示例#1
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def test_quat_inv():

    # Define the quaternion from angle-axis representation
    angle = 0.5*np.pi # Angle for rotation
    x = 0.0
    y = 1.0
    z = 0.0
    quat = Quaternion.from_angle_axis(angle, x, y, z)
    quat_inv_gt = Quaternion.from_angle_axis(angle, -x, -y, -z) # Ground true
    quat_inv = quat.inv()

    inv_arr_gt = quat_inv_gt.to_array()
    inv_arr = quat_inv.to_array()

    assert_allclose(inv_arr, inv_arr_gt)
示例#2
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def test_roll_pitch_yaw():
    # Test the Tait-Bryan angles estimated from quaternion

    angle_gt = 30.0/180*np.pi
    # Roll
    quat = Quaternion.from_angle_axis(angle_gt, 1, 0, 0)
    roll = quat.roll
    assert_allclose(roll, angle_gt)

    # Pitch
    quat = Quaternion.from_angle_axis(angle_gt, 0, 1, 0)
    pitch = quat.pitch
    assert_allclose(pitch, angle_gt)

    # Yaw
    quat = Quaternion.from_angle_axis(angle_gt, 0, 0, 1)
    yaw = quat.yaw
    assert_allclose(yaw, angle_gt)
示例#3
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def test_rotate_axes():

    # Define the quaternion from angle-axis representation
    angle = 0.5*np.pi # Angle for rotation
    quat = Quaternion.from_angle_axis(angle, 1, 0, 0)

    # Define a vector for testing
    vec_ori = np.array([1.0, 0.0, 0.0])

    # Rotate the vector with quaternion
    vec_rot = quat.rotate_axes(vec_ori)

    assert_allclose(vec_rot, vec_ori)
示例#4
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def test_motion_tracker():

    # Sensor fusion
    dt = 1e-2 # Sample period in seconds
    num_iter = 100
    beta = 0.041 # The suggested beta is 0.041 in Madgwick's paper
    fast_version = False

    # Earth magnetic strength and dip angle
    earth_mag=36.0
    earth_dip_deg=30.0
    earth_dip = earth_dip_deg*np.pi/180

    # Sensor orientation
    angle_deg = 3.0
    angle = angle_deg*np.pi/180

    # Rotaion quaternion, sensor axes respective to user axes
    q_se = Quaternion.from_angle_axis(angle, 0, 1, 0)
    angle_axis_in = q_se.to_angle_axis()

    num_dim = 3

    # Angular rate
    gyro_e = np.zeros(num_dim)
    gyro_e[0] = 0.0
    gyro_e[1] = 0.0 #angle/dt
    gyro_e[2] = 0.0

    # Analytic dynamic acceleration in Earth axes
    accel_dyn_e_in = np.zeros(num_dim)
    accel_dyn_e_in[0] = 0.00 # Dynamic acceleration in earth axes
    accel_dyn_e_in[1] = 0.00
    accel_dyn_e_in[2] = 0.00

    # IMU simulator
    imu_simulator = IMUSimulator(gyro_e, accel_dyn_e_in, q_se, earth_mag=earth_mag, earth_dip=earth_dip)
    gyro_in, accel_in, mag_in = imu_simulator.get_imu_data()

    # Eestimate the quaternion
    sf = SensorFusion(dt, beta, num_iter=num_iter, fast_version=fast_version)
    sf.update_ahrs(gyro_in, accel_in, mag_in)
    quat = sf.quat

    # Motion tracker
    tracker = MotionTracker()
    tracker.update(gyro_in, accel_in, mag_in, quat=quat)


    # Analytic dynamic acceleration in Earth axes
    accel_dyn_e_in[0] = 0.1 # Dynamic acceleration in earth axes
    accel_dyn_e_in[1] = 0.1
    accel_dyn_e_in[2] = 0.1

    # IMU simulator
    imu_simulator = IMUSimulator(gyro_e, accel_dyn_e_in, q_se, earth_mag=earth_mag, earth_dip=earth_dip)
    gyro_in, accel_in, mag_in = imu_simulator.get_imu_data()

    # Estimate the quaternion
    sf.update_ahrs(gyro_in, accel_in, mag_in)
    quat = sf.quat
    tracker.update(gyro_in, accel_in, mag_in, quat=quat)

    # Test orientation angles
    roll, pitch, yaw = tracker.get_orientation_angles()
    roll_gt = 0.0
    pitch_gt = angle
    yaw_gt = 0.0

    assert_allclose(roll, roll_gt, atol=1e-3)
    assert_allclose(pitch, pitch_gt, atol=1e-3)
    assert_allclose(yaw, yaw_gt, atol=1e-3)
def test_xsens_motion_tracker():

    dt = 1e-2 # Sample period in seconds
    num_iter = 1000
    beta = 0.041 # The suggested beta is 0.041 in Madgwick's paper
    fast_version = True

    # Earth magnetic strength and dip angle
    earth_mag=36.0

    earth_dip_deg=30.0
    earth_dip = earth_dip_deg*np.pi/180


    # Sensor orientation
    angle_deg = 30.0
    angle = angle_deg*np.pi/180

    # Rotaion quaternion, sensor axes respective to user axes
    q_se = Quaternion.from_angle_axis(angle, 0, 1, 0)
    angle_axis_in = q_se.to_angle_axis()

    num_dim = 3

    # Angular rate
    gyro_e = np.zeros(num_dim)
    gyro_e[0] = 0.0
    gyro_e[1] = 0.0 #angle/dt
    gyro_e[2] = 0.0

    # Analytic dynamic acceleration in Earth axes
    accel_dyn_e_in = np.zeros(num_dim)
    accel_dyn_e_in[0] = 0.00 # Dynamic acceleration in earth axes
    accel_dyn_e_in[1] = 0.00
    accel_dyn_e_in[2] = 0.00

    # IMU simulator
    imu_simulator = IMUSimulator(gyro_e, accel_dyn_e_in, q_se, earth_mag=earth_mag, earth_dip=earth_dip)
    gyro_in, accel_in, mag_in = imu_simulator.get_imu_data()

    # Prepare the video
    timesteps = 5
    rows = 48
    cols = 48
    channels = 1
    shape = (timesteps, rows, cols, channels)
    video = np.zeros(shape, dtype=np.int32)
    video = None

    # Eestimate the quaternion
    sf = SensorFusion(dt, beta, num_iter=num_iter, fast_version=fast_version)
    sf.update_ahrs(gyro_in, accel_in, mag_in)
    quat = sf.quat

    # Xsens motion tracker
    tracker = XsensMotionTracker(accel_th=1e-4, vel_th=1e-5)

    q_se_simu = quat

    tracker.update(gyro_in, accel_in, mag_in, accel_dyn=accel_dyn_e_in,
                   motion_status=1, quat=q_se_simu)

    # Test the estimated position
    x_gt = np.array([np.cos(angle), 0, -np.sin(angle)])

    assert_allclose(tracker.x, x_gt, atol=1e-3)

    # Test orientation angles
    roll, pitch, yaw = tracker.get_orientation_angles()
    roll_gt = 0.0
    pitch_gt = angle
    yaw_gt = 0.0

    assert_allclose(roll, roll_gt, atol=1e-3)
    assert_allclose(pitch, pitch_gt, atol=1e-3)
    assert_allclose(yaw, yaw_gt, atol=1e-3)