<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2015.31006</article-id><article-id pub-id-type="publisher-id">JAMP-53575</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Enumeration of Strength Three Orthogonal Arrays and Their Implementation in Parameter Design
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Julio</surname><given-names>Romero</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>Scott</surname><given-names>H. Murray</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Faculty of Education, Science, Technology and Mathematics, University of Canberra, Canberra, Australia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Julio.Romero@canberra.edu.au(JR)</email>;<email>Scott.Murray@canberra.edu.au(SHM)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>28</day><month>01</month><year>2015</year></pub-date><volume>03</volume><issue>01</issue><fpage>38</fpage><lpage>45</lpage><history><date date-type="received"><day>December</day>	<month>2014</month></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   This paper describes the construction and enumeration of mixed orthogonal arrays (MOA) to produce optimal experimental designs. A MOA is a multiset whose rows are the different combinations of factor levels, discrete values of the variable under study, having very well defined features such as symmetry and strength three (all main interactions are taken in consideration). The applied methodology blends the fields of combinatorics and group theory by applying the ideas of orbits, stabilizers and isomorphisms to array generation and enumeration. Integer linear programming was used in order to exploit the symmetry property of the arrays under study. The backtrack search algorithm was used to find suitable arrays in the underlying space of possible solutions. To test the performance of the MOAs, an engineered system was used as a case study within the stage of parameter design. The analysis showed how the MOAs were capable of meeting the fundamental engineering design axioms and principles, creating optimal experimental designs within the desired context. 
 
</p></abstract><kwd-group><kwd>Experimental Designs</kwd><kwd> Orthogonal Arrays</kwd><kwd> Combinatorics</kwd><kwd> Parameter Design</kwd><kwd> Backtrack Search</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Experimental design is a well-known and broadly applied area of statistics. It started formally with the excellent book of Fisher The Design of Experiments [<xref ref-type="bibr" rid="scirp.53575-ref1">1</xref>] followed by the contributions of Cochran and Cox [<xref ref-type="bibr" rid="scirp.53575-ref2">2</xref>], Kempthorne [<xref ref-type="bibr" rid="scirp.53575-ref3">3</xref>], and complemented with the Analysis of Variance work published by Scheffe in 1959 [<xref ref-type="bibr" rid="scirp.53575-ref4">4</xref>].</p><p>The expansion of this field to the areas of industrial processes and engineered systems, especially through the contribution of Taguchi [<xref ref-type="bibr" rid="scirp.53575-ref5">5</xref>], has boosted a more detailed study of designs constructed by combinatorial techniques such as Hadamard matrices [<xref ref-type="bibr" rid="scirp.53575-ref6">6</xref>], Latin squares and their derivatives [<xref ref-type="bibr" rid="scirp.53575-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.53575-ref8">8</xref>], and orthogonal arrays of strength three [<xref ref-type="bibr" rid="scirp.53575-ref9">9</xref>].</p><p>The basis of the study in parameter design strives in the ability of an experimental design (constructed through whatever method) to observe separately the effects of changing factors individually, but at the same time being able to do this at several different combinations of the other factors. Thus, any interdependence among factors can be detected [<xref ref-type="bibr" rid="scirp.53575-ref10">10</xref>]. In order to deal with this challenge, we classified the approaches in seven categories: enumeration of the arrays, construction of algorithms, backtrack search, integer linear programming, experimental designs, parameter design, and optimality and robustness.</p><p>Techniques for enumeration of the arrays have been broadly studied through different approaches. Schoen and Nguyen [<xref ref-type="bibr" rid="scirp.53575-ref11">11</xref>], by using combinatorics, constructed an algorithm to enumerate a set of non-isomorphic orthogonal arrays of given strength, run-size, number of factors and their correspondent levels. They used a technique called minimum forbidden configuration. A completely different approach was developed by Schoen, Eendebak, and Nguyen [<xref ref-type="bibr" rid="scirp.53575-ref12">12</xref>] who enumerated pure level and mixed-level orthogonal arrays exploiting the properties of asymmetric and non-asymmetric arrays based on the backtrack search algorithm.