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<front>
<journal-meta>
<journal-id journal-id-type="pmc">CMC</journal-id>
<journal-id journal-id-type="nlm-ta">CMC</journal-id>
<journal-id journal-id-type="publisher-id">CMC</journal-id>
<journal-title-group>
<journal-title>Computers, Materials &#x0026; Continua</journal-title>
</journal-title-group>
<issn pub-type="epub">1546-2226</issn>
<issn pub-type="ppub">1546-2218</issn>
<publisher>
<publisher-name>Tech Science Press</publisher-name>
<publisher-loc>USA</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">29484</article-id>
<article-id pub-id-type="doi">10.32604/cmc.2022.029484</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Article</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>Optimum Design for the Magnification Mechanisms Employing Fuzzy Logic&#x2013;ANFIS</article-title>
<alt-title alt-title-type="left-running-head">Optimum Design for the Magnification Mechanisms Employing Fuzzy Logic&#x2013;ANFIS</alt-title>
<alt-title alt-title-type="right-running-head">Optimum Design for the Magnification Mechanisms Employing Fuzzy Logic&#x2013;ANFIS</alt-title>
</title-group>
<contrib-group content-type="authors">
<contrib id="author-1" contrib-type="author">
<name name-style="western"><surname>Huynh</surname><given-names>Ngoc Thai</given-names></name><xref ref-type="aff" rid="aff-1">1</xref></contrib>
<contrib id="author-2" contrib-type="author">
<name name-style="western"><surname>Nguyen</surname><given-names>Tien V. T.</given-names></name><xref ref-type="aff" rid="aff-2">2</xref></contrib>
<contrib id="author-3" contrib-type="author" corresp="yes">
<name name-style="western"><surname>Nguyen</surname><given-names>Quoc Manh</given-names></name><xref ref-type="aff" rid="aff-3">3</xref><email>nguyenquocmanh@utehy.edu.vn</email></contrib>
<aff id="aff-1"><label>1</label><institution>Faculty of Automobile Technology, Industrial University of Ho Chi Minh City</institution>, <addr-line>Ho Chi Minh City, 70000</addr-line>, <country>Vietnam</country></aff>
<aff id="aff-2"><label>2</label><institution>Faculty of Mechanical Technology, Industrial University of Ho Chi Minh City</institution>, <addr-line>Ho Chi Minh City, 70000</addr-line>, <country>Vietnam</country></aff>
<aff id="aff-3"><label>3</label><institution>Faculty of Mechanical Engineering, Hung Yen University of Technology and Education</institution>, <addr-line>Hung Yen, 160000</addr-line>, <country>Vietnam</country></aff>
</contrib-group>
<author-notes>
<corresp id="cor1"><label>&#x002A;</label>Corresponding Author: Quoc Manh Nguyen. Email: <email>nguyenquocmanh@utehy.edu.vn</email></corresp>
</author-notes>
<pub-date pub-type="epub" date-type="pub" iso-8601-date="2022-07-25"><day>25</day>
<month>07</month>
<year>2022</year></pub-date>
<volume>73</volume>
<issue>3</issue>
<fpage>5961</fpage>
<lpage>5983</lpage>
<history>
<date date-type="received"><day>04</day><month>3</month><year>2022</year></date>
<date date-type="accepted"><day>19</day><month>5</month><year>2022</year></date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2022 Huynh et al.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Huynh et al.</copyright-holder>
<license xlink:href="https://creativecommons.org/licenses/by/4.0/">
<license-p>This work is licensed under a <ext-link ext-link-type="uri" xlink:type="simple" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution 4.0 International License</ext-link>, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</license-p>
</license>
</permissions>
<self-uri content-type="pdf" xlink:href="TSP_CMC_29484.pdf"></self-uri>
<abstract>
<p>To achieve high work performance for compliant mechanisms of motion scope, continuous work condition, and high frequency, we propose a new hybrid algorithm that could be applied to multi-objective optimum design. In this investigation, we use the tools of finite element analysis (FEA) for a magnification mechanism to find out the effects of design variables on the magnification ratio of the mechanism and then select an optimal mechanism that could meet design requirements. A poly-algorithm including the Grey-Taguchi method, fuzzy logic system, and adaptive neuro-fuzzy inference system (ANFIS) algorithm, was utilized mainly in this study. The FEA outcomes indicated that design variables have significantly affected on magnification ratio of the mechanism and verified by analysis of variance and analysis of the signal to noise of grey relational grade. The results are also predicted by employing the tool of ANFIS in MATLAB. In conclusion, the optimal findings obtained: Its magnification is larger than 40 times in comparison with the initial design, the maximum principal stress is 127.89&#x2005;MPa, and the first modal shape frequency obtained 397.45&#x2005;Hz. Moreover, we found that the outcomes obtained deviation error compared with predicted results of displacement, stress, and frequency are 8.76&#x0025;, 3.6&#x0025;, and 6.92&#x0025;, respectively.</p>
</abstract>
<kwd-group kwd-group-type="author">
<kwd>Compliant mechanism</kwd>
<kwd>grey relational analysis</kwd>
<kwd>taguchi method</kwd>
<kwd>multi-objective optimization</kwd>
<kwd>fuzzy logic system</kwd>
<kwd>adaptive neuro-fuzzy inference system (ANFIS)</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1"><label>1</label><title>Introduction</title>
<p>Recent theoretical development has revealed that the study of the growth of effectively exact positioning-mechanisms has many challenges. As a result of the basic requirement for cutting edge advances in a few enterprises, for example, semiconductor production, where super exact machining and miniature electro-mechanical-frameworks (MEMS) are obligatory. For instance, the size of 0.15-l (130&#x2005;nm) measurement on 300 mm silicon-wafer created with a 65&#x2005;nm cycle would be realized early. Other activating systems and control methodologies are fundamental to overwhelm the current restrictions and get an accuracy position in the nanometer dimension. One technique for taking care of this sort of issue is to plan new flexure pivots fueled by piezoelectric actuators. The inalienable highlights of piezoelectric actuators (piezo actuators for short) make them tremendously alluring for driving components in these exactness position applications since they give smooth movements. They are interminable control goals, quick reaction time, and high intransigence. Nonetheless, they have experienced the failure effects of the genuine constraint of a little longitudinal expansion. Ordinary piezo actuators broaden just about 0.1&#x0025; of their length. To straightforwardly utilize, the piezo actuator to make an ideal scope of movement in various applications and an extended actuator is required. This is unrealistic. To sidestep this restriction and understand the low scope of work, with an accuracy position of a few nanometers, an amplification system utilizing adaptable pivots and driven by a piezo actuator can be used. The magnification mechanism has a compact size, high magnification ratio, high frequency, and lightweight. Therefore, the leaf flexible hinge is selected for the mechanism. To select appropriated dimensions for the mechanism, this investigation proposes a hybrid Taguchi approach based on grey relational analysis and neural network with fuzzy logic and ANFIS algorithms [<xref ref-type="bibr" rid="ref-1">1</xref>&#x2013;<xref ref-type="bibr" rid="ref-5">5</xref>].</p>
<p>The problem with such an implementation is that many flexure hinges are designed for many compliant mechanisms to eliminate the effects of clearance joints. The circular flexure hinge is designed for the 3-degree of freedom (DOF) mechanism, and 3-DOF parallel mechanism [<xref ref-type="bibr" rid="ref-6">6</xref>&#x2013;<xref ref-type="bibr" rid="ref-8">8</xref>], the stress distribution at all critical points, natural frequencies, and the corresponding modal shape estimated and verified by experiment. The dynamic performance of the 3-DOF flexible mechanical system is determined by FEA and verified by experiments. A recent study by Xu&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-9">9</xref>] concluded designing a compliant mechanism flexible hinge by employing many optimum approaches such as particle swarm optimization, the Taguchi method, grey relational analysis, and artificial neural network [<xref ref-type="bibr" rid="ref-10">10</xref>&#x2013;<xref ref-type="bibr" rid="ref-14">14</xref>]. The shaped flexure hinges were designed for many applications as presented in the reference [<xref ref-type="bibr" rid="ref-15">15</xref>]. The shaped flexure hinges obtained higher motion precision than the circular and V-shaped flexure hinges(such as the general-two segments, circular-axis, symmetry flexure-hinges) was proposed by Lobontiu&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-16">16</xref>]. The novel circular-axis flexure design was compared with the existing straight-axis right circular flexure hinge. The leaf flexible hinge was created by Qi&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-17">17</xref>], which the amplification ratio of the mechanism was determined and compared with existing methods and verified by the experiment. The Triple- Lamina Emergent Torsional (LET) and LET flexible hinge was manufactured by Qiu&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-18">18</xref>]. Triple-LET flexible hinge could obtain 1800 without plastic deformation. Three traditional flexible hinges, filleted V-shaped flexure hinges, and cycloidal hinge were designed by Tian&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-19">19</xref>]. The near form compliant formulation for filleting V-shape flexure-hinges was established and confirmed via FEA. Yang&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-20">20</xref>] proposed the filleted leaf and circular flexible hinge. The static responses of the planar symmetric superplastic flexible hinge with different notches were analyzed and compared. The static deformation and the modal shaped frequency were compared to another existing theoretical method and FEA. This is successfully established as described by Choi&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-21">21</xref>] who designed and manufactured a magnification mechanism model using a flexure hinge and confirmed by the experiment. Chen&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-22">22</xref>] computed, designed, manufactured new ultra compact decoupled XYZ&#x03B8; stage based on bridge-type compliant mechanism. The experiment outcomes are good agree with the computed results and the finite element analysis outcomes with 2&#x0025; error for the first natural frequency of stage. The bridge-type compliant mechanism with one output port was improved double output ports by Ling&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-23">23</xref>]. The improved modeling is also manufactured and experiment. The experiment verified that the stept response time is 0.8, frequency bandwidth of 120&#x2005;Hz. The rhombus-tyoe stick-slip having two driven modes was computed and manufactured for the test by Shi&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-24">24</xref>]. The results pointed out that the stage works stably with input force 1.2&#x2005;N to 1.6&#x2005;N, and work velocity with over 400 &#x03BC;m/s at frequency of 800&#x2005;Hz. Chen&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-25">25</xref>] applied nonlinear modeling method to analyze and optimize microgripper using the bridge-type amplifier. The model for experiment is also manufactured to verified the analyzed outcomes and the optimized results. The bridge-type mechanism amplifier and scott-russel mechanism were applied for a new compliant XY micro positioning stage by Wu&#x00A0;et&#x00A0;al.&#x00A0;[<xref ref-type="bibr" rid="ref-26">26</xref>]. The model for the test is also manufactured with a workspace of 181.0 &#x03BC;m &#x002A; 179.5 &#x03BC;m. The new microgripper with high amplifier was designed and manufactured by Wu et al. [<xref ref-type="bibr" rid="ref-27">27</xref>]. The outcomes displacement and the first frequency obtained 548.2 &#x03BC;m and 334&#x2005;Hz, respectively.</p>
