<?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">CS</journal-id><journal-title-group><journal-title>Circuits and Systems</journal-title></journal-title-group><issn pub-type="epub">2153-1285</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/cs.2016.76068</article-id><article-id pub-id-type="publisher-id">CS-66466</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>
 
 
  Design of Robust Controller for LFC of Interconnected Power System Considering Communication Delays
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>Jesintha Mary</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>P.</surname><given-names>Rangarajan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Electrical and Electronics Engineering, R.M.D Engineering College, Chennai, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>jesintha82eee@gmail.com(.JM)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>05</month><year>2016</year></pub-date><volume>07</volume><issue>06</issue><fpage>794</fpage><lpage>804</lpage><history><date date-type="received"><day>22</day>	<month>March</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>8</month>	<year>May</year>	</date><date date-type="accepted"><day>13</day>	<month>May</month>	<year>2016</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>
 
 
  The usage of open communication infrastructure for transmitting the control signals in the Load Frequency Control (LFC) scheme of power system introduces time delays. These time delays may degrade the dynamic performance of the power system. This paper proposes a robust method to design a controller for multi-area LFC schemes considering communication delays. In existing literature, the controller values of LFC are designed using time domain approach which is less accurate than the proposed method. In proposed method, t
  he controller values are determined by moving the rightmosteigenvalues of the system to the left half plane in a quasi-continuous way for a preset upper bound of time delay. Then the robustness of the proposed controller is assessed by estimating the maximumtolerable value of time delay for maintaining system stability. Simulation studies are carried out for multi-area LFC scheme equipped with the proposed controller using Matlab/simulink. From the results, it has been concluded that the proposed controller guarantees the tolerance for all time delays smaller than the preset upper bound and provides a bigger delay margin than the existing controllers.
 
</p></abstract><kwd-group><kwd>Continuous Pole Placement Technique</kwd><kwd> Delay Margin</kwd><kwd> Delay-Dependent Stability Analysis</kwd><kwd> Frequency Sweeping Test</kwd><kwd> Load Frequency Control with Time Delays</kwd><kwd> Output Feedback Control</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>For many years, the Load Frequency Control (LFC) plays a major role in power system operation and control. The main objective of LFC is to minimize the frequency variations when there is any change in load [<xref ref-type="bibr" rid="scirp.66466-ref1">1</xref>] . In traditional LFC framework, the control signals are transmitted through dedicated communication channels where the communication delays are very minimal. Nowadays, the open communication infrastructure is widely used for transmitting control signals. In such a case, time delays cannot be neglected. These time delays are certain to have an impact on the stability of the power system [<xref ref-type="bibr" rid="scirp.66466-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.66466-ref3">3</xref>] . Therefore it is essential to consider the communication delays while analyzing the stability of power system.</p><p>At present, there is a rapid momentum in the advancement of research to deal LFC with communication delays. X. Yu et al. [<xref ref-type="bibr" rid="scirp.66466-ref4">4</xref>] proposed a Linear Matrix Inequalities (LMI) approach for LFC system with communication delays. Hassa Bevarani et al. [<xref ref-type="bibr" rid="scirp.66466-ref5">5</xref>] designed a robust decentralized PI controller based on H<sub>2</sub>/H<sub>∞</sub> control technique for three area interconnected power system with communication delay. L. Jiang et al. [<xref ref-type="bibr" rid="scirp.66466-ref6">6</xref>] examined the delay dependent stability of multi area LFC scheme with PI controllers using Lyapunov-theory based delay dependent criterion and LMI techniques. R. Dey et al. [<xref ref-type="bibr" rid="scirp.66466-ref7">7</xref>] investigated the delay dependent/independent design of H<sub>∞</sub> controller for LFC of two area system. Chuanke Zhang et al. [<xref ref-type="bibr" rid="scirp.66466-ref8">8</xref>] analyzed the delay dependent stability of LFC of multi area system by finding the delay margin using LMI technique and obtaining the relationship between delay margin and controller parameter. Chuanke Zhang et al. [<xref ref-type="bibr" rid="scirp.66466-ref9">9</xref>] designed a PID controller for delay dependent robust load frequency control. Sahin Sonmez et al. [<xref ref-type="bibr" rid="scirp.66466-ref10">10</xref>] discussed about the computation of time delay margin for single area LFC system using Routh array stability criterion.