Update missing "." in path

matlab/uniaxial_1_micro_station_model.m

@@ -21,11 +21,11 @@ freqs = logspace(0, 3, 1000);
 % #+name: fig:micro_station_uniaxial_model
 % #+caption: Schematic of the Micro-Station measurement setup and uniaxial model.
 % #+begin_figure
-% #+attr_latex: :caption \subcaption{\label{fig:micro_station_meas_dynamics_schematic}Measurement setup - Schematic}
+% #+attr_latex: :caption \subcaption{\label{fig:uniaxial_ustation_meas_dynamics_schematic}Measurement setup - Schematic}
 % #+attr_latex: :options {0.69\textwidth}
 % #+begin_subfigure
 % #+attr_latex: :scale 1
-% [[file:figs/micro_station_meas_dynamics_schematic.png]]
+% [[file:figs/uniaxial_ustation_meas_dynamics_schematic.png]]
 % #+end_subfigure
 % #+attr_latex: :caption \subcaption{\label{fig:uniaxial_model_micro_station}Uniaxial model of the micro-station}
 % #+attr_latex: :options {0.29\textwidth}

matlab/uniaxial_3_disturbances.m

@@ -73,7 +73,7 @@ psd_xf = psd_V.*abs(squeeze(freqresp(G_geo, f, 'Hz'))).^2; % [m^2/Hz]
 
 
 
-% The amplitude spectral density $\Gamma_{x_f}$ of the measured displacement $x_f$ is shown in Figure ref:fig:asd_floor_motion_id31.
+% The amplitude spectral density $\Gamma_{x_f}$ of the measured displacement $x_f$ is shown in Figure ref:fig:uniaxial_asd_floor_motion_id31.
 
 
 %% Amplitude Spectral Density of the measured Floor motion on ID31
@@ -110,7 +110,7 @@ win = hanning(ceil(2*Fs)); % Hanning window
 
 
 
-% 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).
+% 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).
 % It is shown that the spindle rotation induces vibrations in a wide frequency spectrum.
 
 
@@ -127,10 +127,10 @@ xlim([1, 500]); ylim([1e-12, 1e-7])
 
 
 
-% #+name: fig:asd_vibration_spindle_rotation
+% #+name: fig:uniaxial_asd_vibration_spindle_rotation
 % #+caption: Amplitude Spectral Density of the relative motion measured between the granite and the micro-hexapod's top platform during Spindle rotating
 % #+RESULTS:
-% [[file:figs/asd_vibration_spindle_rotation.png]]
+% [[file:figs/uniaxial_asd_vibration_spindle_rotation.png]]
 
 % 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.
 
@@ -166,7 +166,7 @@ psd_ft = (psd_vft./(2*pi*f).^2)./abs(squeeze(freqresp(G('Dh', 'ft') - G('Dg', 'f
 
 
 
-% The obtained amplitude spectral density of the disturbance force $f_t$ is shown in Figure ref:fig:asd_disturbance_force.
+% The obtained amplitude spectral density of the disturbance force $f_t$ is shown in Figure ref:fig:uniaxial_asd_disturbance_force.
 
 %% Estimated disturbance force ft from measurement and uniaxial model
 figure;

matlab/uniaxial_6_hac_lac.m

@@ -264,7 +264,7 @@ K_hac_pz.InputName = {'d'};
 K_hac_pz.OutputName = {'f'};
 
 %% Save High Authority Controllers
-save('/mat/uniaxial_high_authority_controllers.mat', ...
+save('./mat/uniaxial_high_authority_controllers.mat', ...
         'K_hac_vc', 'K_hac_md', 'K_hac_pz');
 
 %% Compute Loop gain for Nyquist Plot

nass-uniaxial-model.org

@@ -3960,7 +3960,7 @@ save('./matlab/mat/uniaxial_high_authority_controllers.mat', ...
 
 #+begin_src matlab :exports none :eval no
 %% Save High Authority Controllers
-save('/mat/uniaxial_high_authority_controllers.mat', ...
+save('./mat/uniaxial_high_authority_controllers.mat', ...
         'K_hac_vc', 'K_hac_md', 'K_hac_pz');
 #+end_src