<?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">EPE</journal-id><journal-title-group><journal-title>Energy and Power Engineering</journal-title></journal-title-group><issn pub-type="epub">1949-243X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/epe.2012.46065</article-id><article-id pub-id-type="publisher-id">EPE-25088</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  A Novel Coordinated Sliding Mode Controller Based on Lyapunov Method for SVC, Excitation and Steam Valving
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>iwei</surname><given-names>Du</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>Hu</surname><given-names>Peng</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ben</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>School of Automation Engineering, University of Electronic Science and Technology of China, Chengdu, China</addr-line></aff><aff id="aff3"><addr-line>School of Electrical Engineering, Southwest Jiaotong University, Chengdu, China</addr-line></aff><aff id="aff1"><addr-line>Suining Breach of Sichuan Power Electric Corporation, Suining, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hunter_djw@163.com(ID)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>22</day><month>11</month><year>2012</year></pub-date><volume>04</volume><issue>06</issue><fpage>523</fpage><lpage>528</lpage><history><date date-type="received"><day>June</day>	<month>10,</month>	<year>2012</year></date><date date-type="rev-recd"><day>July</day>	<month>15,</month>	<year>2012</year>	</date><date date-type="accepted"><day>July</day>	<month>28,</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>
 
 
  A novel coordinated controller is proposed in the paper for SVC, excitation and steam valving for a single machine infinite system. Firstly, the nonlinear mathematic model of the system including the itation and steam valving is exactly linearized via state feedback. Then, the quasi-linearized system after the exact lineariztion is controlled by the sliding model controller based on Lyapunov direct method. At last, the novel coordinated controller is compared with a traditional linear controller and a nonlinear optimal controller respectively by simulations. The simulation results show that the proposed controller gives better dynamic response and stronger robustness.
 
</p></abstract><kwd-group><kwd>SVC; Excitation and Steam Alving; Sliding Mode Control; Lyapunov; Simulation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>[1,2] presented a novel nonlinear optimal excitation controller and a nonlinear variable structure excitation controller. [<xref ref-type="bibr" rid="scirp.25088-ref3">3</xref>] applied nonlinear robustness excitation controller with voltage regulation. [1,4-6] adopted SVC controller to restrain the system sub-synchronous oscillation, and damp the voltage fluctuation. [7-9] designed a cooperated controller for a SVC and excitation controller to improve system stability. The excitation controller and steam valving controller are proposed to increase the performance of the system in [<xref ref-type="bibr" rid="scirp.25088-ref10">10</xref>].</p><p>In this paper, a novel coordinated sliding mode control based on Lyapunov method is used to generate the control schemes for the SVC, Excitation and Steam Valving. In order to achieve superior performance for the power system, the coordination between the SVC, Excitation and Steam Valving is studied to avoid poor interaction.</p></sec><sec id="s2"><title>2. Mathematical Model</title><p>A single generator—infinite bus power system with SVC is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>For a generator set connected to a single generator infinite bus power system with SVC, traditional transient behavior equations can be described as follows [1,6]:</p><disp-formula id="scirp.25088-formula38337"><label>(1)</label><graphic position="anchor" xlink:href="15-620XXX3\12e23d31-164c-4bcf-a4e8-39951b55d971.jpg"  xlink:type="simple"/></disp-formula><p>where, T<sub>d</sub><sub>0</sub> is the direct axis transient short circuit time constant, P<sub>m</sub><sub>0</sub> the initial mechanical power, P<sub>H</sub> the mechanical power generated by the HP turbine in per unit, H the inertia coefficient, D the damping constant, <img src="15-620XXX3\7f436c02-5e5a-4ba6-ab3c-9068c6e30398.jpg" />the transient