<?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">JPEE</journal-id><journal-title-group><journal-title>Journal of Power and Energy Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-588X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jpee.2015.311005</article-id><article-id pub-id-type="publisher-id">JPEE-61606</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>
 
 
  Preferred Economic Dispatch of Thermal Power Units
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>elvaraj</surname><given-names>Durai</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>Srikrishna</surname><given-names>Subramanian</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sivarajan</surname><given-names>Ganesan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Electrical Engineering, Annamalai University, Chidambaram, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>duraiselvaraj86@gmail.com(ED)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>11</day><month>11</month><year>2015</year></pub-date><volume>03</volume><issue>11</issue><fpage>47</fpage><lpage>69</lpage><history><date date-type="received"><day>12</day>	<month>October</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>27</month>	<year>November</year>	</date><date date-type="accepted"><day>30</day>	<month>November</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   Economic Dispatch (ED) problem is one of the main concerns of the power generation operations which are basically solved to generate optimal amount of power from the generating units in the system by minimizing the fuel cost and by satisfying the system constraints. The accuracy of ED solutions is highly influenced by the fuel cost parameters of the generating units. Generally, the parameters are subjected to transform due to aging process and other external issues. Further the parameters associated with the transmission line modelling also change due to aforementioned issues. The loss coefficients which are the functions of transmission line parameters get altered from the original value over a time. Hence, the periodical estimation of these coefficients is highly essential in power system problems for obtaining ideal solutions for ED problem. Estimating the ideal parameters of the ED problem may be the best solution for this issue. This paper presents the Teaching Learning Based Optimization (TLBO) algorithm to estimate the parameters associated with ED problem. The estimation problem is formulated as an error minimization problem. This work provides a frame work for the computation of coefficients for quadratic function, piecewise quadratic cost function, emission function, transmission line parameters and loss coefficients. The effectiveness of TLBO is tested with 2 standard test systems and an Indian utility system. 
 
</p></abstract><kwd-group><kwd>Parameter Estimation</kwd><kwd> Cost Coefficients</kwd><kwd> Emission Coefficients</kwd><kwd> Error Estimation</kwd><kwd> Transmission Line Parameters</kwd><kwd> Teaching Learning Based Optimization</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><sec id="s1_1"><title>1.1. Ideal Economic Dispatch</title><p>The economical operation of power system needs more accurate representation of fuel cost coefficients and transmission loss coefficients. Due to changing weather conditions and other external issues, the aforesaid coefficients are not ideal and hence the existing parameters with ED solutions also change. Therefore, the objective of this article is to revise the existing parameters for the Preferred Economic Dispatch (PED) solutions.</p></sec><sec id="s1_2"><title>1.2. Literature Review</title><p>Various optimization techniques have been proposed by many researchers to deal with the parameter estimation problems. To obtain the exact parameters for ED problems different parameter estimation rehearsal has been projected to solve estimation problems in power systems. State estimation based technique such as Least Error Square (LES) and least absolute value methods have been demonstrated. Among the two techniques, LES technique has been the most famous static estimation technique and in use for a long time as the preferred technique for optimum estimation of parameters. In general, some limitations and disadvantages are associated with this approach. El-Hawary and Mansour conducted performance analysis of LES, Bard algorithm, Marquardt algorithm and Powell regression algorithm for estimating coefficients [<xref ref-type="bibr" rid="scirp.61606-ref1">1</xref>] . The methods based on the least absolute value approximations and curve fitting techniques have been reported for fuel cost coefficients estimation [<xref ref-type="bibr" rid="scirp.61606-ref2">2</xref>] . Two polynomial curve fitting methods, Gram-Schmidt orthonormalization and least square are also applied to evaluate the fuel cost coefficients [<xref ref-type="bibr" rid="scirp.61606-ref3">3</xref>] . Further Henry Y. K. Chen and Charles E. Postel applied sequential regression technique to online parameter estimation of input-output curves for thermal units [<xref ref-type="bibr" rid="scirp.61606-ref4">4</xref>] .</p><p>Research endeavours indicate that the field of Transmission Line Parameters (TLP) estimation in power system studies is less focused. Traditionally, tower and conductor geometric parameters, conductor type, assumed ambient conditions etc., are utilized for estimating TLP [<xref ref-type="bibr" rid="scirp.61606-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.61606-ref7">7</xref>] . The sending and receiving end voltage and current phasors are utilized to derive the TLP and propagation constant [<xref ref-type="bibr" rid="scirp.61606-ref8">8</xref>] . The synchronized phasor measurements at both ends of the transmission line emphasises the online parameter estimation [<xref ref-type="bibr" rid="scirp.61606-ref9">9</xref>] - [<xref ref-type="bibr" rid="scirp.61606-ref12">12</xref>] . Wagenaars et al., have proposed the measurement method, based on a pulse response measurement, to determine the transmission line parameters of the shield-to-phase and phase-to-phase modes [<xref ref-type="bibr" rid="scirp.61606-ref13">13</xref>] . Researchers have reported Newton-Raphson based method for estimating TLP parameters utilizing the measurements of voltage, current and power [<xref ref-type="bibr" rid="scirp.61606-ref14">14</xref>] .</p><p>A new category of classical optimization techniques has emerged to cope with some of the traditional algorithms in the field of power system estimation problems. The heuristic techniques such as Genetic Algorithm (GA) [<xref ref-type="bibr" rid="scirp.61606-ref15">15</xref>] , Particle Swarm Optimization (PSO) [<xref ref-type="bibr" rid="scirp.61606-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.61606-ref17">17</xref>] , Artificial Bee Colony (ABC) [<xref ref-type="bibr" rid="scirp.61606-ref18">18</xref>] , Artificial Neural Network (ANN) [<xref ref-type="bibr" rid="scirp.61606-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.61606-ref20">20</xref>] , Fuzzy Logic (FL) [<xref ref-type="bibr" rid="scirp.61606-ref21">21</xref>] , Ant Colony Optimization (ACO) [<xref ref-type="bibr" rid="scirp.61606-ref22">22</xref>] and Bacterial Foraging Algorithm (BFA) [<xref ref-type="bibr" rid="scirp.61606-ref23">23</xref>] - [<xref ref-type="bibr" rid="scirp.61606-ref25">25</xref>] have been used for solving various estimation problems such as load forecasting, state estimation and induction motor parameters.</p></sec><sec id="s1_3"><title>1.3. Optimization Techniques</title><p>The heuristic techniques outperform the mathematical methods but their solution quality is sensitive to the algorithmic controlling parameters like population size and number of generations. Besides common control parameters, different algorithms require their own algorithm specific control parameters. Major disadvantage of ABC, PSO and GA are the presence of various parameters that need to be carefully tuned to reach acceptable estimation performance. Recently, TLBO, a nature inspired algorithm that is based on the effect of influence of a teacher on the output of learners in a class [<xref ref-type="bibr" rid="scirp.61606-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.61606-ref27">27</xref>] is proposed. It is a powerful evolutionary algorithm that maintains a population of students, where each student represents a potential solution to an optimisation problem. Each searching generation includes initializing of class, teacher phase, learner phase and termination criterion. The advantage of TLBO are simple, easy implementation and necessitates few control parameters for tuning that make it suitable to implement for power system parameter estimation problems. TLBO is an algorithm-specific, parameter-less algorithm that does not require any algorithm-specific parameters to be tuned [<xref ref-type="bibr" rid="scirp.61606-ref28">28</xref>] . This algorithm can find the global solution for nonlinear constrained optimization problems with less computation effort and high consistency [<xref ref-type="bibr" rid="scirp.61606-ref29">29</xref>] . The authors have proposed the TLBO algorithm for estimating the accurate parameters of the input output characteristics of thermal units [<xref ref-type="bibr" rid="scirp.61606-ref30">30</xref>] . The adaptable properties of this algorithm encourage the authors to use TLBO as a parameter estimator.