get_val('traj.phase0.timeseries.time')[-1],
1.8016,
tolerance=1.0E-3)
# Generate the explicitly simulated trajectory
exp_out = traj.simulate()
plot_results(
[('traj.phase0.timeseries.states:x',
'traj.phase0.timeseries.states:y', 'x (m)', 'y (m)'),
('traj.phase0.timeseries.time',
'traj.phase0.timeseries.controls:theta', 'time (s)',
'theta (deg)')],
title='Brachistochrone Solution\nRadau Pseudospectral Method',
p_sol=p,
p_sim=exp_out)
plt.show()
def test_brachistochrone_vector_boundary_constraints_radau_partial_indices(
self):
p = om.Problem(model=om.Group())
p.driver = om.ScipyOptimizeDriver()
p.driver.declare_coloring()
phase = dm.Phase(ode_class=BrachistochroneVectorStatesODE,
transcription=dm.Radau(num_segments=20, order=3))
p.model.add_subsystem('phase0', phase)
phase.set_time_options(fix_initial=True, duration_bounds=(.5, 10))
phase.add_state(
'pos',
shape=(2, ),
rate_source=BrachistochroneVectorStatesODE.states['pos']
['rate_source'],
units=BrachistochroneVectorStatesODE.states['pos']['units'],
fix_initial=True,
fix_final=[True, False])
phase.add_state(
'v',
rate_source=BrachistochroneVectorStatesODE.states['v']
['rate_source'],
targets=BrachistochroneVectorStatesODE.states['v']['targets'],
units=BrachistochroneVectorStatesODE.states['v']['units'],
fix_initial=True,
fix_final=False)
phase.add_control(
'theta',
units='deg',
targets=BrachistochroneVectorStatesODE.parameters['theta']
['targets'],
rate_continuity=False,
lower=0.01,
upper=179.9)
phase.add_design_parameter(
'g',
targets=BrachistochroneVectorStatesODE.parameters['g']['targets'],
units='m/s**2',
opt=False,
val=9.80665)
phase.add_boundary_constraint('pos',
loc='final',
equals=5,
indices=[1])
# Minimize time at the end of the phase
phase.add_objective('time', loc='final', scaler=10)
p.model.linear_solver = om.DirectSolver()
p.setup(check=True, force_alloc_complex=True)
p['phase0.t_initial'] = 0.0
p['phase0.t_duration'] = 2.0
pos0 = [0, 10]
posf = [10, 5]
p['phase0.states:pos'] = phase.interpolate(ys=[pos0, posf],
nodes='state_input')
p['phase0.states:v'] = phase.interpolate(ys=[0, 9.9],
nodes='state_input')
p['phase0.controls:theta'] = phase.interpolate(ys=[5, 100],
nodes='control_input')
p['phase0.design_parameters:g'] = 9.80665
p.run_driver()
assert_rel_error(self,
p.get_val('phase0.time')[-1],
1.8016,
tolerance=1.0E-3)
# Plot results
if SHOW_PLOTS:
p.run_driver()
exp_out = phase.simulate(times_per_seg=20)
fig, ax = plt.subplots()
fig.suptitle('Brachistochrone Solution')
x_imp = p.get_val('phase0.timeseries.states:pos')[:, 0]
y_imp = p.get_val('phase0.timeseries.states:pos')[:, 1]
x_exp = exp_out.get_val('phase0.timeseries.states:pos')[:, 0]
y_exp = exp_out.get_val('phase0.timeseries.states:pos')[:, 1]
ax.plot(x_imp, y_imp, 'ro', label='implicit')
ax.plot(x_exp, y_exp, 'b-', label='explicit')
ax.set_xlabel('x (m)')
ax.set_ylabel('y (m)')
ax.grid(True)
ax.legend(loc='upper right')
fig, ax = plt.subplots()
fig.suptitle('Brachistochrone Solution')
x_imp = p.get_val('phase0.timeseries.time')
y_imp = p.get_val('phase0.timeseries.control_rates:theta_rate2')
x_exp = exp_out.get_val('phase0.timeseries.time')
y_exp = exp_out.get_val(
'phase0.timeseries.control_rates:theta_rate2')
ax.plot(x_imp, y_imp, 'ro', label='implicit')
ax.plot(x_exp, y_exp, 'b-', label='explicit')
ax.set_xlabel('time (s)')
ax.set_ylabel('theta rate2 (rad/s**2)')
ax.grid(True)
ax.legend(loc='lower right')
plt.show()
return p
def test_brachistochrone_integrated_parameter_radau_ps(self):
import numpy as np
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
import dymos as dm
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = 'SLSQP'
p.driver.declare_coloring()
phase = dm.Phase(ode_class=BrachistochroneODE,
transcription=dm.Radau(num_segments=10))
p.model.add_subsystem('phase0', phase)
phase.set_time_options(initial_bounds=(0, 0),
duration_bounds=(.5, 10),
units='s')
phase.add_state('x',
fix_initial=True,
fix_final=True,
rate_source='xdot',
units='m')
phase.add_state('y',
fix_initial=True,
fix_final=True,
rate_source='ydot',
units='m')
phase.add_state('v', fix_initial=True, rate_source='vdot', units='m/s')
phase.add_state('theta',
fix_initial=False,
rate_source='theta_dot',
lower=1E-3)
# theta_dot has no target, therefore we need to explicitly set the units and shape.
phase.add_parameter('theta_dot',
units='deg/s',
shape=(1, ),
opt=True,
lower=0,
upper=100)
phase.add_parameter('g', units='m/s**2', opt=False, val=9.80665)
# Minimize time at the end of the phase
phase.add_objective('time', loc='final', scaler=10)
p.model.linear_solver = om.DirectSolver()
p.setup()
p['phase0.t_initial'] = 0.0
p['phase0.t_duration'] = 2.0
p['phase0.states:x'] = phase.interpolate(ys=[0, 10],
nodes='state_input')
p['phase0.states:y'] = phase.interpolate(ys=[10, 5],
nodes='state_input')
p['phase0.states:v'] = phase.interpolate(ys=[0, 9.9],
nodes='state_input')
p['phase0.states:theta'] = np.radians(
phase.interpolate(ys=[0.05, 100.0], nodes='state_input'))
p['phase0.parameters:theta_dot'] = 60.0
# Solve for the optimal trajectory
dm.run_problem(p, refine_iteration_limit=5)
# Test the results
assert_near_equal(p.get_val('phase0.timeseries.time')[-1],
1.8016,
tolerance=1.0E-3)
sim_out = phase.simulate(times_per_seg=20)
t_sol = p.get_val('phase0.timeseries.time')
x_sol = p.get_val('phase0.timeseries.states:x')
y_sol = p.get_val('phase0.timeseries.states:y')
v_sol = p.get_val('phase0.timeseries.states:v')
theta_sol = p.get_val('phase0.timeseries.states:theta')
t_sim = sim_out.get_val('phase0.timeseries.time')
x_sim = sim_out.get_val('phase0.timeseries.states:x')
y_sim = sim_out.get_val('phase0.timeseries.states:y')
v_sim = sim_out.get_val('phase0.timeseries.states:v')
theta_sim = sim_out.get_val('phase0.timeseries.states:theta')
assert_timeseries_near_equal(t_sol,
x_sol,
t_sim,
x_sim,
tolerance=1.0E-3,
num_points=10)
assert_timeseries_near_equal(t_sol,
y_sol,
t_sim,
y_sim,
tolerance=1.0E-3,
num_points=10)
assert_timeseries_near_equal(t_sol,
v_sol,
t_sim,
v_sim,
tolerance=1.0E-3,
num_points=10)
assert_timeseries_near_equal(t_sol,
theta_sol,
t_sim,
theta_sim,
tolerance=1.0E-3,
num_points=10)
import dymos as dm
from donner_sub_ode import DonnerSubODE
# Create the problem
p = om.Problem(model=om.Group())
# Add the trajectory (optional for single phase problems)
traj = dm.Trajectory()
# Create the phases
phase0 = dm.Phase(ode_class=DonnerSubODE,
transcription=dm.GaussLobatto(num_segments=10, order=3, compressed=False))
phase1 = dm.Phase(ode_class=DonnerSubODE,
transcription=dm.Radau(num_segments=10, order=3, compressed=False))
# Add the phase to the trajectory, and the trajectory to the model
traj.add_phase('phase0', phase=phase0)
traj.add_phase('phase1', phase=phase1)
traj.link_phases(phases=['phase0', 'phase1'], vars=['time', 'x', 'y', 'phi'])
p.model.add_subsystem('traj', traj)
#
# Configure the first phase
#
phase0.set_time_options(units=None, targets=['threat_comp.time'], fix_initial=True, duration_bounds=(0.1, 100))
phase0.add_state('x', rate_source='eom_comp.dx_dt', targets=['nav_comp.x'], fix_initial=True, fix_final=False)
phase0.add_state('y', rate_source='eom_comp.dy_dt', targets=['nav_comp.y'], fix_initial=True, fix_final=False)
# phase0.add_input_parameter('v', targets=['eom_comp.v'])
def test_objective_parameter_radau(self):
p = om.Problem(model=om.Group())
p.driver = om.ScipyOptimizeDriver()
p.driver.declare_coloring()
phase = dm.Phase(ode_class=BrachistochroneODE,
transcription=dm.Radau(num_segments=20,
order=3,
compressed=True))
p.model.add_subsystem('phase0', phase)
phase.set_time_options(fix_initial=True, duration_bounds=(4, 10))
phase.add_state(
'x',
rate_source=BrachistochroneODE.states['x']['rate_source'],
units=BrachistochroneODE.states['x']['units'],
fix_initial=True,
fix_final=True,
solve_segments=False)
phase.add_state(
'y',
rate_source=BrachistochroneODE.states['y']['rate_source'],
units=BrachistochroneODE.states['y']['units'],
fix_initial=True,
fix_final=True,
solve_segments=False)
phase.add_state(
'v',
rate_source=BrachistochroneODE.states['v']['rate_source'],
targets=BrachistochroneODE.states['v']['targets'],
units=BrachistochroneODE.states['v']['units'],
fix_initial=True,
fix_final=False,
solve_segments=False)
phase.add_control(
'theta',
continuity=True,
rate_continuity=True,
opt=True,
targets=BrachistochroneODE.parameters['theta']['targets'],
units='deg',
lower=0.01,
upper=179.9,
ref=1,
ref0=0)
phase.add_parameter(
'g',
targets=BrachistochroneODE.parameters['g']['targets'],
opt=True,
units='m/s**2',
val=9.80665)
# Minimize time at the end of the phase
phase.add_objective('g')
p.model.options['assembled_jac_type'] = 'csc'
p.model.linear_solver = om.DirectSolver()
p.setup(check=True)
p['phase0.t_initial'] = 0.0
p['phase0.t_duration'] = 2.0
p['phase0.states:x'] = phase.interpolate(ys=[0, 10],
nodes='state_input')
p['phase0.states:y'] = phase.interpolate(ys=[10, 5],
nodes='state_input')
p['phase0.states:v'] = phase.interpolate(ys=[0, 9.9],
nodes='state_input')
p['phase0.controls:theta'] = phase.interpolate(ys=[5, 100],
nodes='control_input')
p['phase0.parameters:g'] = 9.80665
p.run_driver()
assert_near_equal(p['phase0.t_duration'], 10, tolerance=1.0E-3)
n_nodes = 60
seed_perturbation = np.zeros(n_nodes)
# seed_perturbation[2] = 1.e-6
# Add an indep_var_comp that will talk to external calls from pyStatReduce
random_perturbations = p.model.add_subsystem('random_perturbations', IndepVarComp())
