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| 1 | +#!/usr/bin/env python3 |
| 2 | + |
| 3 | +import rospy |
| 4 | +import rospkg |
| 5 | + |
| 6 | +from nav_msgs.msg import Odometry |
| 7 | +from geometry_msgs.msg import PointStamped |
| 8 | +import tf |
| 9 | + |
| 10 | +from pozyx_simulation.msg import uwb_data |
| 11 | +import math |
| 12 | + |
| 13 | +import numpy as np |
| 14 | +import scipy.stats |
| 15 | + |
| 16 | +import time |
| 17 | + |
| 18 | + |
| 19 | +rospy.init_node('particle_filter_UWB_node', anonymous=True) |
| 20 | +pub = rospy.Publisher('localization_data_topic', PointStamped, queue_size=10) |
| 21 | +r = rospy.Rate(1) |
| 22 | + |
| 23 | +global particles |
| 24 | +global weights |
| 25 | + |
| 26 | + |
| 27 | +#add random seed for generating comparable pseudo random numbers |
| 28 | +#np.random.seed(123) |
| 29 | + |
| 30 | +def initialize_particles(num_particles, map_limits): |
| 31 | + # randomly initialize the particles inside the map limits |
| 32 | + |
| 33 | + created_particles = [] |
| 34 | + |
| 35 | + for i in range(num_particles): |
| 36 | + particle = dict() |
| 37 | + |
| 38 | + # draw x,y and theta coordinate from uniform distribution |
| 39 | + # inside map limits |
| 40 | + particle['x'] = np.random.uniform(map_limits[0], map_limits[1]) |
| 41 | + particle['y'] = np.random.uniform(map_limits[2], map_limits[3]) |
| 42 | + #particle['theta'] = np.random.uniform(-np.pi, np.pi) |
| 43 | + particle['theta'] = 0 + np.random.uniform(-np.pi, np.pi) |
| 44 | + |
| 45 | + created_particles.append(particle) |
| 46 | + |
| 47 | + return created_particles |
| 48 | + |
| 49 | +def mean_pose(): |
| 50 | + # calculate the mean pose of a particle set. |
| 51 | + # |
| 52 | + # for x and y, the mean position is the mean of the particle coordinates |
| 53 | + # |
| 54 | + # for theta, we cannot simply average the angles because of the wraparound |
| 55 | + # (jump from -pi to pi). Therefore, we generate unit vectors from the |
| 56 | + # angles and calculate the angle of their average |
| 57 | + |
| 58 | + # save x and y coordinates of particles |
| 59 | + xs = [] |
| 60 | + ys = [] |
| 61 | + |
| 62 | + # save unit vectors corresponding to particle orientations |
| 63 | + vxs_theta = [] |
| 64 | + vys_theta = [] |
| 65 | + |
| 66 | + toplam_nokta = 0 |
| 67 | + """ |
| 68 | + for i in range(len(particles)): |
| 69 | + if weights[i]>0.001: |
| 70 | + toplam_nokta = toplam_nokta +1 |
| 71 | + xs.append(particles[i]['x']) |
| 72 | + ys.append(particles[i]['y']) |
| 73 | +
|
| 74 | + #make unit vector from particle orientation |
| 75 | + vxs_theta.append(np.cos(particles[i]['theta'])) |
| 76 | + vys_theta.append(np.sin(particles[i]['theta'])) |
| 77 | + print("toplam :" + str(toplam_nokta)) |
| 78 | + """ |
| 79 | + |
| 80 | + |
| 81 | + for particle in particles: |
| 82 | + xs.append(particle['x']) |
| 83 | + ys.append(particle['y']) |
| 84 | + |
| 85 | + #make unit vector from particle orientation |
| 86 | + vxs_theta.append(np.cos(particle['theta'])) |
| 87 | + vys_theta.append(np.sin(particle['theta'])) |
| 88 | + |
| 89 | + |
| 90 | + #calculate average coordinates |
| 91 | + mean_x = np.mean(xs) |
| 92 | + mean_y = np.mean(ys) |
| 93 | + mean_theta = np.arctan2(np.mean(vys_theta), np.mean(vxs_theta)) |
| 94 | + |
| 95 | + return [mean_x, mean_y, mean_theta] |
| 96 | + |
| 97 | +def sample_motion_model(Odometry): |
