mirror of https://github.com/ArduPilot/ardupilot
527 lines
16 KiB
C++
527 lines
16 KiB
C++
/*
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APM_AHRS_DCM.cpp
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AHRS system using DCM matrices
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Based on DCM code by Doug Weibel, Jordi Muñoz and Jose Julio. DIYDrones.com
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Adapted for the general ArduPilot AHRS interface by Andrew Tridgell
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This library is free software; you can redistribute it and/or
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modify it under the terms of the GNU Lesser General Public License
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as published by the Free Software Foundation; either version 2.1
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of the License, or (at your option) any later version.
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*/
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#include <FastSerial.h>
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#include <AP_AHRS.h>
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// this is the speed in cm/s above which we first get a yaw lock with
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// the GPS
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#define GPS_SPEED_MIN 300
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// this is the speed in cm/s at which we stop using drift correction
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// from the GPS and wait for the ground speed to get above GPS_SPEED_MIN
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#define GPS_SPEED_RESET 100
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// table of user settable parameters
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const AP_Param::GroupInfo AP_AHRS::var_info[] PROGMEM = {
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AP_GROUPINFO("YAW_P", 0, AP_AHRS_DCM, _kp_yaw),
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AP_GROUPEND
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};
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// run a full DCM update round
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void
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AP_AHRS_DCM::update(void)
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{
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float delta_t;
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// tell the IMU to grab some data
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_imu->update();
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// ask the IMU how much time this sensor reading represents
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delta_t = _imu->get_delta_time();
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// Get current values for gyros
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_gyro_vector = _imu->get_gyro();
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_accel_vector = _imu->get_accel();
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// Integrate the DCM matrix using gyro inputs
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matrix_update(delta_t);
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// Normalize the DCM matrix
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normalize();
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// Perform drift correction
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drift_correction(delta_t);
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// paranoid check for bad values in the DCM matrix
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check_matrix();
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// Calculate pitch, roll, yaw for stabilization and navigation
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euler_angles();
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}
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// update the DCM matrix using only the gyros
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void
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AP_AHRS_DCM::matrix_update(float _G_Dt)
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{
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// _omega_integ_corr is used for _centripetal correction
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// (theoretically better than _omega)
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_omega_integ_corr = _gyro_vector + _omega_I;
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// Equation 16, adding proportional and integral correction terms
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_omega = _omega_integ_corr + _omega_P + _omega_yaw_P;
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// this is a replacement of the DCM matrix multiply (equation
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// 17), with known zero elements removed and the matrix
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// operations inlined. This runs much faster than the original
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// version of this code, as the compiler was doing a terrible
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// job of realising that so many of the factors were in common
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// or zero. It also uses much less stack, as we no longer need
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// two additional local matrices
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Vector3f r = _omega * _G_Dt;
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_dcm_matrix.rotate(r);
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}
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// adjust an accelerometer vector for known acceleration forces
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void
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AP_AHRS_DCM::accel_adjust(Vector3f &accel)
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{
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float veloc;
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// compensate for linear acceleration. This makes a
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// surprisingly large difference in the pitch estimate when
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// turning, plus on takeoff and landing
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float acceleration = _gps->acceleration();
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accel.x -= acceleration;
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// compensate for centripetal acceleration
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veloc = _gps->ground_speed * 0.01;
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// We are working with a modified version of equation 26 as
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// our IMU object reports acceleration in the positive axis
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// direction as positive
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// Equation 26 broken up into separate pieces
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accel.y -= _omega_integ_corr.z * veloc;
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accel.z += _omega_integ_corr.y * veloc;
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}
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/*
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reset the DCM matrix and omega. Used on ground start, and on
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extreme errors in the matrix
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*/
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void
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AP_AHRS_DCM::reset(bool recover_eulers)
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{
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if (_compass != NULL) {
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_compass->null_offsets_disable();
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}
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// reset the integration terms
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_omega_I.zero();
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_omega_P.zero();
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_omega_yaw_P.zero();
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_omega_integ_corr.zero();
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_omega.zero();
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// if the caller wants us to try to recover to the current
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// attitude then calculate the dcm matrix from the current
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// roll/pitch/yaw values
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if (recover_eulers && !isnan(roll) && !isnan(pitch) && !isnan(yaw)) {
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_dcm_matrix.from_euler(roll, pitch, yaw);
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} else {
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// otherwise make it flat
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_dcm_matrix.from_euler(0, 0, 0);
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}
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if (_compass != NULL) {
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_compass->null_offsets_enable(); // This call is needed to restart the nulling
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// Otherwise the reset in the DCM matrix can mess up
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// the nulling
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}
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}
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/*
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check the DCM matrix for pathological values
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*/
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void
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AP_AHRS_DCM::check_matrix(void)
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{
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if (_dcm_matrix.is_nan()) {
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//Serial.printf("ERROR: DCM matrix NAN\n");
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SITL_debug("ERROR: DCM matrix NAN\n");
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renorm_blowup_count++;
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reset(true);
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return;
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}
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// some DCM matrix values can lead to an out of range error in
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// the pitch calculation via asin(). These NaN values can
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// feed back into the rest of the DCM matrix via the
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// error_course value.