random_perturbations.add_output('rho_pert', val=seed_perturbation, units='kg/m**3',
desc="perturbations introduced into the density data")
#
# Instantiate the trajectory and phase
#
traj = dm.Trajectory()
phase = dm.Phase(ode_class=MinTimeClimbODE,
transcription=dm.Radau(num_segments=15, compressed=True))
traj.add_phase('phase0', phase)
p.model.add_subsystem('traj', traj)
#
# Set the options on the optimization variables
#
phase.set_time_options(fix_initial=True, duration_bounds=(50, 400),
duration_ref=100.0)
phase.set_state_options('r', fix_initial=True, lower=0, upper=1.0E6,
ref=1.0E3, defect_ref=1.0E3, units='m')
phase.set_state_options('h', fix_initial=True, lower=0, upper=20000.0,
def test_results(self):
# begin code for paper
import numpy as np
from scipy.interpolate import interp1d
import matplotlib.pyplot as plt
import openmdao.api as om
import dymos as dm
from dymos.models.atmosphere.atmos_1976 import USatm1976Data as USatm1976Data
# CREATE an atmosphere interpolant
english_to_metric_rho = om.unit_conversion('slug/ft**3', 'kg/m**3')[0]
english_to_metric_alt = om.unit_conversion('ft', 'm')[0]
rho_interp = interp1d(np.array(USatm1976Data.alt * english_to_metric_alt, dtype=complex),
np.array(USatm1976Data.rho * english_to_metric_rho, dtype=complex),
kind='linear')
class CannonballSize(om.ExplicitComponent):
"""
Static calculations performed before the dynamic model
"""
def setup(self):
self.add_input(name='radius', val=1.0,
desc='cannonball radius', units='m')
self.add_input(name='density', val=7870.,
desc='cannonball density', units='kg/m**3')
self.add_output(name='mass', shape=(1,),
desc='cannonball mass', units='kg')
self.add_output(name='area', shape=(1,),
desc='aerodynamic reference area', units='m**2')
self.declare_partials(of='*', wrt='*', method='cs')
def compute(self, inputs, outputs):
radius = inputs['radius']
rho = inputs['density']
outputs['mass'] = (4 / 3.) * rho * np.pi * radius ** 3
outputs['area'] = np.pi * radius ** 2
class CannonballODE(om.ExplicitComponent):
"""
Cannonball ODE assuming flat earth and accounting for air resistance
"""
def initialize(self):
self.options.declare('num_nodes', types=int)
def setup(self):
nn = self.options['num_nodes']
# static parameters
self.add_input('mass', units='kg')
self.add_input('area', units='m**2')
# time varying inputs
self.add_input('alt', units='m', shape=nn)
self.add_input('v', units='m/s', shape=nn)
self.add_input('gam', units='rad', shape=nn)
# state rates
self.add_output('v_dot', shape=nn, units='m/s**2')
self.add_output('gam_dot', shape=nn, units='rad/s')
self.add_output('h_dot', shape=nn, units='m/s')
self.add_output('r_dot', shape=nn, units='m/s')
self.add_output('ke', shape=nn, units='J')
# Ask OpenMDAO to compute the partial derivatives using complex-step
# with a partial coloring algorithm for improved performance
self.declare_partials('*', '*', method='cs')
self.declare_coloring(wrt='*', method='cs')
def compute(self, inputs, outputs):
gam = inputs['gam']
v = inputs['v']
alt = inputs['alt']
m = inputs['mass']
S = inputs['area']
CD = 0.5 # good assumption for a sphere
GRAVITY = 9.80665 # m/s**2
# handle complex-step gracefully from the interpolant
if np.iscomplexobj(alt):
rho = rho_interp(inputs['alt'])
else:
rho = rho_interp(inputs['alt']).real
q = 0.5 * rho * inputs['v'] ** 2
qS = q * S
D = qS * CD
cgam = np.cos(gam)
sgam = np.sin(gam)
outputs['v_dot'] = - D / m - GRAVITY * sgam
outputs['gam_dot'] = -(GRAVITY / v) * cgam
outputs['h_dot'] = v * sgam
outputs['r_dot'] = v * cgam
outputs['ke'] = 0.5 * m * v ** 2
p = om.Problem()
###################################
# Co-design part of the model,
# static analysis outside of Dymos
###################################
static_calcs = p.model.add_subsystem('static_calcs', CannonballSize())
static_calcs.add_design_var('radius', lower=0.01, upper=0.10,
ref0=0.01, ref=0.10)
p.model.connect('static_calcs.mass', 'traj.parameters:mass')
p.model.connect('static_calcs.area', 'traj.parameters:area')
traj = p.model.add_subsystem('traj', dm.Trajectory())
# Declare parameters that will be constant across
# the two phases of the trajectory, so we can connect to it only once
traj.add_parameter('mass', units='kg', val=0.01, static_target=True)
traj.add_parameter('area', units='m**2', static_target=True)
tx = dm.Radau(num_segments=5, order=3, compressed=True)
ascent = dm.Phase(transcription=tx, ode_class=CannonballODE)
traj.add_phase('ascent', ascent)
###################################
# first phase: ascent
###################################
# All initial states except flight path angle are fixed
ascent.add_state('r', units='m', rate_source='r_dot',
fix_initial=True, fix_final=False)
ascent.add_state('h', units='m', rate_source='h_dot',
fix_initial=True, fix_final=False)
ascent.add_state('v', units='m/s', rate_source='v_dot',
fix_initial=False, fix_final=False)
# Final flight path angle is fixed (
# we will set it to zero so that the phase ends at apogee)
ascent.add_state('gam', units='rad', rate_source='gam_dot',
fix_initial=False, fix_final=True)
ascent.set_time_options(fix_initial=True, duration_bounds=(1, 100),
duration_ref=100, units='s')
ascent.add_parameter('mass', units='kg', val=0.01, static_target=True)
ascent.add_parameter('area', units='m**2', static_target=True)
# Limit the initial muzzle energy to create a well posed problem
# with respect to cannonball size and initial velocity
ascent.add_boundary_constraint('ke', loc='initial', units='J',
upper=400000, lower=0, ref=100000)
###################################
# second phase: descent
###################################
tx = dm.GaussLobatto(num_segments=5, order=3, compressed=True)
descent = dm.Phase(transcription=tx, ode_class=CannonballODE)
traj.add_phase('descent', descent)
# All initial states and time are free so their
# values can be linked to the final ascent values
# Final altitude is fixed to 0 to ensure final impact on the ground
descent.add_state('r', units='m', rate_source='r_dot',
fix_initial=False, fix_final=False)
descent.add_state('h', units='m', rate_source='h_dot',
fix_initial=False, fix_final=True)
descent.add_state('gam', units='rad', rate_source='gam_dot',
fix_initial=False, fix_final=False)
descent.add_state('v', units='m/s', rate_source='v_dot',
fix_initial=False, fix_final=False)
descent.set_time_options(initial_bounds=(.5, 100), duration_bounds=(.5, 100),
duration_ref=100, units='s')
descent.add_parameter('mass', units='kg', val=0.01, static_target=True)
descent.add_parameter('area', units='m**2', static_target=True)
# Link Phases (link time and all state variables)
traj.link_phases(phases=['ascent', 'descent'], vars=['*'])
# maximize range
descent.add_objective('r', loc='final', ref=-1.0)
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = 'SLSQP'
p.driver.declare_coloring()
# Finish Problem Setup
p.setup()
# Set Initial guesses for static dvs and ascent
p.set_val('static_calcs.radius', 0.05, units='m')
p.set_val('traj.ascent.t_duration', 10.0)
p.set_val('traj.ascent.states:r', ascent.interp('r', [0, 100]))
p.set_val('traj.ascent.states:h', ascent.interp('h', [0, 100]))
p.set_val('traj.ascent.states:v', ascent.interp('v', [200, 150]))
p.set_val('traj.ascent.states:gam', ascent.interp('gam', [25, 0]), units='deg')
# more intitial guesses for descent
p.set_val('traj.descent.t_initial', 10.0)
p.set_val('traj.descent.t_duration', 10.0)
p.set_val('traj.descent.states:r', descent.interp('r', [100, 200]))
p.set_val('traj.descent.states:h', descent.interp('h', [100, 0]))
p.set_val('traj.descent.states:v', descent.interp('v', [150, 200]))
p.set_val('traj.descent.states:gam', descent.interp('gam', [0, -45]), units='deg')
dm.run_problem(p, simulate=True, make_plots=True)
fig, ax = plt.subplots()
x0 = p.get_val('traj.ascent.timeseries.states:r', units='m')
y0 = p.get_val('traj.ascent.timeseries.states:h', units='m')
x1 = p.get_val('traj.descent.timeseries.states:r', units='m')
y1 = p.get_val('traj.descent.timeseries.states:h', units='m')
tab20 = plt.cm.get_cmap('tab20').colors
ax.plot(x0, y0, marker='o', label='ascent', color=tab20[0])
ax.plot(x1, y1, marker='o', label='descent', color=tab20[1])
ax.legend(loc='best')
ax.set_xlabel('range (m)')
ax.set_ylabel('height (m)')
fig.savefig('cannonball_hr.png', bbox_inches='tight')
# End code for paper
assert_near_equal(x1[-1], 3064, tolerance=1.0E-4)
def test_ex_double_integrator_input_times_compressed(self):
"""
Tests that externally connected t_initial and t_duration function as expected.
"""
compressed = True
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.declare_coloring()
times_ivc = p.model.add_subsystem('times_ivc',
om.IndepVarComp(),
promotes_outputs=['t0', 'tp'])
times_ivc.add_output(name='t0', val=0.0, units='s')
times_ivc.add_output(name='tp', val=1.0, units='s')
transcription = dm.Radau(num_segments=20,
order=3,
compressed=compressed)
phase = dm.Phase(ode_class=DoubleIntegratorODE,
transcription=transcription)
p.model.add_subsystem('phase0', phase)
p.model.connect('t0', 'phase0.t_initial')
p.model.connect('tp', 'phase0.t_duration')
phase.set_time_options(input_initial=True,
input_duration=True,
units='s')
phase.add_state('v',
fix_initial=True,
fix_final=True,
rate_source='u',
units='m/s')
phase.add_state('x', fix_initial=True, rate_source='v', units='m')
phase.add_control('u',
units='m/s**2',
scaler=0.01,
continuity=False,
rate_continuity=False,
rate2_continuity=False,
shape=(1, ),
lower=-1.0,
upper=1.0)
