Unnumbered conclusion
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		| @@ -144,8 +144,6 @@ Once the system is well damped, a feedback position controller is applied, and t | ||||
|  | ||||
| Two key effects that may limit that positioning performances are then considered: the limited micro-station compliance (Section ref:sec:uniaxial_support_compliance) and the presence of dynamics between the nano-hexapod and the sample's point of interest (Section ref:sec:uniaxial_payload_dynamics). | ||||
|  | ||||
| Conclusion remarks are given in Section ref:sec:uniaxial_conclusion. | ||||
|  | ||||
| #+begin_src latex :file uniaxial_overview_model_sections.pdf | ||||
| \begin{tikzpicture} | ||||
|   % ==================== | ||||
| @@ -6131,9 +6129,12 @@ Having some flexibility between the measurement point and the point of interest | ||||
| It will be therefore important to take special care when designing sampling environments, especially if a soft nano-hexapod is used. | ||||
|  | ||||
| * Conclusion | ||||
| :PROPERTIES: | ||||
| :UNNUMBERED: t | ||||
| :END: | ||||
| <<sec:uniaxial_conclusion>> | ||||
|  | ||||
| # Make a table summarizing the findings | ||||
| # TODO - Make a table summarizing the findings | ||||
|  | ||||
| In this study, a uniaxial model of the nano-active-stabilization-system has been tuned both from dynamical measurements (Section ref:sec:micro_station_model) and from disturbances measurements (Section ref:sec:uniaxial_disturbances). | ||||
|  | ||||
|   | ||||
										
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							| @@ -1,4 +1,4 @@ | ||||
| % Created 2024-04-15 Mon 21:41 | ||||
| % Created 2024-04-16 Tue 09:47 | ||||
| % Intended LaTeX compiler: pdflatex | ||||
| \documentclass[a4paper, 10pt, DIV=12, parskip=full, bibliography=totoc]{scrreprt} | ||||
|  | ||||
| @@ -67,8 +67,6 @@ Once the system is well damped, a feedback position controller is applied, and t | ||||
|  | ||||
| Two key effects that may limit that positioning performances are then considered: the limited micro-station compliance (Section \ref{sec:uniaxial_support_compliance}) and the presence of dynamics between the nano-hexapod and the sample's point of interest (Section \ref{sec:uniaxial_payload_dynamics}). | ||||
|  | ||||
| Conclusion remarks are given in Section \ref{sec:uniaxial_conclusion}. | ||||
|  | ||||
| \begin{figure}[htbp] | ||||
| \centering | ||||
| \includegraphics[scale=1]{figs/uniaxial_overview_model_sections.png} | ||||
| @@ -1197,7 +1195,7 @@ This is why high-bandwidth soft positioning stages are usually restricted to con | ||||
| Having some flexibility between the measurement point and the point of interest (i.e. the sample point to be position on the x-ray) also degrades the position stability as shown in Section \ref{ssec:uniaxial_payload_dynamics_effect_stability}. | ||||
| It will be therefore important to take special care when designing sampling environments, especially if a soft nano-hexapod is used. | ||||
|  | ||||
| \chapter{Conclusion} | ||||
| \chapter*{Conclusion} | ||||
| \label{sec:uniaxial_conclusion} | ||||
|  | ||||
| In this study, a uniaxial model of the nano-active-stabilization-system has been tuned both from dynamical measurements (Section \ref{sec:micro_station_model}) and from disturbances measurements (Section \ref{sec:uniaxial_disturbances}). | ||||
|   | ||||
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