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test-bench-nano-hexapod.org
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@ -553,7 +553,7 @@ The effect of the payload mass on the dynamics is discussed in Section ref:ssec:
\draw[->] ($(F_DAC.west)+(-0.8,0)$) node[above right]{$\mathbf{u}$} node[below right]{$[V]$} -- node[sloped]{$/$} (F_DAC.west);
\draw[->] (F_DAC.east) -- node[midway, above]{$\tilde{\mathbf{u}}$}node[midway, below]{$[V]$} (PD200.west);
\draw[->] (PD200.east) -- node[midway, above]{$\mathbf{V}_a$}node[midway, below]{$[V]$} (F_stack.west);
\draw[->] (F_stack.east) -- (inputF) node[above left]{$\mathbf{f}$}node[below left]{$[N]$};
\draw[->] (F_stack.east) -- (inputF) node[above left]{$\mathbf{\tau}$}node[below left]{$[N]$};
\draw[->] (outputF) -- (Fm_stack.west) node[above left]{$\mathbf{\epsilon}$} node[below left]{$[m]$};
\draw[->] (Fm_stack.east) -- node[midway, above]{$\tilde{\mathbf{V}}_s$}node[midway, below]{$[V]$} (Fm_ADC.west);
@ -1011,7 +1011,7 @@ xlim([10, 2e3]);
exportFig('figs/test_nhexa_identified_frf_Vs_masses.pdf', 'width', 'half', 'height', 600);
#+end_src
#+name: fig:test_nhexa_identified_frf_masses
#+name: fig:test_struts_mounting
#+caption: Measured Frequency Response Functions from $u_i$ to $d_{ei}$ (\subref{fig:test_nhexa_identified_frf_de_masses}) and from $u_i$ to $V_{si}$ (\subref{fig:test_nhexa_identified_frf_Vs_masses}) for all 4 payload conditions. Only diagonal terms are shown.
#+attr_latex: :options [htbp]
#+begin_figure

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test-bench-nano-hexapod.pdf
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