forked from Archive/PX4-Autopilot
1086 lines
51 KiB
C++
1086 lines
51 KiB
C++
/****************************************************************************
|
|
*
|
|
* Copyright (c) 2015 Estimation and Control Library (ECL). All rights reserved.
|
|
*
|
|
* Redistribution and use in source and binary forms, with or without
|
|
* modification, are permitted provided that the following conditions
|
|
* are met:
|
|
*
|
|
* 1. Redistributions of source code must retain the above copyright
|
|
* notice, this list of conditions and the following disclaimer.
|
|
* 2. Redistributions in binary form must reproduce the above copyright
|
|
* notice, this list of conditions and the following disclaimer in
|
|
* the documentation and/or other materials provided with the
|
|
* distribution.
|
|
* 3. Neither the name ECL nor the names of its contributors may be
|
|
* 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
|
|
* COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
|
|
* INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
|
|
* BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS
|
|
* OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED
|
|
* AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
|
|
* LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
|
|
* ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
|
|
* POSSIBILITY OF SUCH DAMAGE.
|
|
*
|
|
****************************************************************************/
|
|
|
|
/**
|
|
* @file heading_fusion.cpp
|
|
* Magnetometer fusion methods.
|
|
*
|
|
* @author Roman Bast <bapstroman@gmail.com>
|
|
* @author Paul Riseborough <p_riseborough@live.com.au>
|
|
*
|
|
*/
|
|
|
|
#include "ekf.h"
|
|
#include <ecl.h>
|
|
#include <mathlib/mathlib.h>
|
|
|
|
void Ekf::fuseMag()
|
|
{
|
|
// assign intermediate variables
|
|
const float q0 = _state.quat_nominal(0);
|
|
const float q1 = _state.quat_nominal(1);
|
|
const float q2 = _state.quat_nominal(2);
|
|
const float q3 = _state.quat_nominal(3);
|
|
|
|
const float magN = _state.mag_I(0);
|
|
const float magE = _state.mag_I(1);
|
|
const float magD = _state.mag_I(2);
|
|
|
|
// XYZ Measurement uncertainty. Need to consider timing errors for fast rotations
|
|
const float R_MAG = sq(fmaxf(_params.mag_noise, 0.0f));
|
|
|
|
// intermediate variables from algebraic optimisation
|
|
float SH_MAG[9];
|
|
SH_MAG[0] = 2.0f*magD*q3 + 2.0f*magE*q2 + 2.0f*magN*q1;
|
|
SH_MAG[1] = 2.0f*magD*q0 - 2.0f*magE*q1 + 2.0f*magN*q2;
|
|
SH_MAG[2] = 2.0f*magD*q1 + 2.0f*magE*q0 - 2.0f*magN*q3;
|
|
SH_MAG[3] = sq(q3);
|
|
SH_MAG[4] = sq(q2);
|
|
SH_MAG[5] = sq(q1);
|
|
SH_MAG[6] = sq(q0);
|
|
SH_MAG[7] = 2.0f*magN*q0;
|
|
SH_MAG[8] = 2.0f*magE*q3;
|
|
|
|
// rotate magnetometer earth field state into body frame
|
|
const Dcmf R_to_body = quat_to_invrotmat(_state.quat_nominal);
|
|
|
|
const Vector3f mag_I_rot = R_to_body * _state.mag_I;
|
|
|
|
// compute magnetometer innovations
|
|
_mag_innov[0] = (mag_I_rot(0) + _state.mag_B(0)) - _mag_sample_delayed.mag(0);
|
|
_mag_innov[1] = (mag_I_rot(1) + _state.mag_B(1)) - _mag_sample_delayed.mag(1);
|
|
|
|
// do not use the synthesized measurement for the magnetomter Z component for 3D fusion
|
|
if (_control_status.flags.synthetic_mag_z) {
|
|
_mag_innov[2] = 0.0f;
|
|
} else {
|
|
_mag_innov[2] = (mag_I_rot(2) + _state.mag_B(2)) - _mag_sample_delayed.mag(2);
|
|
}
|
|
// Observation jacobian and Kalman gain vectors
|
|
float H_MAG[24];
|
|
float Kfusion[24];
|
|
|
|
// X axis innovation variance
|
|
_mag_innov_var[0] = (P(19,19) + R_MAG + P(1,19)*SH_MAG[0] - P(2,19)*SH_MAG[1] + P(3,19)*SH_MAG[2] - P(16,19)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + (2.0f*q0*q3 + 2.0f*q1*q2)*(P(19,17) + P(1,17)*SH_MAG[0] - P(2,17)*SH_MAG[1] + P(3,17)*SH_MAG[2] - P(16,17)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + P(17,17)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,17)*(2.0f*q0*q2 - 2.0f*q1*q3) + P(0,17)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - (2.0f*q0*q2 - 2.0f*q1*q3)*(P(19,18) + P(1,18)*SH_MAG[0] - P(2,18)*SH_MAG[1] + P(3,18)*SH_MAG[2] - P(16,18)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + P(17,18)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,18)*(2.0f*q0*q2 - 2.0f*q1*q3) + P(0,18)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + (SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)*(P(19,0) + P(1,0)*SH_MAG[0] - P(2,0)*SH_MAG[1] + P(3,0)*SH_MAG[2] - P(16,0)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + P(17,0)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,0)*(2.0f*q0*q2 - 2.0f*q1*q3) + P(0,0)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + P(17,19)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,19)*(2.0f*q0*q2 - 2.0f*q1*q3) + SH_MAG[0]*(P(19,1) + P(1,1)*SH_MAG[0] - P(2,1)*SH_MAG[1] + P(3,1)*SH_MAG[2] - P(16,1)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + P(17,1)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,1)*(2.0f*q0*q2 - 2.0f*q1*q3) + P(0,1)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - SH_MAG[1]*(P(19,2) + P(1,2)*SH_MAG[0] - P(2,2)*SH_MAG[1] + P(3,2)*SH_MAG[2] - P(16,2)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + P(17,2)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,2)*(2.0f*q0*q2 - 2.0f*q1*q3) + P(0,2)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + SH_MAG[2]*(P(19,3) + P(1,3)*SH_MAG[0] - P(2,3)*SH_MAG[1] + P(3,3)*SH_MAG[2] - P(16,3)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + P(17,3)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,3)*(2.0f*q0*q2 - 2.0f*q1*q3) + P(0,3)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - (SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6])*(P(19,16) + P(1,16)*SH_MAG[0] - P(2,16)*SH_MAG[1] + P(3,16)*SH_MAG[2] - P(16,16)*(SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6]) + P(17,16)*(2.0f*q0*q3 + 2.0f*q1*q2) - P(18,16)*(2.0f*q0*q2 - 2.0f*q1*q3) + P(0,16)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + P(0,19)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2));
|
|
// check for a badly conditioned covariance matrix
|
|
|
|
if (_mag_innov_var[0] >= R_MAG) {
|
|
// the innovation variance contribution from the state covariances is non-negative - no fault
|
|
_fault_status.flags.bad_mag_x = false;
|
|
|
|
} else {
|
|
// the innovation variance contribution from the state covariances is negative which means the covariance matrix is badly conditioned
|
|
_fault_status.flags.bad_mag_x = true;
|
|
|
|
// we need to re-initialise covariances and abort this fusion step
|
|
resetMagRelatedCovariances();
|
|
ECL_ERR_TIMESTAMPED("magX fusion numerical error - covariance reset");
|
|
return;
|
|
|
|
}
|
|
|
|
// Y axis innovation variance
|
|