</p><p>J. Chen et al. [<xref ref-type="bibr" rid="scirp.66466-ref11">11</xref>] presented a method to compute the delay margin of a linear time delay system by determining eigenvalues and generalized eigenvalues of certain constant matrices. The method of tracing critical eigenvalue [<xref ref-type="bibr" rid="scirp.66466-ref12">12</xref>] and cluster treatment of characteristics roots [<xref ref-type="bibr" rid="scirp.66466-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.66466-ref15">15</xref>] is a direct method of finding delay margin. Another method is the indirect method to determine delay margin based on Lyapunov stability theory and LMI [<xref ref-type="bibr" rid="scirp.66466-ref16">16</xref>] - [<xref ref-type="bibr" rid="scirp.66466-ref18">18</xref>] . Wim Michiels et al. [<xref ref-type="bibr" rid="scirp.66466-ref19">19</xref>] suggested a new method for the determination of controller parameters in a broad class of linear control systems affected by time-delays. In this outlook, the research is focusing on designing a robust controller for LFC affected by communication delays gain prominence.</p><p>This paper proposes a new method to design a robust controller for the multi area LFC scheme considering communication delays in order to maintain the frequency and tie-line power between the areas. The controller is designed to guarantee the stability of power system for any delays smaller than the preset upper bound. The paper is organized as follows. In section 2, the multi area LFC structure is modelled considering time delays and it is represented in state space form. In section 3, the detailed description of a robust method to design the controller for multi area LFC affected by communication delays is presented. In section 4, the efficiency of the proposed controller is evaluated by computing the maximum tolerable value of time delay theoretically using Frequency Sweeping Test. In section 5, simulation is performed to prove the efficiency of the designed controller against delays for multi area LFC.</p></sec><sec id="s2"><title>2. Dynamic Model of Multi Area LFC with Time Delay</title><p>This section illustrates the dynamic model of multi area LFC scheme with time delay. This is obtained by including an exponential term e<sup>−sτ</sup> in the secondary control loop of the conventional LFC model [<xref ref-type="bibr" rid="scirp.66466-ref1">1</xref>] . <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the block diagram of i<sup>th</sup> control area of multi-area LFC scheme where i = 1, 2…N. The exponential term denotes the time delay. The turbine, governor and generator are modelled by a first order transfer function [<xref ref-type="bibr" rid="scirp.66466-ref1">1</xref>] .</p><p>The notations used for i<sup>th</sup> control area are listed below.</p><p>τ transport delay.</p><p>T<sub>gi</sub> Governor time constant.</p><p>T<sub>ti</sub> Turbine time constant.</p><p>M<sub>i</sub> Moment of inertia of generators.</p><p>D<sub>i</sub> Damping co-efficient of generator.</p><p>R<sub>i</sub> Speed droop.</p><p>ACE<sub>i</sub> Area Control Error.</p><p>Δf<sub>i</sub> Deviation in frequency.</p><p>ΔPt<sub>ie</sub> Tie-line power flow.</p><p>ΔPt<sub>i</sub> Turbine power output.</p><p>ΔPg<sub>i</sub> Governor output.</p><p>β<sub>i</sub> Frequency bias factor.</p><p>ΔP<sub>di</sub> Total demands in area i.</p><p>T<sub>ij</sub> Synchronizing coefficient between area i and area j.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Dynamic model of i<sup>th</sup> control area of multi area LFC scheme</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x6.png"/></fig><p>The two-area LFC scheme with time delay can be expressed in state space form as</p><disp-formula id="scirp.66466-formula12"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x7.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66466-formula13"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x8.png"  xlink:type="simple"/></disp-formula><p>where x(t) is state vector and the state variables are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x9.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x10.png" xlink:type="simple"/></inline-formula> . y(t) is output vector, The output variables are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x12.png" xlink:type="simple"/></inline-formula>. w(t) is disturbance vector. The disturbance variables are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x13.png" xlink:type="simple"/></inline-formula>. The frequency deviations and tie line power exchange are combined together as a single variable called Area Control Error signal (ACE).