| 98 | + global particles |
| 99 | + # Samples new particle positions, based on old positions, the odometry measurements and the motion noise |
| 100 | + # (probabilistic motion models slide 27) |
| 101 | + |
| 102 | + |
| 103 | + delta_vel = Odometry.twist.twist.linear.x/30 # redefine r1 odom=>twist=>linear=>x |
| 104 | + delta_w = Odometry.twist.twist.angular.z/30 # redefine t odom=>twist=>angular=>z |
| 105 | + |
| 106 | + |
| 107 | + # "move" each particle according to the odometry measurements plus sampled noise to generate new particle set |
| 108 | + |
| 109 | + new_particles = [] |
| 110 | + for particle in particles: |
| 111 | + new_particle = dict() |
| 112 | + # sample noisy motions |
| 113 | + noise_x = (np.random.uniform() - 0.5) * abs(delta_vel) |
| 114 | + #noise_y = (np.random.uniform()-0.5) * abs(delta_vel) |
| 115 | + noise_theta = (np.random.uniform() - 0.5) * abs(delta_w) |
| 116 | + noisy_delta_vel = delta_vel + noise_x |
| 117 | + #noisy_delta_vel_y = delta_vel + noise_y |
| 118 | + noisy_delta_w = delta_w + noise_theta |
| 119 | + # calculate new particle pose |
| 120 | + new_particle['x'] = particle['x'] + noisy_delta_vel * np.cos(particle['theta']) |
| 121 | + new_particle['y'] = particle['y'] + noisy_delta_vel * np.sin(particle['theta']) |
| 122 | + new_particle['theta'] = particle['theta'] + noisy_delta_w |
| 123 | + new_particles.append(new_particle) |
| 124 | + |
| 125 | + particles = new_particles |
| 126 | + |
| 127 | + |
| 128 | + |
| 129 | +def eval_sensor_model(): |
| 130 | + global weights |
| 131 | + global particles |
| 132 | + # Computes the observation likelihood of all particles, given the particle and landmark positions and sensor measurements |
| 133 | + # (probabilistic sensor models slide 33) |
| 134 | + # |
| 135 | + # The employed sensor model is range only. |
| 136 | + |
| 137 | + sigma_r = 0.5 |
| 138 | + |
| 139 | + while not rospy.is_shutdown(): |
| 140 | + #measured landmark ids and ranges |
| 141 | + ids = g_uwb_data.destination_id |
| 142 | + ranges = g_uwb_data.distance |
| 143 | + |
| 144 | + weights_new = [] |
| 145 | + |
| 146 | + # rate each particle |
| 147 | + for particle in particles: |
| 148 | + all_meas_likelihood = 1.0 # for combining multiple measurements |
| 149 | + # loop for each observed landmark |
| 150 | + for i in range(len(ids)): |
| 151 | + lm_id = ids[i] |
| 152 | + meas_range = ranges[i] |
| 153 | + lx = sensor_pos[i][0] |
| 154 | + ly = sensor_pos[i][1] |
| 155 | + lz = sensor_pos[i][2] |
| 156 | + #calculate expected range |
| 157 | + px = particle['x'] |
| 158 | + py = particle['y'] |
| 159 | + pz = 0 |
| 160 | + ptheta = particle['theta'] |
| 161 | + # calculate expected range measurement |
| 162 | + meas_range_exp = np.sqrt((lx - px) ** 2 + (ly - py) ** 2 + (lz - pz) ** 2) |
| 163 | + # evaluate sensor model (probability density function of normal distribution) |
| 164 | + meas_likelihood = scipy.stats.norm.pdf(meas_range, meas_range_exp, sigma_r) |
| 165 | + #print(meas_likelihood) |
| 166 | + # combine (independent) measurements |
| 167 | + all_meas_likelihood = all_meas_likelihood * meas_likelihood |
| 168 | + |
| 169 | + weights_new.append(all_meas_likelihood) |
| 170 | + |
| 171 | + #normalize weights_new |
| 172 | + normalizer = sum(weights_new) |
| 173 | + weights = weights_new / normalizer |
| 174 | + |