_mag_innov_var[1] = (P(20,20) + R_MAG + P(0,20)*SH_MAG[2] + P(1,20)*SH_MAG[1] + P(2,20)*SH_MAG[0] - P(17,20)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - (2.0f*q0*q3 - 2.0f*q1*q2)*(P(20,16) + P(0,16)*SH_MAG[2] + P(1,16)*SH_MAG[1] + P(2,16)*SH_MAG[0] - P(17,16)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - P(16,16)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,16)*(2.0f*q0*q1 + 2.0f*q2*q3) - P(3,16)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + (2.0f*q0*q1 + 2.0f*q2*q3)*(P(20,18) + P(0,18)*SH_MAG[2] + P(1,18)*SH_MAG[1] + P(2,18)*SH_MAG[0] - P(17,18)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - P(16,18)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,18)*(2.0f*q0*q1 + 2.0f*q2*q3) - P(3,18)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - (SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)*(P(20,3) + P(0,3)*SH_MAG[2] + P(1,3)*SH_MAG[1] + P(2,3)*SH_MAG[0] - P(17,3)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - P(16,3)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,3)*(2.0f*q0*q1 + 2.0f*q2*q3) - P(3,3)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - P(16,20)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,20)*(2.0f*q0*q1 + 2.0f*q2*q3) + SH_MAG[2]*(P(20,0) + P(0,0)*SH_MAG[2] + P(1,0)*SH_MAG[1] + P(2,0)*SH_MAG[0] - P(17,0)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - P(16,0)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,0)*(2.0f*q0*q1 + 2.0f*q2*q3) - P(3,0)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + SH_MAG[1]*(P(20,1) + P(0,1)*SH_MAG[2] + P(1,1)*SH_MAG[1] + P(2,1)*SH_MAG[0] - P(17,1)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - P(16,1)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,1)*(2.0f*q0*q1 + 2.0f*q2*q3) - P(3,1)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + SH_MAG[0]*(P(20,2) + P(0,2)*SH_MAG[2] + P(1,2)*SH_MAG[1] + P(2,2)*SH_MAG[0] - P(17,2)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - P(16,2)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,2)*(2.0f*q0*q1 + 2.0f*q2*q3) - P(3,2)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - (SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6])*(P(20,17) + P(0,17)*SH_MAG[2] + P(1,17)*SH_MAG[1] + P(2,17)*SH_MAG[0] - P(17,17)*(SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6]) - P(16,17)*(2.0f*q0*q3 - 2.0f*q1*q2) + P(18,17)*(2.0f*q0*q1 + 2.0f*q2*q3) - P(3,17)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - P(3,20)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2));
|
|
|
|
// check for a badly conditioned covariance matrix
|
|
if (_mag_innov_var[1] >= R_MAG) {
|
|
// the innovation variance contribution from the state covariances is non-negative - no fault
|
|
_fault_status.flags.bad_mag_y = false;
|
|
|
|
} else {
|
|
// the innovation variance contribution from the state covariances is negtive which means the covariance matrix is badly conditioned
|
|
_fault_status.flags.bad_mag_y = true;
|
|
|
|
// we need to re-initialise covariances and abort this fusion step
|
|
resetMagRelatedCovariances();
|
|
ECL_ERR_TIMESTAMPED("magY fusion numerical error - covariance reset");
|
|
return;
|
|
|
|
}
|
|
|
|
// Z axis innovation variance
|
|
_mag_innov_var[2] = (P(21,21) + R_MAG + P(0,21)*SH_MAG[1] - P(1,21)*SH_MAG[2] + P(3,21)*SH_MAG[0] + P(18,21)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + (2.0f*q0*q2 + 2.0f*q1*q3)*(P(21,16) + P(0,16)*SH_MAG[1] - P(1,16)*SH_MAG[2] + P(3,16)*SH_MAG[0] + P(18,16)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + P(16,16)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,16)*(2.0f*q0*q1 - 2.0f*q2*q3) + P(2,16)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - (2.0f*q0*q1 - 2.0f*q2*q3)*(P(21,17) + P(0,17)*SH_MAG[1] - P(1,17)*SH_MAG[2] + P(3,17)*SH_MAG[0] + P(18,17)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + P(16,17)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,17)*(2.0f*q0*q1 - 2.0f*q2*q3) + P(2,17)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + (SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)*(P(21,2) + P(0,2)*SH_MAG[1] - P(1,2)*SH_MAG[2] + P(3,2)*SH_MAG[0] + P(18,2)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + P(16,2)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,2)*(2.0f*q0*q1 - 2.0f*q2*q3) + P(2,2)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + P(16,21)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,21)*(2.0f*q0*q1 - 2.0f*q2*q3) + SH_MAG[1]*(P(21,0) + P(0,0)*SH_MAG[1] - P(1,0)*SH_MAG[2] + P(3,0)*SH_MAG[0] + P(18,0)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + P(16,0)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,0)*(2.0f*q0*q1 - 2.0f*q2*q3) + P(2,0)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) - SH_MAG[2]*(P(21,1) + P(0,1)*SH_MAG[1] - P(1,1)*SH_MAG[2] + P(3,1)*SH_MAG[0] + P(18,1)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + P(16,1)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,1)*(2.0f*q0*q1 - 2.0f*q2*q3) + P(2,1)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + SH_MAG[0]*(P(21,3) + P(0,3)*SH_MAG[1] - P(1,3)*SH_MAG[2] + P(3,3)*SH_MAG[0] + P(18,3)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + P(16,3)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,3)*(2.0f*q0*q1 - 2.0f*q2*q3) + P(2,3)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + (SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6])*(P(21,18) + P(0,18)*SH_MAG[1] - P(1,18)*SH_MAG[2] + P(3,18)*SH_MAG[0] + P(18,18)*(SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6]) + P(16,18)*(2.0f*q0*q2 + 2.0f*q1*q3) - P(17,18)*(2.0f*q0*q1 - 2.0f*q2*q3) + P(2,18)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2)) + P(2,21)*(SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2));
|
|
|
|
// check for a badly conditioned covariance matrix
|
|
if (_mag_innov_var[2] >= R_MAG) {
|
|
// the innovation variance contribution from the state covariances is non-negative - no fault
|
|
_fault_status.flags.bad_mag_z = false;
|
|
|
|
} else if (_mag_innov_var[2] > 0.0f) {
|
|
// the innovation variance contribution from the state covariances is negative which means the covariance matrix is badly conditioned
|
|
_fault_status.flags.bad_mag_z = true;
|
|
|
|
// we need to re-initialise covariances and abort this fusion step
|
|
resetMagRelatedCovariances();
|
|
ECL_ERR_TIMESTAMPED("magZ fusion numerical error - covariance reset");
|
|
return;
|
|
|
|
}
|
|
|
|
// Perform an innovation consistency check and report the result
|
|
bool healthy = true;
|
|
|
|
for (uint8_t index = 0; index <= 2; index++) {
|
|
_mag_test_ratio[index] = sq(_mag_innov[index]) / (sq(math::max(_params.mag_innov_gate, 1.0f)) * _mag_innov_var[index]);
|
|
|
|
if (_mag_test_ratio[index] > 1.0f) {
|
|
healthy = false;
|
|
_innov_check_fail_status.value |= (1 << (index + 3));
|
|
|
|
} else {
|
|
_innov_check_fail_status.value &= ~(1 << (index + 3));
|
|
}
|
|
}
|
|
|
|
// we are no longer using heading fusion so set the reported test level to zero
|
|
_yaw_test_ratio = 0.0f;
|
|
|
|
// if any axis fails, abort the mag fusion
|
|
if (!healthy) {