# Maximize distance travelled in one second.
phase.add_objective('x', loc='final', scaler=-1)
p.model.linear_solver = om.DirectSolver()
p.setup(check=True)
p['t0'] = 0.0
p['tp'] = 1.0
p['phase0.states:x'] = phase.interp('x', [0, 0.25])
p['phase0.states:v'] = phase.interp('v', [0, 0])
p['phase0.controls:u'] = phase.interp('u', [1, -1])
p.run_driver()
assert_near_equal(p.get_val('phase0.timeseries.states:x')[-1, ...],
[0.25],
tolerance=1.0E-8)
def _make_problem(self, transcription, num_seg, transcription_order=3):
p = om.Problem(model=om.Group())
p.driver = om.ScipyOptimizeDriver()
# Compute sparsity/coloring when run_driver is called
p.driver.declare_coloring()
t = {
'gauss-lobatto':
dm.GaussLobatto(num_segments=num_seg, order=transcription_order),
'radau-ps':
dm.Radau(num_segments=num_seg, order=transcription_order)
}
phase = dm.Phase(ode_class=_BrachistochroneTestODE,
transcription=t[transcription])
p.model.add_subsystem('phase0', phase)
phase.set_time_options(initial_bounds=(1, 1),
duration_bounds=(.5, 10),
units='s',
time_phase_targets=['time_phase'],
t_duration_targets=['t_duration'],
t_initial_targets=['t_initial'],
targets=['time'])
phase.add_state('x', fix_initial=True, rate_source='xdot', units='m')
phase.add_state('y', fix_initial=True, rate_source='ydot', units='m')
phase.add_state('v',
fix_initial=True,
rate_source='vdot',
targets=['v'],
units='m/s')
phase.add_control('theta',
units='deg',
rate_continuity=True,
lower=0.01,
upper=179.9,
targets=['theta'])
phase.add_parameter('g',
units='m/s**2',
opt=False,
val=9.80665,
targets=['g'])
phase.add_boundary_constraint('x', loc='final', equals=10)
phase.add_boundary_constraint('y', loc='final', equals=5)
# Minimize time at the end of the phase
phase.add_objective('time', loc='final', scaler=10)
p.model.linear_solver = om.DirectSolver()
p.setup(check=True)
p['phase0.t_initial'] = 1.0
p['phase0.t_duration'] = 3.0
p['phase0.states:x'] = phase.interpolate(ys=[0, 10],
nodes='state_input')
p['phase0.states:y'] = phase.interpolate(ys=[10, 5],
nodes='state_input')
p['phase0.states:v'] = phase.interpolate(ys=[0, 9.9],
nodes='state_input')
p['phase0.controls:theta'] = phase.interpolate(ys=[5, 100.5],
nodes='control_input')
return p
def test_link_bounded_times_final_to_initial(self):
""" Test that linking phases with times that are fixed at the linkage point raises an exception. """
import openmdao.api as om
import dymos as dm
from dymos.examples.cannonball.size_comp import CannonballSizeComp
from dymos.examples.cannonball.cannonball_phase import CannonballPhase
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = 'SLSQP'
p.driver.declare_coloring()
external_params = p.model.add_subsystem('external_params',
om.IndepVarComp())
external_params.add_output('radius', val=0.10, units='m')
external_params.add_output('dens', val=7.87, units='g/cm**3')
external_params.add_design_var('radius',
lower=0.01,
upper=0.10,
ref0=0.01,
ref=0.10)
p.model.add_subsystem('size_comp', CannonballSizeComp())
traj = p.model.add_subsystem('traj', dm.Trajectory())
transcription = dm.Radau(num_segments=5, order=3, compressed=True)
ascent = CannonballPhase(transcription=transcription)
ascent = traj.add_phase('ascent', ascent)
# All initial states except flight path angle are fixed
# Final flight path angle is fixed (we will set it to zero so that the phase ends at apogee)
ascent.set_time_options(initial_bounds=(0, 0),
duration_bounds=(10, 10),
duration_ref=100,
units='s')
ascent.set_state_options('r', fix_initial=True, fix_final=False)
ascent.set_state_options('h', fix_initial=True, fix_final=False)
ascent.set_state_options('gam', fix_initial=False, fix_final=True)
ascent.set_state_options('v', fix_initial=False, fix_final=False)
ascent.add_parameter('S', targets=['aero.S'], units='m**2')
ascent.add_parameter('mass',
targets=['eom.m', 'kinetic_energy.m'],
units='kg')
# Limit the muzzle energy
ascent.add_boundary_constraint('kinetic_energy.ke',
loc='initial',
units='J',
upper=400000,
lower=0,
ref=100000,
shape=(1, ))
# Second Phase (descent)
transcription = dm.GaussLobatto(num_segments=5,
order=3,
compressed=True)
descent = CannonballPhase(transcription=transcription)
traj.add_phase('descent', descent)
# All initial states and time are free (they will be linked to the final states of ascent.
# Final altitude is fixed (we will set it to zero so that the phase ends at ground impact)
descent.set_time_options(initial_bounds=(10, 10),
duration_bounds=(10, 10),
duration_ref=100,
units='s')
descent.add_state('r', )
descent.add_state('h', fix_initial=False, fix_final=True)
descent.add_state('gam', fix_initial=False, fix_final=False)
descent.add_state('v', fix_initial=False, fix_final=False)
descent.add_parameter('S', targets=['aero.S'], units='m**2')
descent.add_parameter('mass',
targets=['eom.m', 'kinetic_energy.m'],
units='kg')
descent.add_objective('r', loc='final', scaler=-1.0)
# Add internally-managed design parameters to the trajectory.
traj.add_parameter('CD',
targets={
'ascent': ['aero.CD'],
'descent': ['aero.CD']
},
val=0.5,
units=None,
opt=False)
traj.add_parameter('CL',
targets={
'ascent': ['aero.CL'],
'descent': ['aero.CL']
},
val=0.0,
units=None,
opt=False)
traj.add_parameter('T',
targets={
'ascent': ['eom.T'],
'descent': ['eom.T']
},
val=0.0,
units='N',
opt=False)
traj.add_parameter('alpha',
targets={
'ascent': ['eom.alpha'],
'descent': ['eom.alpha']
},
val=0.0,
units='deg',
opt=False)
# Add externally-provided design parameters to the trajectory.
# In this case, we connect 'm' to pre-existing input parameters named 'mass' in each phase.
traj.add_parameter('m',
units='kg',
val=1.0,
targets={
'ascent': 'mass',
'descent': 'mass'
})
# In this case, by omitting targets, we're connecting these parameters to parameters
# with the same name in each phase.
traj.add_parameter('S', units='m**2', val=0.005)
# Link Phases (link time and all state variables)
# Note velocity is not included here. Doing so is equivalent to linking kinetic energy,
# and causes a duplicate row in the constraint jacobian.
traj.link_phases(phases=['ascent', 'descent'],
vars=['time', 'r', 'h', 'gam'],
connected=False)
traj.add_linkage_constraint('ascent',
'descent',
'kinetic_energy.ke',
'kinetic_energy.ke',
ref=100000,
connected=False)
# Issue Connections
p.model.connect('external_params.radius', 'size_comp.radius')
p.model.connect('external_params.dens', 'size_comp.dens')
p.model.connect('size_comp.mass', 'traj.parameters:m')
p.model.connect('size_comp.S', 'traj.parameters:S')
with self.assertRaises(ValueError) as e:
p.setup()
self.assertEqual(
str(e.exception),
'Invalid linkage in Trajectory traj: Cannot link final '
'value of "time" in ascent to initial value of "time" in '
'descent. Values on both sides of the linkage are fixed.')
def brachistochrone_min_time(transcription='gauss-lobatto',
num_segments=8,
transcription_order=3,
compressed=True,
optimizer='SLSQP',
simul_derivs=True):
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
OPT, OPTIMIZER = set_pyoptsparse_opt(optimizer, fallback=True)
p.driver.options['optimizer'] = OPTIMIZER
if simul_derivs:
p.driver.declare_coloring()
if transcription == 'gauss-lobatto':
t = dm.GaussLobatto(num_segments=num_segments,
order=transcription_order,
compressed=compressed)
elif transcription == 'radau-ps':
t = dm.Radau(num_segments=num_segments,
order=transcription_order,
compressed=compressed)
elif transcription == 'runge-kutta':
t = dm.RungeKutta(num_segments=num_segments,
order=transcription_order,
compressed=compressed)
phase = dm.Phase(ode_class=BrachistochroneODE, transcription=t)
p.model.add_subsystem('phase0', phase)
phase.set_time_options(fix_initial=True,
duration_bounds=(.5, 10),
units='s')
phase.add_state('x',
fix_initial=True,
fix_final=False,
solve_segments=False,
units='m',
rate_source='xdot')
phase.add_state('y',
fix_initial=True,
fix_final=False,
solve_segments=False,
units='m',
rate_source='ydot')
phase.add_state('v',
fix_initial=True,
fix_final=False,
solve_segments=False,
units='m/s',
rate_source='vdot',
targets=['v'])
phase.add_control('theta',
continuity=True,
rate_continuity=True,
units='deg',
lower=0.01,
upper=179.9,
targets=['theta'])
phase.add_input_parameter('g', units='m/s**2', val=9.80665, targets=['g'])
phase.add_boundary_constraint('x', loc='final', equals=10)
phase.add_boundary_constraint('y', loc='final', equals=5)
# Minimize time at the end of the phase
phase.add_objective('time_phase', loc='final', scaler=10)
p.model.linear_solver = om.DirectSolver()
p.setup(check=True)
p['phase0.t_initial'] = 0.0
p['phase0.t_duration'] = 2.0
p['phase0.states:x'] = phase.interpolate(ys=[0, 10], nodes='state_input')
p['phase0.states:y'] = phase.interpolate(ys=[10, 5], nodes='state_input')
p['phase0.states:v'] = phase.interpolate(ys=[0, 9.9], nodes='state_input')
p['phase0.controls:theta'] = phase.interpolate(ys=[5, 100],
nodes='control_input')
p['phase0.input_parameters:g'] = 9.80665
p.run_driver()
return p
def test_two_burn_orbit_raise_radau_wildcard_add_timeseries_output(self):
import numpy as np
import matplotlib.pyplot as plt
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
from openmdao.utils.general_utils import set_pyoptsparse_opt
import dymos as dm
from dymos.examples.finite_burn_orbit_raise.finite_burn_eom import FiniteBurnODE
traj = dm.Trajectory()
p = om.Problem(model=om.Group())
p.model.add_subsystem('traj', traj)
p.driver = om.pyOptSparseDriver()
_, optimizer = set_pyoptsparse_opt('IPOPT', fallback=True)
p.driver.options['optimizer'] = optimizer
p.driver.declare_coloring()
traj.add_parameter('c', opt=False, val=1.5, units='DU/TU',
targets={'burn1': ['c'], 'coast': ['c'], 'burn2': ['c']})
# First Phase (burn)
burn1 = dm.Phase(ode_class=FiniteBurnODE,
transcription=dm.Radau(num_segments=10, order=3, compressed=True))
burn1 = traj.add_phase('burn1', burn1)
burn1.set_time_options(fix_initial=True, duration_bounds=(.5, 10), units='TU')
burn1.add_state('r', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='r_dot', targets=['r'], units='DU')
burn1.add_state('theta', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='theta_dot', targets=['theta'], units='rad')
burn1.add_state('vr', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='vr_dot', targets=['vr'], units='DU/TU')
burn1.add_state('vt', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='vt_dot', targets=['vt'], units='DU/TU')
burn1.add_state('accel', fix_initial=True, fix_final=False,
rate_source='at_dot', targets=['accel'], units='DU/TU**2')
burn1.add_state('deltav', fix_initial=True, fix_final=False,
rate_source='deltav_dot', units='DU/TU')
burn1.add_control('u1', rate_continuity=True, rate2_continuity=True, units='deg',
scaler=0.01,
rate_continuity_scaler=0.001, rate2_continuity_scaler=0.001,
