<?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">MSCE</journal-id><journal-title-group><journal-title>Journal of Materials Science and Chemical Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-6045</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msce.2015.37014</article-id><article-id pub-id-type="publisher-id">MSCE-57689</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></subj-group></article-categories><title-group><article-title>
 
 
  Evaluation of Filler Distribution in Particulate Reinforced Composites
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kurganova</surname><given-names>Yuliya</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Lopatina</surname><given-names>Yuliya</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yijin</surname><given-names>Chen</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Engineering Technology, Bauman Moscow State Technical University, Moscow, Russia</addr-line></aff><pub-date pub-type="epub"><day>19</day><month>06</month><year>2015</year></pub-date><volume>03</volume><issue>07</issue><fpage>108</fpage><lpage>112</lpage><history><date date-type="received"><day>31</day>	<month>March</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>24</month>	<year>June</year>	</date><date date-type="accepted"><day>1</day>	<month>July</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   Aluminum matrix particulate reinforced composites are of significant interest to industry, but it’s difficult to provide stable properties for this group of material. The mechanical properties of metal matrix composites are deeply influenced by the distribution of reinforcement particulates in the matrix. In this paper uniformity of SiC particles distribution in Al-based composites produced by stir casting and powder metallurgy technique is assessed. Analysis is carried out by means of classical and computer quantification metallographic image analysis methods. In addition, we suggest setting hardness distribution in cross section of samples as an indicator of reinforcement distribution uniformity in the matrix. 
 
</p></abstract><kwd-group><kwd>Particulate Reinforced Composites</kwd><kwd> Metal Matrix Composites</kwd><kwd> Filler Distribution</kwd><kwd> Quantification Metallographic Analysis</kwd><kwd> Microhardness</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The ever rising of fuel price day to day has led to a renewed urgency to concentrate on the issue of weight reduction in the aerospace and automotive sectors. As monolithic alloys possess low strength to weight ratio, hardness, stiffness etc. so the area of application of these alloys restricted. This limitation has circumvented by incorporation of harder and stiffer ceramic particulates in the matrix, which is known as composite. Composites are significant for engineering materials due to their excellent mechanical properties over monolithic alloys. Aluminum and its alloys based metal matrix composites (MMCs) reinforced by silicon carbide particles are one of the widely known composites because of their superior properties such as high strength to weight ratio, hardness, stiffness, wear and corrosion resistances etc. over monolithic metals &amp; its alloys [<xref ref-type="bibr" rid="scirp.57689-ref1">1</xref>].</p><p>The distribution of particulates in MMCs is a major factor in determining the in-service properties of engineering components [<xref ref-type="bibr" rid="scirp.57689-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.57689-ref3">3</xref>]. Existing techniques of producing particulate reinforced MMCs are not perfect and cannot provide ideal filler distribution, so it’s required to evaluate reinforcement distribution uniformity in the matrix [<xref ref-type="bibr" rid="scirp.57689-ref4">4</xref>].</p></sec><sec id="s2"><title>2. Experimental Procedure</title><sec id="s2_1"><title>2.1. Materials and Fabrication of Composites</title><p>In the present experiment metal matrix composites including various volume fractions of SiC particles were produced by stir casting method and powder metallurgy technique. Set of specimens used in this study is given in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>For liquid state processing aluminum alloys AK12, AL25, V124 and D16 were used as the matrix material, while SiC particles with volume fraction 5, 10 and 15 wt% an average size of 28 μm were used as the reinforcement material. For solid state processing aluminum alloys D16 and V95 were used as the matrix material, while SiC particles with volume fraction 20 wt % were used as the reinforcement material. The chemical composition of matrix alloys is given in <xref ref-type="table" rid="table2">Table 2</xref>. Powder metallurgy technique includes four steps: mixing of metal powder size 10 μm and SiC particles in vibratory agitator, mechanical alloying (MA) in attritor, consolidation and extrusion [<xref ref-type="bibr" rid="scirp.57689-ref5">5</xref>]. Also there were some specimens with the same composition, but produced by modified technology without mechanical alloying.</p></sec><sec id="s2_2"><title>2.2. Metallography</title><p>Analysis of filler distribution is carried out by means of classical and computer quantification metallographic image analysis methods. Samples for metallographic examination were prepared by grinding on Struers equipment. The microstructure observed by using optical microscope Olympys GX51F.</p><p>To determine phase fraction can be used different classical methods, e.g. method of М.