</p></sec><sec id="s1_4"><title>1.4. Research Gap and Motivation</title><p>The most important issue in ED problem is to have an accurate estimate of parameters. The exact ED solution in power generation and the estimation of parameters in transmission systems is an important task in power systems. The demonstration of literature review reveals that the estimation of accurate fuel cost coefficients and transmission line parameters are carried out independently. The impact of change in transmission line parameters on the loss coefficients of ED problem is seldom carried out. These points motivate us to contribute research in estimation of cost and emission coefficients, transmission line parameters and transmission loss coefficients for the exact ED solution. The TLBO algorithm is implemented for solving parameter and ED problems on different scale of test systems.</p></sec><sec id="s1_5"><title>1.5. Highlights</title><p>・ Accurate parameters of different generator cost functions and transmission lines are estimated.</p><p>・ The preferred economic dispatch is carried out.</p><p>・ A 19 unit practical Indian utility system is considered.</p><p>・ A nature inspired TLBO is applied for both estimation of parameters and for solving ED problems.</p></sec><sec id="s1_6"><title>1.6. Paper Organization</title><p>The rest of the paper is structured as follows: Problem formulation is explored in Section 2. Section 3 describes the implementation for preferred ED. The detailed discussions about numerical results achieved by various test systems are detailed in Section 4. Section 5 describes the potential verification of TLBO. Finally, Section 6 presents the conclusions of this article.</p></sec></sec><sec id="s2"><title>2. Problem Formulation</title><sec id="s2_1"><title>2.1. State of the Art Model</title><p>The state of the art multi objective ED model is presented as follows.</p><disp-formula id="scirp.61606-formula1352"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x6.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x7.png" xlink:type="simple"/></inline-formula>is a existing fuel cost function, N is the number of generating units and P<sub>i</sub> is the power generated by ith generating unit.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x8.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x10.png" xlink:type="simple"/></inline-formula>are the existing cost coefficients, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x11.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x12.png" xlink:type="simple"/></inline-formula>are the existing valve point coefficients and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x13.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x14.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x15.png" xlink:type="simple"/></inline-formula>are the existing emission coefficients .</p><p>W<sub>1</sub> and W<sub>2</sub> are the weights of the function.</p><p>r<sub>i</sub> is the error associated with the ith equation.</p><p>Loss function:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x16.png" xlink:type="simple"/></inline-formula> (2)</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x17.png" xlink:type="simple"/></inline-formula>indicates existing transmission loss.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x18.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x19.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x20.png" xlink:type="simple"/></inline-formula>are the existing transmission loss coefficients.</p></sec><sec id="s2_2"><title>2.2. Proposed Parameter Estimation Problems</title><p>For preferred ED solution, the accurate parameters for fuel cost, emission, and transmission line and transmission loss are needed. Those parameters can be estimated by solving the following problems.</p><p>Cost coefficients Estimation, FC<sup>Est</sup> = Estimate [a, b, c, e, f]</p><p>Emission coefficients Estimation, E<sup>Est</sup> = Estimate [e<sub>0</sub>, e<sub>1</sub>, e<sub>2</sub>]</p><p>Transmission line parameters Estimation, TLP<sup>Est</sup> = Estimate [R, X, B]</p><p>Transmission loss coefficients Estimation, KC<sup>Est</sup> = Estimate [B<sub>ij</sub>, B<sub>0i</sub>, B<sub>00</sub>]</p><p>In general to estimate the accurate parameters, the following function are used</p><disp-formula id="scirp.61606-formula1353"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x21.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_3"><title>2.3. Accurate Model Using Estimated Parameters</title><p>The cost function of generating unit is expressed using estimated coefficients as follows,</p><disp-formula id="scirp.61606-formula1354"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x22.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x23.png" xlink:type="simple"/></inline-formula> is an estimated fuel cost.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x24.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x26.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x27.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x28.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x29.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x30.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x31.png" xlink:type="simple"/></inline-formula>are the estimated cost coefficients, valve point coefficients and emission coefficients respectively.</p><p>Loss function:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x32.png" xlink:type="simple"/></inline-formula> (5)</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x33.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x34.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x35.png" xlink:type="simple"/></inline-formula>are the estimated transmission loss coefficients and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x36.png" xlink:type="simple"/></inline-formula> is the estimated transmission loss.</p></sec><sec id="s2_4"><title>2.4. Error Minimization</title><p>As detailed in [<xref ref-type="bibr" rid="scirp.61606-ref30">30</xref>] , the error is estimated for fuel cost and emission coefficients as follows</p><p>The error at each step i can be calculated as,</p><disp-formula id="scirp.61606-formula1355"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x37.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61606-formula1356"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x38.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61606-formula1357"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x39.png"  xlink:type="simple"/></disp-formula><p>The % error for each step k of transmission line parameter is expressed as,</p><disp-formula id="scirp.61606-formula1358"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x40.png"  xlink:type="simple"/></disp-formula><p>The objective function is minimised subjected to physical limits of each coefficients and TLP.</p></sec></sec><sec id="s3"><title>3. Implementation of TLBO for Preferred Economic Dispatch (PED)</title><p>This section details the computational flows for parameter estimation and PED problems.</p><sec id="s3_1"><title>3.1. Parameter Estimation Procedure</title><p>Step 1: Read the required data for estimating the parameters, population size, maximum number of iterations (Iter<sub>max</sub>), maximum and minimum limits of parameters (PA<sup>min</sup>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x41.png" xlink:type="simple"/></inline-formula>).</p><p>Step 2:Randomly generate parameters using the following equation,</p><disp-formula id="scirp.61606-formula1359"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x42.png"  xlink:type="simple"/></disp-formula><p>Step 3: Check for the constraint violation.</p><p>Step 4: If the limit is violated, then upgrade the parameters of the units using the following equation</p><disp-formula id="scirp.61606-formula1360"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1770175x43.png"  xlink:type="simple"/></disp-formula><p>Step 5: Calculate FC<sup>Est</sup> by using Equations (4).</p><p>Step 6: The error and % error associated with each measurement can be calculated by using Equations (6), (7), (8) and (9).</p><p>Step 7: Teacher phase: Compute the difference between existing mean result and best mean by utilizing teaching factor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1770175x44.png" xlink:type="simple"/></inline-formula>.</p><p>Step 8: Learner phase: Evaluate the learners’ parameter values with the help of teacher’s parameter values.</p><p>Step 9: Update the parameters subject to constraints.</p><p>Step 10: Stopping Criterion: If Iter ≥ Iter<sub>max</sub> print the optimal results, otherwise go to step 7.</p></sec><sec id="s3_2"><title>3.2. Computational Flow of PED</title><p>Hence the estimated parameters are suitably achieved. The ED solution is carried out and the computational flow is as follows in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p></sec></sec><sec id="s4"><title>4. Numerical Simulation Results and Discussion</title><p>This section presents three different test systems such as 10 unit, IEEE 30 bus and a practical Indian Utility system to demonstrate the efficacy of the proposed solution technique for perfect estimate of parameters and preferred ED solutions. The algorithm is implemented in Matlab package and simulations are carried out on a personal computer having the configuration of Intel(R) core i3 CPU with 2 GB RAM. The following algorithmic parameters are chosen for all cases in order to validate the performance of the algorithm: Population size = 10;</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Flowchart for preferred economic dispatch using TLBO</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1770175x45.png"/></fig><p>Maximum number of iterations = 120.