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Merge pull request #734 from dstl/accum_state_dens
Add Accumulated State Densities Filter
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#!/usr/bin/env python | ||
# coding: utf-8 | ||
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""" | ||
=========================================================== | ||
Accumulated States Densities - Out-of-Sequence measurements | ||
=========================================================== | ||
""" | ||
# %% | ||
# Smoothing a filtered trajectory is an important task in live systems. Using | ||
# Rauch–Tung–Striebel retrodiction after the normal filtering has a great effect on | ||
# the filtered trajectories but it is not optimal because one has to calculate the | ||
# retrodiction in an own step. In this point the Accumulated-State-Densities (ASDs) can help. | ||
# In the ASDs the retrodiction is calculated in the prediction and update step. | ||
# We use a multistate over time which can be pruned for better performance. Another advantage | ||
# is the possibility to calculate Out-of-Sequence measurements in an optimal way. | ||
# A more detailed introduction and the derivation of the formulas can be found in [#]_. | ||
# | ||
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# %% | ||
# First of all we plot the ground truth of one target moving on the Cartesian 2D plane. | ||
# The target moves in a cubic function. | ||
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# %% | ||
from datetime import timedelta | ||
from datetime import datetime | ||
import numpy as np | ||
from stonesoup.types.groundtruth import GroundTruthPath, GroundTruthState | ||
from stonesoup.plotter import Plotterly | ||
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plotter = Plotterly() | ||
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truth = GroundTruthPath() | ||
start_time = datetime.now() | ||
for n in range(1, 202, 2): | ||
x = n -100 | ||
y = 1e-4 * (n-100)**3 | ||
varxy = np.array([[0.1, 0.], [0., 0.1]]) | ||
xy = np.random.multivariate_normal(np.array([x, y]), varxy) | ||
truth.append(GroundTruthState(np.array([[xy[0]], [xy[1]]]), | ||
timestamp=start_time + timedelta(seconds=n))) | ||
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# Plot the result | ||
plotter.plot_ground_truths({truth}, [0, 1]) | ||
plotter.fig | ||
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# %% | ||
# Following we plot the measurements made of the ground truth. The measurements have | ||
# an error matrix of variance 5 in both dimensions. | ||
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from scipy.stats import multivariate_normal | ||
from stonesoup.types.detection import Detection | ||
from stonesoup.models.measurement.linear import LinearGaussian | ||
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measurements = [] | ||
for state in truth: | ||
x, y = multivariate_normal.rvs( | ||
state.state_vector.ravel(), cov=np.diag([5., 5.])) | ||
measurements.append(Detection( | ||
[x, y], timestamp=state.timestamp)) | ||
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# Plot the result | ||
plotter.plot_measurements(measurements, [0, 1], LinearGaussian(2, (0, 1), None)) | ||
plotter.fig | ||
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# %% | ||
# Now we have to setup a transition model for the prediction and the :class:`~.ASDKalmanPredictor`. | ||
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from stonesoup.models.transition.linear import \ | ||
CombinedLinearGaussianTransitionModel, ConstantVelocity | ||
from stonesoup.predictor.asd import ASDKalmanPredictor | ||
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transition_model = CombinedLinearGaussianTransitionModel( | ||
(ConstantVelocity(0.2), ConstantVelocity(0.2))) | ||
predictor = ASDKalmanPredictor(transition_model) | ||
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# %% | ||
# We have to do the same for the measurement model and the :class:`~.ASDKalmanUpdater`. | ||
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from stonesoup.updater.asd import ASDKalmanUpdater | ||
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measurement_model = LinearGaussian( | ||
4, # Number of state dimensions (position and velocity in 2D) | ||
(0, 2), # Mapping measurement vector index to state index | ||
np.array([[5., 0.], # Covariance matrix for Gaussian PDF | ||
[0., 5.]]) | ||
) | ||
updater = ASDKalmanUpdater(measurement_model) | ||
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# %% | ||
# We set up the state at position (-100, -100) with velocity 0. We set max_nstep | ||
# to 30. | ||
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from stonesoup.types.state import ASDGaussianState | ||
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prior = ASDGaussianState(multi_state_vector=[[-100.], [0.], [-100.], [0.]], | ||
timestamps=start_time, | ||
multi_covar=np.diag([1., 1., 1., 1.]), | ||
max_nstep=30) | ||
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# %% | ||