<p>The analysis and optimization are different from the previous investigation, Gey relational analysis (GRA) based Taguchi method (TM) and ANFIS are applied to predicted displacement amplification ratio of magnification mechanism based on analysis of finite element in ANSYS. Most of the research in this field aims to solve this problem. The Taguchi method is an optimization method for one objective. However, many dimensions are requested for optimal design. Therefore, in this investigation, we utilize grey relational analysis to select one optimum case for a magnification mechanism with three objectives. Then the outcomes are verified by analysis of the signal to noise of the Taguchi method, analysis of variance, analysis of regression, Fuzzy logic, and ANFIS. Designed mechanism set up of the finite element model and boundary condition are presented in Section 2. The Grey-Taguchi, Fuzzy logic system, and ANFIS method are presented in Section 3. The outcomes and arguments will be presented in Section 4. The conclusions will be stated in Section 5.</p>
</sec>
<sec id="s2"><label>2</label><title>Design Mechanism and Setup the Finite Element Model and Boundary Condition</title>
<sec id="s2_1"><label>2.1</label><title>Design Magnification Mechanism Model</title>
<p>This assumption is supported by the fact that the model of the magnification mechanism is illustrated in <xref ref-type="fig" rid="fig-1">Fig. 1</xref>. In this study, we propose a projection of the 3 dimension model of the mechanism study. The dimensions A, B, and C are design variables. The flexure hinge thickness is 0.3 mm. When the model presented in this figure was set like the input value at the input position with an external force or displacement. The output position could be moved vertically up called as the output displacement value. And the value of the output displacement per the input displacement was called as the displacement amplification ratio.</p>
<fig id="fig-1"><label>Figure 1</label><caption><title>Magnification mechanisms employing flexible hinge</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-1.png"/></fig>
</sec>
<sec id="s2_2"><label>2.2</label><title>Setup Finite Element Model and Boundary Condition</title>
<p>The magnification mechanism with dimensions as presented in <xref ref-type="fig" rid="fig-1">Fig. 1</xref> was designed by using Solid-works and then it was imported into the mechanic&#x2019;s static structural module of ANSYS to analyze displacement, principal stress, and modal shape frequency. The material AL-7075 was used for this mechanism as listed in <xref ref-type="table" rid="table-1">Tab. 1</xref>. The young&#x2019;s modulus, Poisson&#x2019;s ratio, and tensile yield strength of the material AL-7075 are 72&#x2005;GPa, 0.33, 503&#x2005;MPa, respectively. The model mesh was divided automatically as shown in <xref ref-type="fig" rid="fig-2">Fig. 2a</xref>. with 68,233 elements and 316,289 nodes, and the element size of 0.5 mm. The boundary condition was set up at the hole surface as the fix support at the A surface, and at the B surface as input displacement of 0.01 mm, see <xref ref-type="fig" rid="fig-2">Fig. 2b</xref>. When set up a force at input position according to the y axis then the output position will translate according to the y axis.</p>
<table-wrap id="table-1"><label>Table 1</label><caption><title>Material mechanical properties</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Material</th>
<th align="left">Young&#x2019;s modulus (GPa)</th>
<th align="left">Poisson&#x2019;s ratio</th>
<th align="left">Tensile yield strength (MPa)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">AL-7075</td>
<td align="left">72</td>
<td align="left">0.33</td>
<td align="left">503</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="fig-2"><label>Figure 2</label><caption><title>Meshing for the mechanism, (b) Boundary condition</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-2.png"/></fig>
</sec>
</sec>
<sec id="s3"><label>3</label><title>Optimization Method</title>
<p>The TM employed by Minitab 18 software to create an orthogonal array. The optimal output characteristics is obtained like the theoretical model which has to be pointed out first, before the optimal methods are applied. However, the deviations seem to be very big in scale in comparison with the theoretical model. After that, the optimal methods could not be approving. Hence, in this investigation, we applied the Taguchi approach based on grey relational analysis and an artificial neural network, fuzzy logic system, and ANFIS to optimize these output characteristics. Step 1: Choosing optimization combination parameters for the output characteristics. Step 2: Designing the control factors and their levels. Step 3: Laying-out L<sub>27</sub> orthogonal array. Step 4: Carrying out simulation and collecting data. Step 5: Generating the GRA in comparison of the changes in a system undergoing analysis to estimate the importance of the design variable. The GRA is the approach applied to discretize-sequences. Normalization: Rewrite each sequence between 0 and 1 as follow [<xref ref-type="bibr" rid="ref-10">10</xref>,<xref ref-type="bibr" rid="ref-14">14</xref>] and larger the better:
<disp-formula id="eqn-1"><label>(1)</label><mml:math id="mml-eqn-1" display="block"><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mo movablelimits="true" form="prefix">min</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mn>0</mml:mn></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mo movablelimits="true" form="prefix">max</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mo movablelimits="true" form="prefix">min</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac></mml:math></disp-formula></p>
<p>Smaller the better:
<disp-formula id="eqn-2"><label>(2)</label><mml:math id="mml-eqn-2" display="block"><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mo movablelimits="true" form="prefix">max</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mn>0</mml:mn></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mo movablelimits="true" form="prefix">max</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mo movablelimits="true" form="prefix">min</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac></mml:math></disp-formula></p>
<p>Grey relational coefficient (GRC) <inline-formula id="ieqn-1"><mml:math id="mml-ieqn-1"><mml:mo stretchy="false">(</mml:mo><mml:mi>&#x03B3;</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> is the quantity approach in the grey-relational-space. GRC is requested before determining a grey-relational-grade (GRG). The deviation could be determined as follows:
<disp-formula id="eqn-3"><label>(3)</label><mml:math id="mml-eqn-3" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mn>0</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mrow><mml:mo symmetric="true">&#x2016;</mml:mo><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mn>0</mml:mn><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo symmetric="true">&#x2016;</mml:mo></mml:mrow></mml:math></disp-formula>
<disp-formula id="eqn-4"><label>(4)</label><mml:math id="mml-eqn-4" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mo movablelimits="true" form="prefix">min</mml:mo></mml:mrow></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:munder><mml:mrow><mml:mo form="prefix">max</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2200;</mml:mi><mml:mi>j</mml:mi><mml:mo>&#x2208;</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:munder><mml:mo>&#x2061;</mml:mo><mml:munder><mml:mrow><mml:mo form="prefix">min</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2200;</mml:mi><mml:mi>k</mml:mi></mml:mrow></mml:munder><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo symmetric="true">&#x2016;</mml:mo><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mn>0</mml:mn><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>j</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo symmetric="true">&#x2016;</mml:mo></mml:mrow></mml:math></disp-formula>
<disp-formula id="eqn-5"><label>(5)</label><mml:math id="mml-eqn-5" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mo movablelimits="true" form="prefix">max</mml:mo></mml:mrow></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:munder><mml:mrow><mml:mo form="prefix">max</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2200;</mml:mi><mml:mi>j</mml:mi><mml:mo>&#x2208;</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:munder><mml:mo>&#x2061;</mml:mo><mml:munder><mml:mrow><mml:mo form="prefix">max</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x2200;</mml:mi><mml:mi>k</mml:mi></mml:mrow></mml:munder><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo symmetric="true">&#x2016;</mml:mo><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mn>0</mml:mn><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>j</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo symmetric="true">&#x2016;</mml:mo></mml:mrow></mml:math></disp-formula></p>
<p>Compute grey relational coefficient (GRC).