</p><p>In a similar way, two major works were undertaken using the aforementioned algorithm. Firstly, Nguyen and Murray [<xref ref-type="bibr" rid="scirp.53575-ref13">13</xref>] listed several designs of strength three OAs using the backtrack search technique together a C program code originally developed by Brouwer [<xref ref-type="bibr" rid="scirp.53575-ref14">14</xref>]. The list was initially thought to enumerate cases up to 100 runs. Secondly, a very detailed information for searching permutation and matrix groups using the backtrack algorithm was given by Butler [<xref ref-type="bibr" rid="scirp.53575-ref15">15</xref>]. He discusses the implementation of the backtrack search algorithm to compute centralisers, intersections, and set stabilisers as well as the determinations of isomorphic groups.</p><p>Tang and Zhou [<xref ref-type="bibr" rid="scirp.53575-ref16">16</xref>] worked to enumerate D-optimal two-level OAs and to estimate main effects and specific interactions. This method also uses sequential collection of array’s columns and is limited to three or less two-factor interactions. Another type of enumeration and construction of OAs was published by Nguyen [<xref ref-type="bibr" rid="scirp.53575-ref9">9</xref>] based on the use of canonical graphs and the orbit algorithm.</p><p>Additionally to the methods previously discussed to the construction of OAs, some new approaches have seen the light. Vincent Brouerius [<xref ref-type="bibr" rid="scirp.53575-ref17">17</xref>] modified the C code wrote by Brouwer in order to implement parallel computation to the main backtrack algorithm. Due the nature of the underlying group theory behind this implementation (orbit algorithm), the results were not satisfactory. Pushing the boundaries further, He and Tang [<xref ref-type="bibr" rid="scirp.53575-ref18">18</xref>] introduced the terminology of strong OAs in terms of space filling properties. These arrays are comparable with strength three OAs but designed for computer experiments only. Moreover, Angelopoulos et al. [<xref ref-type="bibr" rid="scirp.53575-ref19">19</xref>] proposed an original method to the construction of OAs called step-down algorithm. This method is quite original and powerful, however is useful only for specific designs namely OA(24,7,2,t), OA(28,6,2,t), and OA(32,6,2,t), t ≥ 2. One interesting attempt of building OAs up without starting from scratch was done by Man Nguyen [<xref ref-type="bibr" rid="scirp.53575-ref20">20</xref>] who used Latin squares to construct strength three OAs mainly oriented to industry-based applications.</p><p>Glynn and Byatt [<xref ref-type="bibr" rid="scirp.53575-ref21">21</xref>] presented one of the few comparative works in constructing OAs using graphical techniques and projective planes. We are applying a similar technique in this research project called graph colouring developed also by Man [<xref ref-type="bibr" rid="scirp.53575-ref9">9</xref>]. Throughout a different perspective, Tsai, Ye, and Li [<xref ref-type="bibr" rid="scirp.53575-ref22">22</xref>] were able to construct a complete catalogue of geometrically non-isomorphic OAs using the Geometric Isomorphism approach. However, their enumeration was bounded to designs up to 18-runs only.</p><p>Following the idea of OAs construction, Sloane and Stufken [<xref ref-type="bibr" rid="scirp.53575-ref23">23</xref>] developed a linear programming bound of OAs with mixed levels, which challenges the Rao bound in order to decide the existence of some orthogonal arrays. Furthermore, Nguyen and Murray [<xref ref-type="bibr" rid="scirp.53575-ref24">24</xref>] extended the idea of orthogonal arrays construction by using integer linear programming through the algorithms provided by the mathematical software Nauty and Magma.</p><p>From the point of view of application and implementation of the orthogonal arrays, Huynh [<xref ref-type="bibr" rid="scirp.53575-ref25">25</xref>] showed some applications using OAs in order to solve typical experimental designs encountered in systems engineering and architecting optimisation problems. Huynh also presented the applicability of OAs to engineering testing and validation. Huynh’s work highlights one of the main features of OAs which is working directly with non-linear problems rather that their linear equivalent. In Addition, Chatzopulos et al. [<xref ref-type="bibr" rid="scirp.53575-ref26">26</xref>] analysed optimality criteria during the actual construction of the experimental design rather than once is already finished. Evangelaras, Kolaiti, and Koukouvinos [<xref ref-type="bibr" rid="scirp.53575-ref27">27</xref>] applied the robust parameter design concept following Taguchi’s approach and embedded Hadamard Matrices. These two approaches facilitate the construction of combined arrays to overcome the product of arrays and the consequent large number of runs found in the Taguchi method. Similar work was done by Tsai [<xref ref-type="bibr" rid="scirp.53575-ref28">28</xref>] using the idea of a combination between combinatorial optimisation and genetic algorithms.