#!/usr/bin/env python3 # -*- coding: utf-8 -*- """ Copyright (c) 2022-2023 PX4 Development Team 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 PX4 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: derivation.py Description: Derivation of an error-state EKF based on Sola, Joan. "Quaternion kinematics for the error-state Kalman filter." arXiv preprint arXiv:1711.02508 (2017). The derivation is directly done in discrete-time as this allows us to define the desired type of discretization for each element while defining the equations (easier than a continuous-time derivation followed by a block-wise discretization). """ import argparse import symforce symforce.set_epsilon_to_symbol() import symforce.symbolic as sf from symforce import typing as T from symforce import ops from symforce.values import Values import sympy as sp from utils.derivation_utils import * # Initialize parser parser = argparse.ArgumentParser() parser.add_argument("--disable_mag", action='store_true', help="disable mag") parser.add_argument("--disable_wind", action='store_true', help="disable wind") # Read arguments from command line args = parser.parse_args() # The state vector is organized in an ordered dictionary State = Values( quat_nominal = sf.Rot3(), vel = sf.V3(), pos = sf.V3(), gyro_bias = sf.V3(), accel_bias = sf.V3(), mag_I = sf.V3(), mag_B = sf.V3(), wind_vel = sf.V2(), terrain = sf.V1() ) if args.disable_mag: del State["mag_I"] del State["mag_B"] if args.disable_wind: del State["wind_vel"] class IdxDof(): def __init__(self, idx, dof): self.idx = idx self.dof = dof def BuildTangentStateIndex(): # Build a dictionary that can be used to access elements of vectors # and matrices defined in the state tangent space (e.g.: P, K and H) tangent_state_index = {} idx = 0 for key in State.keys_recursive(): dof = State[key].tangent_dim() tangent_state_index[key] = IdxDof(idx, dof) idx += dof return tangent_state_index tangent_idx = BuildTangentStateIndex() class VState(sf.Matrix): SHAPE = (State.storage_dim(), 1) class VTangent(sf.Matrix): SHAPE = (State.tangent_dim(), 1) class MTangent(sf.Matrix): SHAPE = (State.tangent_dim(), State.tangent_dim()) def vstate_to_state(v: VState): state = State.from_storage(v) q_px4 = state["quat_nominal"].to_storage() state["quat_nominal"] = sf.Rot3(sf.Quaternion(xyz=sf.V3(q_px4[1], q_px4[2], q_px4[3]), w=q_px4[0])) return state def predict_covariance( state: VState, P: MTangent, accel: sf.V3, accel_var: sf.V3, gyro: sf.V3, gyro_var: sf.Scalar, dt: sf.Scalar ) -> MTangent: state = vstate_to_state(state) g = sf.Symbol("g") # does not appear in the jacobians state_error = Values( theta = sf.V3.symbolic("delta_theta"), vel = sf.V3.symbolic("delta_v"), pos = sf.V3.symbolic("delta_p"), gyro_bias = sf.V3.symbolic("delta_w_b"), accel_bias = sf.V3.symbolic("delta_a_b"), mag_I = sf.V3.symbolic("mag_I"), mag_B = sf.V3.symbolic("mag_B"), wind_vel = sf.V2.symbolic("wind_vel"), terrain = sf.V1.symbolic("terrain") ) if args.disable_mag: del state_error["mag_I"] del state_error["mag_B"] if args.disable_wind: del state_error["wind_vel"] # True state kinematics state_t = Values() for key in state.keys(): if key == "quat_nominal": # Create true quaternion using small angle approximation of the error rotation state_t["quat_nominal"] = sf.Rot3(sf.Quaternion(xyz=(state_error["theta"] / 2), w=1)) * state["quat_nominal"] else: state_t[key] = state[key] + state_error[key] noise = Values( accel = sf.V3.symbolic("a_n"), gyro = sf.V3.symbolic("w_n"), ) input_t = Values( accel = accel - state_t["accel_bias"] - noise["accel"], gyro = gyro - state_t["gyro_bias"] - noise["gyro"] ) R_t = state_t["quat_nominal"] state_t_pred = state_t.copy() state_t_pred["quat_nominal"] = state_t["quat_nominal"] * sf.Rot3(sf.Quaternion(xyz=(input_t["gyro"] * dt / 2), w=1)) state_t_pred["vel"] = state_t["vel"] + (R_t * input_t["accel"] + sf.V3(0, 0, g)) * dt state_t_pred["pos"] = state_t["pos"] + state_t["vel"] * dt # Nominal state kinematics input = Values( accel = accel - state["accel_bias"], gyro = gyro - state["gyro_bias"] ) R = state["quat_nominal"] state_pred = state.copy() state_pred["quat_nominal"] = state["quat_nominal"] * sf.Rot3(sf.Quaternion(xyz=(input["gyro"] * dt / 2), w=1)) state_pred["vel"] = state["vel"] + (R * input["accel"] + sf.V3(0, 0, g)) * dt state_pred["pos"] = state["pos"] + state["vel"] * dt # Error state kinematics state_error_pred = Values() for key in state_error.keys(): if key == "theta": delta_q = sf.Quaternion.from_storage(state_t_pred["quat_nominal"].to_storage()) * sf.Quaternion.from_storage(state_pred["quat_nominal"].to_storage()).conj() state_error_pred["theta"] = 2 * sf.V3(delta_q.x, delta_q.y, delta_q.z) # Use small angle approximation to obtain a simpler jacobian else: state_error_pred[key] = state_t_pred[key] - state_pred[key] # Simplify angular error state prediction for i in range(state_error_pred["theta"].storage_dim()): state_error_pred["theta"][i] = sp.expand(state_error_pred["theta"][i]).subs(dt**2, 0) # do not consider dt**2 effects in the derivation q_est = sf.Quaternion.from_storage(state["quat_nominal"].to_storage()) state_error_pred["theta"][i] = sp.factor(state_error_pred["theta"][i]).subs(q_est.w**2 + q_est.x**2 + q_est.y**2 + q_est.z**2, 1) # unit norm quaternion zero_state_error = {state_error[key]: state_error[key].zero() for key in state_error.keys()} zero_noise = {noise[key]: noise[key].zero() for key in noise.keys()} # State propagation jacobian A = VTangent(state_error_pred.to_storage()).jacobian(state_error).subs(zero_state_error).subs(zero_noise) G = VTangent(state_error_pred.to_storage()).jacobian(noise).subs(zero_state_error).subs(zero_noise) # Covariance propagation var_u = sf.Matrix.diag([accel_var[0], accel_var[1], accel_var[2], gyro_var, gyro_var, gyro_var]) P_new = A * P * A.T + G * var_u * G.T # Generate the equations for the upper triangular matrix and the diagonal only # Since the matrix is symmetric, the lower triangle does not need to be derived # and can simply be copied in the implementation for index in range(state.tangent_dim()): for j in range(state.tangent_dim()): if index > j: P_new[index,j] = 0 return P_new def jacobian_chain_rule(expr: sf.Scalar , state: State): # First compute the jacobian in the parameter space dh_dx = sf.V1(expr).jacobian(state, tangent_space=False) class MStorageTangent(sf.Matrix): SHAPE = (State.storage_dim(), State.tangent_dim()) # Then compute the jarobian mapping infinitesimal elements of the parameter space to the error state # Note that this jacobian only depends on the structure of the EKF dx_derror = MStorageTangent() q = sf.Quaternion.from_storage(state["quat_nominal"].to_storage()) p = sf.Quaternion.symbolic('p') pq = p * q qR = sf.M41(pq.to_storage()).jacobian(sf.M41(p.to_storage())) # Right quaternion product matrix dx_derror[0:4, 0:3] = qR / 2 * sf.M43([[1, 0, 0], [0, 1, 0], [0, 0, 1], [0, 0, 0]]) # The rest of the matrix is trivial for i in range(4, State.storage_dim()): for j in range(3, State.tangent_dim()): if (i == j+1): dx_derror[i, j] = 1 # Finally use the chain rule: dh/derror = dh/dx * dx/derror H = dh_dx * dx_derror return H def compute_airspeed_innov_and_innov_var( state: VState, P: MTangent, airspeed: sf.Scalar, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, sf.Scalar): state = vstate_to_state(state) wind = sf.V3(state["wind_vel"][0], state["wind_vel"][1], 0.0) vel_rel = state["vel"] - wind airspeed_pred = vel_rel.norm(epsilon=epsilon) innov = airspeed_pred - airspeed H = jacobian_chain_rule(airspeed_pred, state) innov_var = (H * P * H.T + R)[0,0] return (innov, innov_var) def compute_airspeed_h( state: VState, epsilon: sf.Scalar ) -> (VTangent, VTangent): state = vstate_to_state(state) wind = sf.V3(state["wind_vel"][0], state["wind_vel"][1], 0.0) vel_rel = state["vel"] - wind airspeed_pred = vel_rel.norm(epsilon=epsilon) H = jacobian_chain_rule(airspeed_pred, state) return H.T def compute_wind_init_and_cov_from_airspeed( v_local: sf.V3, heading: sf.Scalar, airspeed: sf.Scalar, v_var: sf.V3, heading_var: sf.Scalar, sideslip_var: sf.Scalar, airspeed_var: sf.Scalar, ) -> (sf.V2, sf.M22): # Initialise wind states assuming horizontal flight sideslip = sf.Symbol("beta") wind = sf.V2(v_local[0] - airspeed * sf.cos(heading + sideslip), v_local[1] - airspeed * sf.sin(heading + sideslip)) J = wind.jacobian([v_local[0], v_local[1], heading, sideslip, airspeed]) R = sf.M55() R[0,0] = v_var[0] R[1,1] = v_var[1] R[2,2] = heading_var R[3,3] = sideslip_var R[4,4] = airspeed_var P = J * R * J.T # Assume zero sideslip P = P.subs({sideslip: 0.0}) wind = wind.subs({sideslip: 0.0}) return (wind, P) def compute_wind_init_and_cov_from_wind_speed_and_direction( wind_speed: sf.Scalar, wind_direction: sf.Scalar, wind_speed_var: sf.Scalar, wind_direction_var: sf.Scalar )-> (sf.V2, sf.V2): wind = sf.V2(wind_speed * sf.cos(wind_direction), wind_speed * sf.sin(wind_direction)) H = wind.jacobian([wind_speed, wind_direction]) R = sf.Matrix.diag([wind_speed_var, wind_direction_var]) P = H * R * H.T P_diag = sf.V2(P[0,0], P[1,1]) return (wind, P_diag) def predict_sideslip( state: State, epsilon: sf.Scalar ) -> (sf.Scalar): wind = sf.V3(state["wind_vel"][0], state["wind_vel"][1], 0.0) vel_rel = state["vel"] - wind relative_wind_body = state["quat_nominal"].inverse() * vel_rel sideslip_pred = sf.atan2(relative_wind_body[1], relative_wind_body[0], epsilon) return sideslip_pred def compute_sideslip_innov_and_innov_var( state: VState, P: MTangent, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, sf.Scalar, sf.Scalar): state = vstate_to_state(state) sideslip_pred = predict_sideslip(state, epsilon); innov = sideslip_pred - 0.0 H = jacobian_chain_rule(sideslip_pred, state) innov_var = (H * P * H.T + R)[0,0] return (innov, innov_var) def compute_sideslip_h_and_k( state: VState, P: MTangent, innov_var: sf.Scalar, epsilon: sf.Scalar ) -> (VTangent, VTangent): state = vstate_to_state(state) sideslip_pred = predict_sideslip(state, epsilon); H = jacobian_chain_rule(sideslip_pred, state) K = P * H.T / sf.Max(innov_var, epsilon) return (H.T, K) def predict_vel_body( state: VState ) -> (sf.V3): vel = state["vel"] R_to_body = state["quat_nominal"].inverse() return R_to_body * vel def compute_body_vel_innov_var_h( state: VState, P: MTangent, R: sf.V3, ) -> (sf.V3, VTangent, VTangent, VTangent): state = vstate_to_state(state) meas_pred = predict_vel_body(state) Hx = jacobian_chain_rule(meas_pred[0], state) Hy = jacobian_chain_rule(meas_pred[1], state) Hz = jacobian_chain_rule(meas_pred[2], state) innov_var = sf.V3((Hx * P * Hx.T + R[0])[0,0], (Hy * P * Hy.T + R[1])[0,0], (Hz * P * Hz.T + R[2])[0,0]) return (innov_var, Hx.T, Hy.T, Hz.T) def compute_body_vel_y_innov_var( state: VState, P: MTangent, R: sf.Scalar ) -> (sf.Scalar): state = vstate_to_state(state) meas_pred = predict_vel_body(state) Hy = jacobian_chain_rule(meas_pred[1], state) innov_var = (Hy * P * Hy.T + R)[0,0] return (innov_var) def compute_body_vel_z_innov_var( state: VState, P: MTangent, R: sf.Scalar ) -> (sf.Scalar): state = vstate_to_state(state) meas_pred = predict_vel_body(state) Hz = jacobian_chain_rule(meas_pred[2], state) innov_var = (Hz * P * Hz.T + R)[0,0] return (innov_var) def predict_mag_body(state) -> sf.V3: mag_field_earth = state["mag_I"] mag_bias_body = state["mag_B"] mag_body = state["quat_nominal"].inverse() * mag_field_earth + mag_bias_body return mag_body def compute_mag_innov_innov_var_and_hx( state: VState, P: MTangent, meas: sf.V3, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.V3, sf.V3, VTangent): state = vstate_to_state(state) meas_pred = predict_mag_body(state); innov = meas_pred - meas innov_var = sf.V3() Hx = jacobian_chain_rule(meas_pred[0], state) innov_var[0] = (Hx * P * Hx.T + R)[0,0] Hy = jacobian_chain_rule(meas_pred[1], state) innov_var[1] = (Hy * P * Hy.T + R)[0,0] Hz = jacobian_chain_rule(meas_pred[2], state) innov_var[2] = (Hz * P * Hz.T + R)[0,0] return (innov, innov_var, Hx.T) def compute_mag_y_innov_var_and_h( state: VState, P: MTangent, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, VTangent): state = vstate_to_state(state) meas_pred = predict_mag_body(state); H = jacobian_chain_rule(meas_pred[1], state) innov_var = (H * P * H.T + R)[0,0] return (innov_var, H.T) def compute_mag_z_innov_var_and_h( state: VState, P: MTangent, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, VTangent): state = vstate_to_state(state) meas_pred = predict_mag_body(state); H = jacobian_chain_rule(meas_pred[2], state) innov_var = (H * P * H.T + R)[0,0] return (innov_var, H.T) def compute_yaw_innov_var_and_h( state: VState, P: MTangent, R: sf.Scalar ) -> (sf.Scalar, VTangent): state = vstate_to_state(state) q = sf.Quaternion.from_storage(state["quat_nominal"].to_storage()) r = sf.Quaternion.symbolic('r') delta_q = q * r.conj() # create a quaternion error of the measurement at the origin delta_meas_pred = 2 * delta_q.z # Use small angle approximation to obtain a simpler jacobian H = jacobian_chain_rule(delta_meas_pred, state) H = H.subs({r.w: q.w, r.x: q.x, r.y: q.y, r.z: q.z}) # assume innovation is small for i in range(State.tangent_dim()): H[i] = sp.factor(H[i]).subs(q.w**2 + q.x**2 + q.y**2 + q.z**2, 1) # unit norm quaternion innov_var = (H * P * H.T + R)[0,0] return (innov_var, H.T) def compute_mag_declination_pred_innov_var_and_h( state: VState, P: MTangent, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, sf.Scalar, VTangent): state = vstate_to_state(state) meas_pred = sf.atan2(state["mag_I"][1], state["mag_I"][0], epsilon=epsilon) H = jacobian_chain_rule(meas_pred, state) innov_var = (H * P * H.T + R)[0,0] return (meas_pred, innov_var, H.T) def predict_hagl(state): return state["terrain"][0] - state["pos"][2] def predict_opt_flow(state, epsilon): R_to_body = state["quat_nominal"].inverse() # Calculate earth relative velocity in a non-rotating sensor frame rel_vel_sensor = R_to_body * state["vel"] # Divide by range to get predicted angular LOS rates relative to X and Y # axes. Note these are rates in a non-rotating sensor frame hagl = predict_hagl(state) hagl = add_epsilon_sign(hagl, hagl, epsilon) R_to_earth = state["quat_nominal"].to_rotation_matrix() flow_pred = sf.V2() flow_pred[0] = rel_vel_sensor[1] / hagl * R_to_earth[2, 2] flow_pred[1] = -rel_vel_sensor[0] / hagl * R_to_earth[2, 2] return flow_pred def compute_flow_xy_innov_var_and_hx( state: VState, P: MTangent, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.V2, VTangent): state = vstate_to_state(state) meas_pred = predict_opt_flow(state, epsilon) innov_var = sf.V2() Hx = jacobian_chain_rule(meas_pred[0], state) innov_var[0] = (Hx * P * Hx.T + R)[0,0] Hy = jacobian_chain_rule(meas_pred[1], state) innov_var[1] = (Hy * P * Hy.T + R)[0,0] return (innov_var, Hx.T) def compute_flow_y_innov_var_and_h( state: VState, P: MTangent, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, VTangent): state = vstate_to_state(state) meas_pred = predict_opt_flow(state, epsilon) Hy = jacobian_chain_rule(meas_pred[1], state) innov_var = (Hy * P * Hy.T + R)[0,0] return (innov_var, Hy.T) def compute_hagl_innov_var( P: MTangent, R: sf.Scalar, ) -> (sf.Scalar): state = VState.symbolic("state") state = vstate_to_state(state) meas_pred = predict_hagl(state) H = jacobian_chain_rule(meas_pred, state) innov_var = (H * P * H.T + R)[0,0] return (innov_var) def compute_hagl_h( ) -> (VTangent): state = VState.symbolic("state") state = vstate_to_state(state) meas_pred = predict_hagl(state) H = jacobian_chain_rule(meas_pred, state) return (H.T) def compute_gnss_yaw_pred_innov_var_and_h( state: VState, P: MTangent, antenna_yaw_offset: sf.Scalar, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, sf.Scalar, VTangent): state = vstate_to_state(state) R_to_earth = state["quat_nominal"] # define antenna vector in body frame ant_vec_bf = sf.V3(sf.cos(antenna_yaw_offset), sf.sin(antenna_yaw_offset), 0) # rotate into earth frame ant_vec_ef = R_to_earth * ant_vec_bf # Calculate the yaw angle from the projection meas_pred = sf.atan2(ant_vec_ef[1], ant_vec_ef[0], epsilon=epsilon) H = jacobian_chain_rule(meas_pred, state) innov_var = (H * P * H.T + R)[0,0] return (meas_pred, innov_var, H.T) def predict_drag( state: State, rho: sf.Scalar, cd: sf.Scalar, cm: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar): R_to_body = state["quat_nominal"].inverse() wind = sf.V3(state["wind_vel"][0], state["wind_vel"][1], 0.0) vel_rel = state["vel"] - wind vel_rel_body = R_to_body * vel_rel vel_rel_body_xy = sf.V2(vel_rel_body[0], vel_rel_body[1]) bluff_body_drag = -0.5 * rho * cd * vel_rel_body_xy * vel_rel_body.norm(epsilon=epsilon) momentum_drag = -cm * vel_rel_body_xy return bluff_body_drag + momentum_drag def compute_drag_x_innov_var_and_h( state: VState, P: MTangent, rho: sf.Scalar, cd: sf.Scalar, cm: sf.Scalar, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, VTangent): state = vstate_to_state(state) meas_pred = predict_drag(state, rho, cd, cm, epsilon) Hx = jacobian_chain_rule(meas_pred[0], state) innov_var = (Hx * P * Hx.T + R)[0,0] return (innov_var, Hx.T) def compute_drag_y_innov_var_and_h( state: VState, P: MTangent, rho: sf.Scalar, cd: sf.Scalar, cm: sf.Scalar, R: sf.Scalar, epsilon: sf.Scalar ) -> (sf.Scalar, VTangent): state = vstate_to_state(state) meas_pred = predict_drag(state, rho, cd, cm, epsilon) Hy = jacobian_chain_rule(meas_pred[1], state) innov_var = (Hy * P * Hy.T + R)[0,0] return (innov_var, Hy.T) def predict_gravity_direction(state: State): # get transform from earth to body frame R_to_body = state["quat_nominal"].inverse() # the innovation is the error between measured acceleration # and predicted (body frame), assuming no body acceleration return R_to_body * sf.Matrix([0,0,-1]) def