<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JMMCE</journal-id><journal-title-group><journal-title>Journal of Minerals and Materials Characterization and Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-4077</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmmce.2014.24034</article-id><article-id pub-id-type="publisher-id">JMMCE-48034</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>CHEMISTRY &amp; MATERIALS SCIENCE</subject><subject>ENGINEERING</subject></subj-group></article-categories><title-group><article-title>Statistical Analysis for the Abrasive Wear Behavior of Al 6061</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mohd</surname><given-names>Shadab Khan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zahir</surname><given-names>Hasan</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yaqoob</surname><given-names>Ali Ansari</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Jahagirabad Institute of Technology, Jahangirabad, India</addr-line></aff><aff id="aff1"><addr-line>Department of Mechanical Engineering, Integral University, Lucknow, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mdshadabkhan@yahoo.com(MSK)</email>;<email>zahir_hasan@yahoo.com(ZH)</email>;<email>yaqoob2006@gmail.com(YAA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>13</day><month>06</month><year>2014</year></pub-date><volume>02</volume><issue>04</issue><fpage>292</fpage><lpage>299</lpage><history><date date-type="received"><day>2</day>	<month>April</month>	<year>2014</year></date><date date-type="rev-recd"><day>14</day>	<month>May</month>	<year>2014</year>	</date><date date-type="accepted"><day>3</day>	<month>June</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>In the present study, a mathematical model has been developed to predict the abrasive wear behavior of Al 6061. The experiments have been conducted using central composite design in the design of experiments (DOE) on pin-on-disc type wear testing machine, against abrasive media. A second order polynomial model has been developed for the prediction of wear loss. The model was developed by response surface method (RSM). Analysis of variance technique at the 95% confidence level was applied to check the validity of the model. The effect of volume percentage of reinforcement, applied load and sliding velocity on abrasive wear behavior was analyzed in detail. To judge the efficiency and ability of the model, the comparison of predicted and experimental response values outside the design conditions was carried out. The result shows, good correspondence, implying that, empirical models derived from response surface approach can be used to describe the tribological behavior of the above composite.</p></abstract><kwd-group><kwd>Abrasive Wear</kwd><kwd> Orientation</kwd><kwd> ANOVA</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Wear is related to interactions between surfaces and more specifically the removal and deformation of material on a surface as a result of mechanical action of the opposite surface [<xref ref-type="bibr" rid="scirp.48034-ref1">1</xref>] . The need for relative motion between two surfaces and initial mechanical contact between asperities is an important distinction between mechanical wear compared to other processes with similar outcomes [<xref ref-type="bibr" rid="scirp.48034-ref2">2</xref>] . Wear is a continuous process in which material is degraded at every cycle. Kloss et al. emphasized that the various tools such as wear measuring equipments, mathematical modeling, tribo-meters and simulations were used for measuring wear resistance and wear rate over many decades. It was observed by several authors [<xref ref-type="bibr" rid="scirp.48034-ref3">3</xref>] -[<xref ref-type="bibr" rid="scirp.48034-ref13">13</xref>] that the variation of friction and wear rate depends on interfacial conditions such as normal load, geometry, relative surface motion, sliding speed, surface roughness of the rubbing surfaces, type of material, system rigidity, temperature, stick slip, relative humidity, lubrication and vibration. Al 6061 is widely used in numerous engineering applications including transport and construction where, superior mechanical properties such as tensile strength and hardness are essentially required. This paper is in series with “Effect of Orientation and Applied Load on Abrasive Wear Property of Alumunium Alloy-Al 6061 and Brass 6040” [<xref ref-type="bibr" rid="scirp.48034-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.48034-ref15">15</xref>] .</p><p>The objective of this work is to perform the statistical analysis for the abrasive wear behavior of Al 6061 at different orientation and at different loads and to form the equation wear.</p></sec><sec id="s2"><title>2. Materials and Methods</title><p>In order to carry out the experimental work the following procedure is adopted: 1) specimen preparation; 2) materials selection; 3) response surface methodology (RSM).</p><sec id="s2_1"><title>2.1. Specimen Preparation</title><p>The specimen for wear studies was cut from the Al alloy bar. The specimen cross section used was 1 cm &#215; 1 cm with a length of 4.5 cm. The top and bottom surfaces of specimen were made planer by polishing against emery papers of appropriate grits. For the preparation of the surface to be used for wear studies, the final grit size of the emery paper was the same as the one to be used for the wear studies.