Update missing "." in path
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@ -21,11 +21,11 @@ freqs = logspace(0, 3, 1000);
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% #+name: fig:micro_station_uniaxial_model
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% #+caption: Schematic of the Micro-Station measurement setup and uniaxial model.
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% #+begin_figure
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% #+attr_latex: :caption \subcaption{\label{fig:micro_station_meas_dynamics_schematic}Measurement setup - Schematic}
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% #+attr_latex: :caption \subcaption{\label{fig:uniaxial_ustation_meas_dynamics_schematic}Measurement setup - Schematic}
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% #+attr_latex: :options {0.69\textwidth}
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% #+begin_subfigure
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% #+attr_latex: :scale 1
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% [[file:figs/micro_station_meas_dynamics_schematic.png]]
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% [[file:figs/uniaxial_ustation_meas_dynamics_schematic.png]]
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% #+end_subfigure
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% #+attr_latex: :caption \subcaption{\label{fig:uniaxial_model_micro_station}Uniaxial model of the micro-station}
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% #+attr_latex: :options {0.29\textwidth}
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@ -73,7 +73,7 @@ psd_xf = psd_V.*abs(squeeze(freqresp(G_geo, f, 'Hz'))).^2; % [m^2/Hz]
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% The amplitude spectral density $\Gamma_{x_f}$ of the measured displacement $x_f$ is shown in Figure ref:fig:asd_floor_motion_id31.
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% The amplitude spectral density $\Gamma_{x_f}$ of the measured displacement $x_f$ is shown in Figure ref:fig:uniaxial_asd_floor_motion_id31.
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%% Amplitude Spectral Density of the measured Floor motion on ID31
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@ -110,7 +110,7 @@ win = hanning(ceil(2*Fs)); % Hanning window
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% It is then integrated to obtain the Amplitude Spectral Density of the relative motion which is compared with a non-rotating case (Figure ref:fig:asd_vibration_spindle_rotation).
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% It is then integrated to obtain the Amplitude Spectral Density of the relative motion which is compared with a non-rotating case (Figure ref:fig:uniaxial_asd_vibration_spindle_rotation).
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% It is shown that the spindle rotation induces vibrations in a wide frequency spectrum.
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@ -127,10 +127,10 @@ xlim([1, 500]); ylim([1e-12, 1e-7])
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% #+name: fig:asd_vibration_spindle_rotation
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% #+name: fig:uniaxial_asd_vibration_spindle_rotation
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% #+caption: Amplitude Spectral Density of the relative motion measured between the granite and the micro-hexapod's top platform during Spindle rotating
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% #+RESULTS:
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% [[file:figs/asd_vibration_spindle_rotation.png]]
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% [[file:figs/uniaxial_asd_vibration_spindle_rotation.png]]
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% In order to compute the equivalent disturbance force $f_t$ that induces such motion, the transfer function from $f_t$ to the relative motion of the hexapod's top platform and the granite is extracted from the model.
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@ -166,7 +166,7 @@ psd_ft = (psd_vft./(2*pi*f).^2)./abs(squeeze(freqresp(G('Dh', 'ft') - G('Dg', 'f
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% The obtained amplitude spectral density of the disturbance force $f_t$ is shown in Figure ref:fig:asd_disturbance_force.
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% The obtained amplitude spectral density of the disturbance force $f_t$ is shown in Figure ref:fig:uniaxial_asd_disturbance_force.
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%% Estimated disturbance force ft from measurement and uniaxial model
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figure;
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@ -264,7 +264,7 @@ K_hac_pz.InputName = {'d'};
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K_hac_pz.OutputName = {'f'};
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%% Save High Authority Controllers
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save('/mat/uniaxial_high_authority_controllers.mat', ...
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save('./mat/uniaxial_high_authority_controllers.mat', ...
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'K_hac_vc', 'K_hac_md', 'K_hac_pz');
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%% Compute Loop gain for Nyquist Plot
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@ -3960,7 +3960,7 @@ save('./matlab/mat/uniaxial_high_authority_controllers.mat', ...
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#+begin_src matlab :exports none :eval no
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%% Save High Authority Controllers
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save('/mat/uniaxial_high_authority_controllers.mat', ...
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save('./mat/uniaxial_high_authority_controllers.mat', ...
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'K_hac_vc', 'K_hac_md', 'K_hac_pz');
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#+end_src
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