</p><p>Pure considerations of optimality and robustness were offered by Lekivetz and Tang [<xref ref-type="bibr" rid="scirp.53575-ref29">29</xref>] who have worked focusing on the construction of mixed OAs with more than two levels using saturated orthogonal arrays. There is also an individual contribution by the same author [<xref ref-type="bibr" rid="scirp.53575-ref30">30</xref>] who studied the property of optimality and robustness of factorial designs including OAs derived from fractional factorial designs. This study also highlights the aforementioned features in two-factor interactions and is complemented by a very good alternative to deal with interactions calculations proposed by Byth and Gebski [<xref ref-type="bibr" rid="scirp.53575-ref31">31</xref>] through the use of a graphical aid. The method visually helps to identify multiplicative and additive interactions effects by measuring the lost of statistical power due the presence of a particular interaction.</p></sec><sec id="s2"><title>2. Rationale</title><p>We chose as a starting point the presentation of a case study to explain the overall idea of experimental design, and where our designs and the techniques used to construct them fit in. We also provided the theoretical background to develop functional requirements (FR) and design parameters (DP) to mathematically represent the case study.</p><p>The objectives of this paper are the construction and application of experimental designs through the use of orthogonal arrays of strength three, and to make a comparative analysis against Taguchi’s technique. The study is limited to combinatorial designs and their application to the field of engineering design known as parameter design given particular attention to the design axioms and their relevance in the applicability and validity of our arrays [<xref ref-type="bibr" rid="scirp.53575-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.53575-ref33">33</xref>]. Further research makes comparative studies against traditional techniques such as cross-array designs and combined array designs [<xref ref-type="bibr" rid="scirp.53575-ref8">8</xref>].</p></sec><sec id="s3"><title>3. Case Study: A Passive Filter Network</title><p>Consider the following analysis of a Passive Filter Network (adapted from [<xref ref-type="bibr" rid="scirp.53575-ref32">32</xref>]) which is to be designed to measure the displacement signal generated by a strain-gage transducer shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. This system is similar to the one used in intersections of streets to control cars’ traffic through traffic lights. The network provides the interface between the strain-gage transducer/demodulator and the recording instrument with a galvanometer/ light-beam detection indicator. The purpose is conditioning the signal generated by a strain-gage transducer with demodulated output measuring the original displacement signal by filtering out the carrier frequency [<xref ref-type="bibr" rid="scirp.53575-ref34">34</xref>] [<xref ref-type="bibr" rid="scirp.53575-ref35">35</xref>].</p><p>The functional requirements (FR) are:</p><p>・ FR1 = Minimise output distortion by placing the filter pole at 6.84 Hz.</p><p>・ FR2 = Achieve a full-scale beam detection of &#177;3 in by adjusting the filter gain.</p><p>The design technique here aims to determine the correct set of descriptor parameters (DP, control factors) in order to satisfy the functional requirements. The transfer function obtained by using the Kirchhoff current law is given by:</p><disp-formula id="scirp.53575-formula74"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x3.png"  xlink:type="simple"/></disp-formula><p>where the filter cutoff frequency ω<sub>c</sub> and the galvanometer full-scale deflection D are:</p><disp-formula id="scirp.53575-formula75"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x4.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53575-formula76"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x5.png"  xlink:type="simple"/></disp-formula><p>the characteristic values and tolerances for the transducer and galvanometer are shown in <xref ref-type="table" rid="table1">Table 1</xref>. Thus, the corresponding design parameters (DPs) are R<sub>2</sub>, R<sub>3</sub>, and C. Note that the values of the DPs are required to satisfy the independence axiom and the information axiom [<xref ref-type="bibr" rid="scirp.53575-ref32">32</xref>].</p></sec><sec id="s4"><title>4. Description of the Approaches Applied</title><p>The aforementioned functional requirements can be achieved adjusting the characteristic values shown in <xref ref-type="table" rid="table1">Table 1</xref>. In order to find their optimal values, two approaches were used: Taguchi designs and strength three orthogonal arrays.