</p></sec><sec id="s2_2"><title>2.2. Material for Wear Studies</title><p>For wear study, the material selected is Al 6061 alloy. The wear studies were conducted against grinding disc for different load at different orientation. The selection of load and orientation discussed later.</p></sec><sec id="s2_3"><title>2.3. Selection of Applied Load and the Position of the Specimen</title><p>For wear studies the following loads were selected 1) 5 N, 2) 10 N, 3) 15 N, 4) 20 N. For each load the orientation of the specimen was kept at 0˚, 30˚, 45˚, 60˚ and 90˚<sup> </sup>respectively.</p></sec><sec id="s2_4"><title>2.4. Response Surface Methodology (RSM)</title><p>RSM is a collection of mathematical and statistical techniques that are useful for the modeling and analysis of problems in which output or response is influenced by several input-variables and objective is to find the correlation between the response and the input-variables. Farias et al. [<xref ref-type="bibr" rid="scirp.48034-ref16">16</xref>] studied the sliding wear of austenitic stainless steels. They adopted to obtain an empirical model of wear rate as a function of applied load and sliding velocity using RSM. A polynomial model of second order type was proposed to represent the relationship between wear loss and tribo test independent variables. In the present work, the input variables are angle of orientation (A) measured in degree and normal applied load (L) measured in Newtons and the output (response) is wear loss (W) measured in milligram (mg). A response surface model given in Equation (1) is usually expressed as:</p><disp-formula id="scirp.48034-formula1239"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\5-2710220x\939dd210-cf73-4d15-9de7-91483ec0ab95.png"/></disp-formula><p>where A is constant of equation. B<sub>1</sub>, B<sub>2</sub>, B<sub>3</sub>, B<sub>4</sub>, … B<sub>n</sub> are the unknown regression coefficients and X<sub>1</sub>, X<sub>2</sub>, … X<sub>k</sub> are the input variables that influence the response Y, k is the number of input factors. The method of least square is used to estimate the coefficients of the second order model. The response surface analysis is then done in terms of the fitted surface. The degree of significance of the model was tested by analysis of variance (ANOVA) using the software MINITAB-15.</p></sec><sec id="s2_5"><title>2.5. Design of Experiments (DOE)</title><p>A central composite design (CCD) is used with two design factors of each of three levels to describe response of the wear loss and to estimate the parameters in the second-order model. <xref ref-type="table" rid="table1">Table 1</xref> shows important factors and their levels for abrasive wear. A central composite design (CCD) has following parameters.</p><table-wrap id="table1"  position="float"><object-id pub-id-type="pii">Table 1</object-id><label>Table 1</label><caption><p>. Important factors and their levels for abrasive wear</p></caption><table><thead><tr><th align="center" valign="middle" >S.N.</th><th align="center" valign="middle" >Factors</th><th align="center" valign="middle" >Notation</th><th align="center" valign="middle" >Unit</th><th align="center" valign="middle"  colspan="3"  >Levels</th></tr></thead><tbody><tr><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >Orientation</td><td align="center" valign="middle" >A</td><td align="center" valign="middle" >Deg</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >45</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >2.</td><td align="center" valign="middle" >Applied load</td><td align="center" valign="middle" >L</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >20</td></tr></tbody></table></table-wrap></sec></sec><sec id="s3"><title>3. Result and Discussion</title><sec id="s3_1"><title>3.1. Development of Wear Model</title><p>Central composite design of full factorial was used, a total of 14 experiments are conducted and regression coefficients were calculated as shown in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>By analyzing the estimated regression coefficients of CCD (Full Model-Uncoded Units) as shown in <xref ref-type="table" rid="table3">Table 3</xref>. The mathematical model of wear loss (W) can be expressed in term of the un-coded values of the independent variables in the Equation (2) given below:</p><disp-formula id="scirp.48034-formula1240"><label>(2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\5-2710220x\acfcbdf4-758c-4625-8b12-67689c79a6ad.png"/></disp-formula></sec><sec id="s3_2"><title>3.2. Analysis of Variance (ANOVA)</title><p>Analysis of variance (ANOVA) and the F-ratio test have been performed to check the adequacy of the model as well as the significance of the individual model coefficients. The ANOVA was carried out on the model for a confidence level of 95%. The results of ANOVA tables for wear loss are listed in <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table4">Table 4</xref>. <xref ref-type="table" rid="table2">Table 2</xref> presents the ANOVA table for the second