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if (!(_dcm_matrix.c.x < 1.0 &&
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_dcm_matrix.c.x > -1.0)) {
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// We have an invalid matrix. Force a normalisation.
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renorm_range_count++;
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normalize();
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if (_dcm_matrix.is_nan() ||
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fabs(_dcm_matrix.c.x) > 10) {
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// normalisation didn't fix the problem! We're
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// in real trouble. All we can do is reset
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//Serial.printf("ERROR: DCM matrix error. _dcm_matrix.c.x=%f\n",
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// _dcm_matrix.c.x);
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SITL_debug("ERROR: DCM matrix error. _dcm_matrix.c.x=%f\n",
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_dcm_matrix.c.x);
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renorm_blowup_count++;
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reset(true);
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}
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}
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}
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// renormalise one vector component of the DCM matrix
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// this will return false if renormalization fails
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bool
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AP_AHRS_DCM::renorm(Vector3f const &a, Vector3f &result)
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{
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float renorm_val;
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// numerical errors will slowly build up over time in DCM,
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// causing inaccuracies. We can keep ahead of those errors
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// using the renormalization technique from the DCM IMU paper
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// (see equations 18 to 21).
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// For APM we don't bother with the taylor expansion
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// optimisation from the paper as on our 2560 CPU the cost of
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// the sqrt() is 44 microseconds, and the small time saving of
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// the taylor expansion is not worth the potential of
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// additional error buildup.
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// Note that we can get significant renormalisation values
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// when we have a larger delta_t due to a glitch eleswhere in
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// APM, such as a I2c timeout or a set of EEPROM writes. While
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// we would like to avoid these if possible, if it does happen
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// we don't want to compound the error by making DCM less
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// accurate.
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renorm_val = 1.0 / a.length();
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// keep the average for reporting
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_renorm_val_sum += renorm_val;
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_renorm_val_count++;
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if (!(renorm_val < 2.0 && renorm_val > 0.5)) {
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// this is larger than it should get - log it as a warning
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renorm_range_count++;
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if (!(renorm_val < 1.0e6 && renorm_val > 1.0e-6)) {
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// we are getting values which are way out of
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// range, we will reset the matrix and hope we
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// can recover our attitude using drift
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// correction before we hit the ground!
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//Serial.printf("ERROR: DCM renormalisation error. renorm_val=%f\n",
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// renorm_val);
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SITL_debug("ERROR: DCM renormalisation error. renorm_val=%f\n",
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renorm_val);
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renorm_blowup_count++;
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return false;
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}
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}
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result = a * renorm_val;
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return true;
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}
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/*************************************************
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Direction Cosine Matrix IMU: Theory
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William Premerlani and Paul Bizard
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Numerical errors will gradually reduce the orthogonality conditions expressed by equation 5
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to approximations rather than identities. In effect, the axes in the two frames of reference no
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longer describe a rigid body. Fortunately, numerical error accumulates very slowly, so it is a
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simple matter to stay ahead of it.
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We call the process of enforcing the orthogonality conditions ÒrenormalizationÓ.
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*/
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void
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AP_AHRS_DCM::normalize(void)
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{
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float error;
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Vector3f t0, t1, t2;
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error = _dcm_matrix.a * _dcm_matrix.b; // eq.18
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t0 = _dcm_matrix.a - (_dcm_matrix.b * (0.5f * error)); // eq.19
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t1 = _dcm_matrix.b - (_dcm_matrix.a * (0.5f * error)); // eq.19
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t2 = t0 % t1; // c= a x b // eq.20
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if (!renorm(t0, _dcm_matrix.a) ||
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!renorm(t1, _dcm_matrix.b) ||
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!renorm(t2, _dcm_matrix.c)) {
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// Our solution is blowing up and we will force back
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// to last euler angles
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reset(true);
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}
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}
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// perform drift correction. This function aims to update _omega_P and
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// _omega_I with our best estimate of the short term and long term
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// gyro error. The _omega_P value is what pulls our attitude solution
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// back towards the reference vector quickly. The _omega_I term is an
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// attempt to learn the long term drift rate of the gyros.