</p><p>The ACE signal of area i is expressed as</p><disp-formula id="scirp.66466-formula14"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x14.png"  xlink:type="simple"/></disp-formula><p>The ACE signal is used as the input to load frequency controller, which is designed as</p><disp-formula id="scirp.66466-formula15"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x15.png"  xlink:type="simple"/></disp-formula><p>The closed loop model of two area LFC system can be obtained by modifying Equation (1) using state output feedback method and expressed as</p><disp-formula id="scirp.66466-formula16"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x16.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66466-formula17"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x17.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x18.png" xlink:type="simple"/></inline-formula>;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x19.png" xlink:type="simple"/></inline-formula>;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x20.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x21.png" xlink:type="simple"/></inline-formula>;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x22.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x23.png" xlink:type="simple"/></inline-formula>;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x24.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x25.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x26.png" xlink:type="simple"/></inline-formula>; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x27.png" xlink:type="simple"/></inline-formula></p><p>K<sub>1</sub> and K<sub>2</sub> denote the gain values of PI controller. The controller values are determined using Continuous Pole Placement method which is described in detail in the next section.</p></sec><sec id="s3"><title>3. Controller Design Based on Continuous Pole Placement Method [<xref ref-type="bibr" rid="scirp.66466-ref20">20</xref>]</title><sec id="s3_1"><title>3.1. Description of the Algorithm</title><p>The idea behind the proposed stabilization method is to move the unstable eigenvalues to the left half plane in a quasi-continuous way by applying small changes to the controller gain, in the meanwhile monitoring the other eigenvalues with a large real part. The proposed stabilization method is based on the Theorem given in Appendix 1.</p><p>The algorithm for the proposed method is as follows:</p><p>Step 1. Initialize the number of rightmost eigenvalues m = 1.</p><p>Step 2. Compute the rightmost eigenvalues for a particular preset upper bound of delay.</p><p>Step 3. Find the sensitivity of the m rightmost eigenvalues with respect to the changes in the controller gain K.</p><p>Step 4. Using the sensitivities computed in step 3, shift the m rightmost eigenvalues in the direction towards the left half plane by applying small changes to the controller gain K.</p><p>Step 5. Meanwhile monitor the uncontrolled eigenvalues. Stop when the stability is reached or go to step 2.</p><p>The detailed explanation about the different steps involved in the algorithm is presented in the following sections.</p></sec><sec id="s3_2"><title>3.2. Computation of the Rightmost Eigenvalues</title><p>In 1999, Engelborghs and Roose proposed a method which computes the rightmost eigenvalues of the characteristic equation. In this method, a discretization of the time integration operator of the linearized system is obtained. The eigenvalues of the linearized system are exponential transforms of the roots of the characteristic equation. Then, the selected eigenvalues of the resulting large matrix are computed. A step length heuristic is applied to ensure that all eigenvalues are approximated accurately by discretization and the accuracy is improved by employing Newton iteration on the characteristic equation taking the approximate eigenvalues as starting values. This method is implemented in the Matlab package DDE-BIFTOOL. This package is a collection of matlab routines used to find the right most eigenvalues of the system.</p></sec><sec id="s3_3"><title>3.3. Sensitivity of Eigenvalues with Respect to the Controller Gain K</title><p>The characteristics equation of the two area LFC system Equation (5) can be written as</p><disp-formula id="scirp.66466-formula18"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x28.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66466-formula19"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x29.png"  xlink:type="simple"/></disp-formula><p>where λ<sub>i</sub> is a solution of the characteristic equation and n(v<sub>i</sub>) is a normalizing condition. Differentiating the Equation (7) and Equation (8) w.r.t. a component k<sub>j</sub> of K,</p><disp-formula id="scirp.66466-formula20"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x30.png"  xlink:type="simple"/></disp-formula><p>From Equation (9), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x31.