order model propose for wear loss given in Equation (2). It can be appreciated that the P-value is less than 0.05 which means that the model is significant at 95% confidence level. Furthermore, the significance of each coefficient in the full model was examined by the t-values and P-values and the results are listed in <xref ref-type="table" rid="table4">Table 4</xref>. The larger values of t-test and smaller values of “P” indicate that the corresponding coefficient is highly significant [<xref ref-type="bibr" rid="scirp.48034-ref17">17</xref>] . Hence, the results given in <xref ref-type="table" rid="table4">Table 4</xref> suggest that the influence of load (L<sup>2</sup>) and orientation &#215; load (A &#215; L) are non-significant and therefore can be removed from the full model to further improve the model. By doing so, the full model for the wear loss is expressed in Equation (3).</p><disp-formula id="scirp.48034-formula1241"><label>(3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\5-2710220x\ce51ac1b-5367-43e7-8bd5-9a1e180cb0b9.png"/></disp-formula></sec><sec id="s3_3"><title>3.3. Analysis of Variance for Reduced Model</title><p>ANOVA was performed on the reduced model and the results are presented in <xref ref-type="table" rid="table5">Table 5</xref> in coded units and <xref ref-type="table" rid="table6">Table 6</xref> in un-coded units and found that the model is highly significant. Thus, Equation (4) represents the un-coded form of final empirical model for wear loss of Al 6061. It should be noted that the above equations are valid over the range of conditions 0˚ ≤ orientation (angle) ≤ 90˚ and 10 N &lt; normal applied load &lt; 20 N for abrasive wear of above composite against 400 grit size.</p><p>By taking regression coefficient values for reduced model, the full model for the wear loss can be reduced as:</p><disp-formula id="scirp.48034-formula1242"><label>(4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\5-2710220x\6dd730f8-fa42-4b36-b702-15f63ae15a0d.png"/></disp-formula></sec><sec id="s3_4"><title>3.4. Residual Plots for Wear Loss</title><p>The regression model is used for determining the residuals of each individual experimental run. The difference between the measured values and predicted values are called residuals. The residuals are calculated and ranked in ascending order. The normal probabilities of residuals are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The normal probability plot is used to vary the normality assumption. As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the data are spread roughly along the straight line. Hence it can be concluded that the data are normally distributed [<xref ref-type="bibr" rid="scirp.48034-ref18">18</xref>] .</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> is used to show the correlation between the residuals and from this, it is emphasized that a tendency to have runs of positive and negative residuals indicates the existence of a certain correlation. Also the plot shows that the residuals are distributed evenly in both positive and negative long the run. Hence the data can be said to be independent.</p><table-wrap id="table2"  position="float"><object-id pub-id-type="pii">Table 2</object-id><label>Table 2</label><caption><p>. Analysis of variance for wear (full model)</p></caption><table><thead><tr><th align="center" valign="middle" >Source</th><th align="center" valign="middle" >DF</th><th align="center" valign="middle" >Seq SS</th><th align="center" valign="middle" >Adj SS</th><th align="center" valign="middle" >Adj MS</th><th align="center" valign="middle" >F</th><th align="center" valign="middle" >P</th></tr></thead><tbody><tr><td align="center" valign="middle" >Regression</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.298476</td><td align="center" valign="middle" >0.298476</td><td align="center" valign="middle" >0.059695</td><td align="center" valign="middle" >86.50</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >Linear</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.261252</td><td align="center" valign="middle" >0.261252</td><td align="center" valign="middle" >0.130626</td><td align="center" valign="middle" >189.27</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >Square</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.034929</td><td align="center" valign="middle" >0.034929</td><td align="center" valign="middle" >0.017465</td><td align="center" valign="middle" >25.31</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >Interaction</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.002294</td><td align="center" valign="middle" >0.002294</td><td align="center" valign="middle" >0.002294</td><td align="center" valign="middle" >3.32</td><td align="center" valign="middle" >0.106</td></tr><tr><td align="center" valign="middle" >Residual error</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0.005521</td><td align="center" valign="middle" >0.005521</td><td align="center" valign="middle" >0.000690</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Lack-of-fit</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.004770</td><td align="center" valign="middle" >0.004770</td><td align="center" valign="middle" >0.001590</td><td