EMF in the quadrature axis of the generator. C<sub>H</sub> and C<sub>ML</sub> are the power distribution coefficients of the HP and the MP/LP steam turbine subsystems. T<sub>HΣ</sub> and T<sub>MΣ</sub> are the equivalent time constants of the HP and MP/LP steam value control system respectively. δ is the rotor angle in radian/s and ω the radial speed of the machine. T<sub>C</sub> is the time constant of SVC regulator. <img src="15-620XXX3\83d6dce1-d964-45c3-b2d4-6ea1e49affad.jpg" />is the direct axis transient. x<sub>d</sub> is the direct axis reactance of the generator, B<sub>L</sub> is the susceptance of the inductor in SVC, B<sub>C</sub> is the susceptance of the capacitor in SVC, u<sub>1</sub> is the control input of the excitation system. u<sub>1</sub> is the control input of SVC. u<sub>1</sub> is the control input of the HP steam turbine subsystems.</p><p><img src="15-620XXX3\31438db8-9c50-4b63-a793-9304075bb520.jpg" /></p><p>P<sub>m</sub> is the mechanical power. P<sub>e</sub> is the active electrical power delivered by the generator, and given by:</p><p><img src="15-620XXX3\ce45f9d1-4c46-4b8b-9ff2-54a57902e021.jpg" /></p><p>The equations above describe a five-order three-input three-output affine nonlinear system and can be rewritten in a normal form as follows:</p><disp-formula id="scirp.25088-formula38338"><label>(2)</label><graphic position="anchor" xlink:href="15-620XXX3\8a2a7e04-4bd0-4614-8006-8d53d9121408.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="15-620XXX3\3c63ae30-3891-4b0e-9c43-e891fa6e578b.jpg" /></p><p><img src="15-620XXX3\8bb32381-c113-46da-b6e1-780760bb06bd.jpg" />,</p><p><img src="15-620XXX3\031cc79f-4150-405a-8db2-08090dbd36d2.jpg" />,</p><p><img src="15-620XXX3\e6830dad-c7fb-439f-99f1-3abba0e97eb5.jpg" />,</p><p><img src="15-620XXX3\1d8d2b58-e28b-4410-8752-337560d355e3.jpg" /></p></sec><sec id="s3"><title>3. Global Linearization</title><p>The output functions have a significant relationship with state variables which will be controlled. The output functions may be state variable or the system actual output variable, but system actual output variable must be the function of state variables. In this paper, we choose output functions considering the following aspects:</p><p>1) Consider the Stability of δ, we can choose</p><p><img src="15-620XXX3\6d979df2-85ff-4bee-8378-009e838fa54d.jpg" /></p><p>2) Consider the impact of stream valve on active electrical power, we can choose,</p><p><img src="15-620XXX3\1b1ff17a-ba95-466b-b9c0-68bb673549b3.jpg" /></p><p>3) Consider the Stability of SVC Connection point voltage, y<sub>3</sub> is adopted as follows:</p><p><img src="15-620XXX3\4db4ac73-9a86-4a92-b19a-b010fa0affd9.jpg" /></p><p>According to circuit principle, <img src="15-620XXX3\89e668a2-a324-4a4c-9999-64c63de9dcc1.jpg" />is given by:</p><p><img src="15-620XXX3\a56a8a3e-2bc1-4fe4-a607-df2d3fa76e97.jpg" /></p><p>where</p><p><img src="15-620XXX3\c5c29286-3747-4dd7-bf82-1de93d1e4e64.jpg" />,</p><p><img src="15-620XXX3\16aa5028-3830-4068-896e-9b68ed88d8cc.jpg" />is the reference voltage.</p><p>First, calculate the relative degree of the system as follows:</p><p><img src="15-620XXX3\36248dbb-2e78-4596-972d-b1cdea573075.jpg" /></p><p>The matrix:</p><p><img src="15-620XXX3\972b1806-c54b-49a4-86fd-e565b6ec5975.jpg" /></p><p><img src="15-620XXX3\18854c8c-bfdf-477e-86ab-a31d9cba8104.jpg" />is nonsingular in whole state space, so, the relative</p><p>degree set<img src="15-620XXX3\11995038-ab54-4ed8-a701-ad575c8fe2dd.jpg" />, and<img src="15-620XXX3\75fb6a16-6330-4bdd-bb23-6614cd410187.jpg" />.</p><p><img src="15-620XXX3\8f433cd3-3bca-40a3-81f7-df5133bbe06e.jpg" />as a new state vector, <img src="15-620XXX3\309cc4c9-c4c9-4e16-adaf-b8b0650d14a8.jpg" />can be given by:</p><disp-formula id="scirp.25088-formula38339"><label>(3)</label><graphic position="anchor" xlink:href="15-620XXX3\afec2177-9848-4cb1-9c04-5f0b97d4b5ba.jpg"  xlink:type="simple"/></disp-formula><p>Thus, a Brunowsky canonical form is written as:</p><disp-formula id="scirp.25088-formula38340"><label>(4)</label><graphic position="anchor" xlink:href="15-620XXX3\c66fc18d-0854-46c8-bbdb-74430702ffc5.jpg"  xlink:type="simple"/></disp-formula><p>the model for the power system described in Equation (2) can be rewritten as:</p><disp-formula id="scirp.25088-formula38341"><label>(5)</label><graphic position="anchor" xlink:href="15-620XXX3\73cffbbb-5f8f-482a-8c82-66acb65b5376.jpg"  xlink:type="simple"/></disp-formula><p>A and B are constant matrix, and V is a vector of virtual inputs.