|
|
return;
|
|
}
|
|
|
|
// For the first few seconds after in-flight alignment we allow the magnetic field state estimates to stabilise
|
|
// before they are used to constrain heading drift
|
|
const bool update_all_states = ((_imu_sample_delayed.time_us - _flt_mag_align_start_time) > (uint64_t)5e6);
|
|
|
|
// update the states and covariance using sequential fusion of the magnetometer components
|
|
for (uint8_t index = 0; index <= 2; index++) {
|
|
|
|
// Calculate Kalman gains and observation jacobians
|
|
if (index == 0) {
|
|
// Calculate X axis observation jacobians
|
|
memset(H_MAG, 0, sizeof(H_MAG));
|
|
H_MAG[0] = SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2;
|
|
H_MAG[1] = SH_MAG[0];
|
|
H_MAG[2] = -SH_MAG[1];
|
|
H_MAG[3] = SH_MAG[2];
|
|
H_MAG[16] = SH_MAG[5] - SH_MAG[4] - SH_MAG[3] + SH_MAG[6];
|
|
H_MAG[17] = 2.0f*q0*q3 + 2.0f*q1*q2;
|
|
H_MAG[18] = 2.0f*q1*q3 - 2.0f*q0*q2;
|
|
H_MAG[19] = 1.0f;
|
|
|
|
// Calculate X axis Kalman gains
|
|
float SK_MX[5];
|
|
SK_MX[0] = 1.0f / _mag_innov_var[0];
|
|
SK_MX[1] = SH_MAG[3] + SH_MAG[4] - SH_MAG[5] - SH_MAG[6];
|
|
SK_MX[2] = SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2;
|
|
SK_MX[3] = 2.0f*q0*q2 - 2.0f*q1*q3;
|
|
SK_MX[4] = 2.0f*q0*q3 + 2.0f*q1*q2;
|
|
|
|
if (update_all_states) {
|
|
Kfusion[0] = SK_MX[0]*(P(0,19) + P(0,1)*SH_MAG[0] - P(0,2)*SH_MAG[1] + P(0,3)*SH_MAG[2] + P(0,0)*SK_MX[2] - P(0,16)*SK_MX[1] + P(0,17)*SK_MX[4] - P(0,18)*SK_MX[3]);
|
|
Kfusion[1] = SK_MX[0]*(P(1,19) + P(1,1)*SH_MAG[0] - P(1,2)*SH_MAG[1] + P(1,3)*SH_MAG[2] + P(1,0)*SK_MX[2] - P(1,16)*SK_MX[1] + P(1,17)*SK_MX[4] - P(1,18)*SK_MX[3]);
|
|
Kfusion[2] = SK_MX[0]*(P(2,19) + P(2,1)*SH_MAG[0] - P(2,2)*SH_MAG[1] + P(2,3)*SH_MAG[2] + P(2,0)*SK_MX[2] - P(2,16)*SK_MX[1] + P(2,17)*SK_MX[4] - P(2,18)*SK_MX[3]);
|
|
Kfusion[3] = SK_MX[0]*(P(3,19) + P(3,1)*SH_MAG[0] - P(3,2)*SH_MAG[1] + P(3,3)*SH_MAG[2] + P(3,0)*SK_MX[2] - P(3,16)*SK_MX[1] + P(3,17)*SK_MX[4] - P(3,18)*SK_MX[3]);
|
|
Kfusion[4] = SK_MX[0]*(P(4,19) + P(4,1)*SH_MAG[0] - P(4,2)*SH_MAG[1] + P(4,3)*SH_MAG[2] + P(4,0)*SK_MX[2] - P(4,16)*SK_MX[1] + P(4,17)*SK_MX[4] - P(4,18)*SK_MX[3]);
|
|
Kfusion[5] = SK_MX[0]*(P(5,19) + P(5,1)*SH_MAG[0] - P(5,2)*SH_MAG[1] + P(5,3)*SH_MAG[2] + P(5,0)*SK_MX[2] - P(5,16)*SK_MX[1] + P(5,17)*SK_MX[4] - P(5,18)*SK_MX[3]);
|
|
Kfusion[6] = SK_MX[0]*(P(6,19) + P(6,1)*SH_MAG[0] - P(6,2)*SH_MAG[1] + P(6,3)*SH_MAG[2] + P(6,0)*SK_MX[2] - P(6,16)*SK_MX[1] + P(6,17)*SK_MX[4] - P(6,18)*SK_MX[3]);
|
|
Kfusion[7] = SK_MX[0]*(P(7,19) + P(7,1)*SH_MAG[0] - P(7,2)*SH_MAG[1] + P(7,3)*SH_MAG[2] + P(7,0)*SK_MX[2] - P(7,16)*SK_MX[1] + P(7,17)*SK_MX[4] - P(7,18)*SK_MX[3]);
|
|
Kfusion[8] = SK_MX[0]*(P(8,19) + P(8,1)*SH_MAG[0] - P(8,2)*SH_MAG[1] + P(8,3)*SH_MAG[2] + P(8,0)*SK_MX[2] - P(8,16)*SK_MX[1] + P(8,17)*SK_MX[4] - P(8,18)*SK_MX[3]);
|
|
Kfusion[9] = SK_MX[0]*(P(9,19) + P(9,1)*SH_MAG[0] - P(9,2)*SH_MAG[1] + P(9,3)*SH_MAG[2] + P(9,0)*SK_MX[2] - P(9,16)*SK_MX[1] + P(9,17)*SK_MX[4] - P(9,18)*SK_MX[3]);
|
|
Kfusion[10] = SK_MX[0]*(P(10,19) + P(10,1)*SH_MAG[0] - P(10,2)*SH_MAG[1] + P(10,3)*SH_MAG[2] + P(10,0)*SK_MX[2] - P(10,16)*SK_MX[1] + P(10,17)*SK_MX[4] - P(10,18)*SK_MX[3]);
|
|
Kfusion[11] = SK_MX[0]*(P(11,19) + P(11,1)*SH_MAG[0] - P(11,2)*SH_MAG[1] + P(11,3)*SH_MAG[2] + P(11,0)*SK_MX[2] - P(11,16)*SK_MX[1] + P(11,17)*SK_MX[4] - P(11,18)*SK_MX[3]);
|
|
Kfusion[12] = SK_MX[0]*(P(12,19) + P(12,1)*SH_MAG[0] - P(12,2)*SH_MAG[1] + P(12,3)*SH_MAG[2] + P(12,0)*SK_MX[2] - P(12,16)*SK_MX[1] + P(12,17)*SK_MX[4] - P(12,18)*SK_MX[3]);
|
|
Kfusion[13] = SK_MX[0]*(P(13,19) + P(13,1)*SH_MAG[0] - P(13,2)*SH_MAG[1] + P(13,3)*SH_MAG[2] + P(13,0)*SK_MX[2] - P(13,16)*SK_MX[1] + P(13,17)*SK_MX[4] - P(13,18)*SK_MX[3]);
|
|
Kfusion[14] = SK_MX[0]*(P(14,19) + P(14,1)*SH_MAG[0] - P(14,2)*SH_MAG[1] + P(14,3)*SH_MAG[2] + P(14,0)*SK_MX[2] - P(14,16)*SK_MX[1] + P(14,17)*SK_MX[4] - P(14,18)*SK_MX[3]);
|
|
Kfusion[15] = SK_MX[0]*(P(15,19) + P(15,1)*SH_MAG[0] - P(15,2)*SH_MAG[1] + P(15,3)*SH_MAG[2] + P(15,0)*SK_MX[2] - P(15,16)*SK_MX[1] + P(15,17)*SK_MX[4] - P(15,18)*SK_MX[3]);
|
|
Kfusion[22] = SK_MX[0]*(P(22,19) + P(22,1)*SH_MAG[0] - P(22,2)*SH_MAG[1] + P(22,3)*SH_MAG[2] + P(22,0)*SK_MX[2] - P(22,16)*SK_MX[1] + P(22,17)*SK_MX[4] - P(22,18)*SK_MX[3]);
|
|
Kfusion[23] = SK_MX[0]*(P(23,19) + P(23,1)*SH_MAG[0] - P(23,2)*SH_MAG[1] + P(23,3)*SH_MAG[2] + P(23,0)*SK_MX[2] - P(23,16)*SK_MX[1] + P(23,17)*SK_MX[4] - P(23,18)*SK_MX[3]);
|
|
} else {
|
|
for (uint8_t i = 0; i < 16; i++) {
|
|
Kfusion[i] = 0.0f;
|
|
}
|
|
|
|
Kfusion[22] = 0.0f;
|
|
Kfusion[23] = 0.0f;
|
|
}
|
|
|
|
Kfusion[16] = SK_MX[0]*(P(16,19) + P(16,1)*SH_MAG[0] - P(16,2)*SH_MAG[1] + P(16,3)*SH_MAG[2] + P(16,0)*SK_MX[2] - P(16,16)*SK_MX[1] + P(16,17)*SK_MX[4] - P(16,18)*SK_MX[3]);
|
|
Kfusion[17] = SK_MX[0]*(P(17,19) + P(17,1)*SH_MAG[0] - P(17,2)*SH_MAG[1] + P(17,3)*SH_MAG[2] + P(17,0)*SK_MX[2] - P(17,16)*SK_MX[1] + P(17,17)*SK_MX[4] - P(17,18)*SK_MX[3]);
|
|
Kfusion[18] = SK_MX[0]*(P(18,19) + P(18,1)*SH_MAG[0] - P(18,2)*SH_MAG[1] + P(18,3)*SH_MAG[2] + P(18,0)*SK_MX[2] - P(18,16)*SK_MX[1] + P(18,17)*SK_MX[4] - P(18,18)*SK_MX[3]);
|
|
Kfusion[19] = SK_MX[0]*(P(19,19) + P(19,1)*SH_MAG[0] - P(19,2)*SH_MAG[1] + P(19,3)*SH_MAG[2] + P(19,0)*SK_MX[2] - P(19,16)*SK_MX[1] + P(19,17)*SK_MX[4] - P(19,18)*SK_MX[3]);
|
|
Kfusion[20] = SK_MX[0]*(P(20,19) + P(20,1)*SH_MAG[0] - P(20,2)*SH_MAG[1] + P(20,3)*SH_MAG[2] + P(20,0)*SK_MX[2] - P(20,16)*SK_MX[1] + P(20,17)*SK_MX[4] - P(20,18)*SK_MX[3]);
|
|
Kfusion[21] = SK_MX[0]*(P(21,19) + P(21,1)*SH_MAG[0] - P(21,2)*SH_MAG[1] + P(21,3)*SH_MAG[2] + P(21,0)*SK_MX[2] - P(21,16)*SK_MX[1] + P(21,17)*SK_MX[4] - P(21,18)*SK_MX[3]);
|
|
|
|
} else if (index == 1) {
|
|
// Calculate Y axis observation jacobians
|
|
memset(H_MAG, 0, sizeof(H_MAG));
|
|
H_MAG[0] = SH_MAG[2];
|
|
H_MAG[1] = SH_MAG[1];
|
|
H_MAG[2] = SH_MAG[0];
|
|
H_MAG[3] = 2.0f*magD*q2 - SH_MAG[8] - SH_MAG[7];
|
|
H_MAG[16] = 2.0f*q1*q2 - 2.0f*q0*q3;
|
|
H_MAG[17] = SH_MAG[4] - SH_MAG[3] - SH_MAG[5] + SH_MAG[6];
|
|
H_MAG[18] = 2.0f*q0*q1 + 2.0f*q2*q3;
|
|
H_MAG[20] = 1.0f;
|
|
|
|
// Calculate Y axis Kalman gains
|
|
float SK_MY[5];
|
|
SK_MY[0] = 1.0f / _mag_innov_var[1];
|
|
SK_MY[1] = SH_MAG[3] - SH_MAG[4] + SH_MAG[5] - SH_MAG[6];
|
|
SK_MY[2] = SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2;
|
|
SK_MY[3] = 2.0f*q0*q3 - 2.0f*q1*q2;
|
|
SK_MY[4] = 2.0f*q0*q1 + 2.0f*q2*q3;
|
|
|
|
if (update_all_states) {
|
|
Kfusion[0] = SK_MY[0]*(P(0,20) + P(0,0)*SH_MAG[2] + P(0,1)*SH_MAG[1] + P(0,2)*SH_MAG[0] - P(0,3)*SK_MY[2] - P(0,17)*SK_MY[1] - P(0,16)*SK_MY[3] + P(0,18)*SK_MY[4]);
|
|
Kfusion[1] = SK_MY[0]*(P(1,20) + P(1,0)*SH_MAG[2] + P(1,1)*SH_MAG[1] + P(1,2)*SH_MAG[0] - P(1,3)*SK_MY[2] - P(1,17)*SK_MY[1] - P(1,16)*SK_MY[3] + P(1,18)*SK_MY[4]);
|
|
Kfusion[2] = SK_MY[0]*(P(2,20) + P(2,0)*SH_MAG[2] + P(2,1)*SH_MAG[1] + P(2,2)*SH_MAG[0] - P(2,3)*SK_MY[2] - P(2,17)*SK_MY[1] - P(2,16)*SK_MY[3] + P(2,18)*SK_MY[4]);
|
|