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x32.png" xlink:type="simple"/></inline-formula> can be obtained. e<sub>j</sub> is j<sup>th</sup> unity vector. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x33.png" xlink:type="simple"/></inline-formula>denotes the sensitivity of the eigenvalues with respect to changes in feedback gain k.</p></sec><sec id="s3_4"><title>3.4. Continuation of Eigenvalues as a Function of the Feedback Gain K</title><p>It is assumed that m eigenvalues <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x34.png" xlink:type="simple"/></inline-formula> are to be controlled. The sensitivity of the eigenvalues with respect to changes in feedback gain is denoted as the sensitivity matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x35.png" xlink:type="simple"/></inline-formula> where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x36.png" xlink:type="simple"/></inline-formula>. The desired displacement of the controlled eigenvalues <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x37.png" xlink:type="simple"/></inline-formula> can be expressed as</p><disp-formula id="scirp.66466-formula21"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x38.png"  xlink:type="simple"/></disp-formula><p>From Equation (10) the small changes in gain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x39.png" xlink:type="simple"/></inline-formula> can be calculated</p><disp-formula id="scirp.66466-formula22"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x40.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x41.png" xlink:type="simple"/></inline-formula>is the Moore-Penrose inverse of sensitivity matrix (S<sub>m</sub>). Thus with the availability of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x42.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x43.png" xlink:type="simple"/></inline-formula>, the small adjustments in feedback gain can be obtained one constraint that is imposed on the feedback gain is that its components must be real, but this can be obtained only by taking the components of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x44.png" xlink:type="simple"/></inline-formula> in complex conjugate pairs. For the new feedback gain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x45.png" xlink:type="simple"/></inline-formula>, the displacement of the controlled eigenvalues is not equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x46.png" xlink:type="simple"/></inline-formula>, because Equation (10) is based on linearization, and some correction is required. Since the eigenvalues and eigen functions are continuous with respect to parameter changes, the predictor</p><disp-formula id="scirp.66466-formula23"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x47.png"  xlink:type="simple"/></disp-formula><p>for few Newton iterations on Equation (7) are required when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x48.png" xlink:type="simple"/></inline-formula> is small. Since the research focuses on designing a controller in stability point of view, it is sufficient to control only the real parts of the eigenvalues i.e.,</p><p>sup<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x49.png" xlink:type="simple"/></inline-formula>. The real parts of the rightmost eigenvalues are adjusted in order to shift the rightmost eigenvalues to LHP. Therefore Equation (11) is modified as,</p><disp-formula id="scirp.66466-formula24"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x50.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x51.png" xlink:type="simple"/></inline-formula> is the desired displacement of the real parts of the controlled eigenvalues. To illustrate the</p><p>movement of the real parts of the rightmost eigenvalues of two area LFC scheme for the preset upper bound delay 4s, <xref ref-type="fig" rid="fig2">Figure 2</xref> is shown.</p><p>Here the rightmost unstable eigenvalues whose real part is positive are shifted to negative real axis. The proposed algorithm converges to an optimum value at iteration on 142. At iteration 142 all the rightmost eigenvalues are moved to LHP. The final value of controller gain is K<sub>1</sub> = [−0.0233, −0.0146]<sup>T</sup>, K<sub>2</sub> = [0.0127, −0.0335]<sup>T</sup>. The spectrum of eigenvalues for final value of the controller gain is depicted in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>The proposed controller guarantees the stability for the delays smaller than the preset upper bound. The robustness of the controller is validated by finding an index called delay margin. The delay margin of the system is defined as the maximum tolerable value of time delay after which the system goes unstable. The delay margin of the system is computed using Frequency Sweeping Test which is discussed in the next section.