</p><p>where</p><p><img src="15-620XXX3\c3d002a2-bf74-4acc-9244-03da67a5057f.jpg" /></p><p>Getting easily:</p><disp-formula id="scirp.25088-formula38342"><label>(6)</label><graphic position="anchor" xlink:href="15-620XXX3\d96f0a7d-485b-43c3-8ed9-0b75fb02c5fd.jpg"  xlink:type="simple"/></disp-formula><p>where,</p><p><img src="15-620XXX3\2d87dd4a-fbd4-48e4-9dce-aa37e9cb200d.jpg" /></p><p>the output for the power system described in Equation (2) is represented as follows:：</p><disp-formula id="scirp.25088-formula38343"><label>(7)</label><graphic position="anchor" xlink:href="15-620XXX3\8ae373d7-62b2-4048-bb95-85f62dd22399.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Sliding Mode Controller Based on Lyapunov Method</title><p>Consider the equation of the system described in Equation (5), A is decomposed into three Jordan sub-matrix as</p><p><img src="15-620XXX3\1bef2f58-979f-4e88-a879-c1aa43248e3c.jpg" /></p><p>The system is decomposed into three sub-system for controllers design independently. At First, for the corresponding subsystem A<sub>11</sub>, Sliding mode control based on Lyapunov method is used to design the anticipated dynamic characteristics.</p><p>Here, <img src="15-620XXX3\e44df3da-c857-4856-b6fc-6f7c0f02afc3.jpg" />is Controllable, L<sup>T</sup>Z is introduced to obtain</p><disp-formula id="scirp.25088-formula38344"><label>(8)</label><graphic position="anchor" xlink:href="15-620XXX3\ba4f0963-31b4-44b5-a698-abc382e9a431.jpg"  xlink:type="simple"/></disp-formula><p>where,<img src="15-620XXX3\4339aa07-56c0-49b2-812f-54b3e61487b9.jpg" />. Here, <img src="15-620XXX3\47a3a697-fab1-4b21-bdae-c95846b93b5e.jpg" />Eigenvalues are –2 and –1 &#177; 2j. According to pole allocation method for the controllable canonical form system, we can get</p><p><img src="15-620XXX3\a4ea6c01-0013-4310-974a-dc836b940756.jpg" /></p><p>For the system described in Equation (8), we can choose</p><disp-formula id="scirp.25088-formula38345"><label>(9)</label><graphic position="anchor" xlink:href="15-620XXX3\59a31d1c-86ff-4871-9b6a-0024143e4039.jpg"  xlink:type="simple"/></disp-formula><p>Afterward,</p><disp-formula id="scirp.25088-formula38346"><label>(10)</label><graphic position="anchor" xlink:href="15-620XXX3\006d4814-0abf-42d0-b59b-10c4af830041.jpg"  xlink:type="simple"/></disp-formula><p>where, P is the solution of the Lyapunov equation as</p><disp-formula id="scirp.25088-formula38347"><label>(11)</label><graphic position="anchor" xlink:href="15-620XXX3\ee0797f2-ed63-4f9b-b0d5-24204a281b4b.jpg"  xlink:type="simple"/></disp-formula><p>Q in (11) is a positive definite matrix.</p><p>Switching hypersurface equation is chosen as</p><disp-formula id="scirp.25088-formula38348"><label>(12)</label><graphic position="anchor" xlink:href="15-620XXX3\758aae7e-a52a-4af0-87a4-00f48adc62eb.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="15-620XXX3\87c56be1-7710-44a0-ac47-0871b96a3140.jpg" />.</p><p>On the sliding mode hypersurface, we can get easily <img src="15-620XXX3\f960432c-7bdf-407e-9224-956dcd0e0fc8.jpg" /> according to Equations (10) and (11), we can know <img src="15-620XXX3\319df134-75db-4638-97ab-173d5b11ce27.jpg" />as</p><disp-formula id="scirp.25088-formula38349"><label>(13)</label><graphic position="anchor" xlink:href="15-620XXX3\11cbe1f0-0057-48a7-9890-13abe7f7209e.jpg"  xlink:type="simple"/></disp-formula><p>In Equation (13), V is positive and <img src="15-620XXX3\084fa9bc-066b-4e32-a683-5abe75befd59.jpg" /> is negative, so sliding mode movement is asymptotically stable. The control variable <img src="15-620XXX3\14cce29a-928d-47b5-92f3-67aa32b2488b.jpg" /> is out of service on the switching hypersurface.