compute_gravity_xyz_innov_var_and_hx( state: VState, P: MTangent, R: sf.Scalar ) -> (sf.V3, VTangent): state = vstate_to_state(state) meas_pred = predict_gravity_direction(state) # initialize outputs innov_var = sf.V3() H = [None] * 3 # calculate observation jacobian (H), kalman gain (K), and innovation variance (S) # for each axis for i in range(3): H[i] = jacobian_chain_rule(meas_pred[i], state) innov_var[i] = (H[i] * P * H[i].T + R)[0,0] return (innov_var, H[0].T) def compute_gravity_y_innov_var_and_h( state: VState, P: MTangent, R: sf.Scalar ) -> (sf.V3, VTangent, VTangent, VTangent): state = vstate_to_state(state) meas_pred = predict_gravity_direction(state) # calculate observation jacobian (H), kalman gain (K), and innovation variance (S) H = jacobian_chain_rule(meas_pred[1], state) innov_var = (H * P * H.T + R)[0,0] return (innov_var, H.T) def compute_gravity_z_innov_var_and_h( state: VState, P: MTangent, R: sf.Scalar ) -> (sf.V3, VTangent, VTangent, VTangent): state = vstate_to_state(state) meas_pred = predict_gravity_direction(state) # calculate observation jacobian (H), kalman gain (K), and innovation variance (S) H = jacobian_chain_rule(meas_pred[2], state) innov_var = (H * P * H.T + R)[0,0] return (innov_var, H.T) print("Derive EKF2 equations...") generate_px4_function(predict_covariance, output_names=None) if not args.disable_mag: generate_px4_function(compute_mag_declination_pred_innov_var_and_h, output_names=["pred", "innov_var", "H"]) generate_px4_function(compute_mag_innov_innov_var_and_hx, output_names=["innov", "innov_var", "Hx"]) generate_px4_function(compute_mag_y_innov_var_and_h, output_names=["innov_var", "H"]) generate_px4_function(compute_mag_z_innov_var_and_h, output_names=["innov_var", "H"]) if not args.disable_wind: generate_px4_function(compute_airspeed_h, output_names=None) generate_px4_function(compute_airspeed_innov_and_innov_var, output_names=["innov", "innov_var"]) generate_px4_function(compute_drag_x_innov_var_and_h, output_names=["innov_var", "Hx"]) generate_px4_function(compute_drag_y_innov_var_and_h, output_names=["innov_var", "Hy"]) generate_px4_function(compute_sideslip_h_and_k, output_names=["H", "K"]) generate_px4_function(compute_sideslip_innov_and_innov_var, output_names=["innov", "innov_var"]) generate_px4_function(compute_wind_init_and_cov_from_airspeed, output_names=["wind", "P_wind"]) generate_px4_function(compute_wind_init_and_cov_from_wind_speed_and_direction, output_names=["wind", "P_wind"]) generate_px4_function(compute_yaw_innov_var_and_h, output_names=["innov_var", "H"]) generate_px4_function(compute_flow_xy_innov_var_and_hx, output_names=["innov_var", "H"]) generate_px4_function(compute_flow_y_innov_var_and_h, output_names=["innov_var", "H"]) generate_px4_function(compute_hagl_innov_var, output_names=["innov_var"]) generate_px4_function(compute_hagl_h, output_names=["H"]) generate_px4_function(compute_gnss_yaw_pred_innov_var_and_h, output_names=["meas_pred", "innov_var", "H"]) generate_px4_function(compute_gravity_xyz_innov_var_and_hx, output_names=["innov_var", "Hx"]) generate_px4_function(compute_gravity_y_innov_var_and_h, output_names=["innov_var", "Hy"]) generate_px4_function(compute_gravity_z_innov_var_and_h, output_names=["innov_var", "Hz"]) generate_px4_function(compute_body_vel_innov_var_h, output_names=["innov_var", "Hx", "Hy", "Hz"]) generate_px4_function(compute_body_vel_y_innov_var, output_names=["innov_var"]) generate_px4_function(compute_body_vel_z_innov_var, output_names=["innov_var"]) generate_px4_state(State, tangent_idx)