А. Delesse, A. Rosival, A. A. Glagolev [<xref ref-type="bibr" rid="scirp.57689-ref6">6</xref>]. In the present research is used method of A. A. Glagolev: grid is drawn on the micrograph and number of dots which include phase is counted. Fraction of SiC particles can be calculated from the equation:</p><disp-formula id="scirp.57689-formula530"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57689x3.png"  xlink:type="simple"/></disp-formula><p>where C―SiC fraction, A―number of dots which include SiC particles, B―the total number of dots.</p><p>The size of micrographs was 270 &#215; 200 mm, distance between gird’s lines was 10 mm, and consequently there were 588 dots on micrograph. The example of the image analysis by mean of A. A. Glagolev method is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>Since method of A. A. Glagolev is very laborious [<xref ref-type="bibr" rid="scirp.57689-ref7">7</xref>], only four micrographs of each sample MMC were studied. If computer quantification metallographic image analysis methods were used, efficiency would be in- creased. In the present research is used A. V. Zavodov’s program for quantification analysis of material’s micro-</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Set of spicemens</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Method</th><th align="center" valign="middle"  colspan="4"   rowspan="2"  >Stir casting</th><th align="center" valign="middle"  colspan="4"  >Powder metallurgy</th></tr></thead><tr><td align="center" valign="middle"  colspan="2"  >With MA</td><td align="center" valign="middle"  colspan="2"  >Without MA</td></tr><tr><td align="center" valign="middle" >Matrix</td><td align="center" valign="middle" >AL25</td><td align="center" valign="middle" >AK12</td><td align="center" valign="middle" >V124</td><td align="center" valign="middle" >D16</td><td align="center" valign="middle" >V95</td><td align="center" valign="middle" >D16</td><td align="center" valign="middle" >V95</td><td align="center" valign="middle" >D16</td></tr><tr><td align="center" valign="middle" >SiC, vol%</td><td align="center" valign="middle" >5, 10</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >10, 15</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >20</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The chemical composition of matrix alloys; Al-remained</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >Matrix alloy</th><th align="center" valign="middle"  colspan="8"  >The chemical composition</th></tr></thead><tr><td align="center" valign="middle" >Russian</td><td align="center" valign="middle" >ISO 209:2007</td><td align="center" valign="middle" >Si</td><td align="center" valign="middle" >Fe</td><td align="center" valign="middle" >Cu</td><td align="center" valign="middle" >Mn</td><td align="center" valign="middle" >Mg</td><td align="center" valign="middle" >Zn</td><td align="center" valign="middle" >Ti</td><td align="center" valign="middle" >Others</td></tr><tr><td align="center" valign="middle" >AK12</td><td align="center" valign="middle" >4047</td><td align="center" valign="middle" >10 - 13</td><td align="center" valign="middle" >&lt; 1.5</td><td align="center" valign="middle" >&lt; 0.6</td><td align="center" valign="middle" >&lt; 0.5</td><td align="center" valign="middle" >&lt; 0.1</td><td align="center" valign="middle" >&lt; 0.3</td><td align="center" valign="middle" >&lt; 0.1</td><td align="center" valign="middle" >Zr &lt; 0.1</td></tr><tr><td align="center" valign="middle" >AL25</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >11 - 13</td><td align="center" valign="middle" >&lt; 0.8</td><td align="center" valign="middle" >&lt; 0.2</td><td align="center" valign="middle" >0.3 - 0.6</td><td align="center" valign="middle" >0.8 - 1.3</td><td align="center" valign="middle" >&lt; 0.5</td><td align="center" valign="middle" >0.05 - 0.2</td><td align="center" valign="middle" >Ni 0.8 - 1.3 Cr &lt; 0.2</td></tr><tr><td align="center" valign="middle" >V124</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >8 - 11</td><td align="center" valign="middle" >&lt; 0.3</td><td align="center" valign="middle" >3 - 4</td><td align="center" valign="middle" >0.1 - 0.3</td><td align="center" valign="middle" >0.15 - 0.35</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.1 - 0.3</td><td align="center" valign="middle" >B 0.01 - 0.1</td></tr><tr><td align="center" valign="middle" >D16</td><td align="center" valign="middle" >2024</td><td align="center" valign="middle" >&lt; 0.5</td><td align="center" valign="middle" >&lt; 0.5</td><td align="center" valign="middle" >3.8 - 4.9</td><td align="center" valign="middle" >0.3 - 0.9</td><td align="center" valign="middle" >1.2 - 1.8</td><td align="center" valign="middle" >&lt; 0.3</td><td align="center" valign="middle" >&lt; 0.1</td><td align="center" valign="middle" >Ni &lt; 0.1</td></tr><tr><td align="center" valign="middle" >V95</td><td align="center" valign="middle" >7010</td><td align="center" valign="middle" >&lt; 0.5</td><td align="center" valign="middle" >&lt; 0.5</td><td align="center" valign="middle" >1.4 - 2.0</td><td align="center" valign="middle" >0.2 - 0.8</td><td align="center" valign="middle" >1.8 - 2.8</td><td align="center" valign="middle" >5 - 7</td><td align="center" valign="middle" >&lt; 0.05</td><td align="center" valign="middle" >Cr 0.1 - 0.25</td></tr></tbody></table></table-wrap><p>structure [<xref ref-type="bibr" rid="scirp.57689-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.57689-ref7">7</xref>]. Screenshot of this program is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. Using this program ten micrographs of each sample MMC were studied.