<?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.2012.34038</article-id><article-id pub-id-type="publisher-id">ICA-24866</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></subj-group></article-categories><title-group><article-title>
 
 
  Adaptive Force Control of in Web Handling Systems
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ndrew</surname><given-names>Kadik</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>Wilson</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Control Engineering, Lakehead University, Thunder Bay, Canada</addr-line></aff><aff id="aff2"><addr-line>Mechanical Engineering, Lakehead University, Thunder Bay, Canada</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>akadik@lakeheadu.ca(NK)</email>;<email>wwang3@lakeheadu.ca(WW)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>28</day><month>11</month><year>2012</year></pub-date><volume>03</volume><issue>04</issue><fpage>329</fpage><lpage>336</lpage><history><date date-type="received"><day>June</day>	<month>17,</month>	<year>2012</year></date><date date-type="rev-recd"><day>July</day>	<month>16,</month>	<year>2012</year>	</date><date date-type="accepted"><day>July</day>	<month>24,</month>	<year>2012</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>
 
 
  Winding/unwinding system control is a very important issue to web handling machines. In this paper, a novel adaptive 
  H<sub>∞</sub> control strategy is developed for winding process control. A gain scheduling scheme is proposed based on a neural fuzzy approximator to improve the transient response and enhance tension control; the controller’s convergence and adaptive capability can be further improved by an efficient hybrid training algorithm. The effectiveness of the proposed adaptive 
  H<sub>∞</sub> control is verified by experimental tests. Test results show that the developed gain approximator can adaptively accommodate parameter variations in the system and improve the control performance.
 
</p></abstract><kwd-group><kwd>Web Tension Control; Neural Fuzzy Approximator; Gain Scheduling; Winding/Unwinding Systems</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The term “web” refers to any material in a continuous flexible strip form, whose thickness is much less than its length and width, such as a paper, plastic film, textile, tape, metal plate. Web handling systems are used in a wide array of industries such as printing, pulp and paper, steel mills, and textile. An example is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> as a multistage printing machine, which is a complicated, high-speed, and very expensive piece of equipment. The web is fed from an unwinding roll, transmitted though a series of intermediate units, and usually accumulated unto a winding roll. Web tension may vary from one span to another, due to the imperfections such as rotation nonsynchronization among the related drive motors, vibration, and mechanical/electrical defects in the system [<xref ref-type="bibr" rid="scirp.24866-ref1">1</xref>]. Excessive tension variations in web materials will degrade the production quality [2,3]. Correspondingly winding process control is a very important issue in web handling facilities to improve production quality, productivity, and reliability [<xref ref-type="bibr" rid="scirp.24866-ref4">4</xref>].</p><p>Several control strategies have been studied for winding systems, such as the decentralized control [<xref ref-type="bibr" rid="scirp.24866-ref5">5</xref>], distributed PI control with tension observers [<xref ref-type="bibr" rid="scirp.24866-ref6">6</xref>], noninteracting force control [<xref ref-type="bibr" rid="scirp.24866-ref7">7</xref>], as well as those based on softcomputing tools such as fuzzy logic and neural networks [8,9]. However, the classical control systems usually lack adaptive capability and robustness to accommodate for operation uncertainty and parameter variations. Although certain model-based feedforward loop compensation can be implemented to improve the robustness of web tension control, the effect of the compensation depends on the accuracy of the associated mathematical plant models. However, accurate analytical models are usually difficult to derive especially with parameter uncertainty, disturbances, and measurement noise.