<disp-formula id="eqn-6"><label>(6)</label><mml:math id="mml-eqn-6" display="block"><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mo movablelimits="true" form="prefix">min</mml:mo></mml:mrow></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mi>&#x03BE;</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mo movablelimits="true" form="prefix">max</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mn>0</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mi>&#x03BE;</mml:mi><mml:mo>.</mml:mo><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mo movablelimits="true" form="prefix">max</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:mfrac></mml:math></disp-formula></p>
<p>Here, <inline-formula id="ieqn-2"><mml:math id="mml-ieqn-2"><mml:mi>&#x03BE;</mml:mi><mml:mo>&#x2208;</mml:mo><mml:mo stretchy="false">[</mml:mo><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">]</mml:mo></mml:math></inline-formula> is the distinguishing coefficient. It could usually choose with 0.5.</p>
<p>Computational GRG<bold>:</bold> Determine the weight
<disp-formula id="eqn-7"><label>(7)</label><mml:math id="mml-eqn-7" display="block"><mml:mrow><mml:msub><mml:mi>&#x03C9;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mi>x</mml:mi><mml:mrow><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mo>+</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mrow><mml:msup><mml:mi>e</mml:mi><mml:mi>x</mml:mi></mml:msup></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:math></disp-formula>where <inline-formula id="ieqn-3"><mml:math id="mml-ieqn-3"><mml:mrow><mml:msub><mml:mi>&#x03C9;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> stands for the mapping function in entropy measurement and this function obtain maximum value when x&#x2009;&#x003D;&#x2009;0.5 and <inline-formula id="ieqn-4"><mml:math id="mml-ieqn-4"><mml:mrow><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mn>0.5</mml:mn></mml:mrow></mml:msup><mml:mo>&#x2212;</mml:mo></mml:mrow><mml:mn>1</mml:mn></mml:math></inline-formula>&#x2009;&#x003D;&#x2009;0.6487 and the mapping value in [0,1] obtain as follow:
<disp-formula id="eqn-8"><label>(8)</label><mml:math id="mml-eqn-8" display="block"><mml:mi>w</mml:mi><mml:mo>&#x2261;</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mn>0.5</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>m</mml:mi></mml:munderover><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03C9;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math></disp-formula></p>
<p><inline-formula id="ieqn-5"><mml:math id="mml-ieqn-5"><mml:mo>&#x2208;</mml:mo><mml:mtext>&#xA0;</mml:mtext><mml:mo>=</mml:mo><mml:mtext>&#xA0;</mml:mtext><mml:mo fence="false" stretchy="false">{</mml:mo><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mo>&#x2026;</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo fence="false" stretchy="false">}</mml:mo><mml:mo>.</mml:mo></mml:math></inline-formula> Note that <inline-formula id="ieqn-6"><mml:math id="mml-ieqn-6"><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mn>2</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mo>&#x2026;</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mi>n</mml:mi></mml:math></inline-formula></p>
<p>Determination of the total grey-relational-coefficient
<disp-formula id="eqn-9"><label>(9)</label><mml:math id="mml-eqn-9" display="block"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mo>&#x2261;</mml:mo><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>m</mml:mi></mml:munderover><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>j</mml:mi><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>r</mml:mi><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mspace width="thinmathspace" /><mml:mi>f</mml:mi><mml:mi>r</mml:mi><mml:mi>o</mml:mi><mml:mi>m</mml:mi><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mn>1</mml:mn><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>n</mml:mi></mml:math></disp-formula></p>
<p>Estimation of the normalized coefficient
<disp-formula id="eqn-10"><label>(10)</label><mml:math id="mml-eqn-10" display="block"><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mn>0.5</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x00D7;</mml:mo><mml:mi>m</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mn>0.6487</mml:mn><mml:mo>&#x00D7;</mml:mo><mml:mi>m</mml:mi></mml:mrow></mml:mfrac></mml:math></disp-formula></p>
<p>Determination of the entropy
<disp-formula id="eqn-11"><label>(11)</label><mml:math id="mml-eqn-11" display="block"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mi>k</mml:mi><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>m</mml:mi></mml:munderover><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03C9;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mfrac><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:mfrac><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mn>2</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mo>&#x2026;</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mi>n</mml:mi></mml:math></disp-formula></p>
<p>Here, <inline-formula id="ieqn-7"><mml:math id="mml-ieqn-7"><mml:mrow><mml:msub><mml:mi>&#x03C9;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> uses <xref ref-type="disp-formula" rid="eqn-10">Eq. (10)</xref></p>
<p>Computation of sum of entropy
<disp-formula id="eqn-12"><label>(12)</label><mml:math id="mml-eqn-12" display="block"><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mrow><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></disp-formula></p>
<p>Determination of the weight
<disp-formula id="eqn-13"><label>(13)</label><mml:math id="mml-eqn-13" display="block"><mml:mrow><mml:msub><mml:mi>&#x03C9;</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>E</mml:mi></mml:mrow></mml:mfrac><mml:mo>.</mml:mo><mml:mfrac><mml:mrow><mml:mo stretchy="false">[</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">]</mml:mo></mml:mrow><mml:mrow><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mrow><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>E</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo><mml:mo stretchy="false">[</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">]</mml:mo></mml:mrow></mml:mrow></mml:mfrac><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mspace width="thinmathspace" /><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mn>2</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mo>&#x2026;</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mi>n</mml:mi><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>GRG <inline-formula id="ieqn-8"><mml:math id="mml-ieqn-8"><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03C8;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the average value of GRC which is collected as follows:
<disp-formula id="eqn-14"><label>(14)</label><mml:math id="mml-eqn-14" display="block"><mml:mrow><mml:msub><mml:mi>&#x03C8;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03C9;</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03B3;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>where n is the quantity of experiment.</p>
<p>Step 6: Analysis of Taguchi [<xref ref-type="bibr" rid="ref-28">28</xref>,<xref ref-type="bibr" rid="ref-29">29</xref>]. The target of the Taguchi method is to optimize the processes for minimizing quality loss by employing an objective function. There are three functions: &#x201C;the-smaller-the-best&#x201D;, &#x201C;the-larger-the-better&#x201D;, or &#x201C;the-nominal-the-best&#x201D;. In this study, the larger the better was used to maximize grey relational grade value. The signal to noise (S/N) ratio was analyzed based on this objective function. &#x201C;the larger-the better&#x201D; approach:
<disp-formula id="eqn-15"><label>(15)</label><mml:math id="mml-eqn-15" display="block"><mml:mi>S</mml:mi><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mn>10</mml:mn><mml:mtext>&#xA0;</mml:mtext><mml:mi>l</mml:mi><mml:mi>o</mml:mi><mml:mi>g</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mi>n</mml:mi></mml:mfrac><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:msubsup><mml:mi>y</mml:mi><mml:mi>i</mml:mi><mml:mn>2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:math></disp-formula>where <inline-formula id="ieqn-9"><mml:math id="mml-ieqn-9"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the observed value average of the i<sup>th</sup> experimental step and n is the quantity of experiment that was recorded from the outcomes of FEA in ANSYS. And then all the data in <xref ref-type="table" rid="table-3">Tab. 3</xref>, was entered in to Minitab software. In other to analyze of signal to noise, the left-clicks on the menu bar and selects Stat/DOE/Taguchi/Analysis Taguchi Design. An Analysis Taguchi design dialog box appears as presented in <xref ref-type="fig" rid="fig-3">Fig. 3</xref>. Next step double click GRG in this dialog box and then clicks on Options&#x2026;, the Analysis of Taguchi Design: Options dialog appears, clicks on Lager is better. And results were presented in the results and discussion section (in <xref ref-type="fig" rid="fig-5">Fig. 5</xref> and <xref ref-type="table" rid="table-6">Tab. 6</xref>).</p>
<fig id="fig-3"><label>Figure 3</label><caption><title>Set up in Minitab to analyze signal to noise for GRG</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-3.png"/></fig>
<p>Step 7: Analysis of regression equation [<xref ref-type="bibr" rid="ref-30">30</xref>,<xref ref-type="bibr" rid="ref-31">31</xref>]. From the menu bar, clicks on the Stat/Regression/Regression/Fit Regression model. A Regression dialog box appears as illustrated in <xref ref-type="fig" rid="fig-4">Fig. 4</xref>. In this dialog box clicks on GRG for Response row. And then, selects three variables, A, B, C, for the continuous predictors row. In this dialogue box clicks on Results. At Display of results selects Expanded tables. And last time clicks on ok, clicks on ok. And the results obtained in <xref ref-type="disp-formula" rid="eqn-26">Eq. (26)</xref> as presented in the regression analysis section.</p>
<fig id="fig-4"><label>Figure 4</label><caption><title>Set up analysis of regression for GRG</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-4.png"/></fig>
<p>Step 8: {Analysis of variance (ANOVA)} [<xref ref-type="bibr" rid="ref-32">32</xref>,<xref ref-type="bibr" rid="ref-33">33</xref>]. From the menu bar, clicks on Stat/ANOVA/General linear model/Fit General linear model from the menu bar. A Regression dialog box appears, as illustrated in <xref ref-type="fig" rid="fig-5">Fig. 5</xref>. In this dialog box, clicks on GRG for the Response row., And then selects three variables, A, B, and C, for the factors row. In this dialogue box, clicks on Model. And then set up as presented in <xref ref-type="fig" rid="fig-5">Fig. 5b</xref> and selected OK. And the last one clicks on OK. The results of ANOVA were analyzed in Section 4.6.</p>
<fig id="fig-5"><label>Figure 5</label><caption><title>Set up analysis of variance for GRG</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-5.png"/></fig>
<p>Step 9: Analysis of mean and predicted outcomes [<xref ref-type="bibr" rid="ref-34">34</xref>,<xref ref-type="bibr" rid="ref-35">35</xref>]. Practices as presented in the analysis of the signal to noise section. The outcomes of the analysis of mean were analyzed in Section 4.7.</p>
<p>Step 10: Fuzzy logic system [<xref ref-type="bibr" rid="ref-36">36</xref>&#x2013;<xref ref-type="bibr" rid="ref-38">38</xref>]. The procedures for handling the data followed the suggestions for designing the controller of the fuzzy logic system (FLS). The controlling mechanism had to collect data on the way the artificial determination-creator responding in the system of closed-loop which could be performed from the <italic>knowledgebase</italic>. FLSs were built from <italic>input fuzzy sets, fuzzy rules,</italic> and <italic>output fuzzy sets</italic> depended on FLS&#x2019;s initial <italic>knowledgebase</italic>. Many rules managed and performed the inputs and outputs relationship of that system. Each parameter of inputs and outputs had every single membership function that would have been mentioned among those factor limitations throughout the discourse universe. The greater adaptation of fuzzy factors was set; the finer modification of fuzzy outputs was conducted.</p>
<p>Regarding the reactive control, the vector of fuzzy inputs includes a couple of parameters. The first one is the displacement desirability and the second one is the frequency desirability. In another word, the output of the second stage is the input of the third stage&#x2013;operated by the FLS. In this stage, the output data of the multi-characteristic performance index (MCPI) would be computed by the FLS. Its controller compared the input numerical and output numerical data to solve the problem and to employ the expected MPCI. There are many parts in a FLS such as <italic>(i) a knowledge base, (ii) fuzzier, (iii) inference machine, and (iv) defuzzier</italic>. Contributions of the FLS were considered fresh qualities that contain global optimum values of this present reality. Via the fuzzier, the actual worth was changed into an etymological variable. We considered the inference machine framework as a task of enforcement depended on the rules of fuzzy, fuzzy inference systems (FIS). It controlled the way of the consolidated principles. De-fuzzier: De-fuzzier exchanged the yield of the FIS framework into a fresh worth. Regarding the defuzzed technique, we applied the centroid approach for the change. The performance of the FIS framework, a non-fuzzy worth, was known as MCPI:
<disp-formula id="eqn-16"><label>(16)</label><mml:math id="mml-eqn-16" display="block"><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mi mathvariant="normal">&#x0394;</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mrow><mml:mo>{</mml:mo><mml:mtable columnalign="left" rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>p</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>q</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>p</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>p</mml:mi><mml:mo>&#x2264;</mml:mo><mml:mi>x</mml:mi><mml:mo>&#x2264;</mml:mo><mml:mi>q</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>q</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mi>x</mml:mi><mml:mo>&#x003C;</mml:mo><mml:mi>s</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mfrac><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>o</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mi>o</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>s</mml:mi><mml:mo>&#x2264;</mml:mo><mml:mi>x</mml:mi><mml:mo>&#x2264;</mml:mo><mml:mi>o</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>x</mml:mi><mml:mo>&#x2264;</mml:mo><mml:mi>p</mml:mi><mml:mspace width="thinmathspace" /><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>o</mml:mi><mml:mo>&#x2264;</mml:mo><mml:mi>x</mml:mi></mml:mtd></mml:mtr></mml:mtable><mml:mo fence="true" stretchy="true" symmetric="true"></mml:mo></mml:mrow></mml:math></disp-formula>where <inline-formula id="ieqn-10"><mml:math id="mml-ieqn-10"><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mi mathvariant="normal">&#x0394;</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> notes the Membership Functions (MFs) while <italic>p, q, o, s</italic> stand for the parameters, and <italic>x</italic> stands for the variable.</p>
<p>To execute the FIS framework, the Mandami strategy is utilized in this current study. Thusly, trapezoidal MFs were received for the sources of information and outcomes of the FIS to create the sorts of fuzzy. MFs were in the range from 0 to 1, and MFs could depict how a variable met the sort of fuzzy. Data sources and yields of the fuzzification framework were, after that, changed into etymological variables. The trapezoidal MFs were characterized.</p>
<p>Firstly, we computed the displacement desirability and frequency one. And afterward, we considered both ones as two inputs for the FIS. We consolidated these linguistics inputs to collect the output. We operated the trapezoidal MFs for fuzzification and defuzzification. The accompanying fuzzy principles were quickly portrayed. Fuzzy regulation: If <inline-formula id="ieqn-11"><mml:math id="mml-ieqn-11"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> stands for D<sub>1</sub> and <inline-formula id="ieqn-12"><mml:math id="mml-ieqn-12"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> stands for E<sub>1</sub> then z<sub>i</sub> stands for C<sub>1</sub> else (i runs from 1 to n), where the parameters, <inline-formula id="ieqn-13"><mml:math id="mml-ieqn-13"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula id="ieqn-14"><mml:math id="mml-ieqn-14"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> , stand for a couple of i<sup>th</sup> information sources. Besides, z<sub>i</sub> stands for the outcomes i<sup>th</sup>. We define D<sub>i</sub>, E<sub>i,</sub> with C<sub>i</sub> in comparison to MFs (&#x03BC;<sub>Di</sub>, &#x03BC;<sub>Ei</sub>, and &#x03BC;<sub>Ci</sub>), and those boundaries would be viewed as <italic>fuzzy_subsets.</italic> For processing the fuzzy knowledge base, the maximum-minimum generation of Mamdani seems to be embraced. Hence, the FIS yield would be recovered. The MFs of the FIS yield could be portrayed as an information base comprises of the rule base. Finally, the FIS yield was changed into the actual worth that created numerous fuzzy principles <italic>(programming structure: Begin &#x2026;, if-then, else, &#x2026; end.)</italic> via the defuzzification. Consequently, non-fuzzy values-based contained a data set, characterized as z<sub>o</sub>, known as MCPI:
<disp-formula id="eqn-17"><label>(17)</label><mml:math id="mml-eqn-17" display="block"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>o</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mrow><mml:msub><mml:mi>o</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mrow><mml:msub><mml:mi>o</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow></mml:mfrac></mml:math></disp-formula></p>
<p>In light of the hypothesis of the FIS framework, we found the output of MCPI via the Taguchi technique which was considered the most optimal solution for the general reactions with many optimum designing factors [<xref ref-type="bibr" rid="ref-39">39</xref>&#x2013;<xref ref-type="bibr" rid="ref-41">41</xref>]. The greater <italic>the best</italic> sort picked because of the MCPI maximum, which is depicted as:
<disp-formula id="eqn-18"><label>(18)</label><mml:math id="mml-eqn-18" display="block"><mml:mi>&#x03B7;</mml:mi><mml:mo>=</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mn>10</mml:mn><mml:mo>&#x00D7;</mml:mo><mml:mi>log</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mrow><mml:mstyle displaystyle="false" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:mi>n</mml:mi></mml:mfrac></mml:mrow></mml:mstyle></mml:mrow><mml:mo>&#x00D7;</mml:mo><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mrow><mml:mrow><mml:mstyle displaystyle="false" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mi>M</mml:mi><mml:mi>P</mml:mi><mml:mi>C</mml:mi><mml:msubsup><mml:mi>I</mml:mi><mml:mi>i</mml:mi><mml:mn>2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mrow></mml:mstyle></mml:mrow></mml:mrow></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>where MCPI<sub>i</sub> stands for the i<sup>th</sup> MCPI; n is known as the number i<sup>th</sup> experimental value.</p>
<p>We operated a Taguchi-based fuzzy logic to discover optimum competitors in the multi-objectives optimization (MOO) problem yet this methodology was considered as one of the local optimum solutions. It is clear to see that the Taguchi procedure was utilized to limit or expand a solitary wellness work as far as discrete qualities. After that, an actual issue was wanted to look for a globally optimal solution. To defeat that circumstance, ANFIS was then reached out to demonstrating the MCPI, and the MOO design for the mechanisms of one-DOF could be viably understood by utilizing the lightning attachment procedure optimization (LAPO) calculation.
<disp-formula id="eqn-19"><label>(19)</label><mml:math id="mml-eqn-19" display="block"><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mi>c</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mo movablelimits="true" form="prefix">max</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mtable columnalign="left" rowspacing="4pt" columnspacing="1em"><mml:mtr><mml:mtd><mml:mo movablelimits="true" form="prefix">min</mml:mo><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mn>3</mml:mn><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mo>&#x2026;</mml:mo><mml:mo>,</mml:mo><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mrow><mml:mi>n</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>j</mml:mi></mml:mtd></mml:mtr></mml:mtable><mml:mo>]</mml:mo></mml:mrow><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>i</mml:mi><mml:mtext>&#xA0;</mml:mtext><mml:mrow><mml:mtext>runs from 1 to n</mml:mtext></mml:mrow><mml:mo>.</mml:mo></mml:math></disp-formula></p>
<p>Step 11: ANFIS: We undertook the empirical analysis using data collected in the model of the ANFIS algorithm [<xref ref-type="bibr" rid="ref-42">42</xref>,<xref ref-type="bibr" rid="ref-43">43</xref>]. The scheme of the ANFIS is figured out. While previously mentioned, the FIS framework was the simulation procedure regarding theoretical factors where the Mamdani strategy is utilized. In the interim, ANFIS is a counterfeit approach created by coordinating the neural network with the FIS. These days, ANFIS is viewed as wise models built an association between the inlets and outlets. In the hypothesis of ANFIS, the Sugeno method was utilized to make fuzzy principles [<xref ref-type="bibr" rid="ref-44">44</xref>,<xref ref-type="bibr" rid="ref-45">45</xref>]. We characterized the FLS for the ANFIS model as following:
<disp-formula id="eqn-20"><label>(20)</label><mml:math id="mml-eqn-20" display="block"><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mrow><mml:mrow></mml:mrow><mml:mo>+</mml:mo><mml:mi>b</mml:mi><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow><mml:mrow></mml:mrow><mml:mo>+</mml:mo><mml:mi>c</mml:mi></mml:math></disp-formula>where <inline-formula id="ieqn-15"><mml:math id="mml-ieqn-15"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula id="ieqn-16"><mml:math id="mml-ieqn-16"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are known as the contributions concerning D<sub>1</sub> and D<sub>2</sub> term set, z stands for the outcome. We set a, b, c becoming constant.</p>
<p>It is clear to be seen that the ANFIS algorithm comprises the five-layer feedforward neural network. The first layer has the role of fuzzification which allotted the levels of membership to inputs dependent on the presented MFs. We depicted the first layer outlet as below:
<disp-formula id="eqn-21"><label>(21)</label><mml:math id="mml-eqn-21" display="block"><mml:mi>M</mml:mi><mml:mi>F</mml:mi><mml:msubsup><mml:mi>s</mml:mi><mml:mn>1</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mi>&#x03BD;</mml:mi><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></disp-formula>where <italic>x</italic> stands for the inlets regarding node <italic>i</italic><sup>th</sup>. <italic>Desi<sub>i</sub></italic> stands for the theory. <inline-formula id="ieqn-17"><mml:math id="mml-ieqn-17"><mml:mi>M</mml:mi><mml:mi>F</mml:mi><mml:msubsup><mml:mi>s</mml:mi><mml:mn>1</mml:mn><mml:mi>i</mml:mi></mml:msubsup></mml:math></inline-formula> stands for the MFs value of <italic>Desi<sub>i</sub>.</italic> The second layer took account of the rules of the FLS and nodes&#x2019; rule that obtained inlets and comparing to the rules of firing forte. We labeled every single node like a cycle node, <inline-formula id="ieqn-2001"><mml:math id="mml-ieqn-2001"><mml:mo>&#x220F;</mml:mo></mml:math></inline-formula>, and every single node output would be described as following:
<disp-formula id="eqn-22"><label>(22)</label><mml:math id="mml-eqn-22" display="block"><mml:mi>N</mml:mi><mml:mi>F</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>&#x03BD;</mml:mi><mml:mrow><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2026;</mml:mo><mml:mo>,</mml:mo><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mi>i</mml:mi><mml:mtext>&#xA0;</mml:mtext><mml:mrow><mml:mtext>runs from 1 to n</mml:mtext></mml:mrow></mml:math></disp-formula></p>
<p>The third layer is a standardized layer utilized to assess a proportion of terminating quality of an offered rule to an aggregate of terminating qualities all things considered. Every single node was named a cycle one. Inside that layer, NFS was labeled to the rule standardized terminating quality and characterized as shown in <xref ref-type="disp-formula" rid="eqn-2">Eq. (2)</xref>:
<disp-formula id="eqn-23"><label>(23)</label><mml:math id="mml-eqn-23" display="block"><mml:mover><mml:mrow><mml:mi>N</mml:mi><mml:mi>F</mml:mi><mml:mi>S</mml:mi></mml:mrow><mml:mo accent="false">&#x00AF;</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mrow></mml:mrow><mml:mrow><mml:mstyle displaystyle="false" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:mrow><mml:mtext>NF</mml:mtext></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mtext>S</mml:mtext></mml:mrow><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow><mml:mrow><mml:mrow><mml:mtext>NF</mml:mtext></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mtext>S</mml:mtext></mml:mrow><mml:mn>1</mml:mn></mml:msub></mml:mrow><mml:mrow></mml:mrow><mml:mo>+</mml:mo><mml:mrow><mml:mi mathvariant="normal">N</mml:mi><mml:mi mathvariant="normal">F</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mtext>S</mml:mtext></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:mrow><mml:mrow></mml:mrow><mml:mo>+</mml:mo><mml:mrow><mml:mi mathvariant="normal">N</mml:mi><mml:mi mathvariant="normal">F</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mtext>S</mml:mtext></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mo>&#x2026;</mml:mo><mml:mo>+</mml:mo><mml:mrow><mml:mtext>NFS</mml:mtext></mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:mfrac></mml:mrow></mml:mstyle></mml:mrow><mml:mrow></mml:mrow><mml:mo>,</mml:mo><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mi>i</mml:mi><mml:mtext>&#xA0;</mml:mtext><mml:mrow><mml:mtext>runs from 1 to n</mml:mtext></mml:mrow><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /></mml:math></disp-formula></p>
<p>The 4<sup>th</sup> layer stands for the defuzzification cycle and the <italic>i<sup>th</sup></italic> hub is marked as a square one by
<disp-formula id="eqn-24"><label>(24)</label><mml:math id="mml-eqn-24" display="block"><mml:mi>M</mml:mi><mml:mi>F</mml:mi><mml:msubsup><mml:mi>s</mml:mi><mml:mn>1</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mover><mml:mrow><mml:mi>N</mml:mi><mml:mi>F</mml:mi><mml:mi>S</mml:mi></mml:mrow><mml:mo accent="false">&#x00AF;</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mrow></mml:mrow><mml:mo>+</mml:mo><mml:mrow></mml:mrow><mml:mi>b</mml:mi><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:mi>c</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>,</mml:mo><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mi>i</mml:mi><mml:mtext>&#xA0;</mml:mtext><mml:mrow><mml:mtext>runs from 1 to n</mml:mtext></mml:mrow></mml:math></disp-formula></p>
<p>The 5<sup>th</sup> layer is a general outlet, he whole all things considered, which is characterized as.