lower=-30, upper=30, targets=['u1'])
# Second Phase (Coast)
coast = dm.Phase(ode_class=FiniteBurnODE,
transcription=dm.RungeKutta(num_segments=20))
traj.add_phase('coast', coast)
coast.set_time_options(initial_bounds=(0.5, 20), duration_bounds=(.5, 10), duration_ref=10, units='TU')
coast.add_state('r', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='r_dot', targets=['r'], units='DU')
coast.add_state('theta', fix_initial=False, fix_final=False, defect_scaler=100.0,
units='rad', rate_source='theta_dot', targets=['theta'])
coast.add_state('vr', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='vr_dot', targets=['vr'], units='DU/TU')
coast.add_state('vt', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='vt_dot', targets=['vt'], units='DU/TU')
coast.add_state('accel', fix_initial=True, fix_final=False, ref=1.0E-12, defect_ref=1.0E-12,
rate_source='at_dot', targets=['accel'], units='DU/TU**2')
coast.add_state('deltav', fix_initial=False, fix_final=False,
rate_source='deltav_dot', units='DU/TU')
coast.add_parameter('u1', targets=['u1'], opt=False, val=0.0, units='deg')
# Third Phase (burn)
burn2 = dm.Phase(ode_class=FiniteBurnODE,
transcription=dm.Radau(num_segments=10, order=3, compressed=True))
traj.add_phase('burn2', burn2)
burn2.set_time_options(initial_bounds=(0.5, 20), duration_bounds=(.5, 10), initial_ref=10, units='TU')
burn2.add_state('r', fix_initial=False, fix_final=True,
rate_source='r_dot', targets=['r'], units='DU')
burn2.add_state('theta', fix_initial=False, fix_final=False,
rate_source='theta_dot', targets=['theta'], units='rad')
burn2.add_state('vr', fix_initial=False, fix_final=True,
rate_source='vr_dot', targets=['vr'], units='DU/TU')
burn2.add_state('vt', fix_initial=False, fix_final=True,
rate_source='vt_dot', targets=['vt'], units='DU/TU')
burn2.add_state('accel', fix_initial=False, fix_final=False, defect_ref=1.0E-6,
rate_source='at_dot', targets=['accel'], units='DU/TU**2')
burn2.add_state('deltav', fix_initial=False, fix_final=False,
rate_source='deltav_dot', units='DU/TU')
burn2.add_control('u1', targets=['u1'], rate_continuity=True, rate2_continuity=True,
units='deg', scaler=0.01, lower=-30, upper=30)
burn2.add_objective('deltav', loc='final', scaler=1.0)
# demonstrate adding multiple variables at once using wildcard in add_timeseries_output
burn1.add_timeseries_output('pos_*') # match partial variable in ODE outputs (Radau)
coast.add_timeseries_output('pos_*') # match partial variable in ODE outputs (Runge Kutta)
burn2.add_timeseries_output('*') # add all ODE outputs
# Link Phases
traj.link_phases(phases=['burn1', 'coast', 'burn2'],
vars=['time', 'r', 'vr', 'vt', 'deltav'])
traj.link_phases(phases=['burn1', 'burn2'], vars=['accel'])
# Finish Problem Setup
p.model.linear_solver = om.DirectSolver()
p.setup(check=True, force_alloc_complex=True)
# Set Initial Guesses
p.set_val('traj.parameters:c', value=1.5)
p.set_val('traj.burn1.t_initial', value=0.0)
p.set_val('traj.burn1.t_duration', value=2.25)
p.set_val('traj.burn1.states:r',
value=burn1.interpolate(ys=[1, 1.5], nodes='state_input'))
p.set_val('traj.burn1.states:theta',
value=burn1.interpolate(ys=[0, 1.7], nodes='state_input'))
p.set_val('traj.burn1.states:vr',
value=burn1.interpolate(ys=[0, 0], nodes='state_input'))
p.set_val('traj.burn1.states:vt',
value=burn1.interpolate(ys=[1, 1], nodes='state_input'))
p.set_val('traj.burn1.states:accel',
value=burn1.interpolate(ys=[0.1, 0], nodes='state_input'))
p.set_val('traj.burn1.states:deltav',
value=burn1.interpolate(ys=[0, 0.1], nodes='state_input'), )
p.set_val('traj.burn1.controls:u1',
value=burn1.interpolate(ys=[-3.5, 13.0], nodes='control_input'))
p.set_val('traj.coast.t_initial', value=2.25)
p.set_val('traj.coast.t_duration', value=3.0)
p.set_val('traj.coast.states:r',
value=coast.interpolate(ys=[1.3, 1.5], nodes='state_input'))
p.set_val('traj.coast.states:theta',
value=coast.interpolate(ys=[2.1767, 1.7], nodes='state_input'))
p.set_val('traj.coast.states:vr',
value=coast.interpolate(ys=[0.3285, 0], nodes='state_input'))
p.set_val('traj.coast.states:vt',
value=coast.interpolate(ys=[0.97, 1], nodes='state_input'))
p.set_val('traj.coast.states:accel',
value=coast.interpolate(ys=[0, 0], nodes='state_input'))
p.set_val('traj.burn2.t_initial', value=5.25)
p.set_val('traj.burn2.t_duration', value=1.75)
p.set_val('traj.burn2.states:r',
value=burn2.interpolate(ys=[1.8, 3], nodes='state_input'))
p.set_val('traj.burn2.states:theta',
value=burn2.interpolate(ys=[3.2, 4.0], nodes='state_input'))
p.set_val('traj.burn2.states:vr',
value=burn2.interpolate(ys=[.5, 0], nodes='state_input'))
p.set_val('traj.burn2.states:vt',
value=burn2.interpolate(ys=[1, np.sqrt(1 / 3)], nodes='state_input'))
p.set_val('traj.burn2.states:accel',
value=burn2.interpolate(ys=[0.1, 0], nodes='state_input'))
p.set_val('traj.burn2.states:deltav',
value=burn2.interpolate(ys=[0.1, 0.2], nodes='state_input'))
p.set_val('traj.burn2.controls:u1',
value=burn2.interpolate(ys=[1, 1], nodes='control_input'))
p.run_driver()
assert_near_equal(p.get_val('traj.burn2.timeseries.states:deltav')[-1],
0.3995,
tolerance=2.0E-3)
# test ODE output wildcard matching in solve_ivp
exp_out = traj.simulate()
for prob in (p, exp_out):
# check timeseries: pos_x = r * cos(theta) and pos_y = r * sin(theta)
for phs in ['burn1', 'coast', 'burn2']:
x = np.array(prob.get_val('traj.{0}.timeseries.pos_x'.format(phs))).flatten()
y = np.array(prob.get_val('traj.{0}.timeseries.pos_y'.format(phs))).flatten()
t = np.array(prob.get_val('traj.{0}.timeseries.states:theta'.format(phs))).flatten()
r = np.array(prob.get_val('traj.{0}.timeseries.states:r'.format(phs))).flatten()
xerr = x - r * np.cos(t)
yerr = y - r * np.sin(t)
assert_near_equal(np.sqrt(np.mean(xerr*xerr)), 0.0)
assert_near_equal(np.sqrt(np.mean(yerr*yerr)), 0.0)
ORDER = 5
NUM_FRAMES = 20
ORDER = 3
# Instantiate an OpenMDAO Problem instance.
prob = om.Problem()
# We need an optimization driver. To solve this simple problem ScipyOptimizerDriver will work.
prob.driver = om.ScipyOptimizeDriver()
# Instantiate a Dymos Trajectory and add it to the Problem model.
traj = dm.Trajectory()
prob.model.add_subsystem('traj', traj)
# Instantiate a Phase and add it to the Trajectory.
phase = dm.Phase(ode_class=OscillatorODE, transcription=dm.Radau(num_segments=NUM_SEG, order=ORDER, compressed=False))
traj.add_phase('phase0', phase)
# Tell Dymos that the duration of the phase is bounded.
phase.set_time_options(fix_initial=True, fix_duration=True)
# Tell Dymos the states to be propagated using the given ODE.
phase.add_state('x', fix_initial=True, rate_source='v', targets=['x'], units='m')
phase.add_state('v', fix_initial=True, rate_source='v_dot', targets=['v'], units='m/s')
# The spring constant, damping coefficient, and mass are inputs to the system that are constant throughout the phase.
phase.add_parameter('k', units='N/m', targets=['k'])
phase.add_parameter('c', units='N*s/m', targets=['c'])
phase.add_parameter('m', units='kg', targets=['m'])
# secondary "dense" timeseries
def test_ssto_simulate_root_trajectory(self):
"""
Tests that we can properly simulate a trajectory even if the trajectory is the root
group of the model. In this case the name of the trajectory in the output will
be 'sim_traj'.
"""
import numpy as np
import matplotlib.pyplot as plt
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
import dymos as dm
g = 1.61544 # lunar gravity, m/s**2
class LaunchVehicle2DEOM(om.ExplicitComponent):
"""
Simple 2D Cartesian Equations of Motion for a launch vehicle subject to thrust and drag.
"""
def initialize(self):
self.options.declare('num_nodes', types=int)
def setup(self):
nn = self.options['num_nodes']
# Inputs
self.add_input('vx',
val=np.zeros(nn),
desc='x velocity',
units='m/s')
self.add_input('vy',
val=np.zeros(nn),
desc='y velocity',
units='m/s')
self.add_input('m',
val=np.zeros(nn),
desc='mass',
units='kg')
self.add_input('theta',
val=np.zeros(nn),
desc='pitch angle',
units='rad')
self.add_input('thrust',
val=2100000 * np.ones(nn),
desc='thrust',
units='N')
self.add_input('Isp',
val=265.2 * np.ones(nn),
desc='specific impulse',
units='s')
# Outputs
self.add_output('xdot',
val=np.zeros(nn),
desc='velocity component in x',
units='m/s')
self.add_output('ydot',
val=np.zeros(nn),
desc='velocity component in y',
units='m/s')
self.add_output('vxdot',
val=np.zeros(nn),
desc='x acceleration magnitude',
units='m/s**2')
self.add_output('vydot',
val=np.zeros(nn),
desc='y acceleration magnitude',
units='m/s**2')
self.add_output('mdot',
val=np.zeros(nn),
desc='mass rate of change',
units='kg/s')
# Setup partials
ar = np.arange(self.options['num_nodes'])
self.declare_partials(of='xdot', wrt='vx', rows=ar, cols=ar, val=1.0)
self.declare_partials(of='ydot', wrt='vy', rows=ar, cols=ar, val=1.0)
self.declare_partials(of='vxdot', wrt='vx', rows=ar, cols=ar)
self.declare_partials(of='vxdot', wrt='m', rows=ar, cols=ar)
self.declare_partials(of='vxdot', wrt='theta', rows=ar, cols=ar)
self.declare_partials(of='vxdot', wrt='thrust', rows=ar, cols=ar)
self.declare_partials(of='vydot', wrt='m', rows=ar, cols=ar)
self.declare_partials(of='vydot', wrt='theta', rows=ar, cols=ar)
self.declare_partials(of='vydot', wrt='vy', rows=ar, cols=ar)
self.declare_partials(of='vydot', wrt='thrust', rows=ar, cols=ar)
self.declare_partials(of='mdot', wrt='thrust', rows=ar, cols=ar)
self.declare_partials(of='mdot', wrt='Isp', rows=ar, cols=ar)
def compute(self, inputs, outputs):
theta = inputs['theta']
cos_theta = np.cos(theta)
sin_theta = np.sin(theta)
vx = inputs['vx']
vy = inputs['vy']
m = inputs['m']
F_T = inputs['thrust']
Isp = inputs['Isp']
outputs['xdot'] = vx
outputs['ydot'] = vy
outputs['vxdot'] = F_T * cos_theta / m
outputs['vydot'] = F_T * sin_theta / m - g
outputs['mdot'] = -F_T / (g * Isp)
def compute_partials(self, inputs, jacobian):
theta = inputs['theta']
cos_theta = np.cos(theta)
sin_theta = np.sin(theta)
m = inputs['m']
F_T = inputs['thrust']
Isp = inputs['Isp']
# jacobian['vxdot', 'vx'] = -CDA * rho * vx / m
jacobian['vxdot', 'm'] = -(F_T * cos_theta) / m ** 2
jacobian['vxdot', 'theta'] = -(F_T / m) * sin_theta
jacobian['vxdot', 'thrust'] = cos_theta / m
# jacobian['vydot', 'vy'] = -CDA * rho * vy / m
jacobian['vydot', 'm'] = -(F_T * sin_theta) / m ** 2
jacobian['vydot', 'theta'] = (F_T / m) * cos_theta
jacobian['vydot', 'thrust'] = sin_theta / m
jacobian['mdot', 'thrust'] = -1.0 / (g * Isp)
jacobian['mdot', 'Isp'] = F_T / (g * Isp ** 2)
class LaunchVehicleLinearTangentODE(om.Group):
"""
The LaunchVehicleLinearTangentODE for this case consists of a guidance component and
the EOM. Guidance is simply an OpenMDAO ExecComp which computes the arctangent of the
tan_theta variable.