| 175 | + #print("max weights :" + str(max(weights))) |
| 176 | + resample_particles() |
| 177 | + [mean_x, mean_y, mean_theta] = mean_pose() |
| 178 | + publish_data(mean_x,mean_y) |
| 179 | + |
| 180 | +def resample_particles(): |
| 181 | + global particles |
| 182 | + global weights |
| 183 | + # Returns a new set of particles obtained by performing stochastic universal sampling, according to the particle weights. |
| 184 | + |
| 185 | + new_particles = [] |
| 186 | + #new_weights = [] |
| 187 | + # distance between pointers |
| 188 | + step = 1.0 / len(particles) |
| 189 | + # random start of first pointer |
| 190 | + u = np.random.uniform(0, step) |
| 191 | + # where we are along the weights |
| 192 | + c = weights[0] |
| 193 | + # index of weight container and corresponding particle |
| 194 | + i = 0 |
| 195 | + # loop over all particle weights |
| 196 | + for particle in particles: |
| 197 | + # go through the weights until you find the particle to which the pointer points |
| 198 | + while u > c: |
| 199 | + i = i + 1 |
| 200 | + c = c + weights[i] |
| 201 | + # add that particle |
| 202 | + new_particles.append(particles[i]) |
| 203 | + #new_weights.append(weights[i]) |
| 204 | + # increase the threshold |
| 205 | + u = u + step |
| 206 | + |
| 207 | + #weights = new_weights |
| 208 | + particles = new_particles |
| 209 | + |
| 210 | +def subscribe_odom_data(Odometry): |
| 211 | + sample_motion_model(Odometry) |
| 212 | + |
| 213 | +def subscribe_uwb_data(uwb_data): |
| 214 | + global g_uwb_data |
| 215 | + g_uwb_data = uwb_data |
| 216 | + |
| 217 | + #eval_sensor_model(uwb_data,sensor_pos) |
| 218 | + #particles = resample_particles() |
| 219 | + |
| 220 | +def publish_data(pose_x,pose_y): |
| 221 | + robot_pos = PointStamped() |
| 222 | + robot_pos.header.stamp = rospy.Time.now() |
| 223 | + robot_pos.header.frame_id = "map" |
| 224 | + |
| 225 | + robot_pos.point.x = float(pose_x) |
| 226 | + robot_pos.point.y = float(pose_y) |
| 227 | + robot_pos.point.z = 0.0 |
| 228 | + |
| 229 | + pub.publish(robot_pos) |
| 230 | + |
| 231 | +def get_anchors_pos(): |
| 232 | + max_anchor = 100 |
| 233 | + sensor_pos = [] |
| 234 | + uwb_id = 'uwb_anchor_' |
| 235 | + listener = tf.TransformListener() |
| 236 | + |
| 237 | + for i in range(max_anchor): |
| 238 | + try: |
| 239 | + time.sleep(0.3) |
| 240 | + (trans,rot) = listener.lookupTransform('/map', uwb_id+str(i), rospy.Time(0)) |
| 241 | + sensor_pos.append(trans) |
| 242 | + except (tf.LookupException, tf.ConnectivityException, tf.ExtrapolationException): |
| 243 | + if(i == 0): |
| 244 | + rospy.INFO("Firstly have to run pozyx_simulation package uwb_simulation.py file") |
| 245 | + break |
| 246 | + |
| 247 | + return sensor_pos |
| 248 | + |
| 249 | + |
| 250 | +if __name__ == "__main__": |
| 251 | + global particles |
| 252 | + global sensor_pos |
| 253 | + #get uwb anchors postion |
| 254 | + sensor_pos = get_anchors_pos() |
| 255 | + |
| 256 | + #1800 0 |
| 257 | + map_limits = [-3,3,-3,3] |
| 258 | + particles = initialize_particles(1000, map_limits) |
| 259 | + |
| 260 | + |
| 261 | + rospy.Subscriber("odom", Odometry, subscribe_odom_data) |
| 262 | + rospy.Subscriber("uwb_data_topic", uwb_data, subscribe_uwb_data) |
| 263 | + |
| 264 | + time.sleep(2) |
| 265 | + eval_sensor_model() |
| 266 | + rospy.spin() |
| 267 | + |
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