<disp-formula id="eqn-25"><label>(25)</label><mml:math id="mml-eqn-25" display="block"><mml:mi>M</mml:mi><mml:mi>F</mml:mi><mml:msubsup><mml:mi>s</mml:mi><mml:mn>5</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mrow></mml:mrow><mml:mo>=</mml:mo><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mover><mml:mrow><mml:mi>N</mml:mi><mml:mi>F</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow><mml:mo accent="false">&#x00AF;</mml:mo></mml:mover><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mstyle displaystyle="false" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:munder><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mi>i</mml:mi></mml:munder><mml:mrow><mml:mi>N</mml:mi><mml:mi>F</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo>&#x00D7;</mml:mo><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>F</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:mfrac></mml:mrow></mml:mstyle></mml:mrow></mml:mrow><mml:mspace width="thickmathspace" /></mml:math></disp-formula></p>
<p>In this investigation, the trapezoidal MFs were received for the ANFIS framework too.</p>
</sec>
<sec id="s4"><label>4</label><title>Results and Discussion</title>
<sec id="s4_1"><label>4.1</label><title>Numerical Results</title>
<p>The three-length dimension was selected as three design variables with changed dimensions and presented in <xref ref-type="table" rid="table-2">Tab. 2</xref>, namely variable A (between 0 and 1 mm), variable B (20 mm, 23 mm, and 26 mm), and variable C (60 mm, 63 mm, 66&#x2005;mm). The orthogonal arrays and FEM outcomes were obtained from Minitab 18.0 and ANSYS as listed in <xref ref-type="table" rid="table-3">Tab. 3</xref>. The displacement, maximum principal stress, and the first modal shape frequency outcomes were utilized to select one combination parameters with maximum displacement, minimum stress, and maximum frequency by grey relational analysis. This method is a sort of multi-objective optimization.</p>
<table-wrap id="table-2"><label>Table 2</label><caption><title>Parameters with their design levels</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Parameters</th>
<th align="left">Unit</th>
<th align="center" colspan="3">Design levels</th>
</tr>
<tr>
<th/>
<th/>
<th align="left">1</th>
<th align="left">2</th>
<th align="left">3</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">Length A</td>
<td align="left">mm</td>
<td align="left">0</td>
<td align="left">1.0</td>
<td align="left"/>
</tr>
<tr>
<td align="left">Length B</td>
<td align="left">mm</td>
<td align="left">20</td>
<td align="left">23</td>
<td align="left">26</td>
</tr>
<tr>
<td align="left">Length C</td>
<td align="left">mm</td>
<td align="left">60</td>
<td align="left">63</td>
<td align="left">66</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="table-3"><label>Table 3</label><caption><title>Orthogonal arrays, FEM (finite element method) results</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Trial No.</th>
<th align="left">A</th>
<th align="left">B</th>
<th align="left">C</th>
<th align="left">Displacement (mm)</th>
<th align="left">Stress (MPa)</th>
<th align="left">Frequency (Hz)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">0</td>
<td align="left">20</td>
<td align="left">60</td>
<td align="left">0.364</td>
<td align="left">98.577</td>
<td align="left">264.260</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">0</td>
<td align="left">20</td>
<td align="left">63</td>
<td align="left">0.338</td>
<td align="left">103.830</td>
<td align="left">265.730</td>
</tr>
<tr>
<td align="left">3</td>
<td align="left">0</td>
<td align="left">20</td>
<td align="left">66</td>
<td align="left">0.311</td>
<td align="left">108.210</td>
<td align="left">261.930</td>
</tr>
<tr>
<td align="left">4</td>
<td align="left">0</td>
<td align="left">23</td>
<td align="left">60</td>
<td align="left">0.439</td>
<td align="left">119.310</td>
<td align="left">331.270</td>
</tr>
<tr>
<td align="left">5</td>
<td align="left">0</td>
<td align="left">23</td>
<td align="left">63</td>
<td align="left">0.428</td>
<td align="left">132.790</td>
<td align="left">319.200</td>
</tr>
<tr>
<td align="left">6</td>
<td align="left">0</td>
<td align="left">23</td>
<td align="left">66</td>
<td align="left">0.403</td>
<td align="left">142.920</td>
<td align="left">307.240</td>
</tr>
<tr>
<td align="left">7</td>
<td align="left">0</td>
<td align="left">26</td>
<td align="left">60</td>
<td align="left">0.400</td>
<td align="left">131.510</td>
<td align="left">400.180</td>
</tr>
<tr>
<td align="left">8</td>
<td align="left">0</td>
<td align="left">26</td>
<td align="left">63</td>
<td align="left">0.421</td>
<td align="left">124.940</td>
<td align="left">377.440</td>
</tr>
<tr>
<td align="left">9</td>
<td align="left">0</td>
<td align="left">26</td>
<td align="left">66</td>
<td align="left">0.386</td>
<td align="left">137.210</td>
<td align="left">351.450</td>
</tr>
<tr>
<td align="left">10</td>
<td align="left">1</td>
<td align="left">20</td>
<td align="left">60</td>
<td align="left">0.231</td>
<td align="left">106.450</td>
<td align="left">340.820</td>
</tr>
<tr>
<td align="left">11</td>
<td align="left">1</td>
<td align="left">20</td>
<td align="left">63</td>
<td align="left">0.188</td>
<td align="left">106.950</td>
<td align="left">350.320</td>
</tr>
<tr>
<td align="left">12</td>
<td align="left">1</td>
<td align="left">20</td>
<td align="left">66</td>
<td align="left">0.151</td>
<td align="left">103.540</td>
<td align="left">361.630</td>
</tr>
<tr>
<td align="left">13</td>
<td align="left">1</td>
<td align="left">23</td>
<td align="left">60</td>
<td align="left">0.31</td>
<td align="left">129.650</td>
<td align="left">393.980</td>
</tr>
<tr>
<td align="left">14</td>
<td align="left">1</td>
<td align="left">23</td>
<td align="left">63</td>
<td align="left">0.271</td>
<td align="left">113.230</td>
<td align="left">387.390</td>
</tr>
<tr>
<td align="left">15</td>
<td align="left">1</td>
<td align="left">23</td>
<td align="left">66</td>
<td align="left">0.220</td>
<td align="left">119.590</td>
<td align="left">386.400</td>
</tr>
<tr>
<td align="left">16</td>
<td align="left">1</td>
<td align="left">26</td>
<td align="left">60</td>
<td align="left">0.313</td>
<td align="left">132.180</td>
<td align="left">431.740</td>
</tr>
<tr>
<td align="left">17</td>
<td align="left">1</td>
<td align="left">26</td>
<td align="left">63</td>
<td align="left">0.288</td>
<td align="left">122.870</td>
<td align="left">427.860</td>
</tr>
<tr>
<td align="left">18</td>
<td align="left">1</td>
<td align="left">26</td>
<td align="left">66</td>
<td align="left">0.239</td>
<td align="left">131.500</td>
<td align="left">411.580</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s4_2"><label>4.2</label><title>Analysis of Grey Relational Analysis</title>
<p>Another promising finding in <xref ref-type="table" rid="table-4">Tab. 4</xref> was the values of <inline-formula id="ieqn-18"><mml:math id="mml-ieqn-18"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup></mml:math></inline-formula>(1), <inline-formula id="ieqn-19"><mml:math id="mml-ieqn-19"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup></mml:math></inline-formula>(2) and <inline-formula id="ieqn-20"><mml:math id="mml-ieqn-20"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup></mml:math></inline-formula>(3) obtained by substitute displacement, frequency, and stress in <xref ref-type="table" rid="table-3">Tab. 3</xref> into <xref ref-type="disp-formula" rid="eqn-1">Eqs. (1)</xref> and <xref ref-type="disp-formula" rid="eqn-2">(2)</xref>, respectively. The values of &#x0394;<sub>oi</sub>(1), &#x0394;<sub>oi</sub>(2) and &#x0394;<sub>oi</sub>(3) were obtained by <xref ref-type="disp-formula" rid="eqn-3">Eq. (3)</xref>. Therein <inline-formula id="ieqn-21"><mml:math id="mml-ieqn-21"><mml:msubsup><mml:mi>D</mml:mi><mml:mn>0</mml:mn><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:math></inline-formula>, <inline-formula id="ieqn-22"><mml:math id="mml-ieqn-22"><mml:msubsup><mml:mi>D</mml:mi><mml:mi>i</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> is known as <inline-formula id="ieqn-23"><mml:math id="mml-ieqn-23"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup></mml:math></inline-formula>(1), <inline-formula id="ieqn-24"><mml:math id="mml-ieqn-24"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup></mml:math></inline-formula>(2), <inline-formula id="ieqn-25"><mml:math id="mml-ieqn-25"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup></mml:math></inline-formula>(3) for DI, ST, and Fre, respectively. This is vital to correctly interpret the outcomes. But even better results are obtained when using our algorithm. It is worth discussing these interesting facts revealed by the results of &#x03B3;i(1), &#x03B3;i(2) and &#x03B3;i(3) which are listed in <xref ref-type="table" rid="table-5">Tab. 5</xref> determined by <xref ref-type="disp-formula" rid="eqn-6">Eq. (6)</xref>. The GRG values (&#x03C8;i) were calculated by <xref ref-type="disp-formula" rid="eqn-14">Eq. (14)</xref> and the rank of GRG.</p>