</p><p>Disturbance arises from various sources in a multistage web handling system, such as upstream tension fluctuations and web speed variations. On the other hand, in printing industries, for instance, different web materials may go through a given web-handling machine; that is, the operating characteristics change in operations. Furthermore, line speed variations will also have a strong influence on web tension control. When perturbations exist, robustness of the control system is desired. Baumgart et al. [<xref ref-type="bibr" rid="scirp.24866-ref10">10</xref>] suggested a robust control strategy based on the decoupled tension and speed loops of the nonlinear web model. Several H<sub>∞</sub> controls were also proposed in [11-13] for web transportation system regulation. However, the effectiveness of these controllers heavily relies on the accuracy of the analytical gain scheduling that</p><p>may lack adaptive capability to accommodate for some time-varying system characteristics in real-time applications.</p><p>To tackle the aforementioned problems, a new adaptive H<sub>∞</sub> control strategy is developed in this work for winding process control. A novel gain scheduling scheme is proposed based on a neural fuzzy approximator to improve the transient response and enhance tension control; the adaptive capability of the controller is further improved by the use of a hybrid training strategy.</p><p>The remainder of the paper is organized as follows. Web system modeling is discussed in Section 2. The H<sub>∞</sub> control and the related adaptive gain scheduling techniques are presented in Section 3. The effectiveness of the proposed control techniques is verified experimenttally in Section 4.</p></sec><sec id="s2"><title>2. System Modeling</title><sec id="s2_1"><title>2.1. Plant Modeling</title><p>A simplified winding unwinding process is illustrated in <xref ref-type="fig" rid="fig2">Figure 2</xref>. To simplify analysis, the following assumptions are made [14,15]: 1) the thickness of the web is very small compared with the radius of winding/unwinding rollers; 2) the strain in the web is uniform within the web span; 3) the driving motors of winding and unwinding rolls have identical specifications; 4) no slip occurs between the web and the rollers; 5) neglecting dynamics of the load cell and idler rolls. The dynamics of the winding system can be derived as</p><disp-formula id="scirp.24866-formula127615"><label>(1)</label><graphic position="anchor" xlink:href="6-7900186\8293e608-fb90-4711-9bee-bcbf8e5e6827.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127616"><label>(2)</label><graphic position="anchor" xlink:href="6-7900186\711305a8-fd8d-4c11-ae96-b3d44ae82a47.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127617"><label>(3)</label><graphic position="anchor" xlink:href="6-7900186\0959f97f-8575-4c67-a428-f2765cd09094.jpg"  xlink:type="simple"/></disp-formula><p>where t<sub>w</sub> = total web tension, N;</p><p>L = web length between winding and unwinding rolls, m;</p><p>B<sub>f</sub> = coefficient of bearing viscous friction, Nm&#183;s/rad;</p><p>K<sub>m</sub> = toque constant of the motors, N&#183;m/A;</p><p>t<sub>w</sub><sub>0</sub> = wound-out tension of the unwinding roll, N;</p><p>v<sub>u</sub>, v<sub>w</sub> = tangential velocities of the unwinding and winding rolls, m/s;</p><p>i<sub>u</sub>, i<sub>w</sub> = input current to the driving motors of the unwinding and winding rolls, A;</p><p>R<sub>u</sub>, R<sub>w</sub> = radii of unwinding and winding rolls, m;</p><p>J<sub>u</sub>, J<sub>w</sub> = moments of inertia of the unwinding and winding rolls, kg&#183;m<sup>2</sup>;</p><p>a, E = cross section area (m<sup>2</sup>) and Young’s modulus (GPa) of the web material.