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📄 nc_tanker.m

📁 基于rbf神经网络控制油船航行
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% Radial Basis Function Neural Controller for Tanker Ship Heading Regulation%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% By: Kevin Passino % Version: 1/21/00%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%clear		% Clear all variables in memorypause off% Initialize ship parameters % (can test two conditions, "ballast" or "full"):ell=350;			% Length of the ship (in meters)u=5;				% Nominal speed (in meters/sec)abar=1;             % Parameters for nonlinearitybbar=1;% Define the reference model (we use a first order transfer function % k_r/(s+a_r)):a_r=1/150;k_r=1/150;% Adaptation gain:eta=1;% Parameters for reinforcement function:eta_e=1;eta_c=20;% Parameters for the radial basis function neural network% Define parameters of the approximatornG=11;   % The number of partitions on each edge of the gridnR=nG^2;  % The number of receptive field units in the RBFn=2; % The number of inputs tempe=(-pi/2):(pi)/(nG-1):pi/2;  % Defines a uniformly spaced vector roughly on the input domain			             % that is used to form the uniform grid on the (e,c) spacetempc=(-0.01):(0.02)/(nG-1):0.01;k=0; % Counter for centers below% Place the centers on a gridfor i=1:length(tempe)	for j=1:length(tempc)	  k=k+1;	  center(1,k)=tempe(i);	  center(2,k)=tempc(j);	endend% Define spreads of Gaussian functionssigmae=0.7*((pi/nG)); % Use same value for all on e domainsigmac=0.7*((0.02)/nG); % Next, pick the *initial* strengths for the receptive field units (these are what will% later be adjusted by the reinforcement learning method): % First, you could use the approach from the neural networks chapter:temp=(-((nG-1)/2)):1:((nG-1)/2);for i=1:length(temp) % Across the e dimension	for j=1:length(temp) % Across the c dimension	thetamat(i,j)=-((1/10)*(200*(pi/180))*temp(i)+(1/10)*(200*(pi/180))*temp(j));	% Saturate it between max and min possible inputs to the plant	thetamat(i,j)=max([-80*(pi/180), min([80*(pi/180), thetamat(i,j)])]);						% Note that there are only nR "stregths" to adjust - here we choose them	                    % according to this mathematical formula to get an appropriately shaped surface	endend% And, put them in a vectork=0; % Counter for centers belowfor i=1:length(temp)	for j=1:length(temp)	  k=k+1;	  theta(k,1)=thetamat(i,j);	endend% Another choice is just to use all zero strengths - to test how good it is at synthesizing the% initial controller.thetaold=0*theta;% phi for the RBF NN is initialized below% Compute vectors with points over the whole range of % the neural controller inputs - for use belowe_input=(-pi/2):(pi)/50:(pi/2); c_input=(-0.01):(0.02)/50:(0.01); % Convert from radians to degrees:e_inputd=e_input*(180/pi);c_inputd=c_input*(180/pi);%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% Simulate the RBF regulating the ship heading 	% Next, we initialize the simulation:t=0; 		% Reset time to zeroindex=1;	% This is time's index (not time, its index).  tstop=20000;	% Stopping time for the simulation (in seconds) - normally 20000step=1;     % Integration step sizeT=10;		% The controller is implemented in discrete time and			% this is the sampling time for the controller.			% Note that the integration step size and the sampling			% time are not the same.  In this way we seek to simulate			% the continuous time system via the Runge-Kutta method and			% the discrete time controller as if it were			% implemented by a digital computer.  Hence, we sample			% the plant output every T seconds and at that time			% output a new value of the controller output.counter=10;	% This counter will be used to count the number of integration			% steps that have been taken in the current sampling interval.			% Set it to 10 to begin so that it will compute a controller			% output at the first step.			% For our example, when 10 integration steps have been			% taken we will then we will sample the ship heading			% and the reference heading and compute a new output			% for the controller.  eold=0;     % Initialize the past value of the error (for use            % in computing the change of the error, c).  Notice            % that this is somewhat of an arbitrary choice since             % there is no last time step.  The same problem is            % encountered in implementation.  cold=0;     % Need this to initialize phiold belowpsi_r_old=0; % Initialize the reference trajectoryyeold=0; 	 % Intial condition used to calculate ycymold=0; 	 % Initial condition for the first order reference modelx=[0;0;0];	% First, set the state to be a vector            x(1)=0;		% Set the initial heading to be zerox(2)=0;		% Set the initial heading rate to be zero.  			% We would also like to set x(3) initially but this			% must be done after we have computed the output			% of the controller.  In this case, by			% choosing the reference trajectory to be 			% zero at the beginning and the other initial conditions			% as they are, and the controller as designed,			% we will know that the output of the controller			% will start out at zero so we could have set 			% x(3)=0 here.  