Kfusion[3] = SK_MY[0]*(P(3,20) + P(3,0)*SH_MAG[2] + P(3,1)*SH_MAG[1] + P(3,2)*SH_MAG[0] - P(3,3)*SK_MY[2] - P(3,17)*SK_MY[1] - P(3,16)*SK_MY[3] + P(3,18)*SK_MY[4]);
|
|
Kfusion[4] = SK_MY[0]*(P(4,20) + P(4,0)*SH_MAG[2] + P(4,1)*SH_MAG[1] + P(4,2)*SH_MAG[0] - P(4,3)*SK_MY[2] - P(4,17)*SK_MY[1] - P(4,16)*SK_MY[3] + P(4,18)*SK_MY[4]);
|
|
Kfusion[5] = SK_MY[0]*(P(5,20) + P(5,0)*SH_MAG[2] + P(5,1)*SH_MAG[1] + P(5,2)*SH_MAG[0] - P(5,3)*SK_MY[2] - P(5,17)*SK_MY[1] - P(5,16)*SK_MY[3] + P(5,18)*SK_MY[4]);
|
|
Kfusion[6] = SK_MY[0]*(P(6,20) + P(6,0)*SH_MAG[2] + P(6,1)*SH_MAG[1] + P(6,2)*SH_MAG[0] - P(6,3)*SK_MY[2] - P(6,17)*SK_MY[1] - P(6,16)*SK_MY[3] + P(6,18)*SK_MY[4]);
|
|
Kfusion[7] = SK_MY[0]*(P(7,20) + P(7,0)*SH_MAG[2] + P(7,1)*SH_MAG[1] + P(7,2)*SH_MAG[0] - P(7,3)*SK_MY[2] - P(7,17)*SK_MY[1] - P(7,16)*SK_MY[3] + P(7,18)*SK_MY[4]);
|
|
Kfusion[8] = SK_MY[0]*(P(8,20) + P(8,0)*SH_MAG[2] + P(8,1)*SH_MAG[1] + P(8,2)*SH_MAG[0] - P(8,3)*SK_MY[2] - P(8,17)*SK_MY[1] - P(8,16)*SK_MY[3] + P(8,18)*SK_MY[4]);
|
|
Kfusion[9] = SK_MY[0]*(P(9,20) + P(9,0)*SH_MAG[2] + P(9,1)*SH_MAG[1] + P(9,2)*SH_MAG[0] - P(9,3)*SK_MY[2] - P(9,17)*SK_MY[1] - P(9,16)*SK_MY[3] + P(9,18)*SK_MY[4]);
|
|
Kfusion[10] = SK_MY[0]*(P(10,20) + P(10,0)*SH_MAG[2] + P(10,1)*SH_MAG[1] + P(10,2)*SH_MAG[0] - P(10,3)*SK_MY[2] - P(10,17)*SK_MY[1] - P(10,16)*SK_MY[3] + P(10,18)*SK_MY[4]);
|
|
Kfusion[11] = SK_MY[0]*(P(11,20) + P(11,0)*SH_MAG[2] + P(11,1)*SH_MAG[1] + P(11,2)*SH_MAG[0] - P(11,3)*SK_MY[2] - P(11,17)*SK_MY[1] - P(11,16)*SK_MY[3] + P(11,18)*SK_MY[4]);
|
|
Kfusion[12] = SK_MY[0]*(P(12,20) + P(12,0)*SH_MAG[2] + P(12,1)*SH_MAG[1] + P(12,2)*SH_MAG[0] - P(12,3)*SK_MY[2] - P(12,17)*SK_MY[1] - P(12,16)*SK_MY[3] + P(12,18)*SK_MY[4]);
|
|
Kfusion[13] = SK_MY[0]*(P(13,20) + P(13,0)*SH_MAG[2] + P(13,1)*SH_MAG[1] + P(13,2)*SH_MAG[0] - P(13,3)*SK_MY[2] - P(13,17)*SK_MY[1] - P(13,16)*SK_MY[3] + P(13,18)*SK_MY[4]);
|
|
Kfusion[14] = SK_MY[0]*(P(14,20) + P(14,0)*SH_MAG[2] + P(14,1)*SH_MAG[1] + P(14,2)*SH_MAG[0] - P(14,3)*SK_MY[2] - P(14,17)*SK_MY[1] - P(14,16)*SK_MY[3] + P(14,18)*SK_MY[4]);
|
|
Kfusion[15] = SK_MY[0]*(P(15,20) + P(15,0)*SH_MAG[2] + P(15,1)*SH_MAG[1] + P(15,2)*SH_MAG[0] - P(15,3)*SK_MY[2] - P(15,17)*SK_MY[1] - P(15,16)*SK_MY[3] + P(15,18)*SK_MY[4]);
|
|
Kfusion[22] = SK_MY[0]*(P(22,20) + P(22,0)*SH_MAG[2] + P(22,1)*SH_MAG[1] + P(22,2)*SH_MAG[0] - P(22,3)*SK_MY[2] - P(22,17)*SK_MY[1] - P(22,16)*SK_MY[3] + P(22,18)*SK_MY[4]);
|
|
Kfusion[23] = SK_MY[0]*(P(23,20) + P(23,0)*SH_MAG[2] + P(23,1)*SH_MAG[1] + P(23,2)*SH_MAG[0] - P(23,3)*SK_MY[2] - P(23,17)*SK_MY[1] - P(23,16)*SK_MY[3] + P(23,18)*SK_MY[4]);
|
|
} else {
|
|
for (uint8_t i = 0; i < 16; i++) {
|
|
Kfusion[i] = 0.0f;
|
|
}
|
|
|
|
Kfusion[22] = 0.0f;
|
|
Kfusion[23] = 0.0f;
|
|
}
|
|
|
|
Kfusion[16] = SK_MY[0]*(P(16,20) + P(16,0)*SH_MAG[2] + P(16,1)*SH_MAG[1] + P(16,2)*SH_MAG[0] - P(16,3)*SK_MY[2] - P(16,17)*SK_MY[1] - P(16,16)*SK_MY[3] + P(16,18)*SK_MY[4]);
|
|
Kfusion[17] = SK_MY[0]*(P(17,20) + P(17,0)*SH_MAG[2] + P(17,1)*SH_MAG[1] + P(17,2)*SH_MAG[0] - P(17,3)*SK_MY[2] - P(17,17)*SK_MY[1] - P(17,16)*SK_MY[3] + P(17,18)*SK_MY[4]);
|
|
Kfusion[18] = SK_MY[0]*(P(18,20) + P(18,0)*SH_MAG[2] + P(18,1)*SH_MAG[1] + P(18,2)*SH_MAG[0] - P(18,3)*SK_MY[2] - P(18,17)*SK_MY[1] - P(18,16)*SK_MY[3] + P(18,18)*SK_MY[4]);
|
|
Kfusion[19] = SK_MY[0]*(P(19,20) + P(19,0)*SH_MAG[2] + P(19,1)*SH_MAG[1] + P(19,2)*SH_MAG[0] - P(19,3)*SK_MY[2] - P(19,17)*SK_MY[1] - P(19,16)*SK_MY[3] + P(19,18)*SK_MY[4]);
|
|
Kfusion[20] = SK_MY[0]*(P(20,20) + P(20,0)*SH_MAG[2] + P(20,1)*SH_MAG[1] + P(20,2)*SH_MAG[0] - P(20,3)*SK_MY[2] - P(20,17)*SK_MY[1] - P(20,16)*SK_MY[3] + P(20,18)*SK_MY[4]);
|
|
Kfusion[21] = SK_MY[0]*(P(21,20) + P(21,0)*SH_MAG[2] + P(21,1)*SH_MAG[1] + P(21,2)*SH_MAG[0] - P(21,3)*SK_MY[2] - P(21,17)*SK_MY[1] - P(21,16)*SK_MY[3] + P(21,18)*SK_MY[4]);
|
|
|
|
} else if (index == 2) {
|
|
|
|
// we do not fuse synthesized magnetomter measurements when doing 3D fusion
|
|
if (_control_status.flags.synthetic_mag_z) {
|
|
continue;
|
|
}
|
|
|
|
// calculate Z axis observation jacobians
|
|
memset(H_MAG, 0, sizeof(H_MAG));
|
|
H_MAG[0] = SH_MAG[1];
|
|
H_MAG[1] = -SH_MAG[2];
|
|
H_MAG[2] = SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2;
|
|
H_MAG[3] = SH_MAG[0];
|
|
H_MAG[16] = 2.0f*q0*q2 + 2.0f*q1*q3;
|
|
H_MAG[17] = 2.0f*q2*q3 - 2.0f*q0*q1;
|
|
H_MAG[18] = SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6];
|
|
H_MAG[21] = 1.0f;
|
|
|
|
// Calculate Z axis Kalman gains
|
|
float SK_MZ[5];
|
|
SK_MZ[0] = 1.0f / _mag_innov_var[2];
|
|
SK_MZ[1] = SH_MAG[3] - SH_MAG[4] - SH_MAG[5] + SH_MAG[6];
|
|
SK_MZ[2] = SH_MAG[7] + SH_MAG[8] - 2.0f*magD*q2;
|
|
SK_MZ[3] = 2.0f*q0*q1 - 2.0f*q2*q3;
|
|
SK_MZ[4] = 2.0f*q0*q2 + 2.0f*q1*q3;
|
|
|
|
if (update_all_states) {
|
|
Kfusion[0] = SK_MZ[0]*(P(0,21) + P(0,0)*SH_MAG[1] - P(0,1)*SH_MAG[2] + P(0,3)*SH_MAG[0] + P(0,2)*SK_MZ[2] + P(0,18)*SK_MZ[1] + P(0,16)*SK_MZ[4] - P(0,17)*SK_MZ[3]);
|
|
Kfusion[1] = SK_MZ[0]*(P(1,21) + P(1,0)*SH_MAG[1] - P(1,1)*SH_MAG[2] + P(1,3)*SH_MAG[0] + P(1,2)*SK_MZ[2] + P(1,18)*SK_MZ[1] + P(1,16)*SK_MZ[4] - P(1,17)*SK_MZ[3]);
|
|
Kfusion[2] = SK_MZ[0]*(P(2,21) + P(2,0)*SH_MAG[1] - P(2,1)*SH_MAG[2] + P(2,3)*SH_MAG[0] + P(2,2)*SK_MZ[2] + P(2,18)*SK_MZ[1] + P(2,16)*SK_MZ[4] - P(2,17)*SK_MZ[3]);
|
|
Kfusion[3] = SK_MZ[0]*(P(3,21) + P(3,0)*SH_MAG[1] - P(3,1)*SH_MAG[2] + P(3,3)*SH_MAG[0] + P(3,2)*SK_MZ[2] + P(3,18)*SK_MZ[1] + P(3,16)*SK_MZ[4] - P(3,17)*SK_MZ[3]);
|
|
Kfusion[4] = SK_MZ[0]*(P(4,21) + P(4,0)*SH_MAG[1] - P(4,1)*SH_MAG[2] + P(4,3)*SH_MAG[0] + P(4,2)*SK_MZ[2] + P(4,18)*SK_MZ[1] + P(4,16)*SK_MZ[4] - P(4,17)*SK_MZ[3]);
|
|
Kfusion[5] = SK_MZ[0]*(P(5,21) + P(5,0)*SH_MAG[1] - P(5,1)*SH_MAG[2] + P(5,3)*SH_MAG[0] + P(5,2)*SK_MZ[2] + P(5,18)*SK_MZ[1] + P(5,16)*SK_MZ[4] - P(5,17)*SK_MZ[3]);
|
|
Kfusion[6] = SK_MZ[0]*(P(6,21) + P(6,0)*SH_MAG[1] - P(6,1)*SH_MAG[2] + P(6,3)*SH_MAG[0] + P(6,2)*SK_MZ[2] + P(6,18)*SK_MZ[1] + P(6,16)*SK_MZ[4] - P(6,17)*SK_MZ[3]);
|
|
Kfusion[7] = SK_MZ[0]*(P(7,21) + P(7,0)*SH_MAG[1] - P(7,1)*SH_MAG[2] + P(7,3)*SH_MAG[0] + P(7,2)*SK_MZ[2] + P(7,18)*SK_MZ[1] + P(7,16)*SK_MZ[4] - P(7,17)*SK_MZ[3]);
|
|
Kfusion[8] = SK_MZ[0]*(P(8,21) + P(8,0)*SH_MAG[1] - P(8,1)*SH_MAG[2] + P(8,3)*SH_MAG[0] + P(8,2)*SK_MZ[2] + P(8,18)*SK_MZ[1] + P(8,16)*SK_MZ[4] - P(8,17)*SK_MZ[3]);
|
|
Kfusion[9] = SK_MZ[0]*(P(9,21) + P(9,0)*SH_MAG[1] - P(9,1)*SH_MAG[2] + P(9,3)*SH_MAG[0] + P(9,2)*SK_MZ[2] + P(9,18)*SK_MZ[1] + P(9,16)*SK_MZ[4] - P(9,17)*SK_MZ[3]);
|
|
Kfusion[10] = SK_MZ[0]*(P(10,21) + P(10,0)*SH_MAG[1] - P(10,1)*SH_MAG[2] + P(10,3)*SH_MAG[0] + P(10,2)*SK_MZ[2] + P(10,18)*SK_MZ[1] + P(10,16)*SK_MZ[4] - P(10,17)*SK_MZ[3]);
|
|
Kfusion[11] = SK_MZ[0]*(P(11,21) + P(11,0)*SH_MAG[1] - P(11,1)*SH_MAG[2] + P(11,3)*SH_MAG[0] + P(11,2)*SK_MZ[2] + P(11,18)*SK_MZ[1] + P(11,16)*SK_MZ[4] - P(11,17)*SK_MZ[3]);
|
|
Kfusion[12] = SK_MZ[0]*(P(12,21) + P(12,0)*SH_MAG[1] - P(12,1)*SH_MAG[2] + P(12,3)*SH_MAG[0] + P(12,2)*SK_MZ[2] + P(12,18)*SK_MZ[1] + P(12,16)*SK_MZ[4] - P(12,17)*SK_MZ[3]);
