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mat/conf_log.mat
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@ -325,19 +325,19 @@ And we save the obtained data.
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figure;
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ax1 = subplot(2, 3, 1);
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hold on;
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plot(scans_rz_align_dist.Em.Eg.Time, scans_rz_align_dist.Em.Eg.Data(:, 1))
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plot(scans_rz_align_dist.Em.En.Time, scans_rz_align_dist.Em.En.Data(:, 1))
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hold off;
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ylabel('Displacement $\epsilon_x$ [m]');
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ax2 = subplot(2, 3, 2);
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hold on;
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plot(scans_rz_align_dist.Em.Eg.Time, scans_rz_align_dist.Em.Eg.Data(:, 2))
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plot(scans_rz_align_dist.Em.En.Time, scans_rz_align_dist.Em.En.Data(:, 2))
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hold off;
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ylabel('Displacement $\epsilon_y$ [m]');
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ax3 = subplot(2, 3, 3);
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hold on;
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plot(scans_rz_align_dist.Em.Eg.Time, scans_rz_align_dist.Em.Eg.Data(:, 3))
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plot(scans_rz_align_dist.Em.En.Time, scans_rz_align_dist.Em.En.Data(:, 3))
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hold off;
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ylabel('Displacement $\epsilon_z$ [m]');
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@ -1429,6 +1429,7 @@ exportFig('figs/opt_stiff_hac_dvf_L_act_stroke.pdf', 'width', 'full', 'height',
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#+end_important
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* Further More complex simulations
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** Introduction :ignore:
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** Simulation with Micro-Hexapod Offset
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*** Simulation
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The micro-hexapod is inducing a 10mm offset of the sample center of mass with the rotation axis.
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@ -427,7 +427,7 @@ And we obtain
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&= \frac{m^\prime s^2 + c^\prime s + k^\prime}{(ms^2 + cs + k) (m^\prime s^2 + c^\prime s + k^\prime) + m^\prime s^2 (c^\prime s + k)}
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\end{align*}
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Which is the same transfer function that was obtained in section [[sec:introductory_example]] (Eq. [[eq:plant_simple_system]]).
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Which is the same transfer function that was obtained in section [[sec:introductory_example]] (Eq. eqref:eq:plant_simple_system).
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The impedance of the mass-spring-damper system is shown in Figure [[fig:example_impedance_mass_spring_damper]].
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- Before the resonance frequency $\omega_0^\prime$, the impedance follows the mass line
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@ -392,7 +392,7 @@ In order to verify that the formula is correct, let's take the same mass-spring-
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And we obtain
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\[ \frac{x}{F} = \frac{m^\prime s^2 + c^\prime s + k^\prime}{(ms^2 + cs + k)(m^\prime s^2 + c^\prime s + k^\prime) + ms^2(cs + k)} \]
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Which is the same transfer function that was obtained in section [[sec:introductory_example]] (Eq. [[eq:plant_simple_system]]).
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Which is the same transfer function that was obtained in section [[sec:introductory_example]] (Eq. eqref:eq:plant_simple_system).
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** Matlab Init :noexport:ignore:
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#+begin_src matlab :tangle no :exports none :results silent :noweb yes :var current_dir=(file-name-directory buffer-file-name)
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18
readme.org
18
readme.org
@ -4,21 +4,3 @@
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#+OPTIONS: num:nil toc:nil todo:nil
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The goal of this project is to study the Nano-Active-Stabilization-System concept using Matlab/Simscape.
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#+begin_src emacs-lisp :tangle no
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(setq org-publish-project-alist
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'(("nass-simscape"
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:base-directory "~/Cloud/thesis/matlab/nass-simscape/org/"
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:base-extension "org"
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:publishing-directory "~/Cloud/thesis/matlab/nass-simscape/docs/"
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:author "Dehaeze Thomas"
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:email "dehaeze.thomas@gmail.com/"
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:recursive nil
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:publishing-function org-html-publish-to-html
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:auto-preamble t
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:auto-sitemap nil
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:with-todo-keywords nil
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:html-wrap-src-lines nil
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:table-of-contents nil)
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))
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#+end_src
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