align="center" valign="middle" >10.59</td><td align="center" valign="middle" >0.013</td></tr><tr><td align="center" valign="middle" >Pure error</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.000751</td><td align="center" valign="middle" >0.000751</td><td align="center" valign="middle" >0.000150</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Total</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >0.303997</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table3"  position="float"><object-id pub-id-type="pii">Table 3</object-id><label>Table 3</label><caption><p>. Estimated regression coefficients for wear using data in uncoded units</p></caption><table><thead><tr><th align="center" valign="middle" >Term</th><th align="center" valign="middle" >Coef</th></tr></thead><tbody><tr><td align="center" valign="middle" >Constant</td><td align="center" valign="middle" >0.779142</td></tr><tr><td align="center" valign="middle" >Angle</td><td align="center" valign="middle" >−0.00168839</td></tr><tr><td align="center" valign="middle" >Load</td><td align="center" valign="middle" >0.0166802</td></tr><tr><td align="center" valign="middle" >Angle &#215; angle</td><td align="center" valign="middle" >−4.81743 &#215; 10<sup>−</sup><sup>5</sup></td></tr><tr><td align="center" valign="middle" >Load &#215; load</td><td align="center" valign="middle" >−3.02118 &#215; 10<sup>−</sup><sup>4</sup></td></tr><tr><td align="center" valign="middle" >Angle &#215; load</td><td align="center" valign="middle" >0.000106444</td></tr></tbody></table></table-wrap><table-wrap id="table4"  position="float"><object-id pub-id-type="pii">Table 4</object-id><label>Table 4</label><caption><p>. Estimated regression coefficients of wear (full model)</p></caption><table><thead><tr><th align="center" valign="middle" >Term</th><th align="center" valign="middle" >Coef.</th><th align="center" valign="middle" >SE coef.</th><th align="center" valign="middle" >T</th><th align="center" valign="middle" >P</th><th align="center" valign="middle" >Description</th></tr></thead><tbody><tr><td align="center" valign="middle" >Constant</td><td align="center" valign="middle" >0.859688</td><td align="center" valign="middle" >0.01007</td><td align="center" valign="middle" >85.334</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >Significant</td></tr><tr><td align="center" valign="middle" >Angle</td><td align="center" valign="middle" >−0.199233</td><td align="center" valign="middle" >0.01072</td><td align="center" valign="middle" >−18.577</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >Significant</td></tr><tr><td align="center" valign="middle" >Load</td><td align="center" valign="middle" >0.062033</td><td align="center" valign="middle" >0.01072</td><td align="center" valign="middle" >5.784</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >Significant</td></tr><tr><td align="center" valign="middle" >Angle &#215; angle</td><td align="center" valign="middle" >−0.097553</td><td align="center" valign="middle" >0.01561</td><td align="center" valign="middle" >−6.251</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >Significant</td></tr><tr><td align="center" valign="middle" >Load &#215; load</td><td align="center" valign="middle" >-0.007553</td><td align="center" valign="middle" >0.01561</td><td align="center" valign="middle" >−0.484</td><td align="center" valign="middle" >0.641</td><td align="center" valign="middle" >Non-significant</td></tr><tr><td align="center" valign="middle" >Angle &#215; load</td><td align="center" valign="middle" >0.023950</td><td align="center" valign="middle" >0.01314</td><td align="center" valign="middle" >1.823</td><td align="center" valign="middle" >0.106</td><td align="center" valign="middle" >Non-significant</td></tr></tbody></table></table-wrap><table-wrap id="table5"  position="float"><object-id pub-id-type="pii">Table 5</object-id><label>Table 5</label><caption><p>. Estimated regression coefficients for wear (coded units)</p></caption><table><thead><tr><th align="center" valign="middle" >Term</th><th align="center" valign="middle" >Coef</th><th align="center" valign="middle" >SE</th><th align="center" valign="middle" >T</th><th align="center" valign="middle" >P</th></tr></thead><tbody><tr><td align="center" valign="middle" >Constant</td><td align="center" valign="middle" >0.85780</td><td align="center" valign="middle" >0.009986</td><td align="center" valign="middle" >85.902</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >Angle</td><td align="center" valign="middle" >0.19923</td><td align="center" valign="middle" >0.011531</td><td align="center" valign="middle" >−17.279</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >Load</td><td align="center" valign="middle" >0.06203</td><td align="center" valign="middle" >0.011531</td><td align="center" valign="middle" >5.380</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >Angle &#215; angle</td><td align="center" valign="middle" >−0.10070</td><td align="center" valign="middle" >0.015254</td><td align="center" valign="middle" >−6.602</td><td align="center" valign="middle" >0.000</td></tr></tbody></table></table-wrap><p><xref ref-type="fig" rid="fig3">Figure 3</xref> indicates the residuals versus fitted values, which shows only the maximum variation of −0.04 to +0.04 gm in wear loss between the measured and the fitted values. This plot does not reveal any obvious pattern and hence the fitted model is ample.