"""
def initialize(self):
self.options.declare('num_nodes', types=int,
desc='Number of nodes to be evaluated in the RHS')
def setup(self):
nn = self.options['num_nodes']
self.add_subsystem('guidance', om.ExecComp('theta=arctan(tan_theta)',
theta={'value': np.ones(nn),
'units': 'rad'},
tan_theta={'value': np.ones(nn)}))
self.add_subsystem('eom', LaunchVehicle2DEOM(num_nodes=nn))
self.connect('guidance.theta', 'eom.theta')
#
# Setup and solve the optimal control problem
#
traj = dm.Trajectory()
p = om.Problem(model=traj)
phase = dm.Phase(ode_class=LaunchVehicleLinearTangentODE,
transcription=dm.Radau(num_segments=20, order=3, compressed=False))
traj.add_phase('phase0', phase)
phase.set_time_options(fix_initial=True, duration_bounds=(10, 1000), units='s')
#
# Set the state options. We include rate_source, units, and targets here since the ODE
# is not decorated with their default values.
#
phase.add_state('x', fix_initial=True, lower=0, rate_source='eom.xdot')
phase.add_state('y', fix_initial=True, lower=0, rate_source='eom.ydot')
phase.add_state('vx', fix_initial=True, lower=0, rate_source='eom.vxdot',
units='m/s', targets=['eom.vx'])
phase.add_state('vy', fix_initial=True, rate_source='eom.vydot',
units='m/s', targets=['eom.vy'])
phase.add_state('m', fix_initial=True, rate_source='eom.mdot',
units='kg', targets=['eom.m'])
#
# The tangent of theta is modeled as a linear polynomial over the duration of the phase.
#
phase.add_polynomial_control('tan_theta', order=1, units=None, opt=True,
targets=['guidance.tan_theta'])
#
# Parameters values for thrust and specific impulse are design parameters. They are
# provided by an IndepVarComp in the phase, but with opt=False their values are not
# design variables in the optimization problem.
#
phase.add_parameter('thrust', units='N', opt=False, val=3.0 * 50000.0 * 1.61544,
targets=['eom.thrust'])
phase.add_parameter('Isp', units='s', opt=False, val=1.0E6, targets=['eom.Isp'])
#
# Set the boundary constraints. These are all states which could also be handled
# by setting fix_final=True and including the correct final value in the initial guess.
#
phase.add_boundary_constraint('y', loc='final', equals=1.85E5, linear=True)
phase.add_boundary_constraint('vx', loc='final', equals=1627.0)
phase.add_boundary_constraint('vy', loc='final', equals=0)
phase.add_objective('time', index=-1, scaler=0.01)
#
# Add theta as a timeseries output since it's not included by default.
#
phase.add_timeseries_output('guidance.theta', units='deg')
#
# Set the optimizer
#
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = 'SLSQP'
p.driver.declare_coloring()
#
# We don't strictly need to define a linear solver here since our problem is entirely
# feed-forward with no iterative loops. It's good practice to add one, however, since
# failing to do so can cause incorrect derivatives if iterative processes are ever
# introduced to the system.
#
p.model.linear_solver = om.DirectSolver()
p.setup(check=True)
#
# Assign initial guesses for the independent variables in the problem.
#
p['phase0.t_initial'] = 0.0
p['phase0.t_duration'] = 500.0
p['phase0.states:x'] = phase.interpolate(ys=[0, 350000.0], nodes='state_input')
p['phase0.states:y'] = phase.interpolate(ys=[0, 185000.0], nodes='state_input')
p['phase0.states:vx'] = phase.interpolate(ys=[0, 1627.0], nodes='state_input')
p['phase0.states:vy'] = phase.interpolate(ys=[1.0E-6, 0], nodes='state_input')
p['phase0.states:m'] = phase.interpolate(ys=[50000, 50000], nodes='state_input')
p['phase0.polynomial_controls:tan_theta'] = [[0.5 * np.pi], [0.0]]
#
# Solve the problem.
#
p.run_driver()
#
# Check the results.
#
assert_near_equal(p.get_val('phase0.timeseries.time')[-1], 481, tolerance=0.01)
#
# Get the explitly simulated results
#
exp_out = traj.simulate()
#
# Plot the results
#
fig, axes = plt.subplots(nrows=2, ncols=1, figsize=(10, 8))
axes[0].plot(p.get_val('phase0.timeseries.states:x'),
p.get_val('phase0.timeseries.states:y'),
marker='o',
ms=4,
linestyle='None',
label='solution')
axes[0].plot(exp_out.get_val('sim_traj.phase0.timeseries.states:x'),
exp_out.get_val('sim_traj.phase0.timeseries.states:y'),
marker=None,
linestyle='-',
label='simulation')
axes[0].set_xlabel('range (m)')
axes[0].set_ylabel('altitude (m)')
axes[0].set_aspect('equal')
axes[1].plot(p.get_val('phase0.timeseries.time'),
p.get_val('phase0.timeseries.theta'),
marker='o',
ms=4,
linestyle='None')
axes[1].plot(exp_out.get_val('sim_traj.phase0.timeseries.time'),
exp_out.get_val('sim_traj.phase0.timeseries.theta'),
linestyle='-',
marker=None)
axes[1].set_xlabel('time (s)')
axes[1].set_ylabel('theta (deg)')
plt.suptitle('Single Stage to Orbit Solution Using Polynomial Controls')
fig.legend(loc='lower center', ncol=2)
plt.show()
def test_brachistochrone_undecorated_ode_radau(self):
import numpy as np
import matplotlib
matplotlib.use('Agg')
import matplotlib.pyplot as plt
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
import dymos as dm
p = om.Problem(model=om.Group())
p.driver = om.ScipyOptimizeDriver()
phase = dm.Phase(ode_class=BrachistochroneODE,
transcription=dm.Radau(num_segments=10))
p.model.add_subsystem('phase0', phase)
phase.set_time_options(initial_bounds=(0, 0),
duration_bounds=(.5, 10),
units='s')
phase.add_state('x',
fix_initial=True,
fix_final=True,
rate_source='xdot',
units='m')
phase.add_state('y',
fix_initial=True,
fix_final=True,
rate_source='ydot',
units='m')
phase.add_state('v',
fix_initial=True,
rate_source='vdot',
targets=['v'],
units='m/s')
phase.add_control('theta',
units='deg',
rate_continuity=False,
lower=0.01,
upper=179.9,
targets=['theta'])
phase.add_parameter('g',
units='m/s**2',
opt=False,
val=9.80665,
targets=['g'])
# Minimize time at the end of the phase
phase.add_objective('time', loc='final', scaler=10)
p.model.linear_solver = om.DirectSolver()
p.setup()
p['phase0.t_initial'] = 0.0
p['phase0.t_duration'] = 2.0
p['phase0.states:x'] = phase.interpolate(ys=[0, 10],
nodes='state_input')
p['phase0.states:y'] = phase.interpolate(ys=[10, 5],
nodes='state_input')
p['phase0.states:v'] = phase.interpolate(ys=[0, 9.9],
nodes='state_input')
p['phase0.controls:theta'] = phase.interpolate(ys=[5, 100.5],
nodes='control_input')
# Solve for the optimal trajectory
p.run_driver()
# Test the results
assert_near_equal(p.get_val('phase0.timeseries.time')[-1],
1.8016,
tolerance=1.0E-3)
def test_two_phase_cannonball_ode_output_linkage(self):
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
import dymos as dm
from dymos.examples.cannonball.size_comp import CannonballSizeComp
from dymos.examples.cannonball.cannonball_ode import CannonballODE
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = 'SLSQP'
p.driver.declare_coloring()
p.model.add_subsystem('size_comp',
CannonballSizeComp(),
promotes_inputs=['radius', 'dens'])
p.model.set_input_defaults('dens', val=7.87, units='g/cm**3')
p.model.add_design_var('radius',
lower=0.01,
upper=0.10,
ref0=0.01,
ref=0.10,
units='m')
traj = p.model.add_subsystem('traj', dm.Trajectory())
transcription = dm.Radau(num_segments=5, order=3, compressed=True)
ascent = dm.Phase(ode_class=CannonballODE, transcription=transcription)
ascent = traj.add_phase('ascent', ascent)
# All initial states except flight path angle are fixed
# Final flight path angle is fixed (we will set it to zero so that the phase ends at apogee)
ascent.set_time_options(fix_initial=True,
duration_bounds=(1, 100),
duration_ref=100,
units='s')
ascent.add_state('r',
fix_initial=True,
fix_final=False,
units='m',
rate_source='r_dot')
ascent.add_state('h',
fix_initial=True,
fix_final=False,
units='m',
rate_source='h_dot')
ascent.add_state('gam',
fix_initial=False,
fix_final=True,
units='rad',
rate_source='gam_dot')
ascent.add_state('v',
fix_initial=False,
fix_final=False,
units='m/s',
rate_source='v_dot')
ascent.add_parameter('S', targets=['S'], units='m**2', dynamic=False)
ascent.add_parameter('mass', targets=['m'], units='kg', dynamic=False)
# Limit the muzzle energy
ascent.add_boundary_constraint('ke',
loc='initial',
upper=400000,
lower=0,
ref=100000)
# Second Phase (descent)
transcription = dm.GaussLobatto(num_segments=5,
order=3,
compressed=True)
descent = dm.Phase(ode_class=CannonballODE,
transcription=transcription)
traj.add_phase('descent', descent)
# All initial states and time are free (they will be linked to the final states of ascent.
# Final altitude is fixed (we will set it to zero so that the phase ends at ground impact)
descent.set_time_options(initial_bounds=(.5, 100),
duration_bounds=(.5, 100),
duration_ref=100,
units='s')
descent.add_state('r', units='m', rate_source='r_dot')
descent.add_state('h',
fix_initial=False,
fix_final=True,
units='m',
rate_source='h_dot')
descent.add_state('gam',
fix_initial=False,
fix_final=False,
units='rad',
rate_source='gam_dot')
descent.add_state('v',
fix_initial=False,
fix_final=False,
units='m/s',
rate_source='v_dot')
descent.add_parameter('S', targets=['S'], units='m**2', dynamic=False)
descent.add_parameter('mass', targets=['m'], units='kg', dynamic=False)
descent.add_objective('r', loc='final', scaler=-1.0)
# Add internally-managed design parameters to the trajectory.
traj.add_parameter('CD',
targets={
'ascent': ['CD'],
'descent': ['CD']
},
val=0.5,
units=None,
opt=False,
dynamic=False)
# Add externally-provided design parameters to the trajectory.
# In this case, we connect 'm' to pre-existing input parameters named 'mass' in each phase.
traj.add_parameter('m',
units='kg',
val=1.0,
targets={
'ascent': 'mass',
'descent': 'mass'
})
# In this case, by omitting targets, we're connecting these parameters to parameters
# with the same name in each phase.
traj.add_parameter('S', units='m**2', val=0.005)
