<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">ICA</journal-id><journal-title-group><journal-title>Intelligent Control and Automation</journal-title></journal-title-group><issn pub-type="epub">2153-0653</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ica.2015.61002</article-id><article-id pub-id-type="publisher-id">ICA-53167</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Robust Adaptive Control for a Class of Systems with Deadzone Nonlinearity
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>izar</surname><given-names>J. Ahmad</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mahmud</surname><given-names>J. Alnaser</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ebraheem</surname><given-names>Sultan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Khuloud</surname><given-names>A. Alhendi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Faculty of Electronic Engineering Technology, College of Technological Studies, The Public Authority for Applied Education and Training (PAAET), Kuwait City, Kuwait</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>nj.ahmad@paaet.edu.kw(IJA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>13</day><month>01</month><year>2015</year></pub-date><volume>06</volume><issue>01</issue><fpage>10</fpage><lpage>19</lpage><history><date date-type="received"><day>15</day>	<month>November</month>	<year>2014</year></date><date date-type="rev-recd"><day>accepted</day>	<month>29</month>	<year>December</year>	</date><date date-type="accepted"><day>13</day>	<month>January</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  This paper presents a robust adaptive control scheme for a class of continuous-time linear systems with unknown non-smooth asymmetrical deadzone nonlinearity at the input of the plant. The methodology is applied to handle input deadzone as well as unmeasurable disturbances simultaneously in strictly matched systems. The proposed controller robustly cancels any residual distortion caused by the inaccurate deadzone cancellation scheme. The scheme is shown to successfully cancel the deadzone’s deleterious effect as well as eliminate other unmeasurable disturbances within the span of the input. The new controller ensures the global stability of all states and adaptations, and achieves asymptotic tracking. The asymptotic stability of the closed-loop system is proven by Lyapunov arguments, and simulation results confirm the efficacy of the control methodology. 
 
</p></abstract><kwd-group><kwd>Adaptive Control</kwd><kwd> Non-Symmetric Deadzone</kwd><kwd> Hard Nonlinearity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The significance of the deadzone problem lies in the fact that it affects many physical and practical systems. Examples of such systems are the ones containing hydraulic or pneumatic values, electronic circuits and devices, temperature regulation circuits, and in actuators such as servo valves and DC motors. In most cases, the pa- rameters of the deadzone nonlinearity are unknown and continuously varying with time and temperature. Deadzones exist in a number of industrial applications specially the ones requiring high precision such as medical robots, semiconductor manufacturing, and precision machine tools. It has been shown that deadzone in actuators, such as hydraulic servo-valves, gives rise to limit cycling and instability. The advances reached in the area of adaptive compensation and control theory gave rise to increased interest in handling the deadzone problem. There have been many techniques that addressed the problem and have been shown to reduce if not eliminate the degradation of system performance resulting in an improved tracking accuracy and ensured stabilization of such systems.</p><p>One sensible approach to counter the effect of the deadzone, shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, was presented by [<xref ref-type="bibr" rid="scirp.53167-ref1">1</xref>] which involved designing an inverse deadzone function to cancel its effect. The approach of designing an inverse adaptive deadzone compensator was thoroughly investigated in [<xref ref-type="bibr" rid="scirp.53167-ref2">2</xref>] and [<xref ref-type="bibr" rid="scirp.53167-ref3">3</xref>] which was shown to improve per- formance. Lewis et al. in [<xref ref-type="bibr" rid="scirp.53167-ref4">4</xref>] proposed a fuzzy logic type inverse deadzone compensator, meanwhile, a neural network inverse compensator was designed in [<xref ref-type="bibr" rid="scirp.53167-ref5">5</xref>] . Both approaches show clear improvement in reducing the tracking error. In [<xref ref-type="bibr" rid="scirp.53167-ref6">6</xref>] , a new adaptive controller of linear or nonlinear systems with deadzone is introduced with- out constructing a deadzone inverse. Global and asymptotic tracking was achieved and simulation results were presented.</p><p>An adaptive sliding mode control scheme used to offset a non-symmetrical deadzone nonlinearity in continu- ous time was presented in [<xref ref-type="bibr" rid="scirp.53167-ref7">7</xref>] . The problem of chattering inherent with sliding mode control is handled by al- lowing a small controlled tracking error.</p><p>In recent years, many researchers addressed the deadzone problem with encouraging results. In [<xref ref-type="bibr" rid="scirp.53167-ref8">8</xref>] , a novel function was introduced to describe deadzone nonlinearity. To show the effectiveness of the proposed equivalent function the authors combined it with vibration of a cantilever beam.</p><p>In this paper we are motivated by the success of our earlier results deadzone compensation of DC motor pre- sented in [<xref ref-type="bibr" rid="scirp.53167-ref9">9</xref>] and [<xref ref-type="bibr" rid="scirp.53167-ref10">10</xref>] . The extension involves combining the deadzone for a class of linear systems with uncer- tainties in the span of the input. The uncertainties are assumed to be bounded by a p<sup>th</sup> order polynomial in the state of the system. A robust adaptive controller will compensate for the unmeasurable disturbances as well as any mismatch error in estimating the deadzone parameters. The proposed method does not require any know- ledge of the deadzone parameters or the specialized design of an inverse deadzone controller and only an upper bound of the deadzone spacing which is easily determined a priori.