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122 lines
3.9 KiB
122 lines
3.9 KiB
% Implementation of a simple 3-state EKF that can identify the scale |
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% factor that needs to be applied to a true airspeed measurement |
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% Paul Riseborough 27 June 2013 |
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% Inputs: |
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% Measured true airsped (m/s) |
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clear all; |
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% Define wind speed used for truth model |
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vwn_truth = 4.0; |
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vwe_truth = 3.0; |
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vwd_truth = -0.5; % convection can produce values of up to 1.5 m/s, however |
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% average will zero over longer periods at lower altitudes |
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% Slope lift will be persistent |
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% Define airspeed scale factor used for truth model |
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K_truth = 1.2; |
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% Use a 1 second time step |
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DT = 1.0; |
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% Define the initial state error covariance matrix |
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% Assume initial wind uncertainty of 10 m/s and scale factor uncertainty of |
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% 0.2 |
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P = diag([10^2 10^2 0.001^2]); |
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% Define state error growth matrix assuming wind changes at a rate of 0.1 |
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% m/s/s and scale factor drifts at a rate of 0.001 per second |
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Q = diag([0.1^2 0.1^2 0.001^2])*DT^2; |
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% Define the initial state matrix assuming zero wind and a scale factor of |
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% 1.0 |
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x = [0;0;1.0]; |
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for i = 1:1000 |
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%% Calculate truth values |
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% calculate ground velocity by simulating a wind relative |
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% circular path of of 60m radius and 16 m/s airspeed |
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time = i*DT; |
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radius = 60; |
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TAS_truth = 16; |
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vwnrel_truth = TAS_truth*cos(TAS_truth*time/radius); |
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vwerel_truth = TAS_truth*sin(TAS_truth*time/radius); |
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vwdrel_truth = 0.0; |
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vgn_truth = vwnrel_truth + vwn_truth; |
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vge_truth = vwerel_truth + vwe_truth; |
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vgd_truth = vwdrel_truth + vwd_truth; |
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% calculate measured ground velocity and airspeed, adding some noise and |
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% adding a scale factor to the airspeed measurement. |
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vgn_mea = vgn_truth + 0.1*rand; |
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vge_mea = vge_truth + 0.1*rand; |
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vgd_mea = vgd_truth + 0.1*rand; |
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TAS_mea = K_truth * TAS_truth + 0.5*rand; |
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%% Perform filter processing |
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% This benefits from a matrix library that can handle up to 3x3 |
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% matrices |
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% Perform the covariance prediction |
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% Q is a diagonal matrix so only need to add three terms in |
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% C code implementation |
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P = P + Q; |
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% Perform the predicted measurement using the current state estimates |
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% No state prediction required because states are assumed to be time |
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% invariant plus process noise |
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% Ignore vertical wind component |
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TAS_pred = x(3) * sqrt((vgn_mea - x(1))^2 + (vge_mea - x(2))^2 + vgd_mea^2); |
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% Calculate the observation Jacobian H_TAS |
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SH1 = (vge_mea - x(2))^2 + (vgn_mea - x(1))^2; |
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SH2 = 1/sqrt(SH1); |
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H_TAS = zeros(1,3); |
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H_TAS(1,1) = -(x(3)*SH2*(2*vgn_mea - 2*x(1)))/2; |
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H_TAS(1,2) = -(x(3)*SH2*(2*vge_mea - 2*x(2)))/2; |
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H_TAS(1,3) = 1/SH2; |
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% Calculate the fusion innovaton covariance assuming a TAS measurement |
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% noise of 1.0 m/s |
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S = H_TAS*P*H_TAS' + 1.0; % [1 x 3] * [3 x 3] * [3 x 1] + [1 x 1] |
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% Calculate the Kalman gain |
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KG = P*H_TAS'/S; % [3 x 3] * [3 x 1] / [1 x 1] |
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% Update the states |
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x = x + KG*(TAS_mea - TAS_pred); % [3 x 1] + [3 x 1] * [1 x 1] |
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% Update the covariance matrix |
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P = P - KG*H_TAS*P; % [3 x 3] * |
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% force symmetry on the covariance matrix - necessary due to rounding |
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% errors |
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% Implementation will also need a further check to prevent diagonal |
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% terms becoming negative due to rounding errors |
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% This step can be made more efficient by excluding diagonal terms |
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% (would reduce processing by 1/3) |
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P = 0.5*(P + P'); % [1 x 1] * ( [3 x 3] + [3 x 3]) |
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%% Store results |
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output(i,:) = [time,x(1),x(2),x(3),vwn_truth,vwe_truth,K_truth]; |
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end |
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%% Plot output |
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figure; |
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subplot(3,1,1);plot(output(:,1),[output(:,2),output(:,5)]); |
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ylabel('Wind Vel North (m/s)'); |
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xlabel('time (sec)'); |
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grid on; |
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subplot(3,1,2);plot(output(:,1),[output(:,3),output(:,6)]); |
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ylabel('Wind Vel East (m/s)'); |
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xlabel('time (sec)'); |
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grid on; |
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subplot(3,1,3);plot(output(:,1),[output(:,4),output(:,7)]); |
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ylim([0 1.5]); |
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ylabel('Airspeed scale factor correction'); |
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xlabel('time (sec)'); |
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grid on; |
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