</p><p>The wound-out tension <img src="6-7900186\a86374b4-40d3-4a10-ab4c-a0cb80c731f9.jpg" /> is an initial static tension within the web roll, which is generated by the previous winding and is assumed to be zero in this work for the sake of simplicity.</p><p>With the web material transmitted from the unwinding roll to the winding roll, the roll radius and inertia vary. If the winding and unwinding rolls have the same roll cores, the variations of the radius and inertia can be approximately described as</p><disp-formula id="scirp.24866-formula127618"><label>(4)</label><graphic position="anchor" xlink:href="6-7900186\8cfc9bfb-4245-444f-8396-508773c2fedb.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127619"><label>(5)</label><graphic position="anchor" xlink:href="6-7900186\803eaeeb-25e4-465c-b050-04243414d8d4.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127620"><label>(6)</label><graphic position="anchor" xlink:href="6-7900186\dfbb8c69-ec68-4e8e-898b-f4f4e462b937.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127621"><label>(7)</label><graphic position="anchor" xlink:href="6-7900186\8d029ce7-b06a-4a4e-9739-6be16e07221b.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="6-7900186\4b1bf5db-933d-4559-a55c-dc6d45e38f92.jpg" />= initial radii of unwinding/winding rolls, m;</p><p>R<sub>c</sub>, J<sub>c</sub> = radius (m) and moment of inertia (kg&#183;m<sup>2</sup>) of unwining winding roll core;</p><p>ρ, w, h = density (kg/m<sup>3</sup>), width (m), and thickness (m) of the web material, respectively.</p><p>Taking derivative of Equations (4)-(7) yields</p><disp-formula id="scirp.24866-formula127622"><label>(8)</label><graphic position="anchor" xlink:href="6-7900186\da982f52-ed1d-4d2c-b648-3eb056ff4bec.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127623"><label>(9)</label><graphic position="anchor" xlink:href="6-7900186\12f46a0e-ad54-4a82-82f2-28d452b5ea9a.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127624"><label>(10)</label><graphic position="anchor" xlink:href="6-7900186\39e87554-ddcc-40c3-80f2-467b940e5072.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127625"><label>(11)</label><graphic position="anchor" xlink:href="6-7900186\f3560f52-5447-48e8-a2bf-4d8c6d46d021.jpg"  xlink:type="simple"/></disp-formula><p>Substituting Equations (8)-(11) into (2) and (3) yields</p><disp-formula id="scirp.24866-formula127626"><label>(12)</label><graphic position="anchor" xlink:href="6-7900186\82b16287-b259-4a12-aee5-c38474d3fc35.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127627"><label>(13)</label><graphic position="anchor" xlink:href="6-7900186\fc06afba-d1a9-49af-a2ca-2ef8c8d5b322.jpg"  xlink:type="simple"/></disp-formula><p>Since the web thickness h is much less than its width (e.g. the paper thickness is 0.0762 mm in this work), the last terms in Equations (12) and (13) can be neglected. The real-time model becomes S</p><disp-formula id="scirp.24866-formula127628"><label>(14)</label><graphic position="anchor" xlink:href="6-7900186\2b27c32d-2bf6-4057-a84c-f5ab3f73aee5.jpg"  xlink:type="simple"/></disp-formula><p>The state-space representation of the nominal winding process plant will be</p><disp-formula id="scirp.24866-formula127629"><label>(15)</label><graphic position="anchor" xlink:href="6-7900186\06821909-2d8e-4014-baeb-cbae8ee35de9.jpg"  xlink:type="simple"/></disp-formula><p>where the subscript p represents plant, n stands for nominal, and</p><p><img src="6-7900186\fef2f4ce-aacc-44d7-b7d1-5c8f177a0a45.jpg" /></p><p><img src="6-7900186\f9bac80b-c436-44f6-9ed2-8e9c5e9dae75.jpg" /></p><p><img src="6-7900186\3ac5a4f2-aa48-4111-8688-7a03cdf46a94.jpg" /></p><p><img src="6-7900186\ed70ab20-6f1f-4041-81b4-7c6ad0a976a2.jpg" /></p><p><img src="6-7900186\732229a5-0bad-441d-b573-1056840da41b.jpg" /></p><p><img src="6-7900186\43195378-19e8-41d9-a2af-d8ba311d4462.jpg" /></p><p>Matrix C<sub>n</sub> is defined such that the outputs are the web tension and its line speed<img src="6-7900186\8a901b8d-1111-48a7-8091-3fa4651de9d8.jpg" />.