</p><p>To get better performance, the index asymptotic law control is adopted as follows:</p><disp-formula id="scirp.25088-formula38350"><label>(14)</label><graphic position="anchor" xlink:href="15-620XXX3\72a60e70-0021-4da5-94bb-5562fb12afd4.jpg"  xlink:type="simple"/></disp-formula><p>Thus,</p><disp-formula id="scirp.25088-formula38351"><label>(15)</label><graphic position="anchor" xlink:href="15-620XXX3\8a111836-0d2d-4a84-bcbb-8efcd077d41d.jpg"  xlink:type="simple"/></disp-formula><p>According to Equations (14) and (15), we can obtain the virtual input</p><disp-formula id="scirp.25088-formula38352"><label>(16)</label><graphic position="anchor" xlink:href="15-620XXX3\f9ddfe8f-0f7c-4f8e-b1be-92643a6f076b.jpg"  xlink:type="simple"/></disp-formula><p>For the subsystem A<sub>22</sub> and A<sub>33</sub>, we can design independently two controller v2 and v3 according to pole allocation of linear system. Switching hypersurface equations are taken as follows:</p><p><img src="15-620XXX3\53f07067-11a2-4bc9-9506-205fc998350d.jpg" /></p><p>where, k<sub>4</sub> and k<sub>5</sub> are constants, respectively.</p><p>The index asymptotic law controls for the subsystem A<sub>22</sub> and A<sub>33</sub> are adopted as</p><p><img src="15-620XXX3\80c079dc-614b-44ca-a8a0-51fc4e7555ab.jpg" /></p><p>where, k<sub>2</sub>, k<sub>3</sub>, ε<sub>2</sub> and ε<sub>3 </sub>are positive constants.</p><p>Then,</p><disp-formula id="scirp.25088-formula38353"><label>(17)</label><graphic position="anchor" xlink:href="15-620XXX3\d4bf17a7-a5d8-4889-99aa-40d036af9f6f.jpg"  xlink:type="simple"/></disp-formula><p>To eliminate the chattering phenomenon on the sliding mode surface, we substitute the sign function with a saturation function as</p><p><img src="15-620XXX3\797da220-f7bc-4457-b837-c12a7f60cf44.jpg" /></p><p>where, Δ is the boundary of the saturation function, and <img src="15-620XXX3\5b0de08b-5e0d-40c4-89b0-7a73140ea31e.jpg" /> is the switching control term.</p><p>Therefore, according to Equations (16) and (17), we can formulate the final control laws of the whole system as</p><disp-formula id="scirp.25088-formula38354"><label>(18)</label><graphic position="anchor" xlink:href="15-620XXX3\dc41c74b-daf8-4254-8dce-e2fc68fd89d0.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Simulation Results</title><p>A simulation case is given as follows: H = 8, D = 5, Vs = 1, x<sub>d</sub> = 0.779, x`<sub>d</sub> = 0.14, T<sub>d0</sub> = 6.9, x<sub>L1</sub> = 0.38, x<sub>L2</sub> = 0.54, x<sub>T</sub> = 0.01, T<sub>c</sub> = 0.2, B<sub>L0</sub> = 0.3, B<sub>c</sub> = 1.22, V<sub>ref</sub> = 1, C<sub>H</sub> = 0.4, T<sub>H</sub><sub>∑</sub> = 0.45, ε<sub>1</sub> =ε<sub>2</sub> = ε<sub>3</sub> = 0.1, k<sub>1</sub> = k<sub>2</sub> = k<sub>3</sub><sub> </sub>= 5, k<sub>4</sub> k<sub>5</sub> = 1, Q = I, Δ = 0.2, 0 ≤ E΄<sub>q</sub> ≤ 3.3, 0 ≤ B<sub>L</sub> ≤ 1.5. The parameters of equilibrium point are chosen as P<sub>m0</sub> = 0.79，δ<sub>0</sub> = 60<sup>˚</sup>，ω<sub>0</sub> = 314.16.</p><p>Case 1: by comparing traditional linear controller (TLC) with the controller (NSVC) designed in this paper, we study the controller’s dynamic performances. It is assumed that a short circuit fault occurs at the high voltage side of the transformer at 1s and is cleared at 1.2 s. The swing curves of the dynamic system are given in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>It can be seen from <xref ref-type="fig" rid="fig2">Figure 2</xref> that the novel sliding mode controller based on Lyapunov method for coordinating SVC, excitation, and steam valving improves power angle stability, damps the system frequency oscillation and prevents active electrical power and SVC voltage from fluctuation.</p><p>Case 2: the proposed controller is compared with NOPC in references [<xref ref-type="bibr" rid="scirp.25088-ref1">1</xref>]. It is assumed that the short circuit fault occurs on x<sub>L2</sub> at 1 s, and the faulting line is</p><p>opened at 1.2 s to supply the power with a single line. The second line returns successfully at 1.9 s. The swing curves of the dynamic system are given in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows that the novel coordinated controller gives better dynamic response and stronger robustness.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.25088-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Q. Lu and Y. Z. Sun, “Nonlinear Control in Power System,” Science Press, Beijing, 1993.</mixed-citation></ref><ref id="scirp.25088-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">W. C. Chan and Y. Y. Hsu, “An Optimal Variable Structure Stabilizer for Power System Stabilization,” IEEE Transactions on Power Apparatus and Systems, Vol. PAS-102, No. 6, 1983, pp. 1738-1746.</mixed-citation></ref><ref id="scirp.25088-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Y. Y. Wang and L. 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