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% Copyright (C) 2024, Naoki Sean Pross, ETH Zürich
%
% Compute model for UAV for given set of parameters.
function [model] = uav_model(params, perf, uncert)
model = struct();
% ------------------------------------------------------------------------
% Symbolic variables
% Constant scalar physical quantities and dimensions
syms m g rho a b d S k_T c_d c_0 c_l J_r real;
syms J_1 J_2 J_3 real;
J = diag([J_1, J_2, J_3]);
% Scalar position, rotation and velocities
syms x y z xdot ydot zdot real;
syms phi theta p q r real;
psi = sym('psi', 'real'); % shadow MATLAB's psi() function
% Vector position, rotation and velocities
P = [x; y; z]; % position vector (inertial frame)
Pdot = [xdot; ydot; zdot]; % velocity vector (intertial frame)
Theta = [phi; theta; psi]; % attitude vector: [roll pitch yaw] (body frame)
Omega = [p; q; r]; % angular rates (body frame)
% Inputs: flap angles and ducted fan speed
syms alpha_1 alpha_2 alpha_3 alpha_4 omega real;
alpha = [alpha_1; alpha_2; alpha_3; alpha_4];
% Flap angles are measured relative to the body-frame z-axis and considered
% positive / negative with respect to the roll / pitch axis to which they
% are attached to. Reference table:
%
% angle attached axis lift force direction
% when angle is positive
% ------- ------------- ----------------------
% alpha_1 pos. x axis y direction
% alpha_2 pos. y axis -x direction
% alpha_3 neg. x axis y direction
% alpha_4 neg. y axis -x direction
% Rotation matrix to change between frames of reference:
% multiplying by R moves from the inertial frame to the body frame
% to go from body frame to inertial frame use R transpose (R is SO(3))
R = [
cos(theta) * cos(psi), cos(theta) * sin(psi), -sin(theta);
(sin(phi) * sin(theta) * cos(psi) - cos(phi) * sin(psi)), ...
(sin(phi) * sin(theta) * sin(psi) + cos(phi) * cos(psi)), ...
sin(phi) * cos(theta);
(cos(phi) * sin(theta) * cos(psi) + sin(phi) * sin(psi)), ...
(cos(phi) * sin(theta) * sin(psi) - sin(phi) * cos(psi)), ...
cos(phi) * cos(theta);
];
% Matrix to relate Euler angles to angular velocity in the body frame
% i.e. dTheta/dt = U * Omega. To get the angular velocity in intertial
% coordinates use (R * U).
U = [
1, sin(phi) * tan(theta), cos(phi) * tan(theta);
0, cos(phi), -sin(phi);
0, sin(phi) / cos(theta), cos(phi) / cos(theta);
];
% name of unit vectors in inertial frame
uvec_i = [1; 0; 0];
uvec_j = [0; 1; 0];
uvec_k = [0; 0; 1];
% name of unit vectors in body frame
uvec_x = [1; 0; 0];
uvec_y = [0; 1; 0];
uvec_z = [0; 0; 1];
% ------------------------------------------------------------------------
% Nonlinear system dynamics
% Approximate air velocity field magnitude collinear to uvec_z
nu = omega / pi * sqrt(k_T / (2 * a * rho));
% Aerodynamic force caused by flaps in body frame
F_flap = @(alpha, uvec_n) rho * S * nu^2 / 2 * (...
(c_d * alpha^2 + c_0) * uvec_z + c_l * alpha * uvec_n);
F_1 = F_flap(alpha_1, uvec_y);
F_2 = F_flap(alpha_2, uvec_x);
F_3 = F_flap(alpha_3, uvec_y);
F_4 = F_flap(alpha_4, uvec_x);
% Torque caused by aerodynamics forces in body frame
tau_1 = cross((d * uvec_z + a/3 * uvec_x), F_1);
tau_2 = cross((d * uvec_z + a/3 * uvec_y), F_2);
tau_3 = cross((d * uvec_z - a/3 * uvec_x), F_3);
tau_4 = cross((d * uvec_z - a/3 * uvec_y), F_4);
% Total force acting on the UAV in the body frame
F = R * (m * g * uvec_k) ... % gravity
- k_T * omega^2 * uvec_z ... % thrust
+ F_1 + F_2 + F_3 + F_4; % flaps
% Total torque acting on the UAV in the body frame
tau = J_r * omega * R * cross(uvec_k, Omega) + ... % gyroscopic procession
tau_1 + tau_2 + tau_3 + tau_4; % flaps
% State space form with state variable xi and input u
%
% The 12-dimensional state is given by
%
% - absolute position (inertial frame) in R^3
% - absolute velocity (intertial frame) in R^3
% - Euler angles (body frame) in SO(3)
% - Angular rates (body frame) in R^3
%
xi = [P; Pdot; Theta; Omega];
u = [alpha; omega];
% Right hand side of dynamics dxi = f(xi, u)
f = [
Pdot;
R' * F / m; % translational dynamics
U * Omega;
inv(J) * (tau - cross(Omega, J * Omega)); % rotational dynamics
];
% Save function to compute the rotation matrix
model.FrameRot = @(pitch, roll, yaw) ...
subs(R, [phi, theta, psi], [pitch, roll, yaw]);
% Save equations of non-linear model (algebraic)
model.nonlinear = struct(...