</p><sec id="s4_1"><title>4.1. First Approach: Taguchi Designs</title><p>Taguchi’s arrays were used to measure the relative influence of each control factor on the response (cutoff fre-</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> A passive filter network</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/53575x6.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Characteristic values</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Characteristic Value</th><th align="center" valign="middle" >Nominal Tolerance</th><th align="center" valign="middle"  colspan="2"  ></th></tr></thead><tr><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >(%)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >R<sub>S </sub>(Ω) V<sub>S</sub> (mV) R<sub>g </sub>(Ω) G<sub>sen</sub> (&#181;V/in)</td><td align="center" valign="middle" >120 15 84 563.64</td><td align="center" valign="middle" >&#177; 0.15% &#177; 0.5% &#177; 0.5% &#177; 0.5%</td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>quency of the filter). The selection among control factors was based on those which are both insensitive to noise factors (large η, see Equation (6)) over a broad range of values and have a linear relationship to the output response. In an ideal design, the number of DPs is equal to the number of FRs [<xref ref-type="bibr" rid="scirp.53575-ref32">32</xref>]. Hence, two control factors are required: one to adjust the frequency response ω<sub>c</sub>, and one to adjust the maximum light-beam deflection D. A third condition is required, and is that the control factors (DPs) that maintain the independence of the FRs are chosen [<xref ref-type="bibr" rid="scirp.53575-ref33">33</xref>]. The remaining control factors (those that are not used as adjustments factors) were used to maximise the SN ratio and minimize the information content [<xref ref-type="bibr" rid="scirp.53575-ref33">33</xref>].</p><p>The selection of the factor levels was made taking into consideration the broadest range of values able to yield a meaningful outcome. This is, the levels selected are representative of the range of practical possibilities [<xref ref-type="bibr" rid="scirp.53575-ref33">33</xref>].</p><p>Having determined the necessary combinations of the factor levels, another array (the outer array) is required for the noise factors ω<sub>c</sub> and D. This is to measure the variation in output response due the variation in the tolerance of the control factors. Each run yields a mean value m and a SN value η for each output response calculated according to Equations (4) and (6) [<xref ref-type="bibr" rid="scirp.53575-ref10">10</xref>]:</p><disp-formula id="scirp.53575-formula77"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x7.png"  xlink:type="simple"/></disp-formula><p>where m is the sample mean<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/53575x8.png" xlink:type="simple"/></inline-formula>; V is the total variation of the output y, over the entire range of n samples.</p><disp-formula id="scirp.53575-formula78"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x9.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/53575x10.png" xlink:type="simple"/></inline-formula>.</p><p>The SN ratio is given by:</p><disp-formula id="scirp.53575-formula79"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x11.png"  xlink:type="simple"/></disp-formula><p>and measures the variation in output due the noise factors, giving an indication of how much the desired output response changes as the tolerances of the control factors are varied over their respective ranges.</p></sec><sec id="s4_2"><title>4.2. Second Approach: Orthogonal Arrays of Strength Three</title><p>The method used to construct and enumerate orthogonal arrays of strength three is called the orbit algorithm [<xref ref-type="bibr" rid="scirp.53575-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.53575-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.53575-ref37">37</xref>]. The starting point of this method is using a finite group G acting on a finite set Ω; hence, the follow-</p><p>ing expressions hold: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/53575x12.png" xlink:type="simple"/></inline-formula>for all ω in Ω; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/53575x13.png" xlink:type="simple"/></inline-formula>for all ω in Ω; g, h in G. Defining the orbit of ω</p><p>under the group G as the set of all images such that [<xref ref-type="bibr" rid="scirp.53575-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.53575-ref39">39</xref>]:</p><disp-formula id="scirp.53575-formula80"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x14.png"  xlink:type="simple"/></disp-formula><p>In a similar way, the stabiliser is defined as [<xref