</p><sec id="s4_1"><title>4.1. Test System 1: 10 Unit System with Piecewise Quadratic Functions</title><p>This test system consists of 10-generating units in which each unit has two or three fuel options like coal, oil and gas. As more than one fuel is used, the generator input-output characteristic is expressed as a piecewise quadratic function. The valve point effects are also considered. The test system data is available in [<xref ref-type="bibr" rid="scirp.61606-ref31">31</xref>] .</p><p>The generator characteristic is expressed as a piecewise quadratic function including valve point effects increases the number of variables to be estimated. In this test system, the generator 1 has two fuel options and the remaining units have three fuel options. It is specified that the fuel 2 is uneconomical for generator 9. The simulation is carried out using the proposed TLBO which acquires new values for cost coefficients and are presented in the <xref ref-type="table" rid="table1">Table 1</xref>. The estimation process has been performed for each generation level and the results of existing</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Estimation of piecewise quadratic cost function coefficients using TLBO-10 unit system</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Unit</th><th align="center" valign="middle"  colspan="2"  >P (MW)</th><th align="center" valign="middle"  rowspan="2"  >Fuel type</th><th align="center" valign="middle"  colspan="5"  >Coefficients estimated by TLBO</th><th align="center" valign="middle"  colspan="2"  >FC<sup>Ex</sup><sup>i</sup> ($/h)</th><th align="center" valign="middle"  colspan="3"  >FC<sup>E</sup><sup>st</sup> ($/h)</th><th align="center" valign="middle"  colspan="2"  >∑<sub>error</sub></th></tr></thead><tr><td align="center" valign="middle" >Min</td><td align="center" valign="middle" >Max</td><td align="center" valign="middle" >a<sub>i</sub></td><td align="center" valign="middle" >b<sub>i</sub></td><td align="center" valign="middle" >c<sub>i</sub></td><td align="center" valign="middle" >e<sub>i</sub></td><td align="center" valign="middle" >f<sub>i</sub></td><td align="center" valign="middle" >Min</td><td align="center" valign="middle" >Max</td><td align="center" valign="middle" >Min</td><td align="center" valign="middle"  colspan="2"  >Max</td><td align="center" valign="middle" >TLBO</td><td align="center" valign="middle" >ABC</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >1</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >196</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >25.19938</td><td align="center" valign="middle" >−0.380846</td><td align="center" valign="middle" >0.0021609</td><td align="center" valign="middle" >0.025324</td><td align="center" valign="middle" >−3.028257</td><td align="center" valign="middle" >8.980000</td><td align="center" valign="middle" >32.6800</td><td align="center" valign="middle"  colspan="2"  >8.723994</td><td align="center" valign="middle" >33.59283</td><td align="center" valign="middle" >1.168802</td><td align="center" valign="middle" >3.98151</td></tr><tr><td align="center" valign="middle" >196</td><td align="center" valign="middle" >250</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >20.03000</td><td align="center" valign="middle" >−0.305900</td><td align="center" valign="middle" >0.0018897</td><td align="center" valign="middle" >0.021337</td><td align="center" valign="middle" >−3.009000</td><td align="center" valign="middle" >32.66577</td><td align="center" valign="middle" >60.9879</td><td align="center" valign="middle"  colspan="2"  >32.67157</td><td align="center" valign="middle" >61.67932</td><td align="center" valign="middle" >0.697156</td><td align="center" valign="middle" >2.81373</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >2</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >114</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1.816721</td><td align="center" valign="middle" >−0.037780</td><td align="center" valign="middle" >0.0011015</td><td align="center" valign="middle" >0.001901</td><td align="center" valign="middle" >−0.410800</td><td align="center" valign="middle" >22.54490</td><td align="center" valign="middle" >48.4386</td><td align="center" valign="middle"  colspan="2"  >23.48145</td><td align="center" valign="middle" >49.14125</td><td align="center" valign="middle" >1.639115</td><td align="center" valign="middle" >3.25496</td></tr><tr><td align="center" valign="middle" >114</td><td align="center" valign="middle" >157</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >12.94016</td><td align="center" valign="middle" >−0.198000</td><td align="center" valign="middle" >0.0016731</td><td align="center" valign="middle" >0.013159</td><td align="center" valign="middle" >−1.880000</td><td align="center" valign="middle" >2.716000</td><td align="center" valign="middle" >12.1088</td><td align="center" valign="middle"  colspan="2"  >2.681891</td><td align="center" valign="middle" >11.82574</td><td align="center" valign="middle" >0.317203</td><td align="center" valign="middle" >2.75457</td></tr><tr><td align="center" valign="middle" >157</td><td align="center" valign="middle" >230</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >120.6888</td><td align="center" valign="middle" >−1.282684</td><td align="center" valign="middle" >0.0042228</td><td align="center" valign="middle" >0.112869</td><td align="center" valign="middle" >−11.94430</td><td align="center" valign="middle" >12.13152</td><td align="center" valign="middle" >22.4996</td><td align="center" valign="middle"  colspan="2"  >12.12238</td><td align="center" valign="middle" >23.09567</td><td align="center" valign="middle" >0.605175</td><td align="center" valign="middle" >2.93069</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >3</td><td align="center" valign="middle" >200</td><td align="center" valign="middle" >332</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >39.04620</td><td align="center" valign="middle" >−0.305817</td><td align="center" valign="middle" >0.0014527</td><td align="center" valign="middle" >0.039875</td><td align="center" valign="middle" >−3.115954</td><td align="center" valign="middle" >35.75000</td><td align="center" valign="middle" >96.9444</td><td align="center" valign="middle"  colspan="2"  >35.98904</td><td align="center" valign="middle" >97.64218</td><td align="center" valign="middle" >0.936732</td><td align="center" valign="middle" >1.59272</td></tr><tr><td align="center" valign="middle" >332</td><td align="center" valign="middle" >388</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >−2.97500</td><td align="center" valign="middle" >0.032890</td><td align="center" valign="middle" >0.0008075</td><td align="center" valign="middle" >−0.002976</td><td align="center" valign="middle" >0.336952</td><td align="center" valign="middle" >131.3536</td><td align="center" valign="middle" >187.056</td><td align="center" valign="middle"  colspan="2"  >131.7986</td><td align="center" valign="middle" >187.3240</td><td align="center" valign="middle" >0.712539</td><td align="center" valign="middle" >1.27426</td></tr><tr><td align="center" valign="middle" >388</td><td align="center" valign="middle" >500</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−58.1400</td><td align="center" valign="middle" >0.484892</td><td align="center" valign="middle" >1.196E−05</td><td align="center" valign="middle" >−0.058140</td><td align="center" valign="middle" >4.764000</td><td align="center" valign="middle" >96.94140</td><td align="center" valign="middle" >131.236</td><td align="center" valign="middle"  colspan="2"  >96.94769</td><td align="center" valign="middle" >131.3470</td><td align="center" valign="middle" >0.116458</td><td align="center" valign="middle" >1.66413</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >4</td><td align="center" valign="middle" >99</td><td align="center" valign="middle" >138</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.990265</td><td align="center" valign="middle" >−0.031040</td><td align="center" valign="middle" >0.0010434</td><td align="center" valign="middle" >0.001982</td><td align="center" valign="middle" >−0.310400</td><td align="center" valign="middle" >9.181389</td><td align="center" valign="middle" >17.6636</td><td align="center" valign="middle"  colspan="2"  >9.143991</td><td align="center" valign="middle" >17.57876</td><td align="center" valign="middle" >0.122282</td><td align="center" valign="middle" >1.15842</td></tr><tr><td align="center" valign="middle" >138</td><td align="center" valign="middle" >200</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >52.94079</td><td align="center" valign="middle" >−0.633800</td><td align="center" valign="middle" >0.0027499</td><td align="center" valign="middle" >0.053850</td><td align="center" valign="middle" >−6.248000</td><td align="center" valign="middle" >17.77095</td><td align="center" valign="middle" >36.2506</td><td align="center" valign="middle"  colspan="2"  >17.84586</td><td align="center" valign="middle" >36.22169</td><td align="center" valign="middle" >0.103847</td><td align="center" valign="middle" >0.43500</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >265</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >258.6681</td><td align="center" valign="middle" >−2.290143</td><td align="center" valign="middle" >0.0058688</td><td align="center" valign="middle" >0.269957</td><td align="center" valign="middle" >−22.39430</td><td align="center" valign="middle" >36.60000</td><td align="center" valign="middle" >64.2124</td><td align="center" valign="middle"  colspan="2"  >35.39341</td><td align="center" valign="middle" >64.15721</td><td