2017
DOI: 10.1155/2017/9837349
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Antidisturbance Vibration Suppression of the Aerial Refueling Hose during the Coupling Process

Abstract: In autonomous aerial refueling (AAR), the vibration of the flexible refueling hose caused by the receiver aircraft's excessive closure speed should be suppressed once it appears. This paper proposed an active control strategy based on the permanent magnet synchronous motor (PMSM) angular control for the timely and accurate vibration suppression of the flexible refueling hose. A nonsingular fast terminal sliding-mode (NFTSM) control scheme with adaptive extended state observer (AESO) is proposed for PMSM take-u… Show more

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Cited by 3 publications
(7 citation statements)
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“…\end{equation}$$Furthermore, xfalse(0false)0$x(0)\ge 0$ and xfalse(T1false)=0$x(T_1) = 0$; then we integrate both sides of Equation (23) to obtain the settling time of the dynamics (20) as: T1badbreak=0false|xfalse(0false)false|k21/η2()x+k1xη11/η2dx.$$\begin{equation} T_1=\int\limits _0^{|x(0)|} \frac{k_2^{1 / \eta _2}}{{\left(x+k_1 x^{\eta _1}\right)}^{1 / \eta _2}} d x. \end{equation}$$To improve the convergence rate of the conventional NFTSM, authors in [40] proposed the following sliding surface: S2badbreak=xgoodbreak+k1xη1goodbreak+k2trueẋη2goodbreak+k3exp()x||xgoodbreak=0,$$\begin{equation} S_2 = x +k_1\left\lceil x\right\rfloor ^{\eta _1}+k_2\left\lceil \dot{x}\right\rfloor ^{\eta _2}+k_3\operatorname{exp}{\left({\left|x\right|}\right)}{\left|x\right|} = 0, \end{equation}$$where k3>0$k_3>0$. The settling time of the dynamics in Equation (25) as: T2badbreak=0false|xfalse(0false)false|k21/η2()false|xfalse|+k1|x|η1+…”
Section: Resultsmentioning
confidence: 99%
“…\end{equation}$$Furthermore, xfalse(0false)0$x(0)\ge 0$ and xfalse(T1false)=0$x(T_1) = 0$; then we integrate both sides of Equation (23) to obtain the settling time of the dynamics (20) as: T1badbreak=0false|xfalse(0false)false|k21/η2()x+k1xη11/η2dx.$$\begin{equation} T_1=\int\limits _0^{|x(0)|} \frac{k_2^{1 / \eta _2}}{{\left(x+k_1 x^{\eta _1}\right)}^{1 / \eta _2}} d x. \end{equation}$$To improve the convergence rate of the conventional NFTSM, authors in [40] proposed the following sliding surface: S2badbreak=xgoodbreak+k1xη1goodbreak+k2trueẋη2goodbreak+k3exp()x||xgoodbreak=0,$$\begin{equation} S_2 = x +k_1\left\lceil x\right\rfloor ^{\eta _1}+k_2\left\lceil \dot{x}\right\rfloor ^{\eta _2}+k_3\operatorname{exp}{\left({\left|x\right|}\right)}{\left|x\right|} = 0, \end{equation}$$where k3>0$k_3>0$. The settling time of the dynamics in Equation (25) as: T2badbreak=0false|xfalse(0false)false|k21/η2()false|xfalse|+k1|x|η1+…”
Section: Resultsmentioning
confidence: 99%
“…To improve the convergence rate of the conventional NFTSM surface [20] proposed the following sliding surface:…”
Section: Improved Nonsingular Fast Terminal Sliding Modementioning
confidence: 99%
“…Thus, due to its remarkable benefits, the NFTSM control scheme gained wide acceptance and application in several nonlinear systems. To further improve the convergence speed of the NFTSM control, authors in [20] added an exponential term on the nonlinear sliding surface of the NFTSM control method. The control scheme was implemented to suppress vibrations in autonomous aerial refuelling.…”
Section: Introductionmentioning
confidence: 99%
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“…Vibration control of the refueling hose has been a widely concerned topic [8][9][10][11]. After being released from the refueling pod, the flexible hose is exposed to the complex air environment and moves along with the tanker.…”
Section: Introductionmentioning
confidence: 99%