</p></sec><sec id="s2"><title>2. The Problem Setup: Dynamics of a Non-Symmetrical Deadzone Nonlinearity</title><p>A common representation of a non-symmetrical deadzone nonlinearity, shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, described in [<xref ref-type="bibr" rid="scirp.53167-ref1">1</xref>] as follows</p><disp-formula id="scirp.53167-formula730"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x7.png" xlink:type="simple"/></inline-formula> denotes the output of deadzone function preceding a plant input, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x8.png" xlink:type="simple"/></inline-formula>is the slope of the lines, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x9.png" xlink:type="simple"/></inline-formula>is the width of the deadzone distance, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x10.png" xlink:type="simple"/></inline-formula> is the input of the deadzone block as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. A more convenient representation of a non-symmetrical deadzone was presented in [<xref ref-type="bibr" rid="scirp.53167-ref6">6</xref>] as</p><disp-formula id="scirp.53167-formula731"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x11.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x12.png" xlink:type="simple"/></inline-formula> represents a non-symmetrical saturation function given by</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Non-symmetric deadzone nonlinearity at the input of a linear plant</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x13.png"/></fig><disp-formula id="scirp.53167-formula732"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x14.png"  xlink:type="simple"/></disp-formula><p>A novel representation for (2) was presented in [<xref ref-type="bibr" rid="scirp.53167-ref11">11</xref>] for an exact symmetrical deadzone by defining <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x15.png" xlink:type="simple"/></inline-formula> as the deadzone spacing function as</p><disp-formula id="scirp.53167-formula733"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x16.png"  xlink:type="simple"/></disp-formula><p>Consequently, the saturation function can be written as</p><disp-formula id="scirp.53167-formula734"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x17.png"  xlink:type="simple"/></disp-formula><p>In most applications the deadzone parameters are unknown or time and temperature varying. Instead, for de- veloping an inverse deadzone function as in [<xref ref-type="bibr" rid="scirp.53167-ref9">9</xref>] , we advocate a robust adaptive compensator that handles the variability of the deadzone parameters as part of an input disturbance. However, we outline some necessary and reasonable assumptions to be used in the proof of the efficacy of the proposed control methodology:</p><p>(A1) The deadzone parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x18.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x19.png" xlink:type="simple"/></inline-formula>.</p><p>(A2) The deadzone parameters<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x20.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x21.png" xlink:type="simple"/></inline-formula> are bounded as follows:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x22.png" xlink:type="simple"/></inline-formula>and.</p><p>(A3) Without any loss of generality, the slope of the deadzone <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x24.png" xlink:type="simple"/></inline-formula> is positive and is set to 1.</p><p>(A4) The output of the deadzone block <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x25.png" xlink:type="simple"/></inline-formula> is not available for measurement.</p><p>Remark 1. Assumptions (A1) and (A2) are the actual physical attributes of a real industrial deadzone and is adopted in the literature [<xref ref-type="bibr" rid="scirp.53167-ref6">6</xref>] . Therefore, the saturation function given by (4) can be shown to have an upper bound by closely analysing Equation (5). Using the general inequality rule <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x26.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.53167-formula735"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x27.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53167-formula736"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x28.png"  xlink:type="simple"/></disp-formula><p>From Equations (6) from (7) we can state</p><disp-formula id="scirp.53167-formula737"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x29.png"  xlink:type="simple"/></disp-formula><p>Multiplying by the slope <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x30.png" xlink:type="simple"/></inline-formula> gives</p><disp-formula id="scirp.53167-formula738"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x31.png"  xlink:type="simple"/></disp-formula><p>The left hand side of (9) is the saturation function given by (5). In case of a non-symmetrical deadzone func- tion the upper-bound may be chosen by employing assumption (A2) as follows</p><disp-formula id="scirp.53167-formula739"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x32.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.53167-formula740"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x33.png"  xlink:type="simple"/></disp-formula><p>The upper bounds will play a pivotal role to ensure the overall global stability of the close loop dynamics as will be demonstrated in the following section.</p></sec><sec id="s3"><title>3. Robust Adaptive Controller Design</title><p>Considering the following nonlinear system with input deadzone nonlinearity described as</p><disp-formula id="scirp.53167-formula741"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x34.png"  xlink:type="simple"/></disp-formula><p>where the matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x35.