</p></sec><sec id="s2_2"><title>2.2. The Standard LFT Framework</title><p>The practical connection of the closed-loop system with two weighting functions is illustrated in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a), where P(s) is the interconnection system in the standard linear fractional transformation (LFT) framework as shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b). The standard LFT framework in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) compactly describes the closed-loop system, whose exogenous input and output are w and<img src="6-7900186\8e1710a4-33c9-4d49-9dfa-a0e3e6664315.jpg" />, respectively.</p><p>The weighting function W<sub>e</sub>(s) aims to limit the magnitude of the output sensitivity function<img src="6-7900186\f40e36f0-1496-482c-97e0-52e026ae83a3.jpg" />. With W<sub>e</sub>(s), the H<sub>∞</sub> norm of W<sub>e</sub>S<sub>o</sub> will be minimized by H<sub>∞</sub> synthesis. In general, its desired value is limited to unity [<xref ref-type="bibr" rid="scirp.24866-ref16">16</xref>], that is, <img src="6-7900186\38705b03-e817-4b41-9915-116978a2079b.jpg" />or<img src="6-7900186\b413b3b8-212f-45f2-8ca2-6992d3c2bc64.jpg" />. W<sub>e</sub>(s) is selected with a high gain at low frequency to reject low frequency perturbations</p><disp-formula id="scirp.24866-formula127630"><label>(16)</label><graphic position="anchor" xlink:href="6-7900186\5f323daf-90c9-46f3-8825-97249808f8f4.jpg"  xlink:type="simple"/></disp-formula><p>where M is the peak magnitude of S<sub>0</sub>,<img src="6-7900186\4bd944a3-c549-48b6-bda8-2b1097007f75.jpg" />; <img src="6-7900186\44127321-c310-4a66-a3bd-26e881a1ae9f.jpg" />is the allowed steady-state error; and ω<sub>b</sub> is the required minimum frequency bandwidth.</p><p>The control signal weighting function W<sub>u</sub>(s) is selected to shape the frequency property of control signals</p><disp-formula id="scirp.24866-formula127631"><label>(17)</label><graphic position="anchor" xlink:href="6-7900186\dd7824a1-b4b7-482e-aadd-f34fb456a1e9.jpg"  xlink:type="simple"/></disp-formula><p>where M<sub>u</sub> is the maximum gain of KS<sub>0</sub>, that is, <img src="6-7900186\5093fe24-7b99-4f96-915c-c03a711e8982.jpg" />; ω<sub>u</sub> is the bandwidth of the controller K; and ε<sub>u</sub> is a real value to adjust the pole location of W<sub>u</sub>.</p><p>The selection of weighting function and their numerical realization are based on the following considerations: 1) to achieve the desired control performance; 2) to op-</p><p>timize the control effort and avoid actuator saturation; 3) to obtain the best robustness property to the closed-loop system; and 4) to get the optimal balance among different robustness properties of the closed-loop system. By simulation, the frequency weighting functions W<sub>e</sub>(s) and W<sub>u</sub>(s) are determined as</p><disp-formula id="scirp.24866-formula127632"><label>(18)</label><graphic position="anchor" xlink:href="6-7900186\fc0df4a7-c4a0-4248-8da4-d7a5838b1f6e.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127633"><label>(19)</label><graphic position="anchor" xlink:href="6-7900186\f0462d12-b682-4a09-8bb2-a7ebe16a03d6.jpg"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s3"><title>3. H<sub>∞</sub> Synthesis and Gain Scheduling</title><sec id="s3_1"><title>3.1. H<sub>∞</sub> Control Synthesis</title><p>H<sub>∞</sub> synthesis is an optimization algorithm that aims to design an H<sub>∞</sub> controller to achieve the desired robustness of the closed-loop system. Consider a nominal system represented by a lower LFT framework in <xref ref-type="fig" rid="fig4">Figure 4</xref>. The closed-loop transfer matrix can be represented as <img src="6-7900186\edde6184-8f54-4469-8c81-344e07726d5d.jpg" />. The H<sub>∞</sub> norm of the complex transfer matrix T<sub>zw</sub> is defined as</p><disp-formula id="scirp.24866-formula127634"><label>(20)</label><graphic position="anchor" xlink:href="6-7900186\f2f4b4c9-486b-49ec-adc3-343d25ca3951.