# Link Phases (link time and all state variables)
# Note velocity is not included here. Doing so is equivalent to linking kinetic energy,
# and causes a duplicate row in the constraint jacobian.
traj.link_phases(phases=['ascent', 'descent'],
vars=['time', 'r', 'h', 'gam'],
connected=True)
traj.add_linkage_constraint('ascent',
'descent',
'ke',
'ke',
ref=100000,
connected=False)
p.model.connect('size_comp.mass', 'traj.parameters:m')
p.model.connect('size_comp.S', 'traj.parameters:S')
# Finish Problem Setup
p.model.linear_solver = om.DirectSolver()
p.driver.add_recorder(om.SqliteRecorder('ex_two_phase_cannonball.db'))
p.setup()
# Set Initial Guesses
p.set_val('radius', 0.05, units='m')
p.set_val('dens', 7.87, units='g/cm**3')
p.set_val('traj.parameters:CD', 0.5)
p.set_val('traj.ascent.t_initial', 0.0)
p.set_val('traj.ascent.t_duration', 10.0)
p.set_val('traj.ascent.states:r',
ascent.interpolate(ys=[0, 100], nodes='state_input'))
p.set_val('traj.ascent.states:h',
ascent.interpolate(ys=[0, 100], nodes='state_input'))
p.set_val('traj.ascent.states:v',
ascent.interpolate(ys=[200, 150], nodes='state_input'))
p.set_val('traj.ascent.states:gam',
ascent.interpolate(ys=[25, 0], nodes='state_input'),
units='deg')
p.set_val('traj.descent.t_initial', 10.0)
p.set_val('traj.descent.t_duration', 10.0)
p.set_val('traj.descent.states:r',
descent.interpolate(ys=[100, 200], nodes='state_input'))
p.set_val('traj.descent.states:h',
descent.interpolate(ys=[100, 0], nodes='state_input'))
p.set_val('traj.descent.states:v',
descent.interpolate(ys=[150, 200], nodes='state_input'))
p.set_val('traj.descent.states:gam',
descent.interpolate(ys=[0, -45], nodes='state_input'),
units='deg')
dm.run_problem(p)
assert_near_equal(p.get_val('traj.descent.states:r')[-1],
3183.25,
tolerance=1.0E-2)
exp_out = traj.simulate()
print('optimal radius: {0:6.4f} m '.format(
p.get_val('radius', units='m')[0]))
print('cannonball mass: {0:6.4f} kg '.format(
p.get_val('size_comp.mass', units='kg')[0]))
print('launch angle: {0:6.4f} '
'deg '.format(
p.get_val('traj.ascent.timeseries.states:gam',
units='deg')[0, 0]))
print('maximum range: {0:6.4f} '
'm '.format(
p.get_val('traj.descent.timeseries.states:r')[-1, 0]))
fig, axes = plt.subplots(nrows=1, ncols=1, figsize=(10, 6))
time_imp = {
'ascent': p.get_val('traj.ascent.timeseries.time'),
'descent': p.get_val('traj.descent.timeseries.time')
}
time_exp = {
'ascent': exp_out.get_val('traj.ascent.timeseries.time'),
'descent': exp_out.get_val('traj.descent.timeseries.time')
}
r_imp = {
'ascent': p.get_val('traj.ascent.timeseries.states:r'),
'descent': p.get_val('traj.descent.timeseries.states:r')
}
r_exp = {
'ascent': exp_out.get_val('traj.ascent.timeseries.states:r'),
'descent': exp_out.get_val('traj.descent.timeseries.states:r')
}
h_imp = {
'ascent': p.get_val('traj.ascent.timeseries.states:h'),
'descent': p.get_val('traj.descent.timeseries.states:h')
}
h_exp = {
'ascent': exp_out.get_val('traj.ascent.timeseries.states:h'),
'descent': exp_out.get_val('traj.descent.timeseries.states:h')
}
axes.plot(r_imp['ascent'], h_imp['ascent'], 'bo')
axes.plot(r_imp['descent'], h_imp['descent'], 'ro')
axes.plot(r_exp['ascent'], h_exp['ascent'], 'b--')
axes.plot(r_exp['descent'], h_exp['descent'], 'r--')
axes.set_xlabel('range (m)')
axes.set_ylabel('altitude (m)')
fig, axes = plt.subplots(nrows=4, ncols=1, figsize=(10, 6))
states = ['r', 'h', 'v', 'gam']
for i, state in enumerate(states):
x_imp = {
'ascent':
p.get_val('traj.ascent.timeseries.states:{0}'.format(state)),
'descent':
p.get_val('traj.descent.timeseries.states:{0}'.format(state))
}
x_exp = {
'ascent':
exp_out.get_val(
'traj.ascent.timeseries.states:{0}'.format(state)),
'descent':
exp_out.get_val(
'traj.descent.timeseries.states:{0}'.format(state))
}
axes[i].set_ylabel(state)
axes[i].plot(time_imp['ascent'], x_imp['ascent'], 'bo')
axes[i].plot(time_imp['descent'], x_imp['descent'], 'ro')
axes[i].plot(time_exp['ascent'], x_exp['ascent'], 'b--')
axes[i].plot(time_exp['descent'], x_exp['descent'], 'r--')
params = ['CD', 'mass', 'S']
fig, axes = plt.subplots(nrows=3, ncols=1, figsize=(12, 6))
for i, param in enumerate(params):
p_imp = {
'ascent':
p.get_val(
'traj.ascent.timeseries.parameters:{0}'.format(param)),
'descent':
p.get_val(
'traj.descent.timeseries.parameters:{0}'.format(param))
}
p_exp = {
'ascent':
exp_out.get_val('traj.ascent.timeseries.'
'parameters:{0}'.format(param)),
'descent':
exp_out.get_val('traj.descent.timeseries.'
'parameters:{0}'.format(param))
}
axes[i].set_ylabel(param)
axes[i].plot(time_imp['ascent'], p_imp['ascent'], 'bo')
axes[i].plot(time_imp['descent'], p_imp['descent'], 'ro')
axes[i].plot(time_exp['ascent'], p_exp['ascent'], 'b--')
axes[i].plot(time_exp['descent'], p_exp['descent'], 'r--')
plt.show()
def test_control_rate2_path_constraint_radau(self):
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
import dymos as dm
from dymos.examples.brachistochrone.brachistochrone_ode import BrachistochroneODE
p = om.Problem(model=om.Group())
p.driver = om.ScipyOptimizeDriver()
phase = dm.Phase(ode_class=BrachistochroneODE,
transcription=dm.Radau(num_segments=10,
compressed=False))
p.model.add_subsystem('phase0', phase)
phase.set_time_options(initial_bounds=(0, 0), duration_bounds=(.5, 10))
phase.add_state(
'x',
fix_initial=True,
fix_final=True,
rate_source=BrachistochroneODE.states['x']['rate_source'])
phase.add_state(
'y',
fix_initial=True,
fix_final=True,
rate_source=BrachistochroneODE.states['y']['rate_source'])
phase.add_state(
'v',
fix_initial=True,
rate_source=BrachistochroneODE.states['v']['rate_source'])
phase.add_control('theta',
units='deg',
rate_continuity=False,
lower=0.01,
upper=179.9)
phase.add_parameter('g', units='m/s**2', opt=False, val=9.80665)
# Minimize time at the end of the phase
phase.add_objective('time', loc='final', scaler=10)
phase.add_path_constraint('theta_rate2',
lower=-200,
upper=200,
units='rad/s**2')
p.model.linear_solver = om.DirectSolver()
p.model.options['assembled_jac_type'] = 'csc'
p.setup()
p['phase0.t_initial'] = 0.0
p['phase0.t_duration'] = 2.0
p['phase0.states:x'] = phase.interpolate(ys=[0, 10],
nodes='state_input')
p['phase0.states:y'] = phase.interpolate(ys=[10, 5],
nodes='state_input')
p['phase0.states:v'] = phase.interpolate(ys=[0, 9.9],
nodes='state_input')
p['phase0.controls:theta'] = phase.interpolate(ys=[5, 100.5],
nodes='control_input')
# Solve for the optimal trajectory
p.run_driver()
# Test the results
assert_near_equal(p.get_val('phase0.timeseries.time')[-1],
1.8016,
tolerance=1.0E-3)
def test_traj_param_target_none(self):
# Tests a bug where you couldn't specify None as a target for a specific phase.
import openmdao.api as om
from openmdao.utils.assert_utils import assert_near_equal
import dymos as dm
from dymos.examples.cannonball.size_comp import CannonballSizeComp
from dymos.examples.cannonball.cannonball_ode import CannonballODE
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = 'SLSQP'
p.driver.declare_coloring()
p.model.add_subsystem('size_comp',
CannonballSizeComp(),
promotes_inputs=['radius', 'dens'])
p.model.set_input_defaults('dens', val=7.87, units='g/cm**3')
p.model.add_design_var('radius',
lower=0.01,
upper=0.10,
ref0=0.01,
ref=0.10,
units='m')
traj = p.model.add_subsystem('traj', dm.Trajectory())
transcription = dm.Radau(num_segments=5, order=3, compressed=True)
ascent = dm.Phase(ode_class=CannonballODE, transcription=transcription)
ascent = traj.add_phase('ascent', ascent)
# All initial states except flight path angle are fixed
# Final flight path angle is fixed (we will set it to zero so that the phase ends at apogee)
ascent.set_time_options(fix_initial=True,
duration_bounds=(1, 100),
duration_ref=100,
units='s')
ascent.add_state('r',
fix_initial=True,
fix_final=False,
units='m',
rate_source='r_dot')
ascent.add_state('h',
fix_initial=True,
fix_final=False,
units='m',
rate_source='h_dot')
ascent.add_state('gam',
fix_initial=False,
fix_final=True,
units='rad',
rate_source='gam_dot')
ascent.add_state('v',
fix_initial=False,
fix_final=False,
units='m/s',
rate_source='v_dot')
ascent.add_parameter('S', targets=['S'], units='m**2', dynamic=False)
ascent.add_parameter('mass', targets=['m'], units='kg', dynamic=False)
# Limit the muzzle energy
ascent.add_boundary_constraint('ke',
loc='initial',
units='J',
upper=400000,
lower=0,
ref=100000,
shape=(1, ))
# Second Phase (descent)
transcription = dm.GaussLobatto(num_segments=5,
order=3,
compressed=True)
descent = dm.Phase(ode_class=CannonballODE,
transcription=transcription)
traj.add_phase('descent', descent)
# All initial states and time are free (they will be linked to the final states of ascent.
# Final altitude is fixed (we will set it to zero so that the phase ends at ground impact)
descent.set_time_options(initial_bounds=(.5, 100),
duration_bounds=(.5, 100),
duration_ref=100,
units='s')
descent.add_state('r', units='m', rate_source='r_dot')
descent.add_state('h',
fix_initial=False,
fix_final=True,
units='m',
rate_source='h_dot')
descent.add_state('gam',
fix_initial=False,
fix_final=False,
units='rad',
rate_source='gam_dot')
descent.add_state('v',
fix_initial=False,
fix_final=False,
units='m/s',
rate_source='v_dot')
descent.add_parameter('S', targets=['S'], units='m**2', dynamic=False)
descent.add_parameter('mass', targets=['m'], units='kg', dynamic=False)
descent.add_objective('r', loc='final', scaler=-1.0)
# Add internally-managed design parameters to the trajectory.
traj.add_parameter('CD',
targets={
'ascent': ['CD'],
'descent': ['CD']
},
val=0.5,
units=None,
opt=False,
dynamic=False)
# Add externally-provided design parameters to the trajectory.
# In this case, we connect 'm' to pre-existing input parameters named 'mass' in each phase.
traj.add_parameter('m',
units='kg',
val=1.0,
targets={
'ascent': 'mass',
'descent': 'mass'
},
dynamic=False)
# In this case, by omitting targets, we're connecting these parameters to parameters
# with the same name in each phase.
traj.add_parameter('S', units='m**2', val=0.005, dynamic=False)