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//
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// This function also updates _omega_yaw_P with a yaw correction term
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// from our yaw reference vector
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void
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AP_AHRS_DCM::drift_correction(float deltat)
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{
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float error_course = 0;
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Vector3f accel;
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Vector3f error;
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float error_norm = 0;
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float yaw_deltat = 0;
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accel = _accel_vector;
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// if enabled, use the GPS to correct our accelerometer vector
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// for centripetal forces
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if(_centripetal &&
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_gps != NULL &&
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_gps->status() == GPS::GPS_OK) {
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accel_adjust(accel);
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}
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//*****Roll and Pitch***************
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// normalise the accelerometer vector to a standard length
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// this is important to reduce the impact of noise on the
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// drift correction, as very noisy vectors tend to have
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// abnormally high lengths. By normalising the length we
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// reduce their impact.
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float accel_length = accel.length();
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accel *= (_gravity / accel_length);
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if (accel.is_inf()) {
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// we can't do anything useful with this sample
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_omega_P.zero();
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return;
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}
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// calculate the error, in m/2^2, between the attitude
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// implied by the accelerometers and the attitude
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// in the current DCM matrix
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error = _dcm_matrix.c % accel;
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// Limit max error to limit the effect of noisy values
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// on the algorithm. This limits the error to about 11
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// degrees
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error_norm = error.length();
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if (error_norm > 2) {
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error *= (2 / error_norm);
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}
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// we now want to calculate _omega_P and _omega_I. The
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// _omega_P value is what drags us quickly to the
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// accelerometer reading.
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_omega_P = error * _kp_roll_pitch;
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// the _omega_I is the long term accumulated gyro
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// error. This determines how much gyro drift we can
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// handle.
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_omega_I_sum += error * (_ki_roll_pitch * deltat);
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_omega_I_sum_time += deltat;
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// these sums support the reporting of the DCM state via MAVLink
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_error_rp_sum += error_norm;
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_error_rp_count++;
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// yaw drift correction
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// we only do yaw drift correction when we get a new yaw
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// reference vector. In between times we rely on the gyros for
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// yaw. Avoiding this calculation on every call to
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// update_DCM() saves a lot of time
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if (_compass && _compass->use_for_yaw()) {
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if (_compass->last_update != _compass_last_update) {
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yaw_deltat = 1.0e-6*(_compass->last_update - _compass_last_update);
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if (_have_initial_yaw && yaw_deltat < 2.0) {
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// Equation 23, Calculating YAW error
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// We make the gyro YAW drift correction based
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// on compass magnetic heading
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error_course = (_dcm_matrix.a.x * _compass->heading_y) - (_dcm_matrix.b.x * _compass->heading_x);
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_compass_last_update = _compass->last_update;
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} else {
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// this is our first estimate of the yaw,
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// or the compass has come back online after
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// no readings for 2 seconds.
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//
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// construct a DCM matrix based on the current
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// roll/pitch and the compass heading.
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// First ensure the compass heading has been
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// calculated
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_compass->calculate(_dcm_matrix);
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// now construct a new DCM matrix
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_compass->null_offsets_disable();
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_dcm_matrix.from_euler(roll, pitch, _compass->heading);
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_compass->null_offsets_enable();
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_have_initial_yaw = true;
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_compass_last_update = _compass->last_update;
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error_course = 0;
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}
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}
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} else if (_gps && _gps->status() == GPS::GPS_OK) {
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if (_gps->last_fix_time != _gps_last_update) {
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// Use GPS Ground course to correct yaw gyro drift
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if (_gps->ground_speed >= GPS_SPEED_MIN) {
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yaw_deltat = 1.0e-3*(_gps->last_fix_time - _gps_last_update);
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if (_have_initial_yaw && yaw_deltat < 2.0) {
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float course_over_ground_x = cos(ToRad(_gps->ground_course/100.0));
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float course_over_ground_y = sin(ToRad(_gps->ground_course/100.0));
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// Equation 23, Calculating YAW error
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error_course = (_dcm_matrix.a.x * course_over_ground_y) - (_dcm_matrix.b.x * course_over_ground_x);
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_gps_last_update = _gps->last_fix_time;
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} else {
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// when we first start moving, set the
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// DCM matrix to the current