</p></sec><sec id="s2_3"><title>2.3. Microindentation Hardness Testing</title><p>Except metallography in the present research we suggest set hardness distribution in cross section of samples as an indicator of reinforcement distribution uniformity in the matrix. In the experiment the hardness of aluminium alloy composites were measured by Vickers micro hardness testing machine Emco-test Dura Scan 70 [<xref ref-type="bibr" rid="scirp.57689-ref8">8</xref>]. A series of ten measurements in increments of 0.5 mm is carried out on each sample with load 0.098 N. The distribution of points for the measurement is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>The image analysis results are given in <xref ref-type="table" rid="table3">Table 3</xref>. For each sample dispersion of fraction value were found. Dispersion denotes how stretched or squeezed a distribution is. The image analysis results are showed that the</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> A. A. Glagolev quantification analysis method</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57689x4.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Screenshot of A. V. Zavodov’s program for quantification analysis</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57689x5.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The distribution of points for the hardness measurement</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57689x6.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Hardness distribution in cross section fo the samples, HV</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57689x7.png"/></fig><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> The image analysis results</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample</th><th align="center" valign="middle"  colspan="2"  >Dispersion</th></tr></thead><tr><td align="center" valign="middle" >Method of A. A. Glagolev</td><td align="center" valign="middle" >Computer method</td></tr><tr><td align="center" valign="middle" >AL25 + 5%SiC</td><td align="center" valign="middle" >2.03</td><td align="center" valign="middle" >0.82<sup>a </sup></td></tr><tr><td align="center" valign="middle" >AK12 + 5%SiC</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >1.76</td></tr><tr><td align="center" valign="middle" >D16 + 5%SiC</td><td align="center" valign="middle" >1.06</td><td align="center" valign="middle" >2.71</td></tr><tr><td align="center" valign="middle" >AL25 + 10%SiC</td><td align="center" valign="middle" >1.82</td><td align="center" valign="middle" >0.44<sup>a </sup></td></tr><tr><td align="center" valign="middle" >V124 + 10%SiC</td><td align="center" valign="middle" >0.55</td><td align="center" valign="middle" >1.82</td></tr><tr><td align="center" valign="middle" >V124 + 15%SiC</td><td align="center" valign="middle" >2.39</td><td align="center" valign="middle" >2.40</td></tr><tr><td align="center" valign="middle" >V95 + 20%SiC</td><td align="center" valign="middle" >3.19</td><td align="center" valign="middle" >3.50</td></tr><tr><td align="center" valign="middle" >D16 + 20%SiC</td><td align="center" valign="middle" >3.46</td><td align="center" valign="middle" >3.58</td></tr><tr><td align="center" valign="middle" >V95 + 20%SiC (MA)</td><td align="center" valign="middle" >1.22</td><td align="center" valign="middle" >9.85<sup>b </sup></td></tr><tr><td align="center" valign="middle" >D16 + 20%SiC (MA)</td><td align="center" valign="middle" >4.32</td><td align="center" valign="middle" >22.12<sup>b</sup><sup> </sup></td></tr></tbody></table></table-wrap><p>distribution of SiC particles becomes more evenly with decrease of filler fraction. It can be seen that method of A. A. Gladolev demonstrates a similar results. The most uniform distribution is observed in samples with AL25 matrix. The worst uniform distribution is observed in samples produced by powder metallurgy technique with mechanical alloying step.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows hardness distribution of homogeneously and in homogeneously samples. Significant variation of the hardness range in one specimen indicates the presence of particles agglomeration in one part of the sample and lack of particles in the other. Sharp, clearly visible jumps of hardness are observed in the case of direct penetration of the indenter into the SiC particle (<xref ref-type="fig" rid="fig5">Figure 5</xref>) and may be excluded from consideration. It can be seen that hardness distribution do not completely confirmed image analysis results.</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Penetration of the indenter into the SiC particle</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57689x8.png"/></fig></sec><sec id="s4"><title>4. Conclusion</title><p>To conclusion the uniformity of distribution in all samples sufficient to provide desired level of properties. The most uniform distribution is observed in composites produced by stir-casting with low filler fraction. The worst uniform distribution is observed in composites produced by powder metallurgy technique with mechanical alloying step. Method of A. A. Glagolev demonstrates similar results to the computer method, but it is very laborious. Hardness distribution do not completely confirmed image analysis results, but it can be used for verification and validation.</p></sec><sec id="s5"><title>Cite this paper</title><p>Kurganova Yuliya,Lopatina Yuliya,Yijin Chen, (2015) Evaluation of Filler Distribution in Particulate Reinforced Composites. Journal of Materials Science and Chemical Engineering,03,108-112. doi: 10.4236/msce.2015.37014</p></sec></body><back><ref-list><title>References</title><ref id="scirp.57689-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Rabindra, B., Nihar, R.M. and Sutradhar, G. (2012) Distribution of SiC Particulates in Stir Cast Aluminum Alloy Metal Matrix Composites and Its Effect on Mechanical Properties. 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