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여기서는 파티클필터를 이용한 센서퓨전 위치 추정방법으로

 

파란 선은 실제 궤적

 

검은 선은 추측 항법으로 계산한 궤적

 

빨간선은 파티클 필터로 추정한 궤적입니다.

 

검은 점은 RFID 랜드마크로 로봇은 랜드마크까지의 거리를 측정하여 파티클 필터  위치추정에 사용합니다.

 

 

 

"""
Particle Filter localization sample
author: Atsushi Sakai (@Atsushi_twi)
"""

import math

import matplotlib.pyplot as plt
import numpy as np
from scipy.spatial.transform import Rotation as Rot

# Estimation parameter of PF
Q = np.diag([0.2]) ** 2  # range error
R = np.diag([2.0, np.deg2rad(40.0)]) ** 2  # input error

#  Simulation parameter
Q_sim = np.diag([0.2]) ** 2
R_sim = np.diag([1.0, np.deg2rad(30.0)]) ** 2

DT = 0.1  # time tick [s]
SIM_TIME = 20.0  # simulation time [s]
MAX_RANGE = 20.0  # maximum observation range

# Particle filter parameter
NP = 100  # Number of Particle
NTh = NP / 2.0  # Number of particle for re-sampling

show_animation = True


def calc_input():
    v = 1.0  # [m/s]
    yaw_rate = 0.1  # [rad/s]
    u = np.array([[v, yaw_rate]]).T
    return u


def observation(x_true, xd, u, rf_id):
    x_true = motion_model(x_true, u)

    # add noise to gps x-y
    z = np.zeros((0, 3))

    for i in range(len(rf_id[:, 0])):

        dx = x_true[0, 0] - rf_id[i, 0]
        dy = x_true[1, 0] - rf_id[i, 1]
        d = math.hypot(dx, dy)
        if d <= MAX_RANGE:
            dn = d + np.random.randn() * Q_sim[0, 0] ** 0.5  # add noise
            zi = np.array([[dn, rf_id[i, 0], rf_id[i, 1]]])
            z = np.vstack((z, zi))

    # add noise to input
    ud1 = u[0, 0] + np.random.randn() * R_sim[0, 0] ** 0.5
    ud2 = u[1, 0] + np.random.randn() * R_sim[1, 1] ** 0.5
    ud = np.array([[ud1, ud2]]).T

    xd = motion_model(xd, ud)

    return x_true, z, xd, ud


def motion_model(x, u):
    F = np.array([[1.0, 0, 0, 0],
                  [0, 1.0, 0, 0],
                  [0, 0, 1.0, 0],
                  [0, 0, 0, 0]])

    B = np.array([[DT * math.cos(x[2, 0]), 0],
                  [DT * math.sin(x[2, 0]), 0],
                  [0.0, DT],
                  [1.0, 0.0]])

    x = F.dot(x) + B.dot(u)

    return x


def gauss_likelihood(x, sigma):
    p = 1.0 / math.sqrt(2.0 * math.pi * sigma ** 2) * \
        math.exp(-x ** 2 / (2 * sigma ** 2))

    return p


def calc_covariance(x_est, px, pw):
    """
    calculate covariance matrix
    see ipynb doc
    """
    cov = np.zeros((3, 3))
    n_particle = px.shape[1]
    for i in range(n_particle):
        dx = (px[:, i:i + 1] - x_est)[0:3]
        cov += pw[0, i] * dx @ dx.T
    cov *= 1.0 / (1.0 - pw @ pw.T)

    return cov


def pf_localization(px, pw, z, u):
    """
    Localization with Particle filter
    """

    for ip in range(NP):
        x = np.array([px[:, ip]]).T
        w = pw[0, ip]

        #  Predict with random input sampling
        ud1 = u[0, 0] + np.random.randn() * R[0, 0] ** 0.5
        ud2 = u[1, 0] + np.random.randn() * R[1, 1] ** 0.5
        ud = np.array([[ud1, ud2]]).T
        x = motion_model(x, ud)

        #  Calc Importance Weight
        for i in range(len(z[:, 0])):
            dx = x[0, 0] - z[i, 1]
            dy = x[1, 0] - z[i, 2]
            pre_z = math.hypot(dx, dy)
            dz = pre_z - z[i, 0]
            w = w * gauss_likelihood(dz, math.sqrt(Q[0, 0]))

        px[:, ip] = x[:, 0]
        pw[0, ip] = w

    pw = pw / pw.sum()  # normalize

    x_est = px.dot(pw.T)
    p_est = calc_covariance(x_est, px, pw)