ref-type="bibr" rid="scirp.53575-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.53575-ref39">39</xref>]:</p><disp-formula id="scirp.53575-formula81"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/53575x15.png"  xlink:type="simple"/></disp-formula><p>If G acts on Ω then there is an homomorphism<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/53575x16.png" xlink:type="simple"/></inline-formula>. This is called action homomorphism [<xref ref-type="bibr" rid="scirp.53575-ref36">36</xref>]. By introducing the orbit algorithm, it is required the calculation of orbits and stabilisers, the representatives for each orbit, test if two arrays in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/53575x17.png" xlink:type="simple"/></inline-formula> are within the same orbit (homomorphism), and store the representative arrays including the size of the automorphism group [<xref ref-type="bibr" rid="scirp.53575-ref9">9</xref>].</p><p>Due that orthogonal arrays are actually combinatorial arrays, it is required to search for all possible permutations configurations which satisfy certain requirements. One technique of implicitly searching all possible solutions in systematic manner is called backtrack search [<xref ref-type="bibr" rid="scirp.53575-ref40">40</xref>]. The algorithm of backtrack search enumerates the vectors (rows) starting from the lexicographically smallest, building the arrays up until either all of them are found or certain prescribed condition is violated (strength three).</p><p>In a similar way, we used canonical arrays to classify non-isomorphic fractions of a given design type and run size. This procedure encodes an array as a coloured graph to find the canonical labeling graph of the coloured graph, and decodes the result to a fraction. Basically, the idea is to test isomorphism between coloured graphs rather than test isomorphism among their corresponding arrays [<xref ref-type="bibr" rid="scirp.53575-ref9">9</xref>].</p><p>The stages to follow for this particular approach start by translating an array to a graph assigning a specific colour to it. Then, it is required to find the canonical graph of a coloured graph; finally, the array is demerged from the coloured graph.</p></sec></sec><sec id="s5"><title>5. Results</title><p>The SN ratios shown in <xref ref-type="table" rid="table2">Table 2</xref>, reproduced from [<xref ref-type="bibr" rid="scirp.53575-ref32">32</xref>], represent a measure of output response sensitivity to noise for the control factors’ combinations given. The sample mean m is an indication of the variation in the output response over the nine different combinations of control factor levels. These two parameters η and m, give an indication of the relative influence that each control factor has in the output response.</p><p>To perform the parameter design analysis, it was also required the construction of the analysis of variance tables as shown in <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref> for the SN ratio and Mean of f<sub>c</sub> respectively (reproduced from [<xref ref-type="bibr" rid="scirp.53575-ref32">32</xref>]).</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> SN and Mean Output Responses</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Run</th><th align="center" valign="middle" >fc</th><th align="center" valign="middle"  colspan="2"  >D</th></tr></thead><tr><td align="center" valign="middle" >SN(dB) m(Hz)</td><td align="center" valign="middle" >SN(dB) m(Hz)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >1 2 3 4 5 6 7 8 9</td><td align="center" valign="middle" >25.821 8.008 27.443 2.195 27.517 6.893 25.378 42.295 27.517 1.138 27.591 3.96 25.309 11.748 27.591 13.98 27.443 1.277</td><td align="center" valign="middle" >30.388 3.156 32.218 4.761 30.234 3.066 26.756 0.873 30.233 3.063 43.857 10.952 26.069 0.511 43.858 10.947 32.22 4.765</td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> ANOVA for the SN ratio of f<sub>c</sub></title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Factor</th><th align="center" valign="middle"  colspan="3"  >Level Means Sum of Squares</th></tr></thead><tr><td align="center" valign="middle" >1 2 3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >R<sub>3 </sub> R<sub>2 </sub> C</td><td align="center" valign="middle" >25.503 27.517 27.517 27.001 26.755 26.781 26.927 26.781 26.829</td><td align="center" valign="middle" >12.170 0.164 0.0504</td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> ANOVA for the Mean ratio of f<sub>c</sub></title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Factor</th><th align="center" valign="middle" >Level Means</th><th align="center" valign="middle"  colspan="2"  >Sum of Squares</th></tr></thead><tr><td align="center" valign="middle" >1 2 3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >R<sub>3 </sub> R<sub>2 </sub> C</td><td align="center" valign="middle" >20.684 5.771 4.043 8.649 15.256 6.593 3.474 5.968 21.056</td><td align="center" valign="middle" >753.402 184.358 814.464</td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>The passive filter network presented was worked out using the traditional parameter design technique. This method implies the calculation of one L<sub>9</sub> main factors array and 3 &#215; L<sub>27</sub> noise factors arrays (a crossed design). The results for the first run were shown in <xref ref-type="table" rid="table2">Table 2</xref>, and the corresponding analyses of variance were presented in <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref>.