# Link Phases (link time and all state variables)
# Note velocity is not included here. Doing so is equivalent to linking kinetic energy,
# and causes a duplicate row in the constraint jacobian.
traj.link_phases(phases=['ascent', 'descent'],
vars=['time', 'r', 'h', 'gam'],
connected=True)
traj.add_linkage_constraint('ascent',
'descent',
'ke',
'ke',
ref=100000,
connected=False)
p.model.connect('size_comp.mass', 'traj.parameters:m')
p.model.connect('size_comp.S', 'traj.parameters:S')
# Finish Problem Setup
p.model.linear_solver = om.DirectSolver()
p.driver.add_recorder(om.SqliteRecorder('ex_two_phase_cannonball.db'))
p.setup()
# Set Initial Guesses
p.set_val('radius', 0.05, units='m')
p.set_val('dens', 7.87, units='g/cm**3')
p.set_val('traj.parameters:CD', 0.5)
p.set_val('traj.ascent.t_initial', 0.0)
p.set_val('traj.ascent.t_duration', 10.0)
p.set_val('traj.ascent.states:r',
ascent.interpolate(ys=[0, 100], nodes='state_input'))
p.set_val('traj.ascent.states:h',
ascent.interpolate(ys=[0, 100], nodes='state_input'))
p.set_val('traj.ascent.states:v',
ascent.interpolate(ys=[200, 150], nodes='state_input'))
p.set_val('traj.ascent.states:gam',
ascent.interpolate(ys=[25, 0], nodes='state_input'),
units='deg')
p.set_val('traj.descent.t_initial', 10.0)
p.set_val('traj.descent.t_duration', 10.0)
p.set_val('traj.descent.states:r',
descent.interpolate(ys=[100, 200], nodes='state_input'))
p.set_val('traj.descent.states:h',
descent.interpolate(ys=[100, 0], nodes='state_input'))
p.set_val('traj.descent.states:v',
descent.interpolate(ys=[150, 200], nodes='state_input'))
p.set_val('traj.descent.states:gam',
descent.interpolate(ys=[0, -45], nodes='state_input'),
units='deg')
dm.run_problem(p)
assert_near_equal(p.get_val('traj.descent.states:r')[-1],
3183.25,
tolerance=1.0E-2)
def test_run_HS_problem_radau(self):
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.declare_coloring()
p.driver.options['optimizer'] = optimizer
if optimizer == 'SNOPT':
p.driver.opt_settings['Major iterations limit'] = 200
p.driver.opt_settings['Major feasibility tolerance'] = 1.0E-6
p.driver.opt_settings['Major optimality tolerance'] = 1.0E-6
elif optimizer == 'IPOPT':
p.driver.opt_settings['hessian_approximation'] = 'limited-memory'
# p.driver.opt_settings['nlp_scaling_method'] = 'user-scaling'
p.driver.opt_settings['print_level'] = 4
p.driver.opt_settings['max_iter'] = 200
p.driver.opt_settings['linear_solver'] = 'mumps'
traj = p.model.add_subsystem('traj', dm.Trajectory())
phase0 = traj.add_phase(
'phase0',
dm.Phase(ode_class=HyperSensitiveODE,
transcription=dm.Radau(num_segments=10, order=3)))
phase0.set_time_options(fix_initial=True, fix_duration=True)
phase0.add_state('x',
fix_initial=True,
fix_final=False,
rate_source='x_dot',
targets=['x'])
phase0.add_state('xL',
fix_initial=True,
fix_final=False,
rate_source='L',
targets=['xL'])
phase0.add_control('u', opt=True, targets=['u'], rate_continuity=False)
phase0.add_boundary_constraint('x', loc='final', equals=1)
phase0.add_objective('xL', loc='final')
phase0.set_refine_options(refine=True, tol=1e-6)
p.setup(check=True)
tf = np.float128(20)
p.set_val('traj.phase0.states:x', phase0.interp('x', [1.5, 1]))
p.set_val('traj.phase0.states:xL', phase0.interp('xL', [0, 1]))
p.set_val('traj.phase0.t_initial', 0)
p.set_val('traj.phase0.t_duration', tf)
p.set_val('traj.phase0.controls:u', phase0.interp('u', [-0.6, 2.4]))
dm.run_problem(p, refine_method='hp', refine_iteration_limit=10)
sqrt_two = np.sqrt(2)
val = sqrt_two * tf
c1 = (1.5 * np.exp(-val) - 1) / (np.exp(-val) - np.exp(val))
c2 = (1 - 1.5 * np.exp(val)) / (np.exp(-val) - np.exp(val))
ui = c1 * (1 + sqrt_two) + c2 * (1 - sqrt_two)
uf = c1 * (1 + sqrt_two) * np.exp(val) + c2 * (1 -
sqrt_two) * np.exp(-val)
J = 0.5 * (c1**2 * (1 + sqrt_two) * np.exp(2 * val) + c2**2 *
(1 - sqrt_two) * np.exp(-2 * val) - (1 + sqrt_two) * c1**2 -
(1 - sqrt_two) * c2**2)
assert_near_equal(p.get_val('traj.phase0.timeseries.controls:u')[0],
ui,
tolerance=5e-4)
assert_near_equal(p.get_val('traj.phase0.timeseries.controls:u')[-1],
uf,
tolerance=5e-4)
assert_near_equal(p.get_val('traj.phase0.timeseries.states:xL')[-1],
J,
tolerance=5e-4)
def test_basic(self):
import matplotlib.pyplot as plt
import openmdao.api as om
from openmdao.utils.assert_utils import assert_rel_error
import dymos as dm
from dymos.examples.battery_multibranch.battery_multibranch_ode import BatteryODE
from dymos.utils.lgl import lgl
prob = om.Problem()
opt = prob.driver = om.ScipyOptimizeDriver()
opt.declare_coloring()
opt.options['optimizer'] = 'SLSQP'
num_seg = 5
seg_ends, _ = lgl(num_seg + 1)
traj = prob.model.add_subsystem('traj', dm.Trajectory())
# First phase: normal operation.
transcription = dm.Radau(num_segments=num_seg, order=5, segment_ends=seg_ends, compressed=False)
phase0 = dm.Phase(ode_class=BatteryODE, transcription=transcription)
traj_p0 = traj.add_phase('phase0', phase0)
traj_p0.set_time_options(fix_initial=True, fix_duration=True)
traj_p0.add_state('state_of_charge', fix_initial=True, fix_final=False,
targets=['SOC'], rate_source='dXdt:SOC')
# Second phase: normal operation.
phase1 = dm.Phase(ode_class=BatteryODE, transcription=transcription)
traj_p1 = traj.add_phase('phase1', phase1)
traj_p1.set_time_options(fix_initial=False, fix_duration=True)
traj_p1.add_state('state_of_charge', fix_initial=False, fix_final=False,
targets=['SOC'], rate_source='dXdt:SOC')
traj_p1.add_objective('time', loc='final')
# Second phase, but with battery failure.
phase1_bfail = dm.Phase(ode_class=BatteryODE, ode_init_kwargs={'num_battery': 2},
transcription=transcription)
traj_p1_bfail = traj.add_phase('phase1_bfail', phase1_bfail)
traj_p1_bfail.set_time_options(fix_initial=False, fix_duration=True)
traj_p1_bfail.add_state('state_of_charge', fix_initial=False, fix_final=False,
targets=['SOC'], rate_source='dXdt:SOC')
# Second phase, but with motor failure.
phase1_mfail = dm.Phase(ode_class=BatteryODE, ode_init_kwargs={'num_motor': 2},
transcription=transcription)
traj_p1_mfail = traj.add_phase('phase1_mfail', phase1_mfail)
traj_p1_mfail.set_time_options(fix_initial=False, fix_duration=True)
traj_p1_mfail.add_state('state_of_charge', fix_initial=False, fix_final=False,
targets=['SOC'], rate_source='dXdt:SOC')
traj.link_phases(phases=['phase0', 'phase1'], vars=['state_of_charge', 'time'])
traj.link_phases(phases=['phase0', 'phase1_bfail'], vars=['state_of_charge', 'time'])
traj.link_phases(phases=['phase0', 'phase1_mfail'], vars=['state_of_charge', 'time'])
prob.model.options['assembled_jac_type'] = 'csc'
prob.model.linear_solver = om.DirectSolver(assemble_jac=True)
prob.setup()
prob['traj.phase0.t_initial'] = 0
prob['traj.phase0.t_duration'] = 1.0*3600
prob['traj.phase1.t_initial'] = 1.0*3600
prob['traj.phase1.t_duration'] = 1.0*3600
prob['traj.phase1_bfail.t_initial'] = 1.0*3600
prob['traj.phase1_bfail.t_duration'] = 1.0*3600
prob['traj.phase1_mfail.t_initial'] = 1.0*3600
prob['traj.phase1_mfail.t_duration'] = 1.0*3600
prob.set_solver_print(level=0)
prob.run_driver()
soc0 = prob['traj.phase0.states:state_of_charge']
soc1 = prob['traj.phase1.states:state_of_charge']
soc1b = prob['traj.phase1_bfail.states:state_of_charge']
soc1m = prob['traj.phase1_mfail.states:state_of_charge']
# Final value for State of Chrage in each segment should be a good test.
print('State of Charge after 1 hour')
assert_rel_error(self, soc0[-1], 0.63464982, 1e-6)
print('State of Charge after 2 hours')
assert_rel_error(self, soc1[-1], 0.23794217, 1e-6)
print('State of Charge after 2 hours, battery fails at 1 hour')
assert_rel_error(self, soc1b[-1], 0.0281523, 1e-6)
print('State of Charge after 2 hours, motor fails at 1 hour')
assert_rel_error(self, soc1m[-1], 0.18625395, 1e-6)
# Plot Results
t0 = prob['traj.phases.phase0.time.time']/3600
t1 = prob['traj.phases.phase1.time.time']/3600
t1b = prob['traj.phases.phase1_bfail.time.time']/3600
t1m = prob['traj.phases.phase1_mfail.time.time']/3600
plt.subplot(2, 1, 1)
plt.plot(t0, soc0, 'b')
plt.plot(t1, soc1, 'b')
plt.plot(t1b, soc1b, 'r')
plt.plot(t1m, soc1m, 'c')
plt.xlabel('Time (hour)')
plt.ylabel('State of Charge (percent)')
I_Li0 = prob['traj.phases.phase0.rhs_all.pwr_balance.I_Li']
I_Li1 = prob['traj.phases.phase1.rhs_all.pwr_balance.I_Li']
I_Li1b = prob['traj.phases.phase1_bfail.rhs_all.pwr_balance.I_Li']
I_Li1m = prob['traj.phases.phase1_mfail.rhs_all.pwr_balance.I_Li']
plt.subplot(2, 1, 2)
plt.plot(t0, I_Li0, 'b')
plt.plot(t1, I_Li1, 'b')
plt.plot(t1b, I_Li1b, 'r')
plt.plot(t1m, I_Li1m, 'c')
plt.xlabel('Time (hour)')
plt.ylabel('Line Current (A)')
plt.legend(['Phase 1', 'Phase 2', 'Phase 2 Battery Fail', 'Phase 2 Motor Fail'], loc=2)
plt.show()
def min_time_climb(optimizer='SLSQP',
num_seg=3,
transcription='gauss-lobatto',
transcription_order=3,
force_alloc_complex=False):
p = om.Problem(model=om.Group())
p.driver = om.pyOptSparseDriver()
p.driver.options['optimizer'] = optimizer
p.driver.declare_coloring()
if optimizer == 'SNOPT':
p.driver.opt_settings['Major iterations limit'] = 1000
p.driver.opt_settings['iSumm'] = 6
p.driver.opt_settings['Major feasibility tolerance'] = 1.0E-6
p.driver.opt_settings['Major optimality tolerance'] = 1.0E-6
p.driver.opt_settings['Function precision'] = 1.0E-12
p.driver.opt_settings['Linesearch tolerance'] = 0.1
p.driver.opt_settings['Major step limit'] = 0.5
t = {
'gauss-lobatto':
dm.GaussLobatto(num_segments=num_seg, order=transcription_order),
'radau-ps':
dm.Radau(num_segments=num_seg, order=transcription_order)
}
traj = dm.Trajectory()
phase = dm.Phase(ode_class=_TestODE, transcription=t[transcription])
traj.add_phase('phase0', phase)
p.model.add_subsystem('traj', traj)
phase.set_time_options(fix_initial=True,
duration_bounds=(50, 400),
duration_ref=100.0)
phase.add_state('r',
fix_initial=True,
lower=0,
upper=1.0E6,
ref=1.0E3,
defect_ref=1.0E3,
units='m',
rate_source='flight_dynamics.r_dot')
phase.add_state('h',
fix_initial=True,
lower=0,
upper=20000.0,
ref=1.0E2,
defect_ref=1.0E2,
units='m',
rate_source='flight_dynamics.h_dot',
targets=['h'])
phase.add_state('v',
fix_initial=True,
lower=10.0,
ref=1.0E2,
defect_ref=1.0E2,
units='m/s',
rate_source='flight_dynamics.v_dot',
targets=['v'])
phase.add_state('gam',
fix_initial=True,
lower=-1.5,
upper=1.5,
ref=1.0,
defect_ref=1.0,
units='rad',
rate_source='flight_dynamics.gam_dot',
targets=['gam'])
phase.add_state('m',
fix_initial=True,
lower=10.0,
upper=1.0E5,
ref=1.0E3,
defect_ref=1.0E3,
units='kg',
rate_source='prop.m_dot',
targets=['m'])
phase.add_control('alpha',
units='deg',
lower=-8.0,
upper=8.0,
scaler=1.0,
rate_continuity=True,
rate_continuity_scaler=100.0,
rate2_continuity=False,
targets=['alpha'])
phase.add_parameter('S',
val=49.2386,
units='m**2',
opt=False,
targets=['S'])
phase.add_parameter('Isp',
val=1600.0,
units='s',
opt=False,
targets=['Isp'])
phase.add_parameter('throttle', val=1.0, opt=False, targets=['throttle'])
phase.add_parameter('test',
val=40 * [1],
opt=False,
static_target=True,
targets=['test'])
phase.add_boundary_constraint('h',
loc='final',
equals=20000,
scaler=1.0E-3)
phase.add_boundary_constraint('aero.mach', loc='final', equals=1.0)
phase.add_boundary_constraint('gam', loc='final', equals=0.0)
phase.add_path_constraint(name='h', lower=100.0, upper=20000, ref=20000)
phase.add_path_constraint(name='aero.mach', lower=0.1, upper=1.8)
# Unnecessary but included to test capability
phase.add_path_constraint(name='alpha', lower=-8, upper=8, units='deg')
# Minimize time at the end of the phase
phase.add_objective('time', loc='final', ref=1.0)
# test mixing wildcard ODE variable expansion and unit overrides
phase.add_timeseries_output(['aero.*', 'prop.thrust', 'prop.m_dot'],
units={
'aero.f_lift': 'lbf',
'prop.thrust': 'lbf'
})
phase.set_refine_options(max_order=5)
p.model.linear_solver = om.DirectSolver()
p.setup(check=True, force_alloc_complex=force_alloc_complex)
p['traj.phase0.t_initial'] = 0.0
p['traj.phase0.t_duration'] = 300.0
p['traj.phase0.states:r'] = phase.interp('r', [0.0, 111319.54])
p['traj.phase0.states:h'] = phase.interp('h', [100.0, 20000.0])
p['traj.phase0.states:v'] = phase.interp('v', [135.964, 283.159])
p['traj.phase0.states:gam'] = phase.interp('gam', [0.0, 0.0])
p['traj.phase0.states:m'] = phase.interp('m', [19030.468, 16841.431])
p['traj.phase0.controls:alpha'] = phase.interp('alpha', [0.0, 0.0])
dm.run_problem(p, refine_iteration_limit=1)
return p
jacobian['xdot', 'theta'] = v * cos_theta
jacobian['ydot', 'v'] = -cos_theta
jacobian['ydot', 'theta'] = v * sin_theta
# Define the OpenMDAO problem
p = om.Problem(model=om.Group())
# Define a Trajectory object
traj = dm.Trajectory()
p.model.add_subsystem('traj', subsys=traj)
# Define a Dymos Phase object with Radau Transcription
phase = dm.Phase(ode_class=BrachistochroneEOM,
transcription=dm.Radau(num_segments=10, order=3))
traj.add_phase(name='phase0', phase=phase)
# Set the time options
phase.set_time_options(fix_initial=True,
duration_bounds=(0.5, 10.0))
# Set the state options
phase.add_state('x', rate_source='xdot',
fix_initial=True, fix_final=True)
phase.add_state('y', rate_source='ydot',
fix_initial=True, fix_final=True)
phase.add_state('v', rate_source='vdot',
fix_initial=True, fix_final=False)