To keep things more general, however, 			% we set the intial condition immediately after 			% we compute the first controller output in the 			% loop below.% Need to initialize phifor i=1:nR	phiold(i,1)=exp(-(((eold-center(1,i))^2)/sigmae^2)-(((cold-center(2,i))^2)/sigmac^2));end% Next, we start the simulation of the system.  This is the main % loop for the simulation of the control system.psi_r=0*ones(1,tstop+1);psi=0*ones(1,tstop+1);e=0*ones(1,tstop+1);c=0*ones(1,tstop+1);s=0*ones(1,tstop+1);w=0*ones(1,tstop+1);delta=0*ones(1,tstop+1);ym=0*ones(1,tstop+1);J_R=0*ones(1,tstop+1);ye=0*ones(1,tstop+1);yc=0*ones(1,tstop+1);while t <= tstop% First, we define the reference input psi_r  (desired heading).if t>=0, psi_r(index)=0; end			    % Request heading of 0 degif t>=100, psi_r(index)=45*(pi/180); end     % Request heading of 45 degif t>=1500, psi_r(index)=0; end    			% Request heading of 0 degif t>=3000, psi_r(index)=45*(pi/180); end    % Request heading of -45 degif t>=4500, psi_r(index)=0; end    			% Request heading of 0 degif t>=6000, psi_r(index)=45*(pi/180); end     % Request heading of 45 degif t>=7500, psi_r(index)=0; end    			% Request heading of 0 degif t>=9000, psi_r(index)=45*(pi/180); end     % Request heading of 45 degif t>=10500, psi_r(index)=0; end    			% Request heading of 0 degif t>=12000, psi_r(index)=45*(pi/180); end    % Request heading of -45 degif t>=13500, psi_r(index)=0; end    			% Request heading of 0 degif t>=15000, psi_r(index)=45*(pi/180); end     % Request heading of 45 degif t>=16500, psi_r(index)=0; end    			% Request heading of 0 degif t>=18000, psi_r(index)=45*(pi/180); end     % Request heading of 45 degif t>=19500, psi_r(index)=0; end    			% Request heading of 0 deg% Next, suppose that there is sensor noise for the heading sensor with that is% additive, with a uniform distribution on [- 0.01,+0.01] deg.%s(index)=0.01*(pi/180)*(2*rand-1);s(index)=0;					  % This allows us to remove the noise.psi(index)=x(1)+s(index);     % Heading of the ship (possibly with sensor noise).if counter == 10,  % When the counter reaches 10 then execute the 				   % controllercounter=0; 			% First, reset the counter% Reference model calculations:% The reference model is part of the controller and to simulate it% we take the discrete equivalent of the% reference model to compute psi_m from psi_r (if you use% a continuous-time reference model you will have to augment % the state of the closed-loop system with the state(s) of the % reference model and hence update the state in the Runge-Kutta % equations).%% For the reference model we use a first order transfer function % k_r/(s+a_r) but we use the bilinear transformation where we % replace s by (2/step)(z-1)/(z+1), then find the z-domain % representation of the reference model, then convert this % to a difference equation:ym(index)=(1/(2+a_r*T))*((2-a_r*T)*ymold+...                                    k_r*T*(psi_r(index)+psi_r_old));ymold=ym(index);  psi_r_old=psi_r(index);	% This saves the past value of the ym and psi_r so that we can use it	% the next time around the loop	% Radial basis function neural network controller calculations:e(index)=psi_r(index)-psi(index); % Computes error (first layer of perceptron)c(index)=(e(index)-eold)/T; % Sets the value of ceold=e(index);   % Save the past value of e for use in the above				 % computation the next time around the loop% Next, perform calculations for reinforcement signalye(index)=ym(index)-psi(index);		    % Calculates yeyc(index)=(ye(index)-yeold)/T;			% Calculates ycyeold=ye(index);					    % Saves the value of ye for use the 							            % next time% Compute the reinforcement signal:J_R(index)=eta*(-eta_e*ye(index)-eta_c*yc(index));% When reinforcement signal is very small, simply make it zero (in% this way it will not over-react to small deviations in adjusting% the controller - it will only make adjustments when they are really needed)if abs(J_R(index))<0.005	J_R(index)=0;end% Compute the adjustments to the strengthsfor i=1:nR	theta(i,1)=thetaold(i,1)+J_R(index)*phiold(i,1);end% Next, compute the phi vector for the next time around the loopfor i=1:nR	phi(i,1)=exp(-(((e(index)-center(1,i))^2)/sigmae^2)-(((c(index)-center(2,i))^2)/sigmac^2));endthetaold=theta(:,1); % Save this for next time around the loopphiold=phi(:,1); % Save this for next time so that in the above formula the indices                 % for thetaold and phiold are the same% Compute the RBF outputdelta(index)=theta(:,1)'*phi(:,1); % Performs summing and scaling of receptive field unitselse % This goes with the "if" statement to check if the counter=10     % so the next lines up to the next "end" statement are executed     % whenever counter is not equal to 10% Now, even though we do not compute the neural controller at each% time instant, we do want to save the data at its inputs and output at% each time instant for the sake of plotting it.  Hence, we need to % compute these here (note that we simply hold the values constant):e(index)=e(index-1);	

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