|
|
Kfusion[13] = SK_MZ[0]*(P(13,21) + P(13,0)*SH_MAG[1] - P(13,1)*SH_MAG[2] + P(13,3)*SH_MAG[0] + P(13,2)*SK_MZ[2] + P(13,18)*SK_MZ[1] + P(13,16)*SK_MZ[4] - P(13,17)*SK_MZ[3]);
|
|
Kfusion[14] = SK_MZ[0]*(P(14,21) + P(14,0)*SH_MAG[1] - P(14,1)*SH_MAG[2] + P(14,3)*SH_MAG[0] + P(14,2)*SK_MZ[2] + P(14,18)*SK_MZ[1] + P(14,16)*SK_MZ[4] - P(14,17)*SK_MZ[3]);
|
|
Kfusion[15] = SK_MZ[0]*(P(15,21) + P(15,0)*SH_MAG[1] - P(15,1)*SH_MAG[2] + P(15,3)*SH_MAG[0] + P(15,2)*SK_MZ[2] + P(15,18)*SK_MZ[1] + P(15,16)*SK_MZ[4] - P(15,17)*SK_MZ[3]);
|
|
Kfusion[22] = SK_MZ[0]*(P(22,21) + P(22,0)*SH_MAG[1] - P(22,1)*SH_MAG[2] + P(22,3)*SH_MAG[0] + P(22,2)*SK_MZ[2] + P(22,18)*SK_MZ[1] + P(22,16)*SK_MZ[4] - P(22,17)*SK_MZ[3]);
|
|
Kfusion[23] = SK_MZ[0]*(P(23,21) + P(23,0)*SH_MAG[1] - P(23,1)*SH_MAG[2] + P(23,3)*SH_MAG[0] + P(23,2)*SK_MZ[2] + P(23,18)*SK_MZ[1] + P(23,16)*SK_MZ[4] - P(23,17)*SK_MZ[3]);
|
|
} else {
|
|
for (uint8_t i = 0; i < 16; i++) {
|
|
Kfusion[i] = 0.0f;
|
|
}
|
|
|
|
Kfusion[22] = 0.0f;
|
|
Kfusion[23] = 0.0f;
|
|
}
|
|
|
|
Kfusion[16] = SK_MZ[0]*(P(16,21) + P(16,0)*SH_MAG[1] - P(16,1)*SH_MAG[2] + P(16,3)*SH_MAG[0] + P(16,2)*SK_MZ[2] + P(16,18)*SK_MZ[1] + P(16,16)*SK_MZ[4] - P(16,17)*SK_MZ[3]);
|
|
Kfusion[17] = SK_MZ[0]*(P(17,21) + P(17,0)*SH_MAG[1] - P(17,1)*SH_MAG[2] + P(17,3)*SH_MAG[0] + P(17,2)*SK_MZ[2] + P(17,18)*SK_MZ[1] + P(17,16)*SK_MZ[4] - P(17,17)*SK_MZ[3]);
|
|
Kfusion[18] = SK_MZ[0]*(P(18,21) + P(18,0)*SH_MAG[1] - P(18,1)*SH_MAG[2] + P(18,3)*SH_MAG[0] + P(18,2)*SK_MZ[2] + P(18,18)*SK_MZ[1] + P(18,16)*SK_MZ[4] - P(18,17)*SK_MZ[3]);
|
|
Kfusion[19] = SK_MZ[0]*(P(19,21) + P(19,0)*SH_MAG[1] - P(19,1)*SH_MAG[2] + P(19,3)*SH_MAG[0] + P(19,2)*SK_MZ[2] + P(19,18)*SK_MZ[1] + P(19,16)*SK_MZ[4] - P(19,17)*SK_MZ[3]);
|
|
Kfusion[20] = SK_MZ[0]*(P(20,21) + P(20,0)*SH_MAG[1] - P(20,1)*SH_MAG[2] + P(20,3)*SH_MAG[0] + P(20,2)*SK_MZ[2] + P(20,18)*SK_MZ[1] + P(20,16)*SK_MZ[4] - P(20,17)*SK_MZ[3]);
|
|
Kfusion[21] = SK_MZ[0]*(P(21,21) + P(21,0)*SH_MAG[1] - P(21,1)*SH_MAG[2] + P(21,3)*SH_MAG[0] + P(21,2)*SK_MZ[2] + P(21,18)*SK_MZ[1] + P(21,16)*SK_MZ[4] - P(21,17)*SK_MZ[3]);
|
|
|
|
} else {
|
|
return;
|
|
}
|
|
|
|
// apply covariance correction via P_new = (I -K*H)*P
|
|
// first calculate expression for KHP
|
|
// then calculate P - KHP
|
|
matrix::SquareMatrix<float, _k_num_states> KHP {};
|
|
float KH[10];
|
|
|
|
for (unsigned row = 0; row < _k_num_states; row++) {
|
|
|
|
KH[0] = Kfusion[row] * H_MAG[0];
|
|
KH[1] = Kfusion[row] * H_MAG[1];
|
|
KH[2] = Kfusion[row] * H_MAG[2];
|
|
KH[3] = Kfusion[row] * H_MAG[3];
|
|
KH[4] = Kfusion[row] * H_MAG[16];
|
|
KH[5] = Kfusion[row] * H_MAG[17];
|
|
KH[6] = Kfusion[row] * H_MAG[18];
|
|
KH[7] = Kfusion[row] * H_MAG[19];
|
|
KH[8] = Kfusion[row] * H_MAG[20];
|
|
KH[9] = Kfusion[row] * H_MAG[21];
|
|
|
|
for (unsigned column = 0; column < _k_num_states; column++) {
|
|
float tmp = KH[0] * P(0,column);
|
|
tmp += KH[1] * P(1,column);
|
|
tmp += KH[2] * P(2,column);
|
|
tmp += KH[3] * P(3,column);
|
|
tmp += KH[4] * P(16,column);
|
|
tmp += KH[5] * P(17,column);
|
|
tmp += KH[6] * P(18,column);
|
|
tmp += KH[7] * P(19,column);
|
|
tmp += KH[8] * P(20,column);
|
|
tmp += KH[9] * P(21,column);
|
|
KHP(row,column) = tmp;
|
|
}
|
|
}
|
|
|
|
// if the covariance correction will result in a negative variance, then
|
|
// the covariance matrix is unhealthy and must be corrected
|
|
_fault_status.flags.bad_mag_x = false;
|
|
_fault_status.flags.bad_mag_y = false;
|
|
_fault_status.flags.bad_mag_z = false;
|
|
|
|
for (int i = 0; i < _k_num_states; i++) {
|
|
if (P(i,i) < KHP(i,i)) {
|
|
// zero rows and columns
|
|
P.uncorrelateCovarianceSetVariance<1>(i, 0.0f);
|
|
|
|
//flag as unhealthy
|
|
healthy = false;
|
|
|
|
// update individual measurement health status
|
|
if (index == 0) {
|
|
_fault_status.flags.bad_mag_x = true;
|
|
|
|
} else if (index == 1) {
|
|
_fault_status.flags.bad_mag_y = true;
|
|
|
|
} else if (index == 2) {
|
|
_fault_status.flags.bad_mag_z = true;
|
|
}
|
|
}
|
|
}
|
|
|
|
// only apply covariance and state corrections if healthy
|
|
if (healthy) {
|
|
// apply the covariance corrections
|
|
for (unsigned row = 0; row < _k_num_states; row++) {
|
|
for (unsigned column = 0; column < _k_num_states; column++) {
|
|
P(row,column) = P(row,column) - KHP(row,column);
|
|
}
|
|
}
|
|
|
|
// correct the covariance matrix for gross errors
|
|
fixCovarianceErrors(true);
|
|
|
|
// apply the state corrections
|
|
fuse(Kfusion, _mag_innov[index]);
|
|
|
|
// constrain the declination of the earth field states
|
|
limitDeclination();
|
|
}
|
|
}
|
|
}
|
|
|
|
void Ekf::fuseHeading()
|
|
{
|
|
// assign intermediate state variables
|
|
const float q0 = _state.quat_nominal(0);
|
|
const float q1 = _state.quat_nominal(1);
|
|
const float q2 = _state.quat_nominal(2);
|
|
const float q3 = _state.quat_nominal(3);
|
|
|
|
float R_YAW = 1.0f;
|
|
float predicted_hdg;
|
|
float H_YAW[4];
|
|
Vector3f mag_earth_pred;
|
|
float measured_hdg;
|
|
|
|
// determine if a 321 or 312 Euler sequence is best
|
|
if (fabsf(_R_to_earth(2, 0)) < fabsf(_R_to_earth(2, 1))) {
|
|
// calculate observation jacobian when we are observing the first rotation in a 321 sequence
|
|
float t9 = q0*q3;
|
|
float t10 = q1*q2;
|
|
float t2 = t9+t10;
|
|
float t3 = q0*q0;
|
|
float t4 = q1*q1;
|
|
float t5 = q2*q2;
|
|
float t6 = q3*q3;
|
|
float t7 = t3+t4-t5-t6;
|
|
|
|
float t16 = q3*t3;
|
|
float t17 = q3*t5;
|
|
float t18 = q0*q1*q2*2.0f;
|
|
float t19 = t16+t17+t18-q3*t4+q3*t6;
|
|
|
|
float t24 = q2*t4;
|
|
float t25 = q2*t6;
|
|
float t26 = q0*q1*q3*2.0f;
|
|
float t27 = t24+t25+t26-q2*t3+q2*t5;
|
|
float t28 = q1*t3;
|
|
float t29 = q1*t5;
|
|
float t30 = q0*q2*q3*2.0f;
|
|
float t31 = t28+t29+t30+q1*t4-q1*t6;
|
|
float t32 = q0*t4;
|
|
float t33 = q0*t6;
|
|
float t34 = q1*q2*q3*2.0f;
|
|
float t35 = t32+t33+t34+q0*t3-q0*t5;
|
|
|
|
// two computational paths are provided to work around singularities in calculation of the Jacobians
|
|
float t8 = t7*t7;
|
|
float t15 = t2*t2;
|
|
if (t8 > t15 && t8 > 1E-6f) {
|
|
// this path has a singularities at yaw = +-90 degrees
|
|
t8 = 1.0f/t8;
|
|
float t11 = t2*t2;
|
|
float t12 = t8*t11*4.0f;
|
|
float t13 = t12+1.0f;
|
|
float t14 = 1.0f/t13;
|
|
|
|
H_YAW[0] = t8*t14*t19*(-2.0f);
|
|
H_YAW[1] = t8*t14*t27*(-2.0f);
|
|
H_YAW[2] = t8*t14*t31*2.0f;
|
|
H_YAW[3] = t8*t14*t35*2.0f;
|
|
|
|
} else if (t15 > 1E-6f) {
|
|
// this path has singularities at yaw = 0 and +-180 deg
|
|
t15 = 1.0f/t15;
|
|
float t20 = t7*t7;
|
|
float t21 = t15*t20*0.25f;
|
|
float t22 = t21+1.0f;
|
|
|
|
if (fabsf(t22) > 1E-6f) {
|
|
float t23 = 1.0f/t22;
|
|
|
|
H_YAW[0] = t15*t19*t23*(-0.5f);
|
|
H_YAW[1] = t15*t23*t27*(-0.5f);
|
|
H_YAW[2] = t15*t23*t31*0.5f;
|
|
H_YAW[3] = t15*t23*t35*0.5f;
|
|
|
|
} else {
|
|
return;
|
|
|
|
}
|
|
} else {