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7900186\ce0a95f0-ca29-4909-83b7-ef4793a0a038.jpg" /> is the maximum singular value for a specific frequency ω, and <img src="6-7900186\0789a460-372c-4f0c-8712-01beea3b4411.jpg" /> represents the collection of real numbers. The commonly adopted suboptimal H<sub>∞</sub> control is described in [<xref ref-type="bibr" rid="scirp.24866-ref16">16</xref>]: Given γ &gt; 0, find all admissible controllers <img src="6-7900186\2db59c13-9d1d-4e31-94ea-cb9a048092c0.jpg" /> if there are any, such that<img src="6-7900186\122d287b-4fc4-4518-be44-dae4ac85f78f.jpg" />.</p><p>According to the selected weighting function <img src="6-7900186\a02060a0-bd1b-4bb8-9eaa-8b83cfb56887.jpg" /> in (18), the conditions and assumption on a standard H<sub>∞</sub> problem (as in [<xref ref-type="bibr" rid="scirp.24866-ref17">17</xref>]) are not satisfied. To tackle this problem, in this work, the initial controllers are designed based on the basic linear and time invariant model (15). One of the suboptimal H<sub>∞</sub> controllers is derived for the considered general H<sub>∞</sub> problem by solving two algebraic Riccati equations [16,18]. It can be represented by the following transfer function:</p><disp-formula id="scirp.24866-formula127635"><label>(21)</label><graphic position="anchor" xlink:href="6-7900186\bc2f0041-5255-449c-b613-483ddd8de3cf.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="6-7900186\76601362-8e5b-4df3-89b8-e5baec8060e7.jpg" /></p><p><img src="6-7900186\6637f4ed-547c-48db-88ab-b8aa6dd9f025.jpg" /></p><p><img src="6-7900186\879863e9-70fc-4ef3-a8fb-c60afa8ed00c.jpg" /></p><p><img src="6-7900186\a95974a4-6208-4f77-bba0-5d5aca35ee23.jpg" /></p></sec><sec id="s3_2"><title>3.2. Neural Fuzzy Approximator for Gain Scheduling</title><p>Control system design for web handling processes is conducted based on the basic linear and time invariant model, in which all parameters take their nominal values at the specified operating point. However, the time varying parameters (e.g., roll radius and inertia) will influence the control performance and robustness property of the corresponding closed-loop system. Within the design region where both winding and unwinding rolls are around dimensionally half web loaded, the control performance is satisfactory. However, at starting and ending stages, tension output becomes rather sensitive to line speed variations. It is generally assumed in the literature that the impact from time varying parameters is not significant since the variation is small, especially when the web roll is small [<xref ref-type="bibr" rid="scirp.24866-ref13">13</xref>]. In this work, a neural fuzzy (NF) approximator is developed to adaptively estimate the gain values to improve tension control performance.</p><p>In this case, five input variables are used in the developed NF approximator: the radius of winding roll, radius of the unwinding roll, tension, web speed, and armature current signals for both the winding and unwinding motors. Three membership functions (MFs), small, medium, and large, are assigned to each input variable. The reasoning processing is performed in the following form:</p><disp-formula id="scirp.24866-formula127636"><label>(22)</label><graphic position="anchor" xlink:href="6-7900186\754276e7-a143-45ee-a132-95ab5861e1ca.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7900186\6ff0a940-4094-4fb4-92c3-c05474b3465d.jpg" /> are MFs; <img src="6-7900186\1efaad1a-f215-44a0-b83d-f9c20f3a4021.jpg" />m is the number of rules.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> schematically shows the network architecture of the developed NF approximator. Unless specified, all</p><p>the network links have unity weights. The input nodes in layer 1 transmit the monitoring indices <img src="6-7900186\1769346b-18a9-4d72-8f4e-279b07bd5d92.jpg" /> to the next layer, successively, where n = 5 in this case. Each node in layer 2 acts as an MF, which can be either a single node that performs a simple activation function or multilayer nodes that perform a complex function. The nodes in layer 3 perform the fuzzy T-norm operations. If a max-product operator is used, the firing strength of rule <img src="6-7900186\fad6e991-a8ef-4f6f-9874-bdf8f3d96600.jpg" /> will be</p><disp-formula id="scirp.24866-formula127637"><label>(23)</label><graphic position="anchor" xlink:href="6-7900186\d5072b8a-3c44-4bda-80e8-1cf8045556ca.