nass-metrology-test-bench/index.org

13 KiB

Cercalo Test Bench

Identification

<<sec:plant_identification>>

ZIP file containing the data and matlab files   ignore

All the files (data and Matlab scripts) are accessible here.

Excitation Data

  fs = 1e4;
  Ts = 1/fs;

We generate white noise with the "random number" simulink block, and we filter that noise.

  Gi = (1)/(1+s/2/pi/100);
  c2d(Gi, Ts, 'tustin')
c2d(Gi, Ts, 'tustin')

ans =

  0.030459 (z+1)
  --------------
    (z-0.9391)

Sample time: 0.0001 seconds
Discrete-time zero/pole/gain model.

Input / Output data

The identification data is loaded

  ux = load('mat/data_ux.mat', 't', 'ux', 'yx', 'yy');
  uy = load('mat/data_uy.mat', 't', 'uy', 'yx', 'yy');

We remove the first seconds where the Cercalo is turned on.

  i0x = 20*fs;

  i0y = 10*fs;

  ux.t  = ux.t( i0x:end) - ux.t(i0x);
  ux.ux = ux.ux(i0x:end);
  ux.yx = ux.yx(i0x:end);
  ux.yy = ux.yy(i0x:end);

  uy.t  = uy.t( i0y:end) - uy.t(i0x);
  uy.uy = uy.uy(i0y:end);
  uy.yx = uy.yx(i0y:end);
  uy.yy = uy.yy(i0y:end);
  ux.ux = ux.ux-mean(ux.ux);
  ux.yx = ux.yx-mean(ux.yx);
  ux.yy = ux.yy-mean(ux.yy);

  uy.ux = uy.ux-mean(uy.ux);
  uy.yx = uy.yx-mean(uy.yx);
  uy.yy = uy.yy-mean(uy.yy);
  <<plt-matlab>>
/tdehaeze/nass-metrology-test-bench/media/commit/f5bccf5f61687c8e491ef1ec466e3075d1791eed/figs/identification_ux.png
Identification signals when exciting the $x$ axis (png, pdf)
  <<plt-matlab>>
/tdehaeze/nass-metrology-test-bench/media/commit/f5bccf5f61687c8e491ef1ec466e3075d1791eed/figs/identification_uy.png
Identification signals when exciting the $y$ axis (png, pdf)

Estimation of the Frequency Response Function Matrix

We compute an estimate of the transfer functions.

  [tf_ux_yx, f] = tfestimate(ux.ux, ux.yx, hanning(ceil(1*fs)), [], [], fs);
  [tf_ux_yy, ~] = tfestimate(ux.ux, ux.yy, hanning(ceil(1*fs)), [], [], fs);
  [tf_uy_yx, ~] = tfestimate(uy.uy, uy.yx, hanning(ceil(1*fs)), [], [], fs);
  [tf_uy_yy, ~] = tfestimate(uy.uy, uy.yy, hanning(ceil(1*fs)), [], [], fs);
  <<plt-matlab>>
/tdehaeze/nass-metrology-test-bench/media/commit/f5bccf5f61687c8e491ef1ec466e3075d1791eed/figs/frequency_response_matrix.png
Frequency Response Matrix (png, pdf)

Coherence

  [coh_ux_yx, f] = mscohere(ux.ux, ux.yx, hanning(ceil(1*fs)), [], [], fs);
  [coh_ux_yy, ~] = mscohere(ux.ux, ux.yy, hanning(ceil(1*fs)), [], [], fs);
  [coh_uy_yx, ~] = mscohere(uy.uy, uy.yx, hanning(ceil(1*fs)), [], [], fs);
  [coh_uy_yy, ~] = mscohere(uy.uy, uy.yy, hanning(ceil(1*fs)), [], [], fs);
  <<plt-matlab>>
/tdehaeze/nass-metrology-test-bench/media/commit/f5bccf5f61687c8e491ef1ec466e3075d1791eed/figs/identification_coherence.png
Coherence (png, pdf)

Extraction of a transfer function matrix

First we define the initial guess for the resonance frequencies and the weights associated.

  freqs_res = [410, 250]; % [Hz]
  freqs_res_weights = [10, 10]; % [Hz]

From the number of resonance frequency we want to fit, we define the order N of the system we want to obtain.