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Illustration of the movement of the real parts of the rightmost eigenvalues for each iteration</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x52.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Rightmost eigenvalues for the feedback gain (K<sub>1</sub> = [−0.0233, −0.0146]<sup>T </sup>, K<sub>2</sub> = [0.0127, −0.0335]<sup>T</sup> at iteration 142)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x53.png"/></fig></sec></sec><sec id="s4"><title>4. Computation of Delay Margin</title><sec id="s4_1"><title>4.1. Frequency Sweeping Test (FST)</title><p>Frequency sweeping Test [<xref ref-type="bibr" rid="scirp.66466-ref2">2</xref>] is applied to analyze the asymptotic stability of the system and determine the value of delay margin. The stability of the system exists only for a subset of nonnegative delays. The necessary and sufficient condition for delay-dependent stability of the system is based on the following theorem.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x54.png" xlink:type="simple"/></inline-formula> be the delay margin. It is assumed that the system is stable at τ = 0. The rank of matrix A<sub>d</sub> is k. The delay margin can be defined as</p><disp-formula id="scirp.66466-formula25"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/18-7600588x55.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x56.png" xlink:type="simple"/></inline-formula>.</p><p>That is, the system remains stable for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x57.png" xlink:type="simple"/></inline-formula> and the system becomes unstable at τ = τ<sub>d</sub><sub>.</sub> The explanation for the above theorem is presented below</p><p> The generalized eigenvalues of the matrix pencil <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x58.png" xlink:type="simple"/></inline-formula><sub> </sub>is calculated for various frequencies.</p><p> The generalized eigenvalues of the matrix pencil <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x59.png" xlink:type="simple"/></inline-formula> becomes one at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x60.png" xlink:type="simple"/></inline-formula>. There exists a pair (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x61.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x62.png" xlink:type="simple"/></inline-formula>) at which the absolute value of each eigenvalue variation reaches one such that delay margin <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x63.png" xlink:type="simple"/></inline-formula> can be obtained.</p><p> For time delay<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x64.png" xlink:type="simple"/></inline-formula>, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x65.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x66.png" xlink:type="simple"/></inline-formula>. Then the system remains stable.</p><p> At <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x67.png" xlink:type="simple"/></inline-formula> the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x68.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x69.png" xlink:type="simple"/></inline-formula>. Then the system goes unstable.</p></sec><sec id="s4_2"><title>4.2. Algorithm for Delay Margin Calculation</title><p>The algorithm of Frequency sweeping Test for computing the delay margin is given below:</p><p>1) Obtain the maximum of real parts of all eigenvalues of the matrix A + A<sub>d</sub>. If it is less than zero proceed.</p><p>2) Find the rank of matrix A<sub>d</sub>. Consider rank(A<sub>d</sub>) = k. then the number of crossover points from right half plane to left half plane is k.</p><p>3) Choose the frequency range and step size of frequency range.</p><p>4) For different frequencies<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x70.png" xlink:type="simple"/></inline-formula>, find the absolute values of all the eigenvalues of the matrix pencil<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x71.png" xlink:type="simple"/></inline-formula>.</p><p>5) Determine the angle and frequency at which the absolute value of each eigenvalue variation reaches one. Otherwise go to step 3 and vary the frequency range.</p><p>6) Calculate the delay margin <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x72.png" xlink:type="simple"/></inline-formula></p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x73.png" xlink:type="simple"/></inline-formula>.