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PX4-Autopilot/Tools/ecl_ekf/drag_fusion_tuning/drag_replay.py
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#!/usr/bin/env python
# -*- coding: utf-8 -*-
"""
Copyright (c) 2022 PX4 Development Team
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modification, are permitted provided that the following conditions
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notice, this list of conditions and the following disclaimer in
the documentation and/or other materials provided with the
distribution.
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used to endorse or promote products derived from this software
without specific prior written permission.
THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
"AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
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File: drag_replay.py
Author: Mathieu Bresciani <mathieu@auterion.com>
License: BSD 3-Clause
Description:
Find the best ballistic and momentum drag coefficients for wind estimation
using EKF2 replay data.
NOTE: this script currently assumes no wind.
"""
import matplotlib.pylab as plt
from pyulog import ULog
from pyulog.px4 import PX4ULog
import numpy as np
import quaternion
from scipy import optimize
def getAllData(logfile):
log = ULog(logfile)
v_local = np.matrix([getData(log, 'vehicle_local_position', 'vx'),
getData(log, 'vehicle_local_position', 'vy'),
getData(log, 'vehicle_local_position', 'vz')])
t_v_local = ms2s(getData(log, 'vehicle_local_position', 'timestamp'))
accel = np.matrix([getData(log, 'sensor_combined', 'accelerometer_m_s2[0]'),
getData(log, 'sensor_combined', 'accelerometer_m_s2[1]'),
getData(log, 'sensor_combined', 'accelerometer_m_s2[2]')])
t_accel = ms2s(getData(log, 'sensor_combined', 'timestamp'))
q = np.matrix([getData(log, 'vehicle_attitude', 'q[0]'),
getData(log, 'vehicle_attitude', 'q[1]'),
getData(log, 'vehicle_attitude', 'q[2]'),
getData(log, 'vehicle_attitude', 'q[3]')])
t_q = ms2s(getData(log, 'vehicle_attitude', 'timestamp'))
dist_bottom = getData(log, 'vehicle_local_position', 'dist_bottom')
t_dist_bottom = ms2s(getData(log, 'vehicle_local_position', 'timestamp'))
(t_aligned, v_body_aligned, accel_aligned) = alignData(t_v_local, v_local, t_accel, accel, t_q, q, t_dist_bottom, dist_bottom)
t_aligned -= t_aligned[0]
return (t_aligned, v_body_aligned, accel_aligned)
def alignData(t_v, v_local, t_accel, accel, t_q, q, t_dist_bottom, dist_bottom):
len_accel = len(t_accel)
len_q = len(t_q)
len_db = len(t_dist_bottom)
i_a = 0
i_q = 0
i_db = 0
v_body_aligned = np.empty((3,0))
accel_aligned = np.empty((3,0))
t_aligned = []
for i_v in range(len(t_v)):
t = t_v[i_v]
accel_sum = np.zeros((3,1))
accel_count = 0
while t_accel[i_a] < t and i_a < len_accel-1:
accel_sum += accel[:, i_a] # Integrate accel samples between 2 velocity samples
accel_count += 1
i_a += 1
while t_q[i_q] < t and i_q < len_q-1:
i_q += 1
while t_dist_bottom[i_db] < t and i_db < len_db-1:
i_db += 1
# Only use in air data
if dist_bottom[i_db] < 1.0 or accel_count == 0:
continue
qk = np.quaternion(q[0, i_q],q[1, i_q],q[2, i_q],q[3, i_q])
q_vl = np.quaternion(0, v_local[0, i_v], v_local[1, i_v], v_local[2, i_v])
q_vb = qk.conjugate() * q_vl * qk # Get velocity in body frame
vb = quaternion.as_float_array(q_vb)[1:4]
v_body_aligned = np.append(v_body_aligned, [[vb[0]], [vb[1]], [vb[2]]], axis=1)
accel_aligned = np.append(accel_aligned, accel_sum / accel_count, axis=1)
t_aligned.append(t)
return (t_aligned, v_body_aligned, np.asarray(accel_aligned))
def getData(log, topic_name, variable_name, instance=0):
variable_data = np.array([])
for elem in log.data_list:
if elem.name == topic_name:
if instance == elem.multi_id:
variable_data = elem.data[variable_name]
break
return variable_data
def ms2s(time_ms):
return time_ms * 1e-6
def run(logfile):
(t, v_body, a_body) = getAllData(logfile)
rho = 1.15 # air densitiy
rho15 = 1.225 # air density at 15 degC
# x[0]: momentum drag, scales with v
# x[1]: inverse of ballistic coefficient (X body axis), scales with v^2
# x[2]: inverse of ballistic coefficient (Y body axis), scales with v^2
predict_acc_x = lambda x: -v_body[0] * x[0] - 0.5 * rho * v_body[0]**2 * np.sign(v_body[0]) * x[1]
predict_acc_y = lambda x: -v_body[1] * x[0] - 0.5 * rho * v_body[1]**2 * np.sign(v_body[1]) * x[2]
J = lambda x: np.sum(np.power(abs(a_body[0]-predict_acc_x(x)), 2.0) + np.power(abs(a_body[1]-predict_acc_y(x)), 2.0)) # cost function
x0 = [0.15, 1/100, 1/100] # initial conditions
res = optimize.minimize(J, x0, method='nelder-mead', bounds=[(0,1),(0,10),(0,10)], options={'disp': True})
# Convert results to parameters
innov_var = J(res.x) / (len(v_body[0]) + len(v_body[1]))
mcoef = res.x[0] / np.sqrt(rho / rho15)
bcoef_x = 0.0
bcoef_y = 0.0
if res.x[1] > 1/200:
bcoef_x = 1/res.x[1]
if res.x[2] > 1/200:
bcoef_y = 1/res.x[2]
print(f"param set EKF2_BCOEF_X {bcoef_x:.1f}")
print(f"param set EKF2_BCOEF_Y {bcoef_y:.1f}")
print(f"param set EKF2_MCOEF {mcoef:.2f}")
print(f"/!\EXPERIMENTAL param set EKF2_DRAG_NOISE {innov_var:.2f}")
# Plot data
plt.figure(1)
plt.suptitle(logfile.split('/')[-1])
ax1 = plt.subplot(2, 1, 1)
ax1.plot(t, v_body[0])
ax1.plot(t, v_body[1])
ax1.set_xlabel("time (s)")
ax1.set_ylabel("velocity (m/s)")
ax1.legend(["forward", "right"])
ax2 = plt.subplot(2, 1, 2, sharex=ax1)
ax2.set_title(f"BCoef_x = {bcoef_x:.1f}, BCoef_y = {bcoef_y:.1f}, MCoef = {mcoef:.4f}", loc="right")
ax2.plot(t, a_body[0])
ax2.plot(t, a_body[1])
ax2.plot(t, predict_acc_x(res.x))
ax2.plot(t, predict_acc_y(res.x))
ax2.set_xlabel("time (s)")
ax2.set_ylabel("acceleration (m/s^2)")
ax2.legend(["meas_forward", "meas_right", "predicted_forward", "predicted_right"])
plt.show()
if __name__ == '__main__':
import os
import argparse
# Get the path of this script (without file name)
script_path = os.path.split(os.path.realpath(__file__))[0]
# Parse arguments
parser = argparse.ArgumentParser(
description='Estimate mag biases from ULog file')
# Provide parameter file path and name
parser.add_argument('logfile', help='Full ulog file path, name and extension', type=str)
args = parser.parse_args()
logfile = os.path.abspath(args.logfile) # Convert to absolute path
run(logfile)