<table-wrap id="table-4"><label>Table 4</label><caption><title>The greater and the lower is the better of displacement) (DI ) and stress (ST), the greater is the better of frequency and the deviation error of DI, ST, and Frequency (Fre)</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">No.</th>
<th align="left"><inline-formula id="ieqn-27"><mml:math id="mml-ieqn-27"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula></th>
<th align="left"><inline-formula id="ieqn-28"><mml:math id="mml-ieqn-28"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula></th>
<th align="left"><inline-formula id="ieqn-29"><mml:math id="mml-ieqn-29"><mml:msubsup><mml:mrow><mml:mtext>D</mml:mtext></mml:mrow><mml:mrow><mml:mtext>i</mml:mtext></mml:mrow><mml:mrow><mml:mo>&#x2217;</mml:mo></mml:mrow></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mn>3</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula></th>
<th align="left">&#x0394;<sub>oi</sub>(1)</th>
<th align="left">&#x0394;<sub>oi</sub>(2)</th>
<th align="left">&#x0394;<sub>oi</sub>(3)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">0.739</td>
<td align="left">1.000</td>
<td align="left">0.014</td>
<td align="left">0.261</td>
<td align="left">0.000</td>
<td align="left">0.986</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">0.649</td>
<td align="left">0.882</td>
<td align="left">0.022</td>
<td align="left">0.351</td>
<td align="left">0.119</td>
<td align="left">0.978</td>
</tr>
<tr>
<td align="left">3</td>
<td align="left">0.553</td>
<td align="left">0.783</td>
<td align="left">0.000</td>
<td align="left">0.447</td>
<td align="left">0.217</td>
<td align="left">1.000</td>
</tr>
<tr>
<td align="left">4</td>
<td align="left">1.000</td>
<td align="left">0.532</td>
<td align="left">0.408</td>
<td align="left">0.000</td>
<td align="left">0.468</td>
<td align="left">0.593</td>
</tr>
<tr>
<td align="left">5</td>
<td align="left">0.962</td>
<td align="left">0.228</td>
<td align="left">0.337</td>
<td align="left">0.038</td>
<td align="left">0.772</td>
<td align="left">0.663</td>
</tr>
<tr>
<td align="left">6</td>
<td align="left">0.875</td>
<td align="left">0.000</td>
<td align="left">0.267</td>
<td align="left">0.125</td>
<td align="left">1.000</td>
<td align="left">0.733</td>
</tr>
<tr>
<td align="left">7</td>
<td align="left">0.934</td>
<td align="left">0.556</td>
<td align="left">0.814</td>
<td align="left">0.066</td>
<td align="left">0.444</td>
<td align="left">0.186</td>
</tr>
<tr>
<td align="left">8</td>
<td align="left">0.938</td>
<td align="left">0.405</td>
<td align="left">0.680</td>
<td align="left">0.062</td>
<td align="left">0.595</td>
<td align="left">0.319</td>
</tr>
<tr>
<td align="left">9</td>
<td align="left">0.815</td>
<td align="left">0.129</td>
<td align="left">0.527</td>
<td align="left">0.185</td>
<td align="left">0.871</td>
<td align="left">0.473</td>
</tr>
<tr>
<td align="left">10</td>
<td align="left">0.275</td>
<td align="left">0.823</td>
<td align="left">0.465</td>
<td align="left">0.724</td>
<td align="left">0.178</td>
<td align="left">0.535</td>
</tr>
<tr>
<td align="left">11</td>
<td align="left">0.128</td>
<td align="left">0.811</td>
<td align="left">0.521</td>
<td align="left">0.872</td>
<td align="left">0.188</td>
<td align="left">0.479</td>
</tr>
<tr>
<td align="left">12</td>
<td align="left">0.000</td>
<td align="left">0.888</td>
<td align="left">0.587</td>
<td align="left">1.000</td>
<td align="left">0.112</td>
<td align="left">0.413</td>
</tr>
<tr>
<td align="left">13</td>
<td align="left">0.562</td>
<td align="left">0.299</td>
<td align="left">0.777</td>
<td align="left">0.438</td>
<td align="left">0.701</td>
<td align="left">0.222</td>
</tr>
<tr>
<td align="left">14</td>
<td align="left">0.414</td>
<td align="left">0.669</td>
<td align="left">0.738</td>
<td align="left">0.586</td>
<td align="left">0.330</td>
<td align="left">0.261</td>
</tr>
<tr>
<td align="left">15</td>
<td align="left">0.238</td>
<td align="left">0.526</td>
<td align="left">0.733</td>
<td align="left">0.762</td>
<td align="left">0.474</td>
<td align="left">0.267</td>
</tr>
<tr>
<td align="left">16</td>
<td align="left">0.562</td>
<td align="left">0.242</td>
<td align="left">1.000</td>
<td align="left">0.439</td>
<td align="left">0.758</td>
<td align="left">0.000</td>
</tr>
<tr>
<td align="left">17</td>
<td align="left">0.473</td>
<td align="left">0.452</td>
<td align="left">0.977</td>
<td align="left">0.527</td>
<td align="left">0.548</td>
<td align="left">0.023</td>
</tr>
<tr>
<td align="left">18</td>
<td align="left">0.303</td>
<td align="left">0.258</td>
<td align="left">0.881</td>
<td align="left">0.697</td>
<td align="left">0.743</td>
<td align="left">0.119</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="table-5"><label>Table 5</label><caption><title>Grey relational coefficient of DI, St and Fre, grey relational grade and rank</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">No.</th>
<th align="left">&#x03B3;<sub>i</sub>(1)</th>
<th align="left">&#x03B3;<sub>i</sub>(2)</th>
<th align="left">&#x03B3;<sub>i</sub>(3)</th>
<th align="left">&#x03C8;<sub>i</sub></th>
<th align="left">Rank</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">0.657</td>
<td align="left">1.000</td>
<td align="left">0.336</td>
<td align="left">0.742</td>
<td align="left">2</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">0.588</td>
<td align="left">0.808</td>
<td align="left">0.338</td>
<td align="left">0.646</td>
<td align="left">8</td>
</tr>
<tr>
<td align="left">3</td>
<td align="left">0.528</td>
<td align="left">0.697</td>
<td align="left">0.333</td>
<td align="left">0.580</td>
<td align="left">17</td>
</tr>
<tr>
<td align="left">4</td>
<td align="left">1.000</td>
<td align="left">0.517</td>
<td align="left">0.458</td>
<td align="left">0.735</td>
<td align="left">3</td>
</tr>
<tr>
<td align="left">5</td>
<td align="left">0.929</td>
<td align="left">0.393</td>
<td align="left">0.430</td>
<td align="left">0.653</td>
<td align="left">7</td>
</tr>
<tr>
<td align="left">6</td>
<td align="left">0.799</td>
<td align="left">0.333</td>
<td align="left">0.405</td>
<td align="left">0.573</td>
<td align="left">18</td>
</tr>
<tr>
<td align="left">7</td>
<td align="left">0.883</td>
<td align="left">0.529</td>
<td align="left">0.730</td>
<td align="left">0.797</td>
<td align="left">1</td>
</tr>
<tr>
<td align="left">8</td>
<td align="left">0.889</td>
<td align="left">0.457</td>
<td align="left">0.610</td>
<td align="left">0.728</td>
<td align="left">4</td>
</tr>
<tr>
<td align="left">9</td>
<td align="left">0.729</td>
<td align="left">0.365</td>
<td align="left">0.514</td>
<td align="left">0.599</td>
<td align="left">14</td>
</tr>
<tr>
<td align="left">10</td>
<td align="left">0.408</td>
<td align="left">0.738</td>
<td align="left">0.483</td>
<td align="left">0.606</td>
<td align="left">12</td>
</tr>
<tr>
<td align="left">11</td>
<td align="left">0.365</td>
<td align="left">0.726</td>
<td align="left">0.511</td>
<td align="left">0.596</td>
<td align="left">15</td>
</tr>
<tr>
<td align="left">12</td>
<td align="left">0.333</td>
<td align="left">0.817</td>
<td align="left">0.548</td>
<td align="left">0.632</td>
<td align="left">10</td>
</tr>
<tr>
<td align="left">13</td>
<td align="left">0.533</td>
<td align="left">0.416</td>
<td align="left">0.692</td>
<td align="left">0.611</td>
<td align="left">11</td>
</tr>
<tr>
<td align="left">14</td>
<td align="left">0.461</td>
<td align="left">0.602</td>
<td align="left">0.657</td>
<td align="left">0.640</td>
<td align="left">9</td>
</tr>
<tr>
<td align="left">15</td>
<td align="left">0.396</td>
<td align="left">0.513</td>
<td align="left">0.652</td>
<td align="left">0.581</td>
<td align="left">16</td>
</tr>
<tr>
<td align="left">16</td>
<td align="left">0.533</td>
<td align="left">0.398</td>
<td align="left">1.000</td>
<td align="left">0.719</td>
<td align="left">5</td>
</tr>
<tr>
<td align="left">17</td>
<td align="left">0.487</td>
<td align="left">0.477</td>
<td align="left">0.956</td>
<td align="left">0.715</td>
<td align="left">6</td>
</tr>
<tr>
<td align="left">18</td>
<td align="left">0.418</td>
<td align="left">0.402</td>
<td align="left">0.808</td>
<td align="left">0.606</td>
<td align="left">13</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s4_3"><label>4.3</label><title>Regression Analysis</title>
<p>From these results, it is clear that the regression-equation (RE) of GRG was gained through Minitab 18 as presented in <xref ref-type="disp-formula" rid="eqn-16">Eq. (16)</xref>. The chart of this equation was plotted in <xref ref-type="fig" rid="fig-6">Fig. 6</xref> to compare simulation outcomes with the GRG values of RE.