|
|
return;
|
|
|
|
}
|
|
|
|
// rotate the magnetometer measurement into earth frame
|
|
Eulerf euler321(_state.quat_nominal);
|
|
predicted_hdg = euler321(2); // we will need the predicted heading to calculate the innovation
|
|
|
|
// calculate the observed yaw angle
|
|
if (_control_status.flags.mag_hdg) {
|
|
// Set the yaw angle to zero and rotate the measurements into earth frame using the zero yaw angle
|
|
euler321(2) = 0.0f;
|
|
const Dcmf R_to_earth(euler321);
|
|
|
|
// rotate the magnetometer measurements into earth frame using a zero yaw angle
|
|
if (_control_status.flags.mag_3D) {
|
|
// don't apply bias corrections if we are learning them
|
|
mag_earth_pred = R_to_earth * _mag_sample_delayed.mag;
|
|
|
|
} else {
|
|
mag_earth_pred = R_to_earth * (_mag_sample_delayed.mag - _state.mag_B);
|
|
}
|
|
|
|
// the angle of the projection onto the horizontal gives the yaw angle
|
|
measured_hdg = -atan2f(mag_earth_pred(1), mag_earth_pred(0)) + getMagDeclination();
|
|
|
|
} else if (_control_status.flags.ev_yaw) {
|
|
// calculate the yaw angle for a 321 sequence
|
|
// Expressions obtained from yaw_input_321.c produced by https://github.com/PX4/ecl/blob/master/matlab/scripts/Inertial%20Nav%20EKF/quat2yaw321.m
|
|
const float Tbn_1_0 = 2.0f*(_ev_sample_delayed.quat(0)*_ev_sample_delayed.quat(3)+_ev_sample_delayed.quat(1)*_ev_sample_delayed.quat(2));
|
|
const float Tbn_0_0 = sq(_ev_sample_delayed.quat(0))+sq(_ev_sample_delayed.quat(1))-sq(_ev_sample_delayed.quat(2))-sq(_ev_sample_delayed.quat(3));
|
|
measured_hdg = atan2f(Tbn_1_0,Tbn_0_0);
|
|
|
|
} else if (_mag_use_inhibit) {
|
|
// Special case where we either use the current or last known stationary value
|
|
// so set to current value as a safe default
|
|
measured_hdg = predicted_hdg;
|
|
|
|
} else {
|
|
// Should not be doing yaw fusion
|
|
return;
|
|
|
|
}
|
|
|
|
} else {
|
|
// calculate observation jacobian when we are observing a rotation in a 312 sequence
|
|
float t9 = q0*q3;
|
|
float t10 = q1*q2;
|
|
float t2 = t9-t10;
|
|
float t3 = q0*q0;
|
|
float t4 = q1*q1;
|
|
float t5 = q2*q2;
|
|
float t6 = q3*q3;
|
|
float t7 = t3-t4+t5-t6;
|
|
|
|
float t16 = q3*t3;
|
|
float t17 = q3*t4;
|
|
float t18 = t16+t17-q3*t5+q3*t6-q0*q1*q2*2.0f;
|
|
float t23 = q2*t3;
|
|
float t24 = q2*t4;
|
|
float t25 = t23+t24+q2*t5-q2*t6-q0*q1*q3*2.0f;
|
|
float t26 = q1*t5;
|
|
float t27 = q1*t6;
|
|
float t28 = t26+t27-q1*t3+q1*t4-q0*q2*q3*2.0f;
|
|
float t29 = q0*t5;
|
|
float t30 = q0*t6;
|
|
float t31 = t29+t30+q0*t3-q0*t4-q1*q2*q3*2.0f;
|
|
|
|
// two computational paths are provided to work around singularities in calculation of the Jacobians
|
|
float t8 = t7*t7;
|
|
float t15 = t2*t2;
|
|
if (t8 > t15 && t8 > 1E-6f) {
|
|
// this path has a singularities at yaw = +-90 degrees
|
|
t8 = 1.0f/t8;
|
|
float t11 = t2*t2;
|
|
float t12 = t8*t11*4.0f;
|
|
float t13 = t12+1.0f;
|
|
float t14 = 1.0f/t13;
|
|
|
|
H_YAW[0] = t8*t14*t18*(-2.0f);
|
|
H_YAW[1] = t8*t14*t25*(-2.0f);
|
|
H_YAW[2] = t8*t14*t28*2.0f;
|
|
H_YAW[3] = t8*t14*t31*2.0f;
|
|
|
|
} else if (t15 > 1E-6f) {
|
|
// this path has singularities at yaw = 0 and +-180 deg
|
|
t15 = 1.0f/t15;
|
|
float t19 = t7*t7;
|
|
float t20 = t15*t19*0.25f;
|
|
float t21 = t20+1.0f;
|
|
|
|
if (fabsf(t21) > 1E-6f) {
|
|
float t22 = 1.0f/t21;
|
|
|
|
H_YAW[0] = t15*t18*t22*(-0.5f);
|
|
H_YAW[1] = t15*t22*t25*(-0.5f);
|
|
H_YAW[2] = t15*t22*t28*0.5f;
|
|
H_YAW[3] = t15*t22*t31*0.5f;
|
|
|
|
} else {
|
|
return;
|
|
|
|
}
|
|
|
|
} else {
|
|
return;
|
|
|
|
}
|
|
|
|
|
|
|
|
/* Calculate the 312 sequence euler angles that rotate from earth to body frame
|
|
* Derived from https://github.com/PX4/ecl/blob/master/matlab/scripts/Inertial%20Nav%20EKF/quat2yaw312.m
|
|
* Body to nav frame transformation using a yaw-roll-pitch rotation sequence is given by:
|
|
*
|
|
[ cos(pitch)*cos(yaw) - sin(pitch)*sin(roll)*sin(yaw), -cos(roll)*sin(yaw), cos(yaw)*sin(pitch) + cos(pitch)*sin(roll)*sin(yaw)]
|
|
[ cos(pitch)*sin(yaw) + cos(yaw)*sin(pitch)*sin(roll), cos(roll)*cos(yaw), sin(pitch)*sin(yaw) - cos(pitch)*cos(yaw)*sin(roll)]
|
|
[ -cos(roll)*sin(pitch), sin(roll), cos(pitch)*cos(roll)]
|
|
*/
|
|
float yaw = atan2f(-_R_to_earth(0, 1), _R_to_earth(1, 1)); // first rotation (yaw)
|
|
const float roll = asinf(_R_to_earth(2, 1)); // second rotation (roll)
|
|
const float pitch = atan2f(-_R_to_earth(2, 0), _R_to_earth(2, 2)); // third rotation (pitch)
|
|
|
|
predicted_hdg = yaw; // we will need the predicted heading to calculate the innovation
|
|
|
|
// calculate the observed yaw angle
|
|
if (_control_status.flags.mag_hdg) {
|
|
// Set the first rotation (yaw) to zero and rotate the measurements into earth frame
|
|
yaw = 0.0f;
|
|
|
|
// Calculate the body to earth frame rotation matrix from the euler angles using a 312 rotation sequence
|
|
// Equations from Tbn_312.c produced by https://github.com/PX4/ecl/blob/master/matlab/scripts/Inertial%20Nav%20EKF/quat2yaw312.m
|
|
Dcmf R_to_earth;
|
|
float sy = sinf(yaw);
|
|
float cy = cosf(yaw);
|
|
float sp = sinf(pitch);
|
|
float cp = cosf(pitch);
|
|
float sr = sinf(roll);
|
|
float cr = cosf(roll);
|
|
R_to_earth(0,0) = cy*cp-sy*sp*sr;
|
|
R_to_earth(0,1) = -sy*cr;
|
|
R_to_earth(0,2) = cy*sp+sy*cp*sr;
|
|
R_to_earth(1,0) = sy*cp+cy*sp*sr;
|
|
R_to_earth(1,1) = cy*cr;
|
|
R_to_earth(1,2) = sy*sp-cy*cp*sr;
|
|
R_to_earth(2,0) = -sp*cr;
|
|
R_to_earth(2,1) = sr;
|
|
R_to_earth(2,2) = cp*cr;
|
|
|
|
// rotate the magnetometer measurements into earth frame using a zero yaw angle
|
|
if (_control_status.flags.mag_3D) {
|
|
// don't apply bias corrections if we are learning them
|
|
mag_earth_pred = R_to_earth * _mag_sample_delayed.mag;
|
|
} else {
|
|
mag_earth_pred = R_to_earth * (_mag_sample_delayed.mag - _state.mag_B);
|
|
}
|
|
|
|
// the angle of the projection onto the horizontal gives the yaw angle
|
|
measured_hdg = -atan2f(mag_earth_pred(1), mag_earth_pred(0)) + getMagDeclination();
|
|
|
|
} else if (_control_status.flags.ev_yaw) {
|
|
// calculate the yaw angle for a 312 sequence
|
|
// Values from yaw_input_312.c file produced by https://github.com/PX4/ecl/blob/master/matlab/scripts/Inertial%20Nav%20EKF/quat2yaw312.m
|
|
float Tbn_0_1_neg = 2.0f*(_ev_sample_delayed.quat(0)*_ev_sample_delayed.quat(3)-_ev_sample_delayed.quat(1)*_ev_sample_delayed.quat(2));
|
|
float Tbn_1_1 = sq(_ev_sample_delayed.quat(0))-sq(_ev_sample_delayed.quat(1))+sq(_ev_sample_delayed.quat(2))-sq(_ev_sample_delayed.quat(3));
|
|
measured_hdg = atan2f(Tbn_0_1_neg,Tbn_1_1);
|
|
|
|
} else if (_mag_use_inhibit) {
|
|
// Special case where we either use the current or last known stationary value
|
|
// so set to current value as a safe default
|
|
measured_hdg = predicted_hdg;
|
|
|
|
} else {
|
|
// Should not be doing yaw fusion
|
|
return;
|
|
|
|
}
|
|
}
|
|
|
|
// Calculate the observation variance
|
|
if (_control_status.flags.mag_hdg) {