'State', xi, ...
'Inputs', u, ...
'Dynamics', f ...
);
% ------------------------------------------------------------------------
% Linearization at equilibrium
% Equilibrium point
xi_eq = [
params.linearization.Position;
params.linearization.Velocity;
params.linearization.Angles;
params.linearization.AngularVelocities;
];
u_eq = params.linearization.Inputs;
% Construct linearized state dynamics
A = subs(jacobian(f, xi), [xi; u], [xi_eq; u_eq]);
B = subs(jacobian(f, u), [xi; u], [xi_eq; u_eq]);
% Insert values of parameters
phy = struct(...
'g', params.physics.Gravity, ...
'rho', params.physics.AirDensity ...
);
A = subs(A, phy);
B = subs(B, phy);
mech = struct(...
'm', params.mechanical.Mass, ...
'a', params.mechanical.DuctRadius, ...
'b', params.mechanical.DuctHeight, ...
'd', params.mechanical.FlapZDistance, ...
'J_1', params.mechanical.InertiaTensor(1, 1), ...
'J_2', params.mechanical.InertiaTensor(2, 2), ...
'J_3', params.mechanical.InertiaTensor(3, 3), ...
'J_r', params.mechanical.GyroscopicInertiaZ ...
);
A = subs(A, mech);
B = subs(B, mech);
aero = struct(...
'k_T', params.aerodynamics.ThrustOmegaProp, ...
'S', params.aerodynamics.FlapArea, ...
'c_d', params.aerodynamics.DragCoefficients(1), ...
'c_0', params.aerodynamics.DragCoefficients(2), ...
'c_l', params.aerodynamics.LiftCoefficient ...
);
A = subs(A, aero);
B = subs(B, aero);
% Evaluate constants like pi, etc and convert to double
A = double(vpa(A));
B = double(vpa(B));
% The state is fully observed via hardware and refined with sensor fusion
% algorithms
C = eye(size(A));
D = zeros(12, 5);
% Number of states, inputs and outputs
[nx, nu] = size(B);
[ny, ~] = size(C);
% Create state space object
sys = ss(A, B, C, D);
% T = params.actuators.MeasurementDelay;
% sys = ss(A, B, C, D, 'OutputDelay', T);
% Save linearized dynamics (numerical)
model.linear = struct(...
'Nx', nx, 'Nu', nu, 'Ny', ny, ... % number of states, inputs, and outputs
'State', xi, 'Inputs', u, ... % state and input variables
'StateEq', xi_eq, 'InputEq', u_eq, ... % where the system was linearized
'StateSpace', sys ... % state space object
);
% ------------------------------------------------------------------------
% Check properties of linearized model
eigvals = eig(A);
% Check system controllability / stabilizability
Wc = ctrb(sys);
if rank(Wc) < nx
fprintf('Linearized system has %d uncontrollable states!\n', ...
(nx - rank(Wc)));
% Is the system at least stabilizable?
unstabilizable = 0;
for i = 1:nx
if real(eigvals(i)) >= 0
% PBH test
W = [(A - eigvals(i) * eye(size(A))), B];
if rank(W) < nx
% fprintf(' State %d is not stabilizable\n', i);
unstabilizable = unstabilizable + 1;
end
end
end
if unstabilizable > 0
fprintf('Linearized system has %d unstabilizable modes!\n', ...
unstabilizable);
else
fprintf('However, it is stabilizable.\n');
end
end
% Check system observability / detectability
Wo = obsv(sys);
if rank(Wo) < nx
fprintf('Linearized system has %d unobservable states!\n', ...
(nx - rank(Wo)));
% is the system at least detectable?
undetectable = 0;
for i = 1:nx
if real(eigvals(i)) >= 0
% PBH test
W = [C; (A - eigvals(i) * eye(size(A)))];
if rank(W) < nx
undetectable = undetectable + 1;
end
end
end
if undetectable > 0
fprintf('Linearized system has %d undetectable modes!\n', ...
undetectable);
else
fprintf('However, it is detectable.')
end
end
% ------------------------------------------------------------------------
% Add uncertainties using SIMULINK model
% Load simulink model with uncertainties and pass in parameters
h = load_system('uav_model_uncertain');
hws = get_param('uav_model_uncertain', 'modelworkspace');
hws.assignin('model', model);
hws.assignin('perf', perf);
hws.assignin('uncert', uncert);
% Get uncertain model
ulmod = linmod('uav_model_uncertain');
usys = ss(ulmod.a, ulmod.b, ulmod.c, ulmod.d);
% Save uncertain model
model.uncertain = struct(...
'Simulink', ulmod, ...
'StateSpace', usys ...
);
end
% vim: ts=2 sw=2 et:
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