align="center" valign="middle" >1.261771</td><td align="center" valign="middle" >4.91182</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >5</td><td align="center" valign="middle" >190</td><td align="center" valign="middle" >338</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >13.80777</td><td align="center" valign="middle" >−0.088330</td><td align="center" valign="middle" >0.0010722</td><td align="center" valign="middle" >0.013720</td><td align="center" valign="middle" >−0.870300</td><td align="center" valign="middle" >35.80990</td><td align="center" valign="middle" >106.192</td><td align="center" valign="middle"  colspan="2"  >35.73286</td><td align="center" valign="middle" >106.449</td><td align="center" valign="middle" >0.333505</td><td align="center" valign="middle" >1.15977</td></tr><tr><td align="center" valign="middle" >338</td><td align="center" valign="middle" >407</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >99.87032</td><td align="center" valign="middle" >−0.515692</td><td align="center" valign="middle" >0.0015799</td><td align="center" valign="middle" >0.099573</td><td align="center" valign="middle" >−5.182580</td><td align="center" valign="middle" >106.2448</td><td align="center" valign="middle" >152.504</td><td align="center" valign="middle"  colspan="2"  >106.0639</td><td align="center" valign="middle" >151.7490</td><td align="center" valign="middle" >0.936775</td><td align="center" valign="middle" >5.70216</td></tr><tr><td align="center" valign="middle" >407</td><td align="center" valign="middle" >490</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >−52.9900</td><td align="center" valign="middle" >0.445057</td><td align="center" valign="middle" >0.0001478</td><td align="center" valign="middle" >−0.053890</td><td align="center" valign="middle" >4.560945</td><td align="center" valign="middle" >152.4276</td><td align="center" valign="middle" >200.634</td><td align="center" valign="middle"  colspan="2"  >152.6311</td><td align="center" valign="middle" >200.6286</td><td align="center" valign="middle" >0.208988</td><td align="center" valign="middle" >0.41948</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >6</td><td align="center" valign="middle" >138</td><td align="center" valign="middle" >200</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >52.95000</td><td align="center" valign="middle" >−0.631800</td><td align="center" valign="middle" >0.0027309</td><td align="center" valign="middle" >0.052750</td><td align="center" valign="middle" >−6.308000</td><td align="center" valign="middle" >17.77095</td><td align="center" valign="middle" >36.2506</td><td align="center" valign="middle"  colspan="2"  >17.76962</td><td align="center" valign="middle" >35.88033</td><td align="center" valign="middle" >0.371620</td><td align="center" valign="middle" >1.59502</td></tr><tr><td align="center" valign="middle" >85</td><td align="center" valign="middle" >138</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1.976247</td><td align="center" valign="middle" >−0.031040</td><td align="center" valign="middle" >0.0010540</td><td align="center" valign="middle" >0.001973</td><td align="center" valign="middle" >−0.310400</td><td align="center" valign="middle" >6.915125</td><td align="center" valign="middle" >17.6642</td><td align="center" valign="middle"  colspan="2"  >6.952709</td><td align="center" valign="middle" >17.76567</td><td align="center" valign="middle" >0.139008</td><td align="center" valign="middle" >0.91532</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >265</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >265.4849</td><td align="center" valign="middle" >−2.333976</td><td align="center" valign="middle" >0.0059502</td><td align="center" valign="middle" >0.261282</td><td align="center" valign="middle" >−23.28925</td><td align="center" valign="middle" >36.60000</td><td align="center" valign="middle" >64.2124</td><td align="center" valign="middle"  colspan="2"  >36.69646</td><td align="center" valign="middle" >64.94455</td><td align="center" valign="middle" >0.828617</td><td align="center" valign="middle" >2.44408</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >7</td><td align="center" valign="middle" >200</td><td align="center" valign="middle" >331</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >18.88226</td><td align="center" valign="middle" >−0.132500</td><td align="center" valign="middle" >0.0011050</td><td align="center" valign="middle" >0.018850</td><td align="center" valign="middle" >−1.355000</td><td align="center" valign="middle" >36.71000</td><td align="center" valign="middle" >96.3699</td><td align="center" valign="middle"  colspan="2"  >36.58365</td><td align="center" valign="middle" >96.11233</td><td align="center" valign="middle" >0.383942</td><td align="center" valign="middle" >2.96959</td></tr><tr><td align="center" valign="middle" >331</td><td align="center" valign="middle" >391</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >44.00000</td><td align="center" valign="middle" >−0.220000</td><td align="center" valign="middle" >0.0011464</td><td align="center" valign="middle" >0.043769</td><td align="center" valign="middle" >−2.211000</td><td align="center" valign="middle" >96.37086</td><td align="center" valign="middle" >133.271</td><td align="center" valign="middle"  colspan="2"  >96.77999</td><td align="center" valign="middle" >133.2703</td><td align="center" valign="middle" >0.410536</td><td align="center" valign="middle" >1.94797</td></tr><tr><td align="center" valign="middle" >391</td><td align="center" valign="middle" >500</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >−43.0000</td><td align="center" valign="middle" >0.356873</td><td align="center" valign="middle" >0.0002422</td><td align="center" valign="middle" >−0.043000</td><td align="center" valign="middle" >3.552032</td><td align="center" valign="middle" >133.3239</td><td align="center" valign="middle" >195.993</td><td align="center" valign="middle"  colspan="2"  >133.5603</td><td align="center" valign="middle" >196.0080</td><td align="center" valign="middle" >0.251265</td><td align="center" valign="middle" >2.66318</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >8</td><td align="center" valign="middle" >99</td><td align="center" valign="middle" >138</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.984912</td><td align="center" valign="middle" >−0.031000</td><td align="center" valign="middle" >0.0010294</td><td align="center" valign="middle" >0.001992</td><td align="center" valign="middle" >−0.310000</td><td align="center" valign="middle" >9.181389</td><td align="center" valign="middle" >17.6636</td><td align="center" valign="middle"  colspan="2"  >9.005129</td><td align="center" valign="middle" >17.31185</td><td align="center" valign="middle" >0.528055</td><td align="center" valign="middle" >1.15768</td></tr><tr><td align="center" valign="middle" >138</td><td align="center" valign="middle" >200</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >52.76360</td><td align="center" valign="middle" >−0.630000</td><td align="center" valign="middle" >0.0027294</td><td align="center" valign="middle" >0.052870</td><td align="center" valign="middle" >−6.375000</td><td align="center" valign="middle" >17.77095</td><td align="center" valign="middle" >36.2506</td><td align="center" valign="middle"  colspan="2"  >17.80167</td><td align="center" valign="middle" >35.96774</td><td align="center" valign="middle" >0.313608</td><td align="center" valign="middle" >1.13761</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >265</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >266.5000</td><td align="center" valign="middle" >−2.330000</td><td align="center" valign="middle" >0.0059150</td><td align="center" valign="middle" >0.260000</td><td align="center" valign="middle" >−23.00000</td><td align="center" valign="middle" >36.60000</td><td align="center" valign="middle" >64.2124</td><td align="center" valign="middle"  colspan="2"  >37.10000</td><td align="center" valign="middle" >64.53166</td><td align="center" valign="middle" >0.819262</td><td align="center" valign="middle" >4.66804</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >9</td><td align="center" valign="middle" >213</td><td align="center" valign="middle" >370</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >88.56713</td><td align="center" valign="middle" >−0.566963</td><td align="center" valign="middle" >0.0015544</td><td align="center" valign="middle" >0.088509</td><td align="center" valign="middle" >−5.684923</td><td align="center" valign="middle" >38.15592</td><td align="center" valign="middle" >91.3812</td><td align="center" valign="middle"  colspan="2"  >38.32396</td><td align="center" valign="middle" >91.61140</td><td align="center" valign="middle" >0.398192</td><td align="center" valign="middle" >2.68979</td></tr><tr><td align="center" valign="middle" >130</td><td align="center" valign="middle" >213</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >14.20019</td><td align="center" valign="middle" >−0.018100</td><td align="center" valign="middle" >0.0006124</td><td align="center" valign="middle" >0.014100</td><td align="center" valign="middle" >−0.181000</td><td align="center" valign="middle" >22.21239</td><td align="center" valign="middle" >38.1385</td><td align="center" valign="middle"  colspan="2"  >22.19758</td><td align="center" valign="middle" >38.14001</td><td align="center" valign="middle" >0.016320</td><td align="center" valign="middle" >1.07008</td></tr><tr><td align="center" valign="middle" >370</td><td