# Define theta as a control.
def test_ivp_driver_10_segs(self):
import openmdao.api as om
import dymos as dm
import matplotlib.pyplot as plt
plt.switch_backend('Agg') # disable plotting to the screen
from dymos.examples.oscillator.doc.oscillator_ode import OscillatorODE
# Instantiate an OpenMDAO Problem instance.
prob = om.Problem()
# We need an optimization driver. To solve this simple problem ScipyOptimizerDriver will work.
prob.driver = om.ScipyOptimizeDriver()
# Instantiate a Dymos Trajectory and add it to the Problem model.
traj = dm.Trajectory()
prob.model.add_subsystem('traj', traj)
# Instantiate a Phase and add it to the Trajectory.
phase = dm.Phase(ode_class=OscillatorODE,
transcription=dm.Radau(num_segments=10))
traj.add_phase('phase0', phase)
# Tell Dymos that the duration of the phase is bounded.
phase.set_time_options(fix_initial=True, fix_duration=True)
# Tell Dymos the states to be propagated using the given ODE.
phase.add_state('x',
fix_initial=True,
rate_source='v',
targets=['x'],
units='m')
phase.add_state('v',
fix_initial=True,
rate_source='v_dot',
targets=['v'],
units='m/s')
# The spring constant, damping coefficient, and mass are inputs to the system that
# are constant throughout the phase.
phase.add_parameter('k', units='N/m', targets=['k'])
phase.add_parameter('c', units='N*s/m', targets=['c'])
phase.add_parameter('m', units='kg', targets=['m'])
# Since we're using an optimization driver, an objective is required. We'll minimize
# the final time in this case.
phase.add_objective('time', loc='final')
# Setup the OpenMDAO problem
prob.setup()
# Assign values to the times and states
prob.set_val('traj.phase0.t_initial', 0.0)
prob.set_val('traj.phase0.t_duration', 15.0)
prob.set_val('traj.phase0.states:x', 10.0)
prob.set_val('traj.phase0.states:v', 0.0)
prob.set_val('traj.phase0.parameters:k', 1.0)
prob.set_val('traj.phase0.parameters:c', 0.5)
prob.set_val('traj.phase0.parameters:m', 1.0)
# Now we're using the optimization driver to iteratively run the model and vary the
# phase duration until the final y value is 0.
prob.run_driver()
# Perform an explicit simulation of our ODE from the initial conditions.
sim_out = traj.simulate(times_per_seg=50)
# Plot the state values obtained from the phase timeseries objects in the simulation output.
t_sol = prob.get_val('traj.phase0.timeseries.time')
t_sim = sim_out.get_val('traj.phase0.timeseries.time')
states = ['x', 'v']
fig, axes = plt.subplots(len(states), 1)
for i, state in enumerate(states):
sol = axes[i].plot(
t_sol, prob.get_val(f'traj.phase0.timeseries.states:{state}'),
'o')
sim = axes[i].plot(
t_sim,
sim_out.get_val(f'traj.phase0.timeseries.states:{state}'), '-')
axes[i].set_ylabel(state)
axes[-1].set_xlabel('time (s)')
fig.legend((sol[0], sim[0]), ('solution', 'simulation'),
'lower right',
ncol=2)
plt.tight_layout()
plt.show()
def make_traj(transcription='gauss-lobatto', transcription_order=3, compressed=False,
connected=False):
t = {'gauss-lobatto': dm.GaussLobatto(num_segments=5, order=transcription_order, compressed=compressed),
'radau': dm.Radau(num_segments=20, order=transcription_order, compressed=compressed),
'runge-kutta': dm.RungeKutta(num_segments=5, compressed=compressed)}
traj = dm.Trajectory()
traj.add_design_parameter('c', opt=False, val=1.5, units='DU/TU',
targets={'burn1': ['c'], 'coast': ['c'], 'burn2': ['c']})
# First Phase (burn)
burn1 = dm.Phase(ode_class=FiniteBurnODE, transcription=t[transcription])
burn1 = traj.add_phase('burn1', burn1)
burn1.set_time_options(fix_initial=True, duration_bounds=(.5, 10), units='TU')
burn1.add_state('r', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='r_dot', targets=['r'], units='DU')
burn1.add_state('theta', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='theta_dot', targets=['theta'], units='rad')
burn1.add_state('vr', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='vr_dot', targets=['vr'], units='DU/TU')
burn1.add_state('vt', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='vt_dot', targets=['vt'], units='DU/TU')
burn1.add_state('accel', fix_initial=True, fix_final=False,
rate_source='at_dot', targets=['accel'], units='DU/TU**2')
burn1.add_state('deltav', fix_initial=True, fix_final=False,
rate_source='deltav_dot', units='DU/TU')
burn1.add_control('u1', rate_continuity=True, rate2_continuity=True, units='deg', scaler=0.01,
rate_continuity_scaler=0.001, rate2_continuity_scaler=0.001,
lower=-30, upper=30, targets=['u1'])
# Second Phase (Coast)
coast = dm.Phase(ode_class=FiniteBurnODE, transcription=t[transcription])
coast.set_time_options(initial_bounds=(0.5, 20), duration_bounds=(.5, 50), duration_ref=50, units='TU')
coast.add_state('r', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='r_dot', targets=['r'], units='DU')
coast.add_state('theta', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='theta_dot', targets=['theta'], units='rad')
coast.add_state('vr', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='vr_dot', targets=['vr'], units='DU/TU')
coast.add_state('vt', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='vt_dot', targets=['vt'], units='DU/TU')
coast.add_state('accel', fix_initial=True, fix_final=True,
rate_source='at_dot', targets=['accel'], units='DU/TU**2')
coast.add_state('deltav', fix_initial=False, fix_final=False,
rate_source='deltav_dot', units='DU/TU')
coast.add_design_parameter('u1', opt=False, val=0.0, units='deg', targets=['u1'])
# Third Phase (burn)
burn2 = dm.Phase(ode_class=FiniteBurnODE, transcription=t[transcription])
if connected:
traj.add_phase('burn2', burn2)
traj.add_phase('coast', coast)
burn2.set_time_options(initial_bounds=(1.0, 60), duration_bounds=(-10.0, -0.5),
initial_ref=10, units='TU')
burn2.add_state('r', fix_initial=True, fix_final=False, defect_scaler=100.0,
rate_source='r_dot', targets=['r'], units='DU')
burn2.add_state('theta', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='theta_dot', targets=['theta'], units='rad')
burn2.add_state('vr', fix_initial=True, fix_final=False, defect_scaler=1000.0,
rate_source='vr_dot', targets=['vr'], units='DU/TU')
burn2.add_state('vt', fix_initial=True, fix_final=False, defect_scaler=1000.0,
rate_source='vt_dot', targets=['vt'], units='DU/TU')
burn2.add_state('accel', fix_initial=False, fix_final=False, defect_scaler=1.0,
rate_source='at_dot', targets=['accel'], units='DU/TU**2')
burn2.add_state('deltav', fix_initial=False, fix_final=False, defect_scaler=1.0,
rate_source='deltav_dot', units='DU/TU')
burn2.add_objective('deltav', loc='initial', scaler=100.0)
burn2.add_control('u1', rate_continuity=True, rate2_continuity=True, units='deg',
scaler=0.01, lower=-180, upper=180, targets=['u1'])
else:
traj.add_phase('coast', coast)
traj.add_phase('burn2', burn2)
burn2.set_time_options(initial_bounds=(0.5, 50), duration_bounds=(.5, 10), initial_ref=10, units='TU')
burn2.add_state('r', fix_initial=False, fix_final=True, defect_scaler=100.0,
rate_source='r_dot', targets=['r'], units='DU')
burn2.add_state('theta', fix_initial=False, fix_final=False, defect_scaler=100.0,
rate_source='theta_dot', targets=['theta'], units='rad')
burn2.add_state('vr', fix_initial=False, fix_final=True, defect_scaler=1000.0,
rate_source='vr_dot', targets=['vr'], units='DU/TU')
burn2.add_state('vt', fix_initial=False, fix_final=True, defect_scaler=1000.0,
rate_source='vt_dot', targets=['vt'], units='DU/TU')
burn2.add_state('accel', fix_initial=False, fix_final=False, defect_scaler=1.0,
rate_source='at_dot', targets=['accel'], units='DU/TU**2')
burn2.add_state('deltav', fix_initial=False, fix_final=False, defect_scaler=1.0,
rate_source='deltav_dot', units='DU/TU')
burn2.add_objective('deltav', loc='final', scaler=100.0)
burn2.add_control('u1', rate_continuity=True, rate2_continuity=True, units='deg',
scaler=0.01, targets=['u1'])
burn1.add_timeseries_output('pos_x', units='DU')
coast.add_timeseries_output('pos_x', units='DU')
burn2.add_timeseries_output('pos_x', units='DU')
burn1.add_timeseries_output('pos_y', units='DU')
coast.add_timeseries_output('pos_y', units='DU')
burn2.add_timeseries_output('pos_y', units='DU')
# Link Phases
if connected:
traj.link_phases(phases=['burn1', 'coast'],
vars=['time', 'r', 'theta', 'vr', 'vt', 'deltav'],
connected=True)
# No direct connections to the end of a phase.
traj.link_phases(phases=['burn2', 'coast'],
vars=['r', 'theta', 'vr', 'vt', 'deltav'],
locs=('++', '++'))
traj.link_phases(phases=['burn2', 'coast'],
vars=['time'], locs=('++', '++'))
traj.link_phases(phases=['burn1', 'burn2'], vars=['accel'],
locs=('++', '++'))
else:
traj.link_phases(phases=['burn1', 'coast', 'burn2'],
vars=['time', 'r', 'theta', 'vr', 'vt', 'deltav'])
traj.link_phases(phases=['burn1', 'burn2'], vars=['accel'])
return traj