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x36.png" xlink:type="simple"/></inline-formula> are given by</p><disp-formula id="scirp.53167-formula742"><graphic  xlink:href="http://html.scirp.org/file/2-7900370x37.png"  xlink:type="simple"/></disp-formula><p>And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x38.png" xlink:type="simple"/></inline-formula> represents the unmeasurable disturbance. The collective bounds can be expressed as</p><disp-formula id="scirp.53167-formula743"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x39.png"  xlink:type="simple"/></disp-formula><p>Let the reference model to be tracked given by</p><disp-formula id="scirp.53167-formula744"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x40.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x41.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x42.png" xlink:type="simple"/></inline-formula> is a reference signal. The tracking error dynamics <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x43.png" xlink:type="simple"/></inline-formula> may be written as fol- lows:</p><disp-formula id="scirp.53167-formula745"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x44.png"  xlink:type="simple"/></disp-formula><p>Inserting the deadzone equation (2) into (15) yields</p><disp-formula id="scirp.53167-formula746"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x45.png"  xlink:type="simple"/></disp-formula><p>Therefore, for the class of systems described in (13) and deadzone given in (7), we use the result stated as Lemma RANDM in [<xref ref-type="bibr" rid="scirp.53167-ref12">12</xref>] and modify it to ensure asymptotic convergence. The modified controller is</p><disp-formula id="scirp.53167-formula747"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x46.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x47.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x48.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x50.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x51.png" xlink:type="simple"/></inline-formula> is the positive definite symmetric solution of the Algebraic Riccati equation (ARE). The adaptation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x52.png" xlink:type="simple"/></inline-formula> is used to ensure robustness of the controller. The combined output of the com- pensator and the deadzone nonlinearity may be written as</p><disp-formula id="scirp.53167-formula748"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x53.png"  xlink:type="simple"/></disp-formula><p>Inserting the proposed control laws (17) and the output of the deadzone block given by Equation (18) into the error dynamics (16) results in the closed loop dynamics</p><disp-formula id="scirp.53167-formula749"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x54.png"  xlink:type="simple"/></disp-formula><p>The adaptation law for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x55.png" xlink:type="simple"/></inline-formula> given by</p><disp-formula id="scirp.53167-formula750"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x56.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x57.png" xlink:type="simple"/></inline-formula> is a constant scalar.</p><p>Theorem. For the plant described by (12) with input deadzone (1), and the robust adaptive control law (17) along with the adaptive update law (20) will ensure the closed-loop stability and boundedness of tracking error, hence reducing the effects of deadzone.</p><p>Proof. Using the following positive definite control Lyapunov function</p><disp-formula id="scirp.53167-formula751"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x58.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x59.png" xlink:type="simple"/></inline-formula> differentiating along the trajectories of the system yields</p><disp-formula id="scirp.53167-formula752"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x60.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53167-formula753"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x61.png"  xlink:type="simple"/></disp-formula><p>Substituting for the closed loop dynamics given by (19) in (23) gives</p><disp-formula id="scirp.53167-formula754"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x62.png"  xlink:type="simple"/></disp-formula><p>Collecting terms and simplifying</p><disp-formula id="scirp.53167-formula755"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x63.png"  xlink:type="simple"/></disp-formula><p>Rearranging terms we get</p><disp-formula id="scirp.53167-formula756"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x64.png"  xlink:type="simple"/></disp-formula><p>The first term can be simplified by solving the Algebraic Reccati Equation given by</p><disp-formula id="scirp.53167-formula757"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x65.png"  xlink:type="simple"/></disp-formula><p>resulting in</p><disp-formula id="scirp.53167-formula758"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x66.png"  xlink:type="simple"/></disp-formula><p>Replacing the adaptation law (20) and replacing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x67.png" xlink:type="simple"/></inline-formula> in (28) yields</p><disp-formula id="scirp.53167-formula759"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x68.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53167-formula760"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x69.png"  xlink:type="simple"/></disp-formula><p>So far the first two terms are negative. As for the third term we utilize the general inequality <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x70.png" xlink:type="simple"/></inline-formula> to establish proper bounds as follows</p><disp-formula id="scirp.53167-formula761"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x71.png"  xlink:type="simple"/></disp-formula><p>Using the inequality (13) to modify (31) to become</p><disp-formula id="scirp.53167-formula762"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x72.png"  xlink:type="simple"/></disp-formula><p>Therefore, the inequality of (32) can be incorporated in (30) as</p><disp-formula id="scirp.53167-formula763"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x73.png"  xlink:type="simple"/></disp-formula><p>By choosing the degree of freedom <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x74.png" xlink:type="simple"/></inline-formula> satisfying the condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x75.png" xlink:type="simple"/></inline-formula> and choosing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x76.png" xlink:type="simple"/></inline-formula> to be great-</p><p>er than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x77.png" xlink:type="simple"/></inline-formula> ensures that the first three terms of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x78.png" xlink:type="simple"/></inline-formula> negative. Meanwhile, the last term in (33) can be upper bounded as follow</p><disp-formula id="scirp.53167-formula764"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x79.png"  xlink:type="simple"/></disp-formula><p>Utilizing the upper bounds on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x80.png" xlink:type="simple"/></inline-formula> given by (10) and rewriting the right hand side of (34)</p><disp-formula id="scirp.53167-formula765"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x81.