    N_eff = 1.0 / (pw.dot(pw.T))[0, 0]  # Effective particle number
    if N_eff < NTh:
        px, pw = re_sampling(px, pw)
    return x_est, p_est, px, pw


def re_sampling(px, pw):
    """
    low variance re-sampling
    """

    w_cum = np.cumsum(pw)
    base = np.arange(0.0, 1.0, 1 / NP)
    re_sample_id = base + np.random.uniform(0, 1 / NP)
    indexes = []
    ind = 0
    for ip in range(NP):
        while re_sample_id[ip] > w_cum[ind]:
            ind += 1
        indexes.append(ind)

    px = px[:, indexes]
    pw = np.zeros((1, NP)) + 1.0 / NP  # init weight

    return px, pw


def plot_covariance_ellipse(x_est, p_est):  # pragma: no cover
    p_xy = p_est[0:2, 0:2]
    eig_val, eig_vec = np.linalg.eig(p_xy)

    if eig_val[0] >= eig_val[1]:
        big_ind = 0
        small_ind = 1
    else:
        big_ind = 1
        small_ind = 0

    t = np.arange(0, 2 * math.pi + 0.1, 0.1)

    # eig_val[big_ind] or eiq_val[small_ind] were occasionally negative
    # numbers extremely close to 0 (~10^-20), catch these cases and set the
    # respective variable to 0
    try:
        a = math.sqrt(eig_val[big_ind])
    except ValueError:
        a = 0

    try:
        b = math.sqrt(eig_val[small_ind])
    except ValueError:
        b = 0

    x = [a * math.cos(it) for it in t]
    y = [b * math.sin(it) for it in t]
    angle = math.atan2(eig_vec[big_ind, 1], eig_vec[big_ind, 0])
    rot = Rot.from_euler('z', angle).as_matrix()[0:2, 0:2]
    fx = rot.dot(np.array([[x, y]]))
    px = np.array(fx[0, :] + x_est[0, 0]).flatten()
    py = np.array(fx[1, :] + x_est[1, 0]).flatten()
    plt.plot(px, py, "--r")


def main():
    time = 0.0

    # RF_ID positions [x, y]
    rf_id = np.array([[10.0, 0.0],
                      [10.0, 10.0],
                      [0.0, 15.0],
                      [-5.0, 20.0]])

    # State Vector [x y yaw v]'
    x_est = np.zeros((4, 1))
    x_true = np.zeros((4, 1))

    px = np.zeros((4, NP))  # Particle store
    pw = np.zeros((1, NP)) + 1.0 / NP  # Particle weight
    x_dr = np.zeros((4, 1))  # Dead reckoning

    # history
    h_x_est = x_est
    h_x_true = x_true
    h_x_dr = x_true

    while SIM_TIME >= time:
        time += DT
        u = calc_input()

        x_true, z, x_dr, ud = observation(x_true, x_dr, u, rf_id)

        x_est, PEst, px, pw = pf_localization(px, pw, z, ud)

        # store data history
        h_x_est = np.hstack((h_x_est, x_est))
        h_x_dr = np.hstack((h_x_dr, x_dr))
        h_x_true = np.hstack((h_x_true, x_true))

        if show_animation:
            plt.cla()
            # for stopping simulation with the esc key.
            plt.gcf().canvas.mpl_connect(
                'key_release_event',
                lambda event: [exit(0) if event.key == 'escape' else None])

            for i in range(len(z[:, 0])):
                plt.plot([x_true[0, 0], z[i, 1]], [x_true[1, 0], z[i, 2]], "-k")
            plt.plot(rf_id[:, 0], rf_id[:, 1], "*k")
            plt.plot(px[0, :], px[1, :], ".r")
            plt.plot(np.array(h_x_true[0, :]).flatten(),
                     np.array(h_x_true[1, :]).flatten(), "-b")
            plt.plot(np.array(h_x_dr[0, :]).flatten(),
                     np.array(h_x_dr[1, :]).flatten(), "-k")
            plt.plot(np.array(h_x_est[0, :]).flatten(),
                     np.array(h_x_est[1, :]).flatten(), "-r")
            plot_covariance_ellipse(x_est, PEst)
            plt.axis("equal")
            plt.grid(True)
            plt.pause(0.001)


if __name__ == '__main__':
    main()
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