align="center" valign="middle" >440</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >14.10104</td><td align="center" valign="middle" >−0.018100</td><td align="center" valign="middle" >0.0006111</td><td align="center" valign="middle" >0.014280</td><td align="center" valign="middle" >−0.181000</td><td align="center" valign="middle" >91.30359</td><td align="center" valign="middle" >124.739</td><td align="center" valign="middle"  colspan="2"  >91.06478</td><td align="center" valign="middle" >124.4491</td><td align="center" valign="middle" >0.529615</td><td align="center" valign="middle" >5.65214</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >10</td><td align="center" valign="middle" >200</td><td align="center" valign="middle" >362</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >13.99000</td><td align="center" valign="middle" >−0.099100</td><td align="center" valign="middle" >0.0011054</td><td align="center" valign="middle" >0.013887</td><td align="center" valign="middle" >−0.992500</td><td align="center" valign="middle" >38.17400</td><td align="center" valign="middle" >122.414</td><td align="center" valign="middle"  colspan="2"  >38.38720</td><td align="center" valign="middle" >122.9832</td><td align="center" valign="middle" >0.781727</td><td align="center" valign="middle" >1.87694</td></tr><tr><td align="center" valign="middle" >362</td><td align="center" valign="middle" >407</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >46.65000</td><td align="center" valign="middle" >−0.201400</td><td align="center" valign="middle" >0.0011360</td><td align="center" valign="middle" >0.046801</td><td align="center" valign="middle" >−2.014000</td><td align="center" valign="middle" >152.6864</td><td align="center" valign="middle" >198.035</td><td align="center" valign="middle"  colspan="2"  >152.7299</td><td align="center" valign="middle" >198.0353</td><td align="center" valign="middle" >0.043682</td><td align="center" valign="middle" >1.10165</td></tr><tr><td align="center" valign="middle" >407</td><td align="center" valign="middle" >490</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−61.0900</td><td align="center" valign="middle" >0.508437</td><td align="center" valign="middle" >4.157E−05</td><td align="center" valign="middle" >−0.061100</td><td align="center" valign="middle" >5.074000</td><td align="center" valign="middle" >122.4382</td><td align="center" valign="middle" >152.677</td><td align="center" valign="middle"  colspan="2"  >122.6075</td><td align="center" valign="middle" >152.8768</td><td align="center" valign="middle" >0.368904</td><td align="center" valign="middle" >1.08521</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>fuel cost (FC<sup>Exi</sup>) and estimated fuel cost (FC<sup>Est</sup>) are presented independently for each fuel type in the <xref ref-type="table" rid="table1">Table 1</xref>. The error is also computed by comparing FC<sup>Exi</sup> and FC<sup>Est</sup> using Equation (6). The obtained error using the proposed algorithm is compared with ABC algorithm which clearly illustrates the superiority of TLBO over other algorithm.</p><p>The ED is carried out separately considering both existing and estimated fuel cost coefficients. The obtained results for various demands are presented in <xref ref-type="table" rid="table2">Table 2</xref> along with % error, which clearly illustrates the impact of estimated coefficients on ED problem.</p></sec><sec id="s4_2"><title>4.2. Test System 2: IEEE 30 Bus System</title><p>The TLBO algorithm has been executed on the test system consists of six generating units interconnected with 41 branches of transmission lines. Generator data, emission characteristics and line data are obtained from [<xref ref-type="bibr" rid="scirp.61606-ref32">32</xref>] . TLBO algorithm is applied to estimate the cost, emission coefficients and transmission line parameters. For each unit, the fuel cost and emission coefficients are computed. <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref> show the TLBO outcomes of the</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Economic dispatch with improved parameters for 10 unit system</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Demand (MW)</th><th align="center" valign="middle" >FC<sup>Exi</sup> ($/h)<sup> </sup></th><th align="center" valign="middle" >FC<sup>Est</sup> ($/h)<sup> </sup></th><th align="center" valign="middle" >% Error</th></tr></thead><tr><td align="center" valign="middle" >2500</td><td align="center" valign="middle" >525.7539</td><td align="center" valign="middle" >532.2159</td><td align="center" valign="middle" >1.22090</td></tr><tr><td align="center" valign="middle" >2600</td><td align="center" valign="middle" >608.7376</td><td align="center" valign="middle" >615.3032</td><td align="center" valign="middle" >1.07856</td></tr><tr><td align="center" valign="middle" >2700</td><td align="center" valign="middle" >627.2440</td><td align="center" valign="middle" >634.3932</td><td align="center" valign="middle" >1.13978</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Estimation of quadratic cost function coefficients by TLBO-IEEE 30 bus system</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Unit</th><th align="center" valign="middle"  rowspan="2"  >P (MW)</th><th align="center" valign="middle"  colspan="3"  >Coefficients</th><th align="center" valign="middle"  rowspan="2"  >FC <sup>Exi</sup> ($/h)<sup> </sup></th><th align="center" valign="middle"  rowspan="2"  >FC <sup>Est</sup> ($/h)<sub> </sub></th><th align="center" valign="middle"  rowspan="2"  >Error</th><th align="center" valign="middle"  rowspan="2"  >Total Error</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >Existing</td><td align="center" valign="middle" >TLBO</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >1</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >a<sub>i</sub></td><td align="center" valign="middle" >0.00375</td><td align="center" valign="middle" >0.003709</td><td align="center" valign="middle" >109.375</td><td align="center" valign="middle" >109.6930</td><td align="center" valign="middle" >0.318013</td><td align="center" valign="middle"  rowspan="3"  >0.763171</td></tr><tr><td align="center" valign="middle" >125</td><td align="center" valign="middle" >bi</td><td align="center" valign="middle" >2.00000</td><td align="center" valign="middle" >2.008420</td><td align="center" valign="middle" >308.594</td><td align="center" valign="middle" >309.0026</td><td align="center" valign="middle" >0.408860</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >c<sub>i</sub></td><td align="center" valign="middle" >0.00000</td><td align="center" valign="middle" >0.000000</td><td align="center" valign="middle" >550.000</td><td align="center" valign="middle" >550.0363</td><td align="center" valign="middle" >0.036298</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >2</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >a<sub>i</sub></td><td align="center" valign="middle" >0.01750</td><td align="center" valign="middle" >0.017377</td><td align="center" valign="middle" >42.0000</td><td align="center" valign="middle" >41.95063</td><td align="center" valign="middle" >0.049366</td><td align="center" valign="middle"  rowspan="3"  >1.283524</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >b<sub>i</sub></td><td align="center" valign="middle" >1.75000</td><td align="center" valign="middle" >1.750000</td><td align="center" valign="middle" >168.000</td><td align="center" valign="middle" >167.5557</td><td align="center" valign="middle" >0.444297</td></tr><tr><td align="center" valign="middle" >80</td><td align="center" valign="middle" >ci</td><td align="center" valign="middle" >0.00000</td><td align="center" valign="middle" >0.000000</td><td align="center" valign="middle" >252.000</td><td align="center" valign="middle" >251.2101</td><td align="center" valign="middle" >0.789861</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >3</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >a<sub>i</sub></td><td align="center" valign="middle" >0.06250</td><td align="center" valign="middle" >0.061676</td><td align="center" valign="middle" >29.0625</td><td align="center" valign="middle" >29.55164</td><td align="center" valign="middle" >0.489144</td><td align="center" valign="middle"  rowspan="3"  >1.286063</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >b<sub>i</sub></td><td align="center" valign="middle" >1.00000</td><td align="center" valign="middle" >1.044963</td><td align="center" valign="middle" >86.2500</td><td align="center" valign="middle" >86.85768</td><td align="center" valign="middle" >0.607683</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >c<sub>i</sub></td><td align="center" valign="middle" >0.00000</td><td align="center" valign="middle" >0.000000</td><td align="center" valign="middle" >206.250</td><td align="center" valign="middle" >206.4392</td><td align="center" valign="middle" >0.189236</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >4</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >a<sub>i</sub></td><td align="center" valign="middle" >0.00834</td><td align="center" valign="middle" >0.008000</td><td align="center" valign="middle" >33.3340</td><td align="center" valign="middle" >33.30000</td><td align="center" valign="middle" >0.034000</td><td align="center" valign="middle"  rowspan="3"  >0.586500</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >b<sub>i</sub></td><td align="center" valign="middle" >3.25000</td><td align="center" valign="middle" >3.250000</td><td align="center" valign="middle" >68.3360</td><td align="center" valign="middle" >68.20000</td><td