  N = 2*length(freqs_res);

We then make an initial guess on the complex values of the poles.

  xi = 0.001; % Approximate modal damping
  poles = [2*pi*freqs_res*(xi + 1i), 2*pi*freqs_res*(xi - 1i)];

We then define the weight that will be used for the fitting. Basically, we want more weight around the resonance and at low frequency (below the first resonance). Also, we want more importance where we have a better coherence.

  weight = ones(1, length(f));
  % weight = G_coh';

  % alpha = 0.1;

  % for freq_i = 1:length(freqs_res)
  %   weight(f>(1-alpha)*freqs_res(freq_i) & omega<(1 + alpha)*2*pi*freqs_res(freq_i)) = freqs_res_weights(freq_i);
  % end

Ignore data above some frequency.

  weight(f>1000) = 0;
  <<plt-matlab>>
/tdehaeze/nass-metrology-test-bench/media/commit/f5bccf5f61687c8e491ef1ec466e3075d1791eed/figs/weights.png
Weights amplitude (png, pdf)

When we set some options for vfit3.

  opts = struct();

  opts.stable = 1;    % Enforce stable poles
  opts.asymp = 1;     % Force D matrix to be null
  opts.relax = 1;     % Use vector fitting with relaxed non-triviality constraint
  opts.skip_pole = 0; % Do NOT skip pole identification
  opts.skip_res = 0;  % Do NOT skip identification of residues (C,D,E)
  opts.cmplx_ss = 0;  % Create real state space model with block diagonal A

  opts.spy1 = 0;      % No plotting for first stage of vector fitting
  opts.spy2 = 0;      % Create magnitude plot for fitting of f(s)

We define the number of iteration.

  Niter = 5;

An we run the vectfit3 algorithm.

  for iter = 1:Niter
    [SER_ux_yx, poles, ~, fit_ux_yx] = vectfit3(tf_ux_yx.', 1i*2*pi*f, poles, weight, opts);
  end
  for iter = 1:Niter
    [SER_uy_yx, poles, ~, fit_uy_yx] = vectfit3(tf_uy_yx.', 1i*2*pi*f, poles, weight, opts);
  end
  for iter = 1:Niter
    [SER_ux_yy, poles, ~, fit_ux_yy] = vectfit3(tf_ux_yy.', 1i*2*pi*f, poles, weight, opts);
  end
  for iter = 1:Niter
    [SER_uy_yy, poles, ~, fit_uy_yy] = vectfit3(tf_uy_yy.', 1i*2*pi*f, poles, weight, opts);
  end
  <<plt-matlab>>
/tdehaeze/nass-metrology-test-bench/media/commit/f5bccf5f61687c8e491ef1ec466e3075d1791eed/figs/identification_matrix_fit.png
Transfer Function Extraction of the FRF matrix (png, pdf)

And finally, we create the identified state space model:

  G_ux_yx = minreal(ss(full(SER_ux_yx.A),SER_ux_yx.B,SER_ux_yx.C,SER_ux_yx.D));
  G_uy_yx = minreal(ss(full(SER_uy_yx.A),SER_uy_yx.B,SER_uy_yx.C,SER_uy_yx.D));
  G_ux_yy = minreal(ss(full(SER_ux_yy.A),SER_ux_yy.B,SER_ux_yy.C,SER_ux_yy.D));
  G_uy_yy = minreal(ss(full(SER_uy_yy.A),SER_uy_yy.B,SER_uy_yy.C,SER_uy_yy.D));

  G = [G_ux_yx, G_uy_yx;
       G_ux_yy, G_uy_yy];
  save('mat/plant.mat', 'G');

Plant Analysis

Control