</p><p>The total number of arrays needed for this design comprises 3 &#215; 27 = 81 runs or experiments to be undertaken. Moreover, the original L<sub>27</sub> design can handle up to 13 factors with 3 levels each (symmetric array). Hence, the selection of only 7 out of 13 columns was made arbitrarily. Moreover, although these designs are either saturated or near-saturated, the crossed array resulting from the product between them does not produce an economical design.</p><p>There are also some restrictions in terms of the degrees of freedom of the final crossed-design. In this situation, all degrees of freedom account for main effects and control x noise interactions. No degrees of freedom account for noise x noise interactions or control x control interactions if they are required. In addition, if a new restriction needs to be checked (for instance optimality) the whole process has to be made again.</p><p>In contrast, our designs overcame these issues by meeting the design axioms of independence of functional requirements and minimization of information content. Furthermore, OA’s had the flexibility to be customised according to the factors and corresponding levels required, being economically feasible in comparison with current known techniques. The process of implementation was far simpler than its Taguchi’s counterpart, besides the feature of expandability in using more than one combination of factor levels for the same design.</p><p>There are some additional findings though that we will need to address. Firstly, we do not have knowledge about any computational technique to construct orthogonal arrays (the combinatorial form) than the method described by Hedayat [<xref ref-type="bibr" rid="scirp.53575-ref6">6</xref>] and the approaches proposed mainly by Schoen, Murray, and Man [<xref ref-type="bibr" rid="scirp.53575-ref11">11</xref>]. The former uses Hadamard matrices and the latter the orbit algorithm; both are based on backtrack search though; and secondly, we will need to undertake a comparative performance against a combined arrays design as well, which seems to be a very good competitor.</p><p>We are also considering dealing with some foreseen disadvantages and limitations of our designs, such as to choose the interactions to be measured, identify the representatives of each orbit and the size of them, choose a specific design within non-isomorphic arrays, and have enough computational power to run the algorithms.</p></sec><sec id="s6"><title>6. Discussion and Further Studies</title><p>The outcomes of this paper and the research project can be seen in terms of two main streams: construction and enumeration of orthogonal arrays and their practical application. From the orthogonal arrays’ construction and enumeration point of view, we are working in providing a new set of isomorphism classes and sizes of automorphism groups for some of the incomplete designs listed in [<xref ref-type="bibr" rid="scirp.53575-ref9">9</xref>]. This enumeration is being performed using a special type of backtrack search algorithm. The implementation of the arrays in the context of parameter design will improve and facilitate the maintainability and reliability activities of electrical and hydraulic-powered mechanical systems. In a similar way, using suitable comparative performance indicators, we will measure and compare pros and cons of using Crossed Array Designs, Combined Array Designs, and Symmetric Orthogonal Arrays in the context of parameter design through a new case study.</p></sec><sec id="s7"><title>Acknowledgements</title><p>My deepest gratitude to Dr Scott H. Murray for his continuous support throughout the development of this project. Many thanks also to Dr Judith A. and Dr Alice R. for your candid help during the early stages of preparing this manuscript.</p></sec><sec id="s8"><title>Cite this paper</title><p>Julio Romero,Scott H. Murray, (2015) Enumeration of Strength Three Orthogonal Arrays and Their Implementation in Parameter Design. Journal of Applied Mathematics and Physics,03,38-45. doi: 10.4236/jamp.2015.31006</p></sec></body><back><ref-list><title>References</title><ref id="scirp.53575-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Fisher, R.A. 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