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x82.png" xlink:type="simple"/></inline-formula>.Therefore the last term in (35) insures that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x83.png" xlink:type="simple"/></inline-formula> as long as</p><disp-formula id="scirp.53167-formula766"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x84.png"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.53167-formula767"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x85.png"  xlink:type="simple"/></disp-formula><p>To conclude, by choosing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x86.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x87.png" xlink:type="simple"/></inline-formula> is rendered negative and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x88.png" xlink:type="simple"/></inline-formula> converges to a closed and vanishing region as time increases. Therefore, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x89.png" xlink:type="simple"/></inline-formula> as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x90.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x91.png" xlink:type="simple"/></inline-formula></p><p>implies that by choosing the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x92.png" xlink:type="simple"/></inline-formula> vector as the coefficient of a strictly Hurwitz polynomial will make the closed loop system error asymptotically stable. For a more through conclusion of the proof one may refer to [<xref ref-type="bibr" rid="scirp.53167-ref13">13</xref>] .</p></sec><sec id="s4"><title>4. Illustrative Example</title><p>In this section, we illustrate the proposed controller to compensate for a system with a deadzone nonlinearity presented in [<xref ref-type="bibr" rid="scirp.53167-ref14">14</xref>] as</p><disp-formula id="scirp.53167-formula768"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x93.png"  xlink:type="simple"/></disp-formula><p>The parameter used for the simulation is shown in <xref ref-type="table" rid="table1">Table 1</xref>. The plant (41) may be written in state space form by defining <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x94.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x95.png" xlink:type="simple"/></inline-formula> then</p><disp-formula id="scirp.53167-formula769"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x96.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53167-formula770"><graphic  xlink:href="http://html.scirp.org/file/2-7900370x97.png"  xlink:type="simple"/></disp-formula><p>Resulting in</p><disp-formula id="scirp.53167-formula771"><graphic  xlink:href="http://html.scirp.org/file/2-7900370x98.png"  xlink:type="simple"/></disp-formula><p>The solution of the ARE equation was chosen to be</p><disp-formula id="scirp.53167-formula772"><graphic  xlink:href="http://html.scirp.org/file/2-7900370x99.png"  xlink:type="simple"/></disp-formula><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Parameters utilized in the example</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Item</th><th align="center" valign="middle"  colspan="3"  >Systems Physical Attributes</th></tr></thead><tr><td align="center" valign="middle" >Parameter</td><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >Unit</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x100.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >40.0</td><td align="center" valign="middle" >PD Gain</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x101.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >13.0</td><td align="center" valign="middle" >PD gain</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x102.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >20.0</td><td align="center" valign="middle" >Deadzone Right</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x103.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >15.0</td><td align="center" valign="middle" >Deadzone Left</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x104.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >10.0</td><td align="center" valign="middle" >Gains</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x105.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >Scalars</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x106.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >4.0</td><td align="center" valign="middle" >Gain</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x107.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >Gain</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x108.