</p></sec></sec><sec id="s5"><title>5. Case Study</title><p>Simulation studies have been carried out for multi- area LFC equipped with PI controller assuming the load change of 0.1 p.u in Area 1. The system parameters of each control area are listed in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The upper bounds of time delay in each area are preset as same value while designing the controllers. First the controller values are determined by using continuous pole placement method and then for the designed controller values, delay margin is theoretically calculated using FST. The theoretical results are presented in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>The theoretical value of delay margin is calculated as 34.612 s. That is, the controller designed using the proposed method for the preset upper bound of delay 8 s not only retains stability for time delays up to 8s, it can also ensure stability till 34.612 s (delay margin). To validate the theoretical results, simulation is performed using MATLAB/SIMULINK by increasing the delay step by step from zero until the LFC system becomes unstable. The simulation results are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref> from which it is observed that the delay margin of the system is 34.6 s which is very closer to the theoretical delay margin (34.612).</p><p>Similarly, the controller values of three-area LFC are determined using the proposed method for preset upper bound of time delay 10 s. The results are compared with the controller gain reported in [<xref ref-type="bibr" rid="scirp.66466-ref9">9</xref>] and shown in <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>The delay margin of the three-area LFC system with PI controller (designed using proposed method) is theoretically computed as 21.115 s whereas the method reported in (9) can maintain the stability only up to 14 s. This</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Frequency deviation of two area LFC for preset time delay 8s. (a) Area 1, (b) Area 2.</title></caption><fig id ="fig4_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x74.png"/></fig><fig id ="fig4_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x75.png"/></fig></fig-group><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> System parameters</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >T<sub>g</sub></th><th align="center" valign="middle" >T<sub>t</sub></th><th align="center" valign="middle" >R</th><th align="center" valign="middle" >D</th><th align="center" valign="middle" >Β</th><th align="center" valign="middle" >M</th><th align="center" valign="middle" >T<sub>o</sub></th></tr></thead><tr><td align="center" valign="middle" >Area 1</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.1986</td></tr><tr><td align="center" valign="middle" >Area 2</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >21.5</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >0.2148</td></tr><tr><td align="center" valign="middle" >Area 3</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >21.8</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >0.183</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Controller parameters of two area LFC system or preset upper bound of time delay 8 s</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Area</th><th align="center" valign="middle"  colspan="2"  >Controller parameters</th><th align="center" valign="middle"  colspan="2"  >Delay margin(s)</th></tr></thead><tr><td align="center" valign="middle" >K<sub>P</sub></td><td align="center" valign="middle" >K<sub>I</sub></td><td align="center" valign="middle" >Theoretical</td><td align="center" valign="middle" >From simulation</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >−0.0113</td><td align="center" valign="middle" >−0.0446</td><td align="center" valign="middle"  rowspan="2"  >34.612</td><td align="center" valign="middle"  rowspan="2"  >34.6</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.0125</td><td align="center" valign="middle" >−0.0405</td></tr></tbody></table></table-wrap><p>clearly shows that the proposed controller is highly robust compared to the existing method.</p><p>To validate the theoretical delay margin values, simulation is performed for three area LFC scheme keeping the preset upper bound of time delay as 10 s and the results are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>. The solid line shows the response of system for preset upper bound of delay 10 s and dashed line shows the response of the system for delay margin. The simulation results reveal that, the stability of the system is guaranteed for all time delays smaller than the delay margin. From the figure, it can be concluded that the delay margin of the system is 21.1s which is nearer to the theoretical delay margin 21.115 s.</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Frequency deviation of three area LFC for preset time delay 10 s. (a) Area 1, (b) Area 2, (c) Area 3.