</p><table-wrap id="table6"  position="float"><object-id pub-id-type="pii">Table 6</object-id><label>Table 6</label><caption><p>. Estimated regression coefficients for wear using data in uncoded units</p></caption><table><thead><tr><th align="center" valign="middle" >Term</th><th align="center" valign="middle" >Coef.</th></tr></thead><tbody><tr><td align="center" valign="middle" >Constant</td><td align="center" valign="middle" >0.770233</td></tr><tr><td align="center" valign="middle" >Angle</td><td align="center" valign="middle" >4.81481 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Load</td><td align="center" valign="middle" >0.0124067</td></tr><tr><td align="center" valign="middle" >Angle &#215; angle</td><td align="center" valign="middle" >−4.97284 &#215; 10<sup>−5</sup></td></tr></tbody></table></table-wrap><fig id="fig1"><label>Figure 1</label><caption><p> Normal probability plot of the residuals</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\5-2710220x\593a1ec1-2672-4cde-920d-4d716fabaab9.png"/></fig><fig id="fig2"><label>Figure 2</label><caption><p> Residual versus order of the data</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\5-2710220x\2ae22538-212e-4015-8b9c-6d2d5a8ce8df.png"/></fig></sec><sec id="s3_5"><title>3.5. Checking Adequacy of Mathematical Models</title><p>The goodness of fit of the mathematical models was also tested by coefficient of determination (R<sup>2</sup>) and adjusted coefficient of determination (R<sup>2</sup> adj). The R<sup>2</sup> is the proportion of the variation in the dependent variable explained by the regression model. On the other hand, R<sup>2</sup> adj is the coefficient of determination adjusted for the number of independent variables in the regression model. Unlike R<sup>2</sup>, the R<sup>2</sup> adj may decrease if the variables are entered in the model that does not add significantly to the model fit. The R<sup>2</sup> and R<sup>2</sup> adj values of mathematical models are found 0.974 and 0.967 respectively which clearly indicate the very good correlation between the experimental and the predicted values of the responses.</p></sec><sec id="s3_6"><title>3.6. Validity of the Models</title><p>The performance of the developed model was tested using five experimental data which were never used in the modeling process. The results predicted by the developed model were compared with the measured values and also average percentage deviation (φp) was calculated and presented in the <xref ref-type="table" rid="table7">Table 7</xref>. The results indicate that the model predicted wear loss has good validity with acceptable percentage deviation.</p><fig id="fig3"><label>Figure 3</label><caption><p> Residuals versus the fitted values</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\5-2710220x\0355a671-bea2-4bb0-a46f-358dcf0ad085.png"/></fig><table-wrap id="table7"  position="float"><object-id pub-id-type="pii">Table 7</object-id><label>Table 7</label><caption><p>. Comparison of the predicted and measured results</p></caption><table><thead><tr><th align="center" valign="middle"  colspan="2"  >Parameters</th><th align="center" valign="middle"  colspan="3"  >Wear loss</th></tr></thead><tbody><tr><td align="center" valign="middle" >A</td><td align="center" valign="middle" >L</td><td align="center" valign="middle" >Measured</td><td align="center" valign="middle" >Predicted</td><td align="center" valign="middle" >Deviation (%)</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.811</td><td align="center" valign="middle" >0.832</td><td align="center" valign="middle" >2.622</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.761</td><td align="center" valign="middle" >0.786</td><td align="center" valign="middle" >3.294</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.653</td><td align="center" valign="middle" >0.650</td><td align="center" valign="middle" >0.405</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.867</td><td align="center" valign="middle" >0.848</td><td align="center" valign="middle" >2.180</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.766</td><td align="center" valign="middle" >0.712</td><td align="center" valign="middle" >6.999</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >0.899</td><td align="center" valign="middle" >0.910</td><td align="center" valign="middle" >1.238</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >0.799</td><td align="center" valign="middle" >0.774</td><td align="center" valign="middle" >3.076</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.965</td><td align="center" valign="middle" >0.972</td><td align="center" valign="middle" >0.743</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.854</td><td align="center" valign="middle" >0.836</td><td align="center" valign="middle" >2.054</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Avg. deviation</td><td align="center" valign="middle" >2.512%</td></tr></tbody></table></table-wrap></sec></sec><sec id="s4"><title>4. 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