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@ -566,6 +566,8 @@ While having very different implementations, both proposed modifications are ver
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Future work will focus on the experimental validation of the proposed active damping techniques.
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The Matlab code that was used for this study is available under a MIT License and archived in Zenodo cite:dehaeze20_activ_dampin_rotat_posit_platf.
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* Acknowledgment
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:PROPERTIES:
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:UNNUMBERED: t
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paper/paper.pdf
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paper/paper.pdf
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@ -1,4 +1,4 @@
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% Created 2020-07-08 mer. 18:02
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% Created 2020-07-08 mer. 18:07
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% Intended LaTeX compiler: pdflatex
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\documentclass{ISMA_USD2020}
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\usepackage[utf8]{inputenc}
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@ -58,7 +58,7 @@ The results reveal that, despite their different implementations, both modified
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}
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\section{Introduction}
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\label{sec:org639dbba}
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\label{sec:orgc580a8f}
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\label{sec:introduction}
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There is an increasing need to reduce the undesirable vibration of many sensitive equipment.
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A common method to reduce vibration is to mount the sensitive equipment on a suspended platform which attenuates the vibrations above the frequency of the suspension modes.
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@ -78,7 +78,7 @@ Section \ref{sec:iff_kp} proposes to add springs in parallel with the force sens
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Section \ref{sec:comparison} compares both proposed modifications to the classical IFF in terms of damping authority and closed-loop system behavior.
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\section{Dynamics of Rotating Platforms}
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\label{sec:orgea844f7}
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\label{sec:orgf7cef1f}
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\label{sec:dynamics}
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In order to study how the rotation does affect the use of IFF, a model of a suspended platform on top of a rotating stage is used.
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Figure \ref{fig:system} represents the model schematically which is the simplest in which gyroscopic forces can be studied.
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@ -225,7 +225,7 @@ For \(\Omega > \omega_0\), the low frequency pair of complex conjugate poles \(p
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\end{figure}
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\section{Decentralized Integral Force Feedback}
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\label{sec:org7bfaed6}
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\label{sec:orgcb8c9c7}
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\label{sec:iff}
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In order to apply IFF to the system, force sensors are added in series with the two actuators (Figure \ref{fig:system_iff}).
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As this study focuses on decentralized control, two identical controllers \(K_F\) are used to feedback each of the sensed force to its associated actuator and no attempt is made to counteract the interactions in the system.
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@ -322,7 +322,7 @@ In order to apply Decentralized IFF on rotating platforms, two solutions are pro
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The first one consists of slightly modifying the control law (Section \ref{sec:iff_hpf}) while the second one consists of adding springs in parallel with the force sensors (Section \ref{sec:iff_kp}).
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\section{Integral Force Feedback with High Pass Filter}
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\label{sec:org380bd8d}
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\label{sec:org0b913ec}
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\label{sec:iff_hpf}
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As was explained in the previous section, the instability comes in part from the high gain at low frequency caused by the pure integrators.
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@ -393,7 +393,7 @@ Three regions can be observed:
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\end{itemize}
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\section{Integral Force Feedback with Parallel Springs}
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\label{sec:org93348b6}
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\label{sec:org082b3c2}
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\label{sec:iff_kp}
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In this section additional springs in parallel with the force sensors are added to counteract the negative stiffness induced by the rotation.
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Such springs are schematically shown in Figure \ref{fig:system_parallel_springs} where \(k_a\) is the stiffness of the actuator and \(k_p\) the stiffness in parallel with the actuator and force sensor.
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@ -494,7 +494,7 @@ This is confirmed in Figure \ref{fig:mod_iff_damping_kp} where the attainable cl
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\end{minipage}
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\section{Comparison and Discussion}
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\label{sec:org5f56e74}
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\label{sec:org1f46ad4}
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\label{sec:comparison}
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Two modifications to adapt the IFF control strategy to rotating platforms have been proposed in Sections \ref{sec:iff_hpf} and \ref{sec:iff_kp}.
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These two methods are now compared in terms of added damping, closed-loop compliance and transmissibility.
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@ -554,7 +554,7 @@ On can see in Figure \ref{fig:comp_transmissibility} that the problem of the deg
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The addition of the HPF or the use of the parallel stiffness permit to limit the degradation of the compliance as compared with classical IFF (Figure \ref{fig:comp_compliance}).
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\section{Conclusion}
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\label{sec:org6ee721e}
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\label{sec:org071db57}
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\label{sec:conclusion}
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Due to gyroscopic effects, decentralized IFF with pure integrators was shown not to be stable when applied to rotating platforms.
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@ -572,8 +572,10 @@ While having very different implementations, both proposed modifications are ver
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Future work will focus on the experimental validation of the proposed active damping techniques.
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The Matlab code that was used for this study is available under a MIT License and archived in Zenodo \cite{dehaeze20_activ_dampin_rotat_posit_platf}.
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\section*{Acknowledgment}
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\label{sec:orgd2f72ff}
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\label{sec:orgd8daf24}
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This research benefited from a FRIA grant from the French Community of Belgium.
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\bibliography{ref.bib}
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