|
|
// using magnetic heading tuning parameter
|
|
R_YAW = sq(fmaxf(_params.mag_heading_noise, 1.0e-2f));
|
|
|
|
} else if (_control_status.flags.ev_yaw) {
|
|
// using error estimate from external vision data
|
|
R_YAW = fmaxf(_ev_sample_delayed.angVar, sq(1.0e-2f));
|
|
|
|
} else {
|
|
// default value
|
|
R_YAW = 0.01f;
|
|
}
|
|
|
|
// wrap the heading to the interval between +-pi
|
|
measured_hdg = wrap_pi(measured_hdg);
|
|
|
|
// calculate the innovation and define the innovation gate
|
|
float innov_gate = math::max(_params.heading_innov_gate, 1.0f);
|
|
if (_mag_use_inhibit) {
|
|
// The magnetometer cannot be trusted but we need to fuse a heading to prevent a badly
|
|
// conditioned covariance matrix developing over time.
|
|
if (!_control_status.flags.vehicle_at_rest) {
|
|
// Vehicle is not at rest so fuse a zero innovation and record the
|
|
// predicted heading to use as an observation when movement ceases.
|
|
_heading_innov = 0.0f;
|
|
_last_static_yaw = predicted_hdg;
|
|
|
|
} else {
|
|
// Vehicle is at rest so use the last moving prediction as an observation
|
|
// to prevent the heading from drifting and to enable yaw gyro bias learning
|
|
// before takeoff.
|
|
_heading_innov = predicted_hdg - _last_static_yaw;
|
|
innov_gate = 5.0f;
|
|
|
|
}
|
|
} else {
|
|
_heading_innov = predicted_hdg - measured_hdg;
|
|
_last_static_yaw = predicted_hdg;
|
|
|
|
}
|
|
_mag_use_inhibit_prev = _mag_use_inhibit;
|
|
|
|
// wrap the innovation to the interval between +-pi
|
|
_heading_innov = wrap_pi(_heading_innov);
|
|
|
|
// Calculate innovation variance and Kalman gains, taking advantage of the fact that only the first 4 elements in H are non zero
|
|
// calculate the innovation variance
|
|
float PH[4];
|
|
_heading_innov_var = R_YAW;
|
|
|
|
for (unsigned row = 0; row <= 3; row++) {
|
|
PH[row] = 0.0f;
|
|
|
|
for (uint8_t col = 0; col <= 3; col++) {
|
|
PH[row] += P(row,col) * H_YAW[col];
|
|
}
|
|
|
|
_heading_innov_var += H_YAW[row] * PH[row];
|
|
}
|
|
|
|
float heading_innov_var_inv;
|
|
|
|
// check if the innovation variance calculation is badly conditioned
|
|
if (_heading_innov_var >= R_YAW) {
|
|
// the innovation variance contribution from the state covariances is not negative, no fault
|
|
_fault_status.flags.bad_hdg = false;
|
|
heading_innov_var_inv = 1.0f / _heading_innov_var;
|
|
|
|
} else {
|
|
// the innovation variance contribution from the state covariances is negative which means the covariance matrix is badly conditioned
|
|
_fault_status.flags.bad_hdg = true;
|
|
|
|
// we reinitialise the covariance matrix and abort this fusion step
|
|
initialiseCovariance();
|
|
ECL_ERR_TIMESTAMPED("mag yaw fusion numerical error - covariance reset");
|
|
return;
|
|
}
|
|
|
|
// calculate the Kalman gains
|
|
// only calculate gains for states we are using
|
|
float Kfusion[_k_num_states] = {};
|
|
|
|
for (uint8_t row = 0; row <= 15; row++) {
|
|
Kfusion[row] = 0.0f;
|
|
|
|
for (uint8_t col = 0; col <= 3; col++) {
|
|
Kfusion[row] += P(row,col) * H_YAW[col];
|
|
}
|
|
|
|
Kfusion[row] *= heading_innov_var_inv;
|
|
}
|
|
|
|
if (_control_status.flags.wind) {
|
|
for (uint8_t row = 22; row <= 23; row++) {
|
|
Kfusion[row] = 0.0f;
|
|
|
|
for (uint8_t col = 0; col <= 3; col++) {
|
|
Kfusion[row] += P(row,col) * H_YAW[col];
|
|
}
|
|
|
|
Kfusion[row] *= heading_innov_var_inv;
|
|
}
|
|
}
|
|
|
|
// innovation test ratio
|
|
_yaw_test_ratio = sq(_heading_innov) / (sq(innov_gate) * _heading_innov_var);
|
|
|
|
// we are no longer using 3-axis fusion so set the reported test levels to zero
|
|
memset(_mag_test_ratio, 0, sizeof(_mag_test_ratio));
|
|
|
|
// set the magnetometer unhealthy if the test fails
|
|
if (_yaw_test_ratio > 1.0f) {
|
|
_innov_check_fail_status.flags.reject_yaw = true;
|
|
|
|
// if we are in air we don't want to fuse the measurement
|
|
// we allow to use it when on the ground because the large innovation could be caused
|
|
// by interference or a large initial gyro bias
|
|
if (_control_status.flags.in_air) {
|
|
return;
|
|
|
|
} else {
|
|
// constrain the innovation to the maximum set by the gate
|
|
float gate_limit = sqrtf((sq(innov_gate) * _heading_innov_var));
|
|
_heading_innov = math::constrain(_heading_innov, -gate_limit, gate_limit);
|
|
}
|
|
|
|
} else {
|
|
_innov_check_fail_status.flags.reject_yaw = false;
|
|
}
|
|
|
|
// apply covariance correction via P_new = (I -K*H)*P
|
|
// first calculate expression for KHP
|
|
// then calculate P - KHP
|
|
matrix::SquareMatrix<float, _k_num_states> KHP;
|
|
float KH[4];
|
|
|
|
for (unsigned row = 0; row < _k_num_states; row++) {
|
|
|
|
KH[0] = Kfusion[row] * H_YAW[0];
|
|
KH[1] = Kfusion[row] * H_YAW[1];
|
|
KH[2] = Kfusion[row] * H_YAW[2];
|
|
KH[3] = Kfusion[row] * H_YAW[3];
|
|
|
|
for (unsigned column = 0; column < _k_num_states; column++) {
|
|
float tmp = KH[0] * P(0,column);
|
|
tmp += KH[1] * P(1,column);
|
|
tmp += KH[2] * P(2,column);
|
|
tmp += KH[3] * P(3,column);
|
|
KHP(row,column) = tmp;
|
|
}
|
|
}
|
|
|
|
// if the covariance correction will result in a negative variance, then
|
|
// the covariance matrix is unhealthy and must be corrected
|
|
bool healthy = true;
|
|
_fault_status.flags.bad_hdg = false;
|
|
|
|
for (int i = 0; i < _k_num_states; i++) {
|
|
if (P(i,i) < KHP(i,i)) {
|
|
// zero rows and columns
|
|
P.uncorrelateCovarianceSetVariance<1>(i, 0.0f);
|
|
|
|
//flag as unhealthy
|
|
healthy = false;
|
|
|
|
// update individual measurement health status
|
|
_fault_status.flags.bad_hdg = true;
|
|
|
|
}
|
|
}
|
|
|
|
// only apply covariance and state corrections if healthy
|
|
if (healthy) {
|
|
// apply the covariance corrections
|
|
for (unsigned row = 0; row < _k_num_states; row++) {
|
|
for (unsigned column = 0; column < _k_num_states; column++) {
|
|
P(row,column) = P(row,column) - KHP(row,column);
|
|
}
|
|
}
|
|
|
|
// correct the covariance matrix for gross errors
|
|
fixCovarianceErrors(true);
|
|
|
|
// apply the state corrections
|
|
fuse(Kfusion, _heading_innov);
|
|
|
|
}
|
|
}
|
|
|
|
void Ekf::fuseDeclination(float decl_sigma)
|
|
{
|
|
// assign intermediate state variables
|
|
const float magN = _state.mag_I(0);
|
|
const float magE = _state.mag_I(1);
|
|
|
|
// minimum horizontal field strength before calculation becomes badly conditioned (T)
|
|
const float h_field_min = 0.001f;
|
|
|
|
// observation variance (rad**2)
|
|
const float R_DECL = sq(decl_sigma);
|
|
|
|
// Calculate intermediate variables
|
|
float t2 = magE*magE;
|
|
float t3 = magN*magN;
|
|
float t4 = t2+t3;
|
|
// if the horizontal magnetic field is too small, this calculation will be badly conditioned
|
|
if (t4 < h_field_min*h_field_min) {
|
|
return;
|
|
}
|
|
float t5 = P(16,16)*t2;
|
|
float t6 = P(17,17)*t3;
|
|
float t7 = t2*t2;
|
|
float t8 = R_DECL*t7;
|
|
float t9 = t3*t3;
|
|
float t10 = R_DECL*t9;
|
|
float t11 = R_DECL*t2*t3*2.0f;