<disp-formula id="eqn-26"><label>(26)</label><mml:math id="mml-eqn-26" display="block"><mml:mtable columnalign='left'>
<mml:mtr>
<mml:mtd>
<mml:mi>G</mml:mi><mml:mi>R</mml:mi><mml:mi>G</mml:mi><mml:mo>=</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mn>5.74</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mn>1.523</mml:mn><mml:mi>A</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>0.0002</mml:mn><mml:mi>B</mml:mi><mml:mo>+</mml:mo><mml:mn>0.229</mml:mn><mml:mi>C</mml:mi><mml:mo>+</mml:mo><mml:mn>0.00352</mml:mn><mml:msup>
<mml:mi>B</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2212;</mml:mo><mml:mn>0.0016</mml:mn><mml:msup>
<mml:mi>C</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>+</mml:mo><mml:mn>0.00272</mml:mn><mml:mi>A</mml:mi><mml:mi>B</mml:mi>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mtext>&#x2003;&#x2003;</mml:mtext><mml:mo>+</mml:mo><mml:mn>0.02257</mml:mn><mml:mi>A</mml:mi><mml:mi>C</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>0.002429</mml:mn><mml:mi>B</mml:mi><mml:mi>C</mml:mi>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:math></disp-formula></p>
<fig id="fig-6"><label>Figure 6</label><caption><title>Plot of GRG</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-6.png"/></fig>
<p>We found that the results agree well with the other single methods. The graph of GRG was painted in <xref ref-type="fig" rid="fig-6">Fig. 6</xref> with the values of GRG as listed in <xref ref-type="table" rid="table-3 table-4">Tabs. 3&#x2013;4</xref>. The maximum value of GRG is 0.7973 and the minimum value of GRG is 0.5802. The predicted values of GRG as drawn in <xref ref-type="fig" rid="fig-6">Fig. 6</xref> to compare with the FEM values (simulation values). The predicted and simulated values are approximated with each other because the graphs of GRG lie near each other.</p>
</sec>
<sec id="s4_4"><label>4.4</label><title>Surface Plot</title>
<p>Overall, our proposed approach is obtained the most robust results. The surface plot of GRG as shown in <xref ref-type="fig" rid="fig-7">Fig. 7</xref>, revealed that the output GRG has been significantly affected by three design variables. Therein, variable C has influenced more than variables A and B. The value of GRG slightly increases as variables A and B which are presented in <xref ref-type="fig" rid="fig-7">Fig. 7a</xref>. The value of GRG reduces from 0.8 to 0.6 as variable C increases from 60&#x2005;mm to 62&#x2005;mm as presented in <xref ref-type="fig" rid="fig-7">Figs. 7b</xref>&#x2013;<xref ref-type="fig" rid="fig-7">7c</xref>.</p>
<fig id="fig-7"><label>Figure 7</label><caption><title>Surface plot of GRG <italic>vs.</italic> three variables A, B, C</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-7.png"/></fig>
</sec>
<sec id="s4_5"><label>4.5</label><title>Analysis Signal to Noise</title>
<p>From these results, it is clear that the graph of S/N of GRG was painted from the values in <xref ref-type="table" rid="table-6">Tab. 6</xref>. <xref ref-type="fig" rid="fig-8">Fig. 8</xref> pointed out that the design variables optimal value at A<sub>1</sub>, B<sub>3</sub>, C<sub>1</sub>, respectively, to the seventh case in <xref ref-type="table" rid="table-5">Tab. 5</xref>, and the optimal value of GRG obtained 0.7973.</p>
<table-wrap id="table-6"><label>Table 6</label><caption><title>Response for the S/N ratios</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Level</th>
<th align="left">A</th>
<th align="left">B</th>
<th align="left">C</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">&#x2212;3.501</td>
<td align="left">&#x2212;6.990</td>
<td align="left">&#x2212;3.120</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">&#x2212;3.979</td>
<td align="left">&#x2212;4.013</td>
<td align="left">&#x2212;3.590</td>
</tr>
<tr>
<td align="left">3</td>
<td align="center"/>
<td align="left">&#x2212;3.218</td>
<td align="left">&#x2212;4.511</td>
</tr>
<tr>
<td align="left">Delta</td>
<td align="left">0.478</td>
<td align="left">0.795</td>
<td align="left">1.391</td>
</tr>
<tr>
<td align="left">Rank</td>
<td align="left">3</td>
<td align="left">2</td>
<td align="left">1</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="fig-8"><label>Figure 8</label><caption><title>Plot S/N of GRG</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-8.png"/></fig>
</sec>
<sec id="s4_6"><label>4.6</label><title>Analysis of Variance of GRG</title>
<p><xref ref-type="table" rid="table-7">Tab. 7</xref> presents the analysis of the variance of GRG and it is worth discussing these interesting facts revealed by the results of the <italic>P</italic>-values. They are less than 0.05 indicated design variables playing an important role in the optimal design amplification ratio of the magnification mechanism. The contribution percent of factors namely the following: Variable A is 8.39&#x0025;, variable B is 18.83&#x0025;, variable C is 44.09&#x0025;, variable A&#x00D7;C is 17.88&#x0025; and variable B&#x00D7;C is 8.27&#x0025; with a deviation error is 2.54&#x0025;. The problem indicated that FEM and optimization outcomes are good agreement with the theory [<xref ref-type="bibr" rid="ref-46">46</xref>&#x2013;<xref ref-type="bibr" rid="ref-48">48</xref>].</p>
<table-wrap id="table-7"><label>Table 7</label><caption><title>ANOVA results of GRG</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Source</th>
<th align="left">DF</th>
<th align="left">Seq SS</th>
<th align="left">Contribution</th>
<th align="left">Adj SS</th>
<th align="left">Adj MS</th>
<th align="left">F-Value</th>
<th align="left"><italic>P</italic>-Value</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">A</td>
<td align="left">1</td>
<td align="left">0.006643</td>
<td align="left">8.39&#x0025;</td>
<td align="left">0.006643</td>
<td align="left">0.006643</td>
<td align="left">19.84</td>
<td align="left">0.004</td>
</tr>
<tr>
<td align="left">B</td>
<td align="left">2</td>
<td align="left">0.014899</td>
<td align="left">18.83&#x0025;</td>
<td align="left">0.014899</td>
<td align="left">0.007450</td>
<td align="left">22.24</td>
<td align="left">0.002</td>
</tr>
<tr>
<td align="left">C</td>
<td align="left">2</td>
<td align="left">0.034893</td>
<td align="left">44.09&#x0025;</td>
<td align="left">0.034893</td>
<td align="left">0.017446</td>
<td align="left">52.09</td>
<td align="left">0.000</td>
</tr>
<tr>
<td align="left">A &#x00D7; C</td>
<td align="left">2</td>
<td align="left">0.014152</td>
<td align="left">17.88&#x0025;</td>
<td align="left">0.014152</td>
<td align="left">0.007076</td>
<td align="left">21.13</td>
<td align="left">0.002</td>
</tr>
<tr>
<td align="left">B &#x00D7; C</td>
<td align="left">4</td>
<td align="left">0.006546</td>
<td align="left">8.27&#x0025;</td>
<td align="left">0.006546</td>
<td align="left">0.001636</td>
<td align="left">4.89</td>
<td align="left">0.043</td>
</tr>
<tr>
<td align="left">Error</td>
<td align="left">6</td>
<td align="left">0.002009</td>
<td align="left">2.54&#x0025;</td>
<td align="left">0.002009</td>
<td align="left">0.000335</td>
<td align="right"/>
<td align="right"/>
</tr>
<tr>
<td align="left">Total</td>
<td align="left">17</td>
<td align="left">0.079143</td>
<td align="left">100.00&#x0025;</td>
<td align="right"/>
<td align="right"/>
<td align="right"/>
<td align="right"/>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s4_7"><label>4.7</label><title>Mean Analysis and Confirmation of Predicted and Optimization Values</title>
<p>The finding in this investigation is equal to or better than an outcome that is presently accepted. The outcome of the mean analysis of GRG is illustrated in <xref ref-type="table" rid="table-8">Tab. 8</xref> and <xref ref-type="fig" rid="fig-9">Fig. 9</xref>. The maximum values of GRG are optimal, namely is A1B3C1 with the value of variable A is 0.6726, variable B is 0.694 and variable C is 0.7018, respectively. The optimal outcome is the seventh case in <xref ref-type="table" rid="table-5">Tab. 5</xref>.</p>
<table-wrap id="table-8"><label>Table 8</label><caption><title>Response for means of GRG</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Level</th>
<th align="left">A</th>
<th align="left">B</th>
<th align="left">C</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">0.6726</td>
<td align="left">0.6338</td>
<td align="left">0.7018</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">0.6341</td>
<td align="left">0.6322</td>
<td align="left">0.6630</td>
</tr>
<tr>
<td align="left">3</td>
<td align="center"/>
<td align="left">0.6940</td>
<td align="left">0.5953</td>
</tr>
<tr>
<td align="left">Delta</td>
<td align="left">0.0384</td>
<td align="left">0.0618</td>
<td align="left">0.1066</td>
</tr>
<tr>
<td align="left">Rank</td>
<td align="left">3</td>
<td align="left">2</td>
<td align="left">1</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="fig-9"><label>Figure 9</label><caption><title>Plot means of GRG</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-9.png"/></fig>
<p>It is significant to pay attention that the current outcome relies on the mean analysis of displacement as illustrated in <xref ref-type="table" rid="table-9">Tab. 9</xref> and <xref ref-type="fig" rid="fig-10">Fig. 10</xref>. Whereby, the optimal values of displacement were A<sub>1</sub>, B<sub>3</sub>, C<sub>1</sub>. The value of variable A is 0.3901&#x2005;mm, the variable B is 0.3444&#x2005;mm and the value of variable C is 0.3466&#x2005;mm, respectively. Together, the present findings confirm that the outcome of the mean analysis of maximum principal stress as illustrated in <xref ref-type="table" rid="table-11">Tab. 11</xref> and <xref ref-type="fig" rid="fig-12">Fig. 12</xref>. whereby, the optimal values of stress A1B3C1 with the value: Variable A is 120.7&#x2005;MPa, variable B is 127.8&#x2005;MPa and variable C is 117.4&#x2005;MPa, respectively. A further novel finding is that the outcome of the mean analysis of the first model shape of frequency as illustrated in <xref ref-type="table" rid="table-10">Tab. 10</xref> and <xref ref-type="fig" rid="fig-11">Fig. 11</xref>. Whereby, the optimal values of stress A1B3C1 with the value of variable A is 319.3&#x2005;Hz, variable B is 399.2&#x2005;MPa and variable C is 359.5&#x2005;MPa, respectively.</p>
<table-wrap id="table-9"><label>Table 9</label><caption><title>Responses for the displacement means</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Level</th>
<th align="left">A</th>
<th align="left">B</th>
<th align="left">C</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">0.3879</td>
<td align="left">0.2638</td>
<td align="left">0.3433</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">0.2459</td>
<td align="left">0.3457</td>
<td align="left">0.3224</td>
</tr>
<tr>
<td align="left">3</td>
<td align="center"/>
<td align="left">0.3411</td>
<td align="left">0.2849</td>
</tr>
<tr>
<td align="left">Delta</td>
<td align="left">0.1442</td>
<td align="left">0.0819</td>
<td align="left">0.0617</td>
</tr>
<tr>
<td align="left">Rank</td>
<td align="left">1</td>
<td align="left">2</td>
<td align="left">3</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="fig-10"><label>Figure 10</label><caption><title>Plot means of DI</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-10.png"/></fig>
<table-wrap id="table-10"><label>Table 10</label><caption><title>Responses for the frequency means</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Level</th>
<th align="left">A</th>
<th align="left">B</th>
<th align="left">C</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">319.3</td>
<td align="left">307.4</td>
<td align="left">359.5</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">388.0</td>
<td align="left">354.2</td>
<td align="left">354.7</td>
</tr>
<tr>
<td align="left">3</td>
<td align="center"/>
<td align="left">399.2</td>
<td align="left">346.7</td>
</tr>
<tr>
<td align="left">Delta</td>
<td align="left">68.7</td>
<td align="left">91.8</td>
<td align="left">12.8</td>
</tr>
<tr>
<td align="left">Rank</td>
<td align="left">2</td>
<td align="left">1</td>
<td align="left">3</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="table-11"><label>Table 11</label><caption><title>Responses for the stress means</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Level</th>
<th align="left">A</th>
<th align="left">B</th>
<th align="left">C</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">1</td>
<td align="left">120.7</td>
<td align="left">104.6</td>
<td align="left">117.4</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">118.4</td>
<td align="left">126.2</td>
<td align="left">117.4</td>
</tr>
<tr>
<td align="left">3</td>
<td align="center"/>
<td align="left">127.8</td>
<td align="left">123.8</td>
</tr>
<tr>
<td align="left">Delta</td>
<td align="left">2.2</td>
<td align="left">23.2</td>
<td align="left">6.4</td>
</tr>
<tr>
<td align="left">Rank</td>
<td align="left">3</td>
<td align="left">1</td>
<td align="left">2</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="fig-11"><label>Figure 11</label><caption><title>Plot means of the 1<sup>st</sup> model shape FR</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-11.png"/></fig>
<fig id="fig-12"><label>Figure 12</label><caption><title>Plot means of ST</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-12.png"/></fig>
<p>As listed in <xref ref-type="table" rid="table-12">Tabs. 12</xref> and <xref ref-type="table" rid="table-13">13</xref>, size element and type meshed have slightly affected displacement, maximum principal stress and frequency.