align="center" valign="middle" >0.136000</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >c<sub>i</sub></td><td align="center" valign="middle" >0.00000</td><td align="center" valign="middle" >0.000000</td><td align="center" valign="middle" >123.967</td><td align="center" valign="middle" >123.5500</td><td align="center" valign="middle" >0.416500</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >5</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >a<sub>i</sub></td><td align="center" valign="middle" >0.02500</td><td align="center" valign="middle" >0.022322</td><td align="center" valign="middle" >32.5000</td><td align="center" valign="middle" >33.03565</td><td align="center" valign="middle" >0.535646</td><td align="center" valign="middle"  rowspan="3"  >1.071758</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >b<sub>i</sub></td><td align="center" valign="middle" >3.00000</td><td align="center" valign="middle" >3.080341</td><td align="center" valign="middle" >70.0000</td><td align="center" valign="middle" >70.53576</td><td align="center" valign="middle" >0.535763</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >c<sub>i</sub></td><td align="center" valign="middle" >0.00000</td><td align="center" valign="middle" >0.000000</td><td align="center" valign="middle" >112.500</td><td align="center" valign="middle" >112.5003</td><td align="center" valign="middle" >0.000349</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >6</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >a<sub>i</sub></td><td align="center" valign="middle" >0.02500</td><td align="center" valign="middle" >0.023081</td><td align="center" valign="middle" >39.6000</td><td align="center" valign="middle" >40.22570</td><td align="center" valign="middle" >0.625698</td><td align="center" valign="middle"  rowspan="3"  >1.369166</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >b<sub>i</sub></td><td align="center" valign="middle" >3.00000</td><td align="center" valign="middle" >3.075169</td><td align="center" valign="middle" >90.6250</td><td align="center" valign="middle" >91.30487</td><td align="center" valign="middle" >0.679869</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >c<sub>i</sub></td><td align="center" valign="middle" >0.00000</td><td align="center" valign="middle" >0.000000</td><td align="center" valign="middle" >160.000</td><td align="center" valign="middle" >159.9364</td><td align="center" valign="middle" >0.063598</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Estimation of emission function coefficients by TLBO-IEEE 30 bus system</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Unit</th><th align="center" valign="middle"  rowspan="2"  >P<sub> </sub>(MW)<sub> </sub></th><th align="center" valign="middle"  colspan="3"  >Coefficients</th><th align="center" valign="middle"  rowspan="2"  >E<sup>Exi</sup> (Kg/h)<sup> </sup></th><th align="center" valign="middle"  rowspan="2"  >E<sup>Est</sup> (Kg/h)<sub> </sub></th><th align="center" valign="middle"  rowspan="2"  >Error</th><th align="center" valign="middle"  rowspan="2"  >Total Error</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >Existing</td><td align="center" valign="middle" >TLBO</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >1</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >e<sub>0i </sub></td><td align="center" valign="middle" >0.01260</td><td align="center" valign="middle" >0.012470</td><td align="center" valign="middle" >−0.5170</td><td align="center" valign="middle" >−0.01556</td><td align="center" valign="middle" >0.501437</td><td align="center" valign="middle"  rowspan="3"  >2.212806</td></tr><tr><td align="center" valign="middle" >125</td><td align="center" valign="middle" >e<sub>1i</sub></td><td align="center" valign="middle" >−1.1000</td><td align="center" valign="middle" >−1.08064</td><td align="center" valign="middle" >82.3580</td><td align="center" valign="middle" >82.60794</td><td align="center" valign="middle" >0.249943</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >e<sub>2i</sub></td><td align="center" valign="middle" >22.9830</td><td align="center" valign="middle" >22.84106</td><td align="center" valign="middle" >306.983</td><td align="center" valign="middle" >305.5216</td><td align="center" valign="middle" >1.461426</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >2</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >e<sub>0i</sub></td><td align="center" valign="middle" >0.0200</td><td align="center" valign="middle" >0.019823</td><td align="center" valign="middle" >31.3130</td><td align="center" valign="middle" >31.64200</td><td align="center" valign="middle" >0.329003</td><td align="center" valign="middle"  rowspan="3"  >1.354070</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >e<sub>1i</sub></td><td align="center" valign="middle" >−0.1000</td><td align="center" valign="middle" >−0.08000</td><td align="center" valign="middle" >91.3130</td><td align="center" valign="middle" >91.87402</td><td align="center" valign="middle" >0.561024</td></tr><tr><td align="center" valign="middle" >80</td><td align="center" valign="middle" >e<sub>2i</sub></td><td align="center" valign="middle" >25.3130</td><td align="center" valign="middle" >25.31300</td><td align="center" valign="middle" >145.313</td><td align="center" valign="middle" >145.7770</td><td align="center" valign="middle" >0.464043</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >3</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >e<sub>0i</sub></td><td align="center" valign="middle" >0.02700</td><td align="center" valign="middle" >0.026724</td><td align="center" valign="middle" >31.4300</td><td align="center" valign="middle" >31.29213</td><td align="center" valign="middle" >0.137871</td><td align="center" valign="middle"  rowspan="3"  >1.178847</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >e<sub>1i</sub></td><td align="center" valign="middle" >−0.0100</td><td align="center" valign="middle" >−0.00900</td><td align="center" valign="middle" >49.5050</td><td align="center" valign="middle" >49.19559</td><td align="center" valign="middle" >0.309407</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >e<sub>2i</sub></td><td align="center" valign="middle" >25.5050</td><td align="center" valign="middle" >25.41431</td><td align="center" valign="middle" >92.5050</td><td align="center" valign="middle" >91.77343</td><td align="center" valign="middle" >0.731569</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >4</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >e<sub>0i</sub></td><td align="center" valign="middle" >0.02910</td><td align="center" valign="middle" >0.028212</td><td align="center" valign="middle" >27.7600</td><td align="center" valign="middle" >27.81122</td><td align="center" valign="middle" >0.051223</td><td align="center" valign="middle"  rowspan="3"  >1.073847</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >e<sub>1i</sub></td><td align="center" valign="middle" >−0.0050</td><td align="center" valign="middle" >−0.00100</td><td align="center" valign="middle" >36.4400</td><td align="center" valign="middle" >36.26489</td><td align="center" valign="middle" >0.175107</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >e<sub>2i</sub></td><td align="center" valign="middle" >24.9000</td><td align="center" valign="middle" >25.00000</td><td align="center" valign="middle" >60.3725</td><td align="center" valign="middle" >59.52498</td><td align="center" valign="middle" >0.847516</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >5</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >e<sub>0i</sub></td><td align="center" valign="middle" >0.02900</td><td align="center" valign="middle" >0.030000</td><td align="center" valign="middle" >27.5600</td><td align="center" valign="middle" >26.67813</td><td align="center" valign="middle" >0.881871</td><td align="center" valign="middle"  rowspan="3"  >1.455612</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >e<sub>1i</sub></td><td align="center" valign="middle" >−0.0040</td><td align="center" valign="middle" >−0.00100</td><td align="center" valign="middle" >36.2200</td><td align="center" valign="middle" >35.66813</td><td align="center" valign="middle" >0.551871</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >e<sub>2i</sub></td><td align="center" valign="middle" >24.7000</td><td align="center" valign="middle" >23.68813</td><td align="center" valign="middle" >50.6800</td><td align="center" valign="middle" >50.65813</td><td align="center" valign="middle" >0.021871</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >6</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >e<sub>0i</sub></td><td align="center" valign="middle" >0.02710</td><td align="center" valign="middle" >0.028000</td><td align="center" valign="middle" >29.1364</td><td align="center" valign="middle" >28.48005</td><td align="center" valign="middle" >0.656352</td><td align="center" valign="middle"  rowspan="3"  >1.541352</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >e<sub>1i</sub></td><td align="center" valign="middle" >−0.0055</td><td align="center" valign="middle" >−0.00500</td><td align="center" valign="middle" >42.1000</td><td align="center" valign="middle" >41.88305</td><td align="center" valign="middle" >0.216952</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >e<sub>2i</sub></td><td align="center" valign="middle" >25.3000</td><td align="center" valign="middle" >24.50805</td><td align="center" valign="middle" >68.4400</td><td align="center" valign="middle" >69.10805</td><td align="center" valign="middle" >0.668048</td></tr></tbody></table></table-wrap><p>estimated coefficients. Existing fuel cost and existing emission for three different power generations are compared with its FC<sup>Est</sup> and E<sup>Est</sup> and it is found that those values are very close to each other. The new values of coefficients and their related total error are presented in the <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref>. From the results the error obtained by TLBO for all specified output of generating units is less which shows the accurate estimation of the system parameters.