Output the analysis both to pdf and html

This commit is contained in:
Thomas Dehaeze 2021-06-04 12:15:32 +02:00
parent 757e429aac
commit fe52c24729
5 changed files with 1821 additions and 1397 deletions

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@ -2558,7 +2558,7 @@ exportFig('figs/strut_1_comp_enc_int.pdf', 'width', 'wide', 'height', 'tall');
#+end_src #+end_src
#+name: fig:strut_1_comp_enc_int #+name: fig:strut_1_comp_enc_int
#+caption: #+caption: Comparison of the transfer functions from excitation voltage $V_a$ to either the encoder $d_e$ or the interferometer $d_a$
#+RESULTS: #+RESULTS:
[[file:figs/strut_1_comp_enc_int.png]] [[file:figs/strut_1_comp_enc_int.png]]
@ -2581,7 +2581,7 @@ text(290, 4e-6, {'290Hz'},'VerticalAlignment','bottom','HorizontalAlignment','c
text(376, 1.4e-6,{'376Hz'},'VerticalAlignment','bottom','HorizontalAlignment','center') text(376, 1.4e-6,{'376Hz'},'VerticalAlignment','bottom','HorizontalAlignment','center')
hold off; hold off;
set(gca, 'XScale', 'log'); set(gca, 'YScale', 'log'); set(gca, 'XScale', 'log'); set(gca, 'YScale', 'log');
ylabel('Amplitude $d_e/V_a$ [m/V]'); set(gca, 'XTickLabel',[]); ylabel('Amplitude $d_e/V_a$ [m/V]'); xlabel('Frequency [Hz]');
hold off; hold off;
ylim([1e-7, 1e-3]); xlim([10, 2e3]); ylim([1e-7, 1e-3]); xlim([10, 2e3]);
#+end_src #+end_src
@ -2591,16 +2591,16 @@ exportFig('figs/strut_1_spurious_resonances.pdf', 'width', 'wide', 'height', 'ta
#+end_src #+end_src
#+name: fig:strut_1_spurious_resonances #+name: fig:strut_1_spurious_resonances
#+caption: #+caption: Magnitude of the transfer function from excitation voltage $V_a$ to encoder measurement $d_e$. The frequency of the resonances are noted.
#+RESULTS: #+RESULTS:
[[file:figs/strut_1_spurious_resonances.png]] [[file:figs/strut_1_spurious_resonances.png]]
These resonances correspond to parasitic resonances of the APA itself. These resonances correspond to parasitic resonances of the APA itself.
They are very close to what was estimated using the FEM: They are very close to what was estimated using the FEM:
- X-bending mode at ~190Hz (Figure [[fig:mode_bending_x_bis]]) - X-bending mode at around 190Hz (Figure [[fig:mode_bending_x_bis]])
- Y-bending mode at ~290Hz (Figure [[fig:mode_bending_y_bis]]) - Y-bending mode at around 290Hz (Figure [[fig:mode_bending_y_bis]])
- Z-torsion mode at ~400Hz (Figure [[fig:mode_torsion_z_bis]]) - Z-torsion mode at around 400Hz (Figure [[fig:mode_torsion_z_bis]])
#+name: fig:mode_bending_x_bis #+name: fig:mode_bending_x_bis
#+caption: X-bending mode (189Hz) #+caption: X-bending mode (189Hz)
@ -2943,7 +2943,11 @@ exportFig('figs/struts_frf_dvf_plant_tf.pdf', 'width', 'wide', 'height', 'tall')
#+RESULTS: #+RESULTS:
[[file:figs/struts_frf_dvf_plant_tf.png]] [[file:figs/struts_frf_dvf_plant_tf.png]]
#+begin_important
Depending on how the APA are mounted with the flexible joints, the dynamics can change a lot as shown in Figure [[fig:struts_frf_dvf_plant_tf]].
In the future, a "pin" will be used to better align the APA with the flexible joints.
We can expect the amplitude of the spurious resonances to decrease.
#+end_important
*** FRF Identification - DVF with interferometer *** FRF Identification - DVF with interferometer
In this section, the dynamics from $V_a$ to $d_a$ is identified. In this section, the dynamics from $V_a$ to $d_a$ is identified.

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