<disp-formula id="ueqn-1">
<mml:math id="mml-ueqn-1" display="block"><mml:mrow><mml:msub><mml:mi>&#x03BC;</mml:mi><mml:mi>G</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>G</mml:mi></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:munderover><mml:mo movablelimits="false">&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>q</mml:mi></mml:munderover><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>o</mml:mi></mml:msub></mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>G</mml:mi></mml:msub></mml:mrow></mml:mrow><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mi>A</mml:mi><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi>B</mml:mi><mml:mn>3</mml:mn><mml:mo>+</mml:mo><mml:mi>C</mml:mi><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mn>2</mml:mn><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>G</mml:mi></mml:msub></mml:mrow><mml:mspace width="thinmathspace" /><mml:mspace width="thinmathspace" /><mml:mo>=</mml:mo><mml:mn>0.6726</mml:mn><mml:mo>+</mml:mo><mml:mn>0.694</mml:mn><mml:mo>+</mml:mo><mml:mn>0.7018</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mn>2</mml:mn><mml:mo>&#x00D7;</mml:mo><mml:mn>0.65334</mml:mn><mml:mo>=</mml:mo><mml:mn>0.7616</mml:mn></mml:math></disp-formula>
<disp-formula id="ueqn-2">
<mml:math id="mml-ueqn-2" display="block"><mml:mi>C</mml:mi><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mi>E</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mo>&#x00B1;</mml:mo><mml:msqrt><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>&#x03B1;</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mi>f</mml:mi><mml:mi>e</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mi>V</mml:mi><mml:mi>e</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mrow><mml:mi>e</mml:mi><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:mfrac><mml:mo>+</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:mfrac></mml:msqrt><mml:mo stretchy="false">)</mml:mo></mml:math></disp-formula>at &#x03B1;&#x2009;&#x003D;&#x2009;0.05, Fe&#x2009;&#x003D;&#x2009;&#x2009;16, F<sub>0.05</sub>(1, 6)&#x2009;&#x003D;&#x2009;5.9874 [<xref ref-type="bibr" rid="ref-22">22</xref>] , Ve&#x2009;&#x003D;&#x2009;0.000335, R&#x2009;&#x003D;&#x2009;11, Re&#x2009;&#x003D;&#x2009;1, n&#x2009;&#x003D;&#x2009;18.</p>
<table-wrap id="table-12"><label>Table 12</label><caption><title>Output value with the different size element value</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Type mesh</th>
<th align="center" colspan="3">Fine</th>
</tr>
<tr>
<th align="left">Size element</th>
<th align="left">Displacement (mm)</th>
<th align="left">Maximum principle stress (MPa)</th>
<th align="left">Frequency(Hz)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">0.2</td>
<td align="left">0.40536</td>
<td align="left">135.81</td>
<td align="left">398.52</td>
</tr>
<tr>
<td align="left">0.5</td>
<td align="left">0.40345</td>
<td align="left">131.51</td>
<td align="left">400.18</td>
</tr>
<tr>
<td align="left">0.8</td>
<td align="left">0.4049</td>
<td align="left">133.22</td>
<td align="left">402.3</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="table-13"><label>Table 13</label><caption><title>Output value with a different type of mesh</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left">Type mesh</th>
<th align="center" colspan="3">0.5 mm</th>
</tr>
<tr>
<th align="left">Size element</th>
<th align="left">Displacement (mm)</th>
<th align="left">Maximum principle stress (MPa)</th>
<th align="left">Frequency(Hz)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">Coarse</td>
<td align="left">0.40213</td>
<td align="left">128.7</td>
<td align="left">398.50</td>
</tr>
<tr>
<td align="left">Fine</td>
<td align="left">0.40232</td>
<td align="left">128.7</td>
<td align="left">398.53</td>
</tr>
</tbody>
</table>
</table-wrap>
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<p>We showed that, whereby, the predicted values of GRG, DI, ST, frequency are 0.7616, 0.4385&#x2005;mm, 126.7882&#x2005;MPa and 372.4756&#x2005;Hz, respectively. The GREY relational analysis outcome gained one optimization case and then use this case to simulate and obtained optimization outcomes of GRG, DI, ST and Fre are 0.7973, 0.4001&#x2005;mm, 131.51&#x2005;MPa and 400.18&#x2005;Hz as shown in <xref ref-type="table" rid="table-14">Tab. 14</xref>. In this Tab, the optimal value of GRG archived from the proposed method is 0.8212 is higher than the grey based on Taguchi method of 0.7973. However, the deviation between two methods are 2.91&#x0025;. The outcomes proved the optimal methods obtained the output values approximate to the predicted values [<xref ref-type="bibr" rid="ref-49">49</xref>&#x2013;<xref ref-type="bibr" rid="ref-55">55</xref>] because the deviation error of GRG, DI, ST, and frequency between the forecast and optimal value is less than 9&#x0025;.</p>
<table-wrap id="table-14"><label>Table 14</label><caption><title>Compare the predicted and optimal values of method</title></caption>
<table frame="hsides">
<colgroup>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
<col align="left"/>
</colgroup>
<thead>
<tr>
<th align="left"/>
<th align="left">Hybrid optimization</th>
<th align="left">GRG</th>
<th align="left">DI (mm)</th>
<th align="left">ST (MPa)</th>
<th align="left">Frequency (Hz)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">Predicted values (i)</td>
<td align="left" rowspan="5">A1B3C1</td>
<td align="left">0.7616</td>
<td align="left">0.4385</td>
<td align="left">126.7882</td>
<td align="left">372.4756</td>
</tr>
<tr>
<td align="left">Optimization without Fuzzy logic ANFIS (ii)</td>
<td align="left">0.7973</td>
<td align="left">0.4001</td>
<td align="left">131.51</td>
<td align="left">400.18</td>
</tr>
<tr>
<td align="left">Our proposed approach (iii)</td>
<td align="left">0.8212</td>
<td align="left">0.4521</td>
<td align="left">127.894</td>
<td align="left">397.45</td>
</tr>
<tr>
<td align="left">Error (&#x0025;) between (i) <italic>vs.</italic> (ii)</td>
<td align="left">4.48</td>
<td align="left">8.76</td>
<td align="left">3.6</td>
<td align="left">6.92</td>
</tr>
<tr>
<td align="left">Error (&#x0025;) between (ii) <italic>vs.</italic> (iii)</td>
<td align="left">2.91</td>
<td align="left">11.50</td>
<td align="left">2.83</td>
<td align="left">0.69</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The findings are equal to or better than those of previous studies that are currently agreed upon. From these results, it is clear that after choosing the mechanism with combination variables at optimal values, the static structural and modal shape were used to obtain the optimum value of displacement, maximum principal stress, and the first modal shape of frequency which are 0.4521&#x2005;mm, 127.894&#x2005;MPa, and 397.45&#x2005;Hz as depicted in <xref ref-type="fig" rid="fig-13">Figs. 13a</xref> and <xref ref-type="fig" rid="fig-13">13b</xref>&#x2013;<xref ref-type="fig" rid="fig-13">13c</xref>, respectively. We found that our outcomes are currently better than those of the previous studies [<xref ref-type="bibr" rid="ref-17">17</xref>,<xref ref-type="bibr" rid="ref-21">21</xref>&#x2013;<xref ref-type="bibr" rid="ref-28">28</xref>].</p>
<fig id="fig-13"><label>Figure 13</label><caption><title>The FEM outcomes with variables at optimal levels: (a) displacement, (b) maximum principal stress, (c) the first model shape frequency</title></caption><graphic mimetype="image" mime-subtype="png" xlink:href="CMC_29484-fig-13.png"/></fig>
</sec>
</sec>
<sec id="s5"><label>5</label><title>Remarkable Conclusions</title>
<p>This conclusion follows from the fact that the influences of three variables (A, B, C) on displacement, maximum principal stress, and frequency of the first modeling shape case were analyzed through using FEA. Our findings identified that these variables have strongly affected three outputs as proved by S/N analysis, ANOVA, regression analysis, prediction of the artificial neural network, statistical analysis, Fuzzy logic system, and ANFIS. Besides, these findings provided additional information about the simulation, optimization, prediction results which are good to agree with and better than the previous publication as presented and discussed. The magnification ratio, maximum principal stress, and the first modal shape frequency were obtained larger than 40.35 times, 127.894&#x2005;MPa, and 397.45&#x2005;Hz, respectively. Nevertheless, we found that the optimal method was permitted to utilize optimization analysis for variables of the compliant mechanism because the outcomes of the research have errors that are less than 9&#x0025;. From the obtained outputs pointed out that the Taguchi method based on grey relational analysis and ANFIS are the robust optimization methods. The methods proposed to apply for optimal problem in the fields technique, industry, life and society.</p>
</sec>
</body>
<back>
<fn-group>
<fn fn-type="other"><p><bold>Funding Statement:</bold> This work is funded by Hung Yen University of Technology and Education and Industrial University of Ho Chi Minh City.</p></fn>
<fn fn-type="conflict"><p><bold>Conflicts of Interest:</bold> The authors declare that they have no conflicts of interest to report regarding the present study.</p></fn>
</fn-group>
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