</p><p>TLP are obtained using Equations (A.2-A.5) for each line and the estimated TLP results are listed in <xref ref-type="table" rid="table5">Table 5</xref>. The estimated TLP values are compared with base case values and the percentage error is computed using Equation (9). The % error values for transmission lines are almost close to zero except for the lines 24 and 29 for which the TLP values are above 1. The efficiency of transmission lines 11-16, 37 are high as compared to other transmission lines, due to the presence of three winding transformer in the transmission lines. The estimated R, X, B values for each transmission line are presented in <xref ref-type="table" rid="table5">Table 5</xref>. The estimated transmission loss coefficients using Equations (A.10-A.11) are detailed in the <xref ref-type="table" rid="table6">Table 6</xref>.</p><p>By using existing parameters, economic emission dispatch is carried out and the results are listed in <xref ref-type="table" rid="table7">Table 7</xref>. The dispatch results are obtained for three different load demands of 275 MW, 284.4 MW and 300 MW. With the new estimated parameters for fuel cost function, emission and loss, the multi-objective ED problem is solved and the results are compared with the existing results. From the results, the percentage deviation of fuel cost, emission and network loss for estimated parameters are slightly elevated as compared to the existing parameters. The % error of all these values reveals the impact of accurate parameter estimation for ED problems.</p></sec><sec id="s4_3"><title>4.3. Test System 3: 62 Bus Indian Utility System</title><p>In this case, a 62 bus Indian utility system is considered for estimating the improved parameters by using the proposed algorithm. The chosen test system consists of nineteen power producers, eighty nine (220KV) lines</p>
<table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Estimation of transmission line parameters for IEEE 30 bus system (in p.u)</title></caption></table-wrap>
<p>nl: start bus of a line; nr: end bus of a line; Re, Xe and Be: Errors in TLP.</p>
<p>with eleven tap changing transformers. The bus, line and generator data of the test system are taken from [32] .</p>
<p>The proposed method of determining the improved parameters is applied for the chosen test system and the obtained results are listed in Table 8. For each unit the fuel costs using improved parameters for three different real power outputs are also specified. In comparison with base case values the error is calculated for each generating unit. The obtained error is small which reveals that the estimation of the coefficient is accurate.</p>
<p>Further the estimation of TLP is carried out using A.2-A.5. The obtained TLP values by TLBO algorithm are listed in Table 9. The % error values for each transmission line are close to zero, except for few lines, which shows that the obtained TLP values are accurate. With the improved TLP values, the transmission line efficiency is calculated and is listed in Table 9. It is also inferred from Table 9 that the efficiency of each transmission line obtained using TLBO is nearly the same as compared to the base case.</p>
<p>The PED is carried out with improved cost coefficients of generators and improved TLP for three different load demands of 2900 MW, 2967 MW, 3200 MW are obtained and the results are presented in Table 10. The estimated transmission loss coefficients using Equations (A.10-A.11) are presented in the Table 11. The results obtained are compared with the existing fuel cost and loss and the % deviation of fuel cost and transmission loss is computed and presented. The obtained results clearly illustrate the impact of improved parameters on ED problem.</p></sec></sec>
<sec id="s5"><title>5. Potential Verification of TLBO</title>
<sec id="s5_1"><title>5.1. Solution Quality</title>
<p>Using the proposed algorithm several runs have been carried out by varying the population size.In this analysis there is no larger difference in the average fitness value above the population size of 10. Hence the population size of 10 is preferred for all estimation process. The simulations are performed to estimate the quadratic cost function coefficients, piecewise quadratic valve point coefficients, emission coefficients, transmission line parameters and transmission loss coefficients using three different test cases. For these cases the existing coefficients at the time of installation are only available, hence the obtained improved parameters are compared with only these values. From the obtained simulation results, the cost coefficients, emission coefficients and transmission line parameters are very close to the existing values and are presented in Tables 2-6 and Tables 8-10. The comparisons of total error in each case clearly indicate that the proposed method provides the best estimate of accurate coefficients.</p></sec>
<sec id="s5_2"><title>5.2. Statistical Analysis</title>
<p>The reliability of the algorithm in finding the best solution can be viewed by performing statistical analysis. The convergence property and the robustness characteristics are focused primly for the statistical analysis. The standard statistical parameters of the objective functions such as best, worst and average values in addition to standard deviation and solution iter are also worked out and analyzed and are given in Table 12. The standard deviation value is small which indicates the accuracy of estimate.</p>
<p>Convergence: The TLBO algorithm is implemented on different scale of test systems and for all cases, the convergence characteristics are plotted. The convergence pattern illustrates the searching ability of algorithm.</p>
<p>Figure 2 shows the convergence characteristics of 10 unit multiple fuels system; the proposed approach converged to a good solution within the 50 iterations for the three different fuels. For the IEEE 30 bus and 62 bus Indian utility systems, the convergence graphs are shown in Figure 3. Figure 2 and Figure 3 show that the TLBO has good convergence property, thus resulting in good evaluation value and low error.</p>
<p>Robustness: Many trials with different initial population have been carried out to test the consistency of the TLBO algorithm. The algorithm is executed for 50 trials and the obtained objective function values are presented in Figure 4. The mean value is close to the optimal value for all the cases. This description clears that the TLBO provides great searching ability, higher solution quality and the best estimate.</p></sec>
<sec id="s5_3"><title>5.3. Observations</title>
<p>・ Accurate parameters are estimated for three different test systems involving a practical test system.</p>
<p>・ For the first time in the literature, both the parameter estimation and economic dispatch are carried out</p>
<p>concurrently.</p>
<p>・ The % error estimation of parameters reveals the rate of change in parameters over the years due to physical conditions like aging.</p>
<p>・ The results clearly signify the impact of accurate parameters on ED problems on fetching the accurate dispatch results over existing results.</p></sec></sec>
<sec id="s6"><title>6. Conclusion</title>
<p>In this paper, the TLBO algorithm is successfully implemented for both the operation of parameter estimations and ED solution. The operational aspects of the generators such as valve-point loading, emission, multiple fuel options and transmission loss are considered. The three different test systems involving a practical test system are selected for this estimation and dispatch problem. The results obtained by satisfying all the constraints for all cases by the proposed algorithm are always comparable or better than the other methods. It is revealed that the</p>
<p>TLBO possesses better convergence characteristics and robustness. The proposed TLBO approach has shown merits such as better results, easy implementation for the accurate parameter estimation for PED problems. It can be concluded that the estimated parameters obtained show that the proposed method can be used as a very accurate tool for estimating the fuel cost, emission and loss coefficients.</p></sec></body>