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// roll/pitch values, but with yaw
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// from the GPS
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if (_compass) {
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_compass->null_offsets_disable();
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}
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_dcm_matrix.from_euler(roll, pitch, ToRad(_gps->ground_course));
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if (_compass) {
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_compass->null_offsets_enable();
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}
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_have_initial_yaw = true;
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error_course = 0;
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_gps_last_update = _gps->last_fix_time;
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}
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} else if (_gps->ground_speed >= GPS_SPEED_RESET) {
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// we are not going fast enough to use GPS for
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// course correction, but we won't reset
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// _have_initial_yaw yet, instead we just let
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// the gyro handle yaw
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error_course = 0;
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} else {
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// we are moving very slowly. Reset
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// _have_initial_yaw and adjust our heading
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// rapidly next time we get a good GPS ground
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// speed
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error_course = 0;
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_have_initial_yaw = false;
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}
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}
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}
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// see if there is any error in our heading relative to the
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// yaw reference. This will be zero most of the time, as we
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// only calculate it when we get new data from the yaw
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// reference source
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if (yaw_deltat == 0 || error_course == 0) {
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// we don't have a new reference heading. Slowly
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// decay the _omega_yaw_P to ensure that if we have
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// lost the yaw reference sensor completely we don't
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// keep using a stale offset
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_omega_yaw_P *= 0.97;
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return;
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}
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// ensure the course error is scaled from -PI to PI
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if (error_course > PI) {
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error_course -= 2*PI;
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} else if (error_course < -PI) {
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error_course += 2*PI;
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}
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// Equation 24, Applys the yaw correction to the XYZ rotation of the aircraft
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// this gives us an error in radians
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error = _dcm_matrix.c * error_course;
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// Adding yaw correction to proportional correction vector. We
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// allow the yaw reference source to affect all 3 components
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// of _omega_yaw_P as we need to be able to correctly hold a
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// heading when roll and pitch are non-zero
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_omega_yaw_P = error * _kp_yaw.get();
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// add yaw correction to integrator correction vector, but
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// only for the z gyro. We rely on the accelerometers for x
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// and y gyro drift correction. Using the compass or GPS for
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// x/y drift correction is too inaccurate, and can lead to
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// incorrect builups in the x/y drift. We rely on the
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// accelerometers to get the x/y components right
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_omega_I_sum.z += error.z * (_ki_yaw * yaw_deltat);
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// we keep the sum of yaw error for reporting via MAVLink.
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_error_yaw_sum += error_course;
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_error_yaw_count++;
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if (_omega_I_sum_time > 10) {
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// every 10 seconds we apply the accumulated
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// _omega_I_sum changes to _omega_I. We do this to
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// prevent short term feedback between the P and I
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// terms of the controller. The _omega_I vector is
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// supposed to refect long term gyro drift, but with
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// high noise it can start to build up due to short
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// term interactions. By summing it over 10 seconds we
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// prevent the short term interactions and can apply
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// the slope limit more accurately
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float drift_limit = _gyro_drift_limit * _omega_I_sum_time;
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_omega_I_sum.x = constrain(_omega_I_sum.x, -drift_limit, drift_limit);
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_omega_I_sum.y = constrain(_omega_I_sum.y, -drift_limit, drift_limit);
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_omega_I_sum.z = constrain(_omega_I_sum.z, -drift_limit, drift_limit);
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_omega_I += _omega_I_sum;
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// zero the sum
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_omega_I_sum.zero();
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_omega_I_sum_time = 0;
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}
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}
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// calculate the euler angles which will be used for high level
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// navigation control
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void
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AP_AHRS_DCM::euler_angles(void)
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{
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_dcm_matrix.to_euler(&roll, &pitch, &yaw);
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roll_sensor = degrees(roll) * 100;
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pitch_sensor = degrees(pitch) * 100;
|
|
yaw_sensor = degrees(yaw) * 100;
|
|
|
|
if (yaw_sensor < 0)
|
|
yaw_sensor += 36000;
|
|
}
|
|
|
|
/* reporting of DCM state for MAVLink */
|
|
|
|
// average error_roll_pitch since last call
|
|
float AP_AHRS_DCM::get_error_rp(void)
|
|
{
|
|
if (_error_rp_count == 0) {
|
|
// this happens when telemetry is setup on two
|
|
// serial ports
|
|
return _error_rp_last;
|
|
}
|
|
_error_rp_last = _error_rp_sum / _error_rp_count;
|
|
_error_rp_sum = 0;
|
|
_error_rp_count = 0;
|
|
return _error_rp_last;
|
|
}
|
|
|
|
// average error_yaw since last call
|
|
float AP_AHRS_DCM::get_error_yaw(void)
|
|
{
|
|
if (_error_yaw_count == 0) {
|
|
// this happens when telemetry is setup on two
|
|
// serial ports
|
|
return _error_yaw_last;
|
|
}
|
|
_error_yaw_last = _error_yaw_sum / _error_yaw_count;
|
|
_error_yaw_sum = 0;
|
|
_error_yaw_count = 0;
|
|
return _error_yaw_last;
|
|
}
|