2012 IEEE 51st IEEE Conference on Decision and Control (CDC) 2012
DOI: 10.1109/cdc.2012.6426406
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A continuous extension of the LuGre friction model with application to the control of a pneumatic servo positioner

Abstract: This work presents a novel continuous approximation of the LuGre model, with the aim of improving its applicability in the control of a class of systems that include fluid-driven servo positioners. The main attractive of the proposed approximation is the preservation of the properties of boundedness and passivity that are inherent to the original LuGre model, a feature that is not guaranteed in the approximate models that are usually encountered in the specialized literature. The most relevant properties of th… Show more

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Cited by 6 publications
(7 citation statements)
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“…We introduce S u = 2 π arctan(K u U[n]) and define it as a smoothness coefficient based on the inverse trigonometric function. In order to obtain a MLM of the continuum type and maintain its own model structure, we introduced (24) to obtain the MLM with reference to [34] and verified its effectiveness in improving the model's stability with simulation experiments. The expressions of MLM in the discrete time domain are as follows:…”
Section: Improvement Of Model Stabilitymentioning
confidence: 99%
“…We introduce S u = 2 π arctan(K u U[n]) and define it as a smoothness coefficient based on the inverse trigonometric function. In order to obtain a MLM of the continuum type and maintain its own model structure, we introduced (24) to obtain the MLM with reference to [34] and verified its effectiveness in improving the model's stability with simulation experiments. The expressions of MLM in the discrete time domain are as follows:…”
Section: Improvement Of Model Stabilitymentioning
confidence: 99%
“…However, this model contains discontinuous terms in its original form, which cannot be resolved for certain classes of systems or controllers that require the time derivative of the estimated friction force. The continuous extension of the LuGre model proposed in solves this problem by introducing continuous and differentiable approximations of the discontinuous terms, such that the passivity and boundedness of the internal states are not affected. This model is represented by the following equations, alignedrightż left= S1ω αMathClass-open(ωMathClass-close)S2z, right rightF left= σoz + σ1ż+ σ2S1ω, rightαMathClass-open(ωMathClass-close)left= 1 FC + FS FCeω xs2 , where z is the friction state, x S is the Stribeck velocity, and F S and F C are the static friction and dynamic friction forces, respectively.…”
Section: Problem Formulationmentioning
confidence: 99%
“…Remark We note that according to LuGre model, the dynamics of z are given by leftalign-star rightalign-oddż = ω αMathClass-open(ωMathClass-close)|ω|z. align-even rightalign-label In , the authors propose first : | ω | = ω × sign ( ω ) ≈ S 0 ( ω ) ω , with S 0 ( ω ) = tanh( k v ω ) and k v > 0. This implies the following dynamics of z leftalign-star rightalign-oddż = ω ω ×αMathClass-open(ωMathClass-close)S0MathClass-open(ωMathClass-close)z. align-even rightalign-label to obtain a nontrivial equilibrium condition z(t) MathClass-rel= 1 α(ω)S0(ω) MathClass-rel→MathClass-rel∞MathClass-punc,when ω MathClass-rel→0MathClass-punc. In order to solve this problem, the following dynamics have been proposed leftalign-star rightalign-oddż align-even = S1ω αMathClass-open(ωMathClass-close)S2z rightalign-label align-label As in , we propose to introduce the term S 1 in friction force F leftalign-star rightalign-oddF = σoz + σ1ż+ σ2ω align-even rightalign-label to obtain …”
Section: Problem Formulationmentioning
confidence: 99%
“…The modeling of pneumatic servo systems is discussed in many different works [1,2,5]. The model used in this work is developed in detail in [7,8]. Essentially, the system consists of a pressure source, a piston and correspondent load, and a servovalve.…”
Section: Mathematical Modelmentioning
confidence: 99%
“…where M is the mass of the piston-load assembly, y is the acceleration of the piston, f is the friction force, A is the cylinder cross-sectional area, and 1 p and 2 p are the pressures in the two chambers. The friction force is represented by means of a continuous approximation of the LuGre model [8,9], which is largely employed in control applications [2,8,10,11]. The approximation used in this work was developed specifically for systems where the control signal affects the time derivative of the developed mechanical forces, such as hydraulic and pneumatic actuators [1,2,3,5,6,8].…”
Section: Mathematical Modelmentioning
confidence: 99%