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >Scalars</td></tr></tbody></table></table-wrap><p>The reference model to be tracked is</p><disp-formula id="scirp.53167-formula773"><graphic  xlink:href="http://html.scirp.org/file/2-7900370x109.png"  xlink:type="simple"/></disp-formula><p>for a sinusoidal reference trajectory given by</p><disp-formula id="scirp.53167-formula774"><graphic  xlink:href="http://html.scirp.org/file/2-7900370x110.png"  xlink:type="simple"/></disp-formula><p>Meanwhile, the unmeasurable disturbance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x111.png" xlink:type="simple"/></inline-formula> can be collectively bounded as</p><disp-formula id="scirp.53167-formula775"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7900370x112.png"  xlink:type="simple"/></disp-formula><p>Simulations of the system in (39) under the adaptive control law (17) and (20) have been performed. The up- per bounds on actuator actual spacing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x113.png" xlink:type="simple"/></inline-formula> is assumed unknown. In order to demonstrate the performance improvement accomplished by our proposed method, the system under test given in (39) was used. The efficacy of the proposed method is proven by comparing its performance against the performance of a clas- sic PD controller having equivalent gains. The complete parameters of the system under test and controller gains are listed in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The simulation results presented in <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref>, clearly show the tracking performance for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x114.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x115.png" xlink:type="simple"/></inline-formula> states along with their respective reference trajectory. <xref ref-type="fig" rid="fig4">Figure 4</xref> and <xref ref-type="fig" rid="fig5">Figure 5</xref> demonstrate the tracking error for the states <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x116.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x117.png" xlink:type="simple"/></inline-formula> in blue in addition to the same tracking errors for the system under a PD con- troller in red. In both figures, the PD controller resulted in limit cycles where as the adaptive controller proved to be stable with no limit cycles and improved performance with a zero approaching tracking error. <xref ref-type="fig" rid="fig6">Figure 6</xref> shows the control effort <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x118.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x119.png" xlink:type="simple"/></inline-formula>. In <xref ref-type="fig" rid="fig7">Figure 7</xref> the evolution of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x120.png" xlink:type="simple"/></inline-formula> which clearly demonstrates the boundedness of the adaptation. In <xref ref-type="fig" rid="fig8">Figure 8</xref>, the reference trajectory is changed to demonstrates a superior a step response performance when compared with PD controller. While the step error is approaching zero for the system under the proposed adaptive controller, a steady state error is persistent with the PD controller.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The tracking performance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x122.png" xlink:type="simple"/></inline-formula> state of the system under the proposed robust controller</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x121.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The tracking performance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x124.png" xlink:type="simple"/></inline-formula> state of the system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x123.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The adaptively compensated tracking error <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x126.png" xlink:type="simple"/></inline-formula> (blue) vs. the same tracking error of the system under a PD controller (red)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x125.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The adaptively compensated tracking error <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x128.png" xlink:type="simple"/></inline-formula> (blue) vs. the same tracking error of the system under a PD controller (red)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x127.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> The control effort <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x130.png" xlink:type="simple"/></inline-formula> in red vs. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x131.png" xlink:type="simple"/></inline-formula>for the deadzone compensated system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x129.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Evolution of the adaptation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x133.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x132.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Step tracking performance error for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x135.png" xlink:type="simple"/></inline-formula> for input<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7900370x136.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7900370x134.png"/></fig></sec><sec id="s5"><title>5. Conclusion</title><p>A robust adaptive controller is used to control a class of nonlinear systems with input deadzone nonlinearity at the input. The robust controller was shown to be superior in performance when compared to a more conventional control method such as a PD controller. The system under the proposed scheme has been shown to not only ef- fectively stabilize a second order complex nonlinear system with disturbance, but also achieve asymptotic tracking. The advantage of the proposed method lies in the fact that no knowledge of the deadzone parameters needed and only an upper bound for the deadzone spacing is required. The adaptive deadzone inverse controller is smoothly differentiable and can easily be combined with any of the advanced control methodologies. The asymptotic stability of the closed-loop system has been proven by using Lyapunov arguments and simulation results confirmed the efficacy of the control methodology.</p></sec><sec id="s6"><title>Funding</title><p>This work is supported and funded by the Public Authority of Applied Education and Training, Research Project No. (TS-14-03) t, Research Title (Adaptive Control of Systems with Output Deadzone).</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.53167-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Recker, D.A. and Kokotovic, P.V. (1993) Indirect Adaptive Nonlinear Control of Discrete-Time Systems Containing a Deadzone. Proceedings of the 32nd Conference on Decision and Control, 15-17 December 1993, San Antonio, 2647, 2653.</mixed-citation></ref><ref id="scirp.53167-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Toa, G. and Kokotovic, P. 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