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7900186\70166c86-e04e-4988-a9ff-181e77ecac53.jpg" /> denote MF grades.</p><p>After normalization in layer 4, defuzzification is performed in layer 5. The predicted gain grades to each motor will be:</p><disp-formula id="scirp.24866-formula127638"><label>(24)</label><graphic position="anchor" xlink:href="6-7900186\5ef79e7a-dd47-4e2f-a1a0-d395efbfef63.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7900186\1213e6f6-c6cb-4cea-94dd-f661996be6e5.jpg" /> and <img src="6-7900186\45373e4a-ceb2-42a8-a7d7-6254f0dde0bc.jpg" /> are the number of rules associated with the decisions of <img src="6-7900186\fc6f099a-d03a-4f79-a343-326acff788c7.jpg" /> and<img src="6-7900186\7d0d3ac1-7b78-4e16-b1d9-f2bbb437fadf.jpg" />, respectively.</p><p>Correspondingly, the compensated input signals to the drive motors will be</p><disp-formula id="scirp.24866-formula127639"><label>(25)</label><graphic position="anchor" xlink:href="6-7900186\84a63950-d288-4066-8f04-290ddc4deb02.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7900186\4e501b2d-dfb7-4865-bcae-385fccf140a3.jpg" /> and <img src="6-7900186\7f3900aa-e69a-4a28-81b2-a4653c69701c.jpg" /> are the input current signals to the unwinding motor and winding motor, respectively.</p></sec><sec id="s3_3"><title>3.3. Online Training of the NF Approximator</title><p>Once the NF approximator is established, the related parameters should be optimized properly in order to achieve the desired input-output mapping. In training nonlinear system parameters, the classical method is the use of gradient algorithms [<xref ref-type="bibr" rid="scirp.24866-ref9">9</xref>]. The classical gradient algorithm, however, is slow in convergence especially when the approximation error becomes smaller [<xref ref-type="bibr" rid="scirp.24866-ref1">1</xref>]. To tackle this problem, an efficient fast gradient method, recently proposed in our research group [<xref ref-type="bibr" rid="scirp.24866-ref18">18</xref>], will be used in this work to optimize the nonlinear parameters of the NF approximator.</p><p>A hybrid training strategy is employed in this case to train the NF approximator. Each training epoch consists of two runs: in the backward pass, the nonlinear parameters of the NF approximator are updated by the fast gradient method [<xref ref-type="bibr" rid="scirp.24866-ref18">18</xref>]. In the backward pass, the linear parameters of the NF approximator, <img src="6-7900186\c6840e9d-d297-4703-bf9b-10d0a40b6a16.jpg" />, are fine-tuned using a recurrent LSE method [<xref ref-type="bibr" rid="scirp.24866-ref1">1</xref>].</p></sec></sec><sec id="s4"><title>4. Evaluation and Comparison</title><p>In order to verify the effectiveness of the developed adaptive H<sub>∞</sub> controller and the related techniques, a comparison study is taken in this section by experimental tests.</p><sec id="s4_1"><title>4.1. Experimental Setup</title><p>The experimental setup used in this work is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>, which has been developed by the authors’ research team. It consists of four DC motors and four idler rolls. Each motor can be controlled separately to simulate different drive/load conditions. Eight encoders (2048- lines) are used to measure shaft angular velocity. Tension can be measured by a tension transducer or an alternative spring-link-idler system. In this work, only two DC motors are set up as winding and unwinding rolls, whereas</p><p>no control actions are provided in the intermediate zone.