<back><ref-list><title>References</title><ref id="scirp.61606-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">El-Hawary, M.E. and Mansour, S.Y. (1982) Performance Evaluation of Parameter Estimation Algorithms for Economic Operation of Power Systems. IEEE Transaction on Power Apparatus Systems, 101, 574-582.&lt;/br&gt;http://dx.doi.org/10.1109/TPAS.1982.317270</mixed-citation></ref><ref id="scirp.61606-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Soliman, S.A., Emam, S.E.A. and Christensen, G.S. (1991) Optimization of the Optimal Coefficients of Non-Monotonically Increasing Incremental Cost Curves. Electric Power System Research, 21, 99-106.&lt;/br&gt;http://dx.doi.org/10.1016/0378-7796(91)90023-G</mixed-citation></ref><ref id="scirp.61606-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Liang, Z.X. and Glover, J.D. (1991) Improved Cost Functions for Economic Dispatch Computations. IEEE Transactions of Power System, 6, 821-829. &lt;/br&gt;http://dx.doi.org/10.1109/59.76731</mixed-citation></ref><ref id="scirp.61606-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Chen, H.Y.K. and Postel, C.E. (1986) On-Line Parameters Identification of Input Output Curves for Thermal Units. IEEE Transaction Power System, 1, 221-224. &lt;/br&gt;http://dx.doi.org/10.1109/TPWRS.1986.4334933</mixed-citation></ref><ref id="scirp.61606-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Grainger, J. and Stevenson, W. (1994) Power System Analysis. McGraw-Hill., New York.</mixed-citation></ref><ref id="scirp.61606-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Chan, S.M. (1993) Computing Overhead Line Parameters. Computer Applications and Power, 6, 43-45.&lt;/br&gt;http://dx.doi.org/10.1109/67.180436</mixed-citation></ref><ref id="scirp.61606-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Dommel, H.W. (1985) Overhead Line Parameters from Handbook Formulas and Computer Programs. IEEE Transactions on Power Apparatus and Systems, 4, 366-372. &lt;/br&gt;http://dx.doi.org/10.1109/TPAS.1985.319051</mixed-citation></ref><ref id="scirp.61606-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Thorp, J.S., Phadke, A.G., Horowitz, S.H. and Begovic, M.M. (1988) Some Applications of Phasor Measurements To Adaptive Protection. IEEE Transaction Power System, 3, 791-798. &lt;/br&gt;http://dx.doi.org/10.1109/59.192936</mixed-citation></ref><ref id="scirp.61606-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Chen, C.S., Liu, C.W. and Jiang, J.A. (2002) A New Adaptive PMU Based Protection Scheme for Transposed/ Untransposed Parallel Transmission Lines. IEEE Transactions on Power Delivery, 17, 395-404.&lt;/br&gt;http://dx.doi.org/10.1109/61.997906</mixed-citation></ref><ref id="scirp.61606-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Kim, I.-D., and Aggarwal, R.K. (2006) A Study on the On-Line Measurement of Transmission Line Impedances for Improved Relaying Protection. Electric Power and Energy System, 28, 359-366.&lt;/br&gt;http://dx.doi.org/10.1016/j.ijepes.2006.01.002</mixed-citation></ref><ref id="scirp.61606-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Liao, Y. and Kezunovic, M. (2009) Online Optimal Transmission Line Parameter Estimation for Relaying Applications. IEEE Transactions on Power Delivery, 24, 96-102. &lt;/br&gt;http://dx.doi.org/10.1109/TPWRD.2008.2002875</mixed-citation></ref><ref id="scirp.61606-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Sivanagaraju, G., Chakrabarti, S. and Srivastava, S.C. (2014) Uncertainty in Transmission Line Parameters Estimation and Impact on Line Current Differential Protection. IEEE Transactions on Instrumentation and Measurement, 63, 1496-1504.&lt;/br&gt; http://dx.doi.org/10.1109/TIM.2013.2292276</mixed-citation></ref><ref id="scirp.61606-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Wagenaars, P., Wouters, P.A.A.F., van der Wielen, P.C.J.M. and Steennis, E.F. (2010) Measurement of Transmission Line Parameters of Three-Core Power Cables with Common Earth Screen. IET Science Measurement and Technology, 4, 146-155. &lt;/br&gt;http://dx.doi.org/10.1049/iet-smt.2009.0062</mixed-citation></ref><ref id="scirp.61606-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Indulkar, C.S. and Ramalingam, K. (2008) Estimation of Transmission Line Parameters from Measurements. Electric Power and Energy Systems, 30, 337-342. &lt;/br&gt;http://dx.doi.org/10.1016/j.ijepes.2007.08.003</mixed-citation></ref><ref id="scirp.61606-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Al-Kandari, A.M. and El-Naggar, K.M. (2006) A Genetic-Based Algorithm for Optimal Estimation of Input-Output Curve Parameters of Thermal Power Plants. Electrical Engineering, 89, 585-590. &lt;/br&gt;http://dx.doi.org/10.1007/s00202-006-0047-x</mixed-citation></ref><ref id="scirp.61606-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">El-Naggar, K.M. and Alrashidi, M.R. and Al-Othman, A.K. (2009) Estimating the Input-Output Parameters of Thermal Power Plants Using PSO. Energy Conversion and Management, 50, 1767-1772.&lt;/br&gt;http://dx.doi.org/10.1016/j.enconman.2009.03.019</mixed-citation></ref><ref id="scirp.61606-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Alrashidi, M.R., El-Naggar, K.M. and Al-Othman, A.K. (2009) Particle Swarm Optimization Based Approach for Estimating the Fuel-Cost Function Parameters of Thermal Power Plants with Valve Loading Effects. Electric Power Components and Systems, 37, 1219-1230. http://dx.doi.org/10.1080/15325000902993589.</mixed-citation></ref><ref id="scirp.61606-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Sonmez, Y. (2013) Estimation of Fuel Cost Curve Parameters for Thermal Power Plants Using the ABC Algorithm. Turkish Journal of Electrical Engineering and Computer Science, 21, 1827-1841.&lt;/br&gt;http://dx.doi.org/10.3906/elk-1203-10</mixed-citation></ref><ref id="scirp.61606-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Sinha, A.K. and Mandal, J.K. (1999) Hierarchical Dynamic State Estimator Using ANN-Based Dynamic Load Prediction. IET Generation Transmission and Distribution, 146, 541-549. http://dx.doi.org/10.1049/ip-gtd:19990462</mixed-citation></ref><ref id="scirp.61606-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Kumar, D.M.V. and Srivastava, S.C. (1999) Power System State Forecasting Using Artificial Neural Networks. Electric Machine and Power System, 27, 653-664. http://dx.doi.org/10.1080/073135699269091</mixed-citation></ref><ref id="scirp.61606-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Lin, J.M., Huang, S.J. and Shih, K.R. (2003) Application of Sliding Surface Enhanced Fuzzy Control for Dynamic State Estimation of a Power System. IEEE Transaction Power System, 18, 570-577.&lt;/br&gt;http://dx.doi.org/10.1109/TPWRS.2003.810894</mixed-citation></ref><ref id="scirp.61606-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Bhuvaneswari, R., Subramanian, S. and Madhu, A. (2008) A Novel State Estimation Based on Minimum Errors between Measurements Using Ant Colony Optimization Technique. International Journal of Electric Engineering, 15, 457-568.</mixed-citation></ref><ref id="scirp.61606-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Sakthivel, V.P., Bhuvaneswari, R. and Subramanian, S. (2010) Design Optimization of Three-Phase Energy efficient Induction Motor Using Adaptive Bacterial Foraging Algorithm. International Journal of Computation and Mathematics in Electrical and Electronics Engineering, 29, 699-726.</mixed-citation></ref><ref id="scirp.61606-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Sakthivel, V.P., Bhuvaneswari, R. and Subramanian, S. (2010) Non-Intrusive Efficiency Estimation Method for Energy Auditing and Management of In-Service Induction Motor Using Bacterial Foraging Algorithm. IET Electric Power Applications, 4, 579-590. &lt;/br&gt;http://dx.doi.org/10.1049/iet-epa.2009.0313</mixed-citation></ref><ref id="scirp.61606-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Sakthivel, V.P., Bhuvaneswari, R. and Subramanian, S. (2011) An Accurate and Economical Approach for induction motor Field Efficiency Estimation Using Bacterial Foraging Algorithm. Measurement, 44, 674-684.&lt;/br&gt;http://dx.doi.org/10.1016/j.measurement.2010.12.008</mixed-citation></ref><ref id="scirp.61606-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Rao, R.V., Savsani, V.J. and Vakharia, D.P. (2011) Teaching-Learning-Based Optimization: A Novel Method for Mechanical Design Optimization Problems. Computer Aided Design, 43, 303-315. &lt;/br&gt;http://dx.doi.org/10.1016/j.cad.2010.12.015</mixed-citation></ref><ref id="scirp.61606-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Rao, R.V. and Waghmare, G.G. (2014) Complex Constrained Design Optimisation Using an Elitist Teaching-Learning-Based Optimisation. International Journal of Metaheuristics, 3, 81-102.&lt;/br&gt;http://dx.doi.org/10.1504/IJMHEUR.2014.058863</mixed-citation></ref><ref id="scirp.61606-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">Rao, R.V., Savsani, V.J. and Vakharia, D.P. (2012) Teaching-Learning-Based Optimization: An Optimization Method for Continuous Non-Linear Large Scale Problems. Information Science, 183, 1-15. &lt;/br&gt;http://dx.doi.org/10.1016/j.ins.2011.08.006</mixed-citation></ref><ref id="scirp.61606-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Rao, R.V., Savsani, V.J. and Vakharia, D.P. (2011) Teaching-Learning-Based Optimization: A Novel Method for Mechanical Design Optimization Problems. Computer-Aided Design, 43, 303-315.&lt;/br&gt;http://dx.doi.org/10.1016/j.cad.2010.12.015</mixed-citation></ref><ref id="scirp.61606-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Durai, S., Subramanian, S. and Ganesan, S. (2015) Improved Parameters for Economic Dispatch Problems by Teaching Learning Optimization. Electric Power and Energy System, 67, 11-24. &lt;/br&gt;http://dx.doi.org/10.1016/j.ijepes.2014.11.010</mixed-citation></ref><ref id="scirp.61606-ref31"><label>31</label><mixed-citation publication-type="other" xlink:type="simple">Chiang, C.-L. (2005) Improved Genetic Algorithm for Power Economic Dispatch of Units with Valve-Point Effects and Multiple Fuels. IEEE Transaction Power System, 20, 1690-1699. &lt;/br&gt;http://dx.doi.org/10.1109/TPWRS.2005.857924</mixed-citation></ref><ref id="scirp.61606-ref32"><label>32</label><mixed-citation publication-type="other" xlink:type="simple">Tamilnadu Electricity Board Statistics at a Glance (1999-2000), Compiled by Planning Wing of Tamilnadu Electricity Board, Chennai, India.</mixed-citation></ref></ref-list></back></article>