</title></caption><fig id ="fig5_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x76.png"/></fig><fig id ="fig5_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x77.png"/></fig><fig id ="fig5_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/18-7600588x78.png"/></fig></fig-group><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Controller parameters of three area LFC system for preset upper bound of time delay 10 s</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="4"  >Area</th><th align="center" valign="middle"  colspan="8"  >Controller gain and Delay margin</th></tr></thead><tr><td align="center" valign="middle"  colspan="4"  >Existing method [<xref ref-type="bibr" rid="scirp.66466-ref9">9</xref>]</td><td align="center" valign="middle"  colspan="4"  >Proposed method</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >K<sub>P</sub></td><td align="center" valign="middle"  rowspan="2"  >K<sub>I</sub></td><td align="center" valign="middle"  rowspan="2"  >K<sub>D</sub></td><td align="center" valign="middle"  rowspan="2"  >Delay margin (s)</td><td align="center" valign="middle"  rowspan="2"  >K<sub>P</sub></td><td align="center" valign="middle"  rowspan="2"  >K<sub>I</sub></td><td align="center" valign="middle"  colspan="2"  >Delay margin(s)</td></tr><tr><td align="center" valign="middle" >Theoretical</td><td align="center" valign="middle" >From simulation</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.0669</td><td align="center" valign="middle" >−0.0615</td><td align="center" valign="middle" >−0.0311</td><td align="center" valign="middle"  rowspan="3"  >14</td><td align="center" valign="middle" >0.0509</td><td align="center" valign="middle" >−0.0702</td><td align="center" valign="middle"  rowspan="3"  >21.115</td><td align="center" valign="middle"  rowspan="3"  >21.1</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.0305</td><td align="center" valign="middle" >−0.0885</td><td align="center" valign="middle" >−0.0325</td><td align="center" valign="middle" >0.0627</td><td align="center" valign="middle" >−0.0635</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.0704</td><td align="center" valign="middle" >−0.0688</td><td align="center" valign="middle" >−0.0302</td><td align="center" valign="middle" >0.0425</td><td align="center" valign="middle" >−0.0455</td></tr></tbody></table></table-wrap></sec><sec id="s6"><title>6. Conclusion</title><p>In this paper, a robust controller based on continuous pole placement method is designed for multi area LFC scheme affected by communication delays. The controller values are determined by shifting the rightmost eigenvalues to left half plane in a quasi continuous way for any particular preset upper bound of time delay. The proposed controller is highly robust in sustaining the stability of the system even for delays greater than the preset upper bound of time delay. Case studies have been carried out for two area and three area LFC schemes. The efficiency of the controller is validated by finding the value of time delay margin theoretically using Frequency Sweeping test. The theoretical value of delay margin is verified using simulation studies. Simulation result shows that the proposed controller gives larger stability margin.</p></sec><sec id="s7"><title>Cite this paper</title><p>T. Jesintha Mary,P. Rangarajan, (2016) Design of Robust Controller for LFC of Interconnected Power System Considering Communication Delays. Circuits and Systems,07,794-804. doi: 10.4236/cs.2016.76068</p></sec><sec id="s8"><title>Appendix 1</title><p>Lemma.</p><p>Let f(λ) and the sequence {f<sub>n</sub>(λ)}<sub>n≥</sub><sub>1</sub> be analytic functions on an (open) domain D ⊆ C. Suppose that {f<sub>n</sub>(λ)}<sub>n≥</sub><sub>1</sub> converges uniformly to f(λ) on the disc <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x79.png" xlink:type="simple"/></inline-formula> for some R&gt;0 and that on this disc</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x80.png" xlink:type="simple"/></inline-formula>is the only zero of f(λ); with multiplicity k≥0 (k = 0 means no zeros in D). Then there exists a number N ∈ N such that ∀n≥N; f<sub>n</sub>(λ) has exactly k zeros <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x81.png" xlink:type="simple"/></inline-formula> in D and lim<sub>n→∞</sub>λ<sub>n,j</sub> = λ<sub>0</sub>;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x82.png" xlink:type="simple"/></inline-formula>.</p><p>With this lemma, continuity properties of the spectrum with respect to the feedback gain K can easily be deduced.</p><p>Theorem. For the system <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x83.png" xlink:type="simple"/></inline-formula> the individual eigenvalues are continuous with respect to changes in the controller gain K. Moreover <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/18-7600588x84.png" xlink:type="simple"/></inline-formula> is continuous w.r.t. K.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.66466-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kundur, P. (1994) Power System Stability and Control. McGraw-Hill Inc., New York.</mixed-citation></ref><ref id="scirp.66466-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Gu, K., Kharitonoy, V.L. and Chen, J. (2003) Stability of Time Delay Systems. 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