# Last but not least we set up a track and execute the filtering. The first and last 10 steps | ||
# are processed in sequence. All other measurements are divided in groups of 10 following in time. | ||
# The latest one is processed first and the other 9 are used for filtering. In the end we plot the | ||
# filtered trajectory. The animated plot will show the changing state estimate across `max_nstep` | ||
# set above. | ||
import matplotlib | ||
from matplotlib import animation | ||
matplotlib.rcParams['animation.html'] = 'jshtml' | ||
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from stonesoup.plotter import Plotter | ||
from stonesoup.types.hypothesis import SingleHypothesis | ||
from stonesoup.types.track import Track | ||
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ani_plotter = Plotter() | ||
frames = [] | ||
artists = [] | ||
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track = Track() # For ASD track | ||
track2 = Track() # For Gaussian state equivalent without ASD | ||
processed_measurements = set() | ||
for i in range(0, len(measurements)): | ||
if i > 10: | ||
if i % 10 != 0: # or i%10==3: | ||
m = measurements[i] | ||
prediction = predictor.predict(prior, timestamp=m.timestamp) | ||
track2.append(prediction.state) # This track will ignore OoS measurements | ||
else: | ||
# prediction and update of the newest measurement | ||
m = measurements[i] | ||
processed_measurements.add(m) | ||
prediction = predictor.predict(prior, timestamp=m.timestamp) | ||
hypothesis = SingleHypothesis(prediction, m) | ||
# Used to group a prediction and measurement together | ||
post = updater.update(hypothesis) | ||
track.append(post) | ||
track2.append(post.state) | ||
prior = track[-1] | ||
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artists.extend(ani_plotter.plot_tracks(Track(track[-1].states), [0, 2], color='r')) | ||
artists.extend( | ||
ani_plotter.plot_measurements(processed_measurements, [0, 2], measurement_model)) | ||
frames.append(artists); artists =[] | ||
for j in range(9, 0, -1): | ||
# prediction and update for all OOS measurement. Beginning with the latest one. | ||
m = measurements[i - j] | ||
processed_measurements.add(m) | ||
prediction = predictor.predict(prior, timestamp=m.timestamp) | ||
hypothesis = SingleHypothesis(prediction, m) | ||
# Used to group a prediction and measurement together | ||
post = updater.update(hypothesis) | ||
track.append(post) | ||
prior = track[-1] | ||
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artists.extend(ani_plotter.plot_tracks(Track(track[-1].states), [0, 2], color='r')) | ||
artists.extend(ani_plotter.plot_measurements( | ||
processed_measurements, [0, 2], measurement_model)) | ||
frames.append(artists); artists = [] | ||
else: | ||
# the first 10 steps are for beginning of the ASD so that it is numerically stable | ||
m = measurements[i] | ||
processed_measurements.add(m) | ||
prediction = predictor.predict(prior, timestamp=m.timestamp) | ||
hypothesis = SingleHypothesis(prediction, m) | ||
# Used to group a prediction and measurement together | ||
post = updater.update(hypothesis) | ||
track.append(post) | ||
track2.append(post.state) | ||
prior = track[-1] | ||
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artists.extend(ani_plotter.plot_tracks(Track(track[-1].states), [0, 2], color='r')) | ||
artists.extend( | ||
ani_plotter.plot_measurements(processed_measurements, [0, 2], measurement_model)) | ||
frames.append(artists); artists = [] | ||
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animation.ArtistAnimation(ani_plotter.fig, frames) | ||
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# %% | ||
# For comparision, the plot below shows a approximately equivalent track if | ||
# at each step the prediction was stored, and out of sequence measurements were ignored. | ||
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# sphinx_gallery_thumbnail_number = 4 | ||
from operator import attrgetter | ||
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asd_states = [] | ||
for state in reversed(list(track.last_timestamp_generator())): | ||
if state.timestamp not in (asd_state.timestamp for asd_state in asd_states): | ||
asd_states.extend(state.states) | ||
asd_states = sorted(asd_states, key=attrgetter('timestamp')) | ||
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plotter.plot_tracks({track2}, [0, 2], uncertainty=True, line=dict(color='green'), | ||
track_label="Equivalent track without ASD") | ||
plotter.plot_tracks({Track(asd_states)}, [0, 2], line=dict(color='red'), | ||
track_label="ASD Track") | ||
plotter.fig | ||
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# %% | ||
# References | ||
# ---------- | ||
# .. [#] W. Koch and F. Govaers, On Accumulated State Densities with Applications to | ||
# Out-of-Sequence Measurement Processing in IEEE Transactions on Aerospace and Electronic Systems, | ||
# vol. 47, no. 4, pp. 2766-2778, OCTOBER 2011, doi: 10.1109/TAES.2011.6034663. | ||
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