</p><p>The experiments are taken in two parts: tests in the middle stage of a winding process and tests in the starting stage of a winding process. In modeling, the radii of unwinding and wingding rolls can be approximately calculated by</p><disp-formula id="scirp.24866-formula127640"><label>(24)</label><graphic position="anchor" xlink:href="6-7900186\f969684a-e0b3-4e04-9e9c-59e9cd27d404.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24866-formula127641"><label>(25)</label><graphic position="anchor" xlink:href="6-7900186\42883371-3324-48c2-944e-c5d434aa708f.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7900186\ba672840-1a48-4c8b-baca-799ee4a81836.jpg" /> and <img src="6-7900186\c816be3b-aee1-4d2c-98a6-79a126f32146.jpg" /> are the initial radii of unwinding and winding rolls, respectively; <img src="6-7900186\65871971-f5bd-42b2-be5f-8fd339e1a7f2.jpg" />and <img src="6-7900186\65dead74-f45d-4b93-b7ad-08b5ba207e6d.jpg" /> are the integrated angular displacements of the rolls; and h is the web thickness. Angular displacements are measured by two encoders mounted on the driving shafts of unwinding and winding rolls.</p></sec><sec id="s4_2"><title>4.2. Middle Stage Experimental Test</title><p>In this test, both the winding roll and unwinding roll are operating around dimensionally half web wounded. The performance of the developed adaptive H<sub>∞</sub> control is compared with a classical linear quadratic regulator (LQR) control. From our previous investigation [<xref ref-type="bibr" rid="scirp.24866-ref4">4</xref>], the LQR has been shown to outperform other related classical control modes (e.g., PI and PID) in web system control.</p><p><xref ref-type="fig" rid="fig7">Figure 7</xref> shows the test results of web tension control and line speed control by the developed adaptive H<sub>∞</sub> control using the NF approximator and without using the NF approximator (i.e., the gains are estimated with the classical method as suggested in [<xref ref-type="bibr" rid="scirp.24866-ref13">13</xref>]). It is seen that the NF approximator can effectively predict the gain values and process the tension and speed control operations.</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows the corresponding results using the <sub></sub></p><p>LQR control with and without using the NF approximator. Comparing the corresponding results in <xref ref-type="fig" rid="fig7">Figure 7</xref>, the adaptive H<sub>∞</sub> control outperforms the LQR in both force control and speed control, in terms of overshooting/undershooting and settling time. The proposed gain scheduling scheme can improve the control performance: specifically, 1) suppress the tension fluctuation due to line speed variations; 2) reduce the settling time for both tension and speed responses; and 3) the decrease overshot of speed response. The effectiveness of the classical gain scheduling method relies on the accuracy of the mathematical models, and the robustness to attenuate disturbances in web handling operations.</p></sec><sec id="s4_3"><title>4.3. Starting Stage Experimental Test </title><p>In this test, the winding process is running from the starting point, at which the winding roll is web unloaded and the unwinding roll is fully web loaded. <xref ref-type="fig" rid="fig9">Figure 9</xref> illustrates the test results by the adaptive H<sub>∞</sub> control using the NF approximator and the classical gain scheduling methods, respectively. It is seen that the NF approximator can accommodate for more system uncertainty in gain scheduling, and provide more accurate control performance.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows the control results using LQR control corresponding to different gain compensation strategies. Comparing Figures 8 and 9, it is clear the adaptive H<sub>∞</sub><sub> </sub>control is superior to the classical LQR control.</p></sec></sec></body><back><ref-list><title>References</title><ref id="scirp.24866-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">W. 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