|
|
float t14 = P(16,17)*magE*magN;
|
|
float t15 = P(17,16)*magE*magN;
|
|
float t12 = t5+t6+t8+t10+t11-t14-t15;
|
|
float t13;
|
|
if (fabsf(t12) > 1e-6f) {
|
|
t13 = 1.0f / t12;
|
|
} else {
|
|
return;
|
|
}
|
|
float t18 = magE*magE;
|
|
float t19 = magN*magN;
|
|
float t20 = t18+t19;
|
|
float t21;
|
|
if (fabsf(t20) > 1e-6f) {
|
|
t21 = 1.0f/t20;
|
|
} else {
|
|
return;
|
|
}
|
|
|
|
// Calculate the observation Jacobian
|
|
// Note only 2 terms are non-zero which can be used in matrix operations for calculation of Kalman gains and covariance update to significantly reduce cost
|
|
float H_DECL[24] = {};
|
|
H_DECL[16] = -magE*t21;
|
|
H_DECL[17] = magN*t21;
|
|
|
|
// Calculate the Kalman gains
|
|
float Kfusion[_k_num_states] = {};
|
|
Kfusion[0] = -t4*t13*(P(0,16)*magE-P(0,17)*magN);
|
|
Kfusion[1] = -t4*t13*(P(1,16)*magE-P(1,17)*magN);
|
|
Kfusion[2] = -t4*t13*(P(2,16)*magE-P(2,17)*magN);
|
|
Kfusion[3] = -t4*t13*(P(3,16)*magE-P(3,17)*magN);
|
|
Kfusion[4] = -t4*t13*(P(4,16)*magE-P(4,17)*magN);
|
|
Kfusion[5] = -t4*t13*(P(5,16)*magE-P(5,17)*magN);
|
|
Kfusion[6] = -t4*t13*(P(6,16)*magE-P(6,17)*magN);
|
|
Kfusion[7] = -t4*t13*(P(7,16)*magE-P(7,17)*magN);
|
|
Kfusion[8] = -t4*t13*(P(8,16)*magE-P(8,17)*magN);
|
|
Kfusion[9] = -t4*t13*(P(9,16)*magE-P(9,17)*magN);
|
|
Kfusion[10] = -t4*t13*(P(10,16)*magE-P(10,17)*magN);
|
|
Kfusion[11] = -t4*t13*(P(11,16)*magE-P(11,17)*magN);
|
|
Kfusion[12] = -t4*t13*(P(12,16)*magE-P(12,17)*magN);
|
|
Kfusion[13] = -t4*t13*(P(13,16)*magE-P(13,17)*magN);
|
|
Kfusion[14] = -t4*t13*(P(14,16)*magE-P(14,17)*magN);
|
|
Kfusion[15] = -t4*t13*(P(15,16)*magE-P(15,17)*magN);
|
|
Kfusion[16] = -t4*t13*(P(16,16)*magE-P(16,17)*magN);
|
|
Kfusion[17] = -t4*t13*(P(17,16)*magE-P(17,17)*magN);
|
|
Kfusion[18] = -t4*t13*(P(18,16)*magE-P(18,17)*magN);
|
|
Kfusion[19] = -t4*t13*(P(19,16)*magE-P(19,17)*magN);
|
|
Kfusion[20] = -t4*t13*(P(20,16)*magE-P(20,17)*magN);
|
|
Kfusion[21] = -t4*t13*(P(21,16)*magE-P(21,17)*magN);
|
|
Kfusion[22] = -t4*t13*(P(22,16)*magE-P(22,17)*magN);
|
|
Kfusion[23] = -t4*t13*(P(23,16)*magE-P(23,17)*magN);
|
|
|
|
const float innovation = math::constrain(atan2f(magE, magN) - getMagDeclination(), -0.5f, 0.5f);
|
|
|
|
// apply covariance correction via P_new = (I -K*H)*P
|
|
// first calculate expression for KHP
|
|
// then calculate P - KHP
|
|
// take advantage of the empty columns in KH to reduce the number of operations
|
|
matrix::SquareMatrix<float, _k_num_states> KHP;
|
|
float KH[2];
|
|
for (unsigned row = 0; row < _k_num_states; row++) {
|
|
|
|
KH[0] = Kfusion[row] * H_DECL[16];
|
|
KH[1] = Kfusion[row] * H_DECL[17];
|
|
|
|
for (unsigned column = 0; column < _k_num_states; column++) {
|
|
float tmp = KH[0] * P(16,column);
|
|
tmp += KH[1] * P(17,column);
|
|
KHP(row,column) = tmp;
|
|
}
|
|
}
|
|
|
|
// if the covariance correction will result in a negative variance, then
|
|
// the covariance matrix is unhealthy and must be corrected
|
|
bool healthy = true;
|
|
_fault_status.flags.bad_mag_decl = false;
|
|
for (int i = 0; i < _k_num_states; i++) {
|
|
if (P(i,i) < KHP(i,i)) {
|
|
// zero rows and columns
|
|
P.uncorrelateCovarianceSetVariance<1>(i, 0.0f);
|
|
|
|
//flag as unhealthy
|
|
healthy = false;
|
|
|
|
// update individual measurement health status
|
|
_fault_status.flags.bad_mag_decl = true;
|
|
|
|
}
|
|
}
|
|
|
|
// only apply covariance and state corrections if healthy
|
|
if (healthy) {
|
|
// apply the covariance corrections
|
|
for (unsigned row = 0; row < _k_num_states; row++) {
|
|
for (unsigned column = 0; column < _k_num_states; column++) {
|
|
P(row,column) = P(row,column) - KHP(row,column);
|
|
}
|
|
}
|
|
|
|
// correct the covariance matrix for gross errors
|
|
fixCovarianceErrors(true);
|
|
|
|
// apply the state corrections
|
|
fuse(Kfusion, innovation);
|
|
|
|
// constrain the declination of the earth field states
|
|
limitDeclination();
|
|
}
|
|
}
|
|
|
|
void Ekf::limitDeclination()
|
|
{
|
|
// get a reference value for the earth field declinaton and minimum plausible horizontal field strength
|
|
// set to 50% of the horizontal strength from geo tables if location is known
|
|
float decl_reference;
|
|
float h_field_min = 0.001f;
|
|
if (_params.mag_declination_source & MASK_USE_GEO_DECL) {
|
|
// use parameter value until GPS is available, then use value returned by geo library
|
|
if (_NED_origin_initialised) {
|
|
decl_reference = _mag_declination_gps;
|
|
h_field_min = fmaxf(h_field_min , 0.5f * _mag_strength_gps * cosf(_mag_inclination_gps));
|
|
} else {
|
|
decl_reference = math::radians(_params.mag_declination_deg);
|
|
}
|
|
} else {
|
|
// always use the parameter value
|
|
decl_reference = math::radians(_params.mag_declination_deg);
|
|
}
|
|
|
|
// do not allow the horizontal field length to collapse - this will make the declination fusion badly conditioned
|
|
// and can result in a reversal of the NE field states which the filter cannot recover from
|
|
// apply a circular limit
|
|
float h_field = sqrtf(_state.mag_I(0)*_state.mag_I(0) + _state.mag_I(1)*_state.mag_I(1));
|
|
if (h_field < h_field_min) {
|
|
if (h_field > 0.001f * h_field_min) {
|
|
float h_scaler = h_field_min / h_field;
|
|
_state.mag_I(0) *= h_scaler;
|
|
_state.mag_I(1) *= h_scaler;
|
|
} else {
|
|
// too small to scale radially so set to expected value
|
|
float mag_declination = getMagDeclination();
|
|
_state.mag_I(0) = 2.0f * h_field_min * cosf(mag_declination);
|
|
_state.mag_I(1) = 2.0f * h_field_min * sinf(mag_declination);
|
|
}
|
|
h_field = h_field_min;
|
|
}
|
|
|
|
// do not allow the declination estimate to vary too much relative to the reference value
|
|
const float decl_tolerance = 0.5f;
|
|
const float decl_max = decl_reference + decl_tolerance;
|
|
const float decl_min = decl_reference - decl_tolerance;
|
|
const float decl_estimate = atan2f(_state.mag_I(1) , _state.mag_I(0));
|
|
if (decl_estimate > decl_max) {
|
|
_state.mag_I(0) = h_field * cosf(decl_max);
|
|
_state.mag_I(1) = h_field * sinf(decl_max);
|
|
} else if (decl_estimate < decl_min) {
|
|
_state.mag_I(0) = h_field * cosf(decl_min);
|
|
_state.mag_I(1) = h_field * sinf(decl_min);
|
|
}
|
|
}
|
|
|
|
float Ekf::calculate_synthetic_mag_z_measurement(const Vector3f& mag_meas, const Vector3f& mag_earth_predicted)
|
|
{
|
|
// theoretical magnitude of the magnetometer Z component value given X and Y sensor measurement and our knowledge
|
|
// of the earth magnetic field vector at the current location
|
|
const float mag_z_abs = sqrtf(math::max(sq(mag_earth_predicted.length()) - sq(mag_meas(0)) - sq(mag_meas(1)), 0.0f));
|
|
|
|
// calculate sign of synthetic magnetomter Z component based on the sign of the predicted magnetomer Z component
|
|
const float mag_z_body_pred = mag_earth_predicted.dot(_R_to_earth.slice<3,1>(0,2));
|
|
|
|
return mag_z_body_pred < 0 ? -mag_z_abs : mag_z_abs;
|
|
}
|