<?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.2015.37011</article-id><article-id pub-id-type="publisher-id">MSCE-57686</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>
 
 
  Phase Relations in Si-Al-Y-O-C Systems
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kan</surname><given-names>Wu</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>Laner</surname><given-names>Wu</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>Zhenkun</surname><given-names>Huang</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>Yong</surname><given-names>Jiang</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>Yun</surname><given-names>Ma</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Material Science &amp;amp; Engineering, Beifang University of Nationalities, Yinchuan, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>lanerwu@126.com(LW)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>19</day><month>06</month><year>2015</year></pub-date><volume>03</volume><issue>07</issue><fpage>90</fpage><lpage>96</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>
 
 
   The present work investigated the phase relations in SiC-Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> (Si-Al-Y-O-C) system. As a continuation of our previous works, the purpose of this study is to understand the high temperature reaction behaviors of SiO<sub>2</sub> in the system and its effect on the phase relations of the valuable system of SiC-Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub>. The phase compositions of six solid-state reacted samples with different components of Y<sub>2</sub>O<sub>3</sub>:Al<sub>2</sub>O<sub>3</sub>:SiC:SiO<sub>2</sub> were analyzed by XRD. The phase relations of the systems were determined. The subsolidus phase diagrams of ternary Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system and the tentative phase diagram of an extended quaternary Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system were presented latter involving several coexisting regions of four phases. The high temperature reaction behavior of SiO<sub>2</sub> in the system and its effect on the phase relations of system were discussed. 
 
</p></abstract><kwd-group><kwd>Phase Relation</kwd><kwd> Phase Diagram</kwd><kwd> SiC</kwd><kwd> SiO2</kwd><kwd> YAG</kwd><kwd> YAM</kwd><kwd> YAP</kwd><kwd> Al&lt;sub&gt;6&lt;/sub&gt;Si&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;13&lt;/sub&gt;</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>SiC ceramic is one of advanced structural ceramics with excellent mechanical properties, mainly in high temperature properties, high hardness, wear resistance, as well as good chemical resistance. It is widely applied in the industry. But its low strength and poor toughness restrict its more extensively applications [<xref ref-type="bibr" rid="scirp.57686-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.57686-ref2">2</xref>]. Y<sub>2</sub>O<sub>3</sub>- Al<sub>2</sub>O<sub>3</sub> as sintering additives of SiC ceramic have been used for many years [<xref ref-type="bibr" rid="scirp.57686-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.57686-ref4">4</xref>]. The phase relationship of SiC-Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub> system has also been studied by calculation [<xref ref-type="bibr" rid="scirp.57686-ref5">5</xref>] and experiment [<xref ref-type="bibr" rid="scirp.57686-ref6">6</xref>]. However a few of SiO<sub>2</sub> on SiC surface caused by oxidation of SiC has the non-ignorable effect on the sintering of SiC-Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub> system at high temperature. Thus the effect of SiO<sub>2</sub> on phase relations of SiC-Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub> ternary systems is being concerned. For made it clear this effect, understanding the reaction of SiO<sub>2</sub> with other members in the system at high temperature is required. The phase relations of SiC-Si<sub>3</sub>N<sub>4</sub>-R<sub>2</sub>O<sub>3</sub> (Si-C-N-O-R; R = La, Gd, Y) [<xref ref-type="bibr" rid="scirp.57686-ref7">7</xref>] and SiC- AlN-R<sub>2</sub>O<sub>3</sub> (R = Nd, Gd, Yb, Y [<xref ref-type="bibr" rid="scirp.57686-ref8">8</xref>] systems have been reported by the authors. Within systems the effect of SiO<sub>2</sub> impurity on the formation of serial rare-earth nitrogen-containing silicates and silicon-aluminates had been revealed. As the continuation work of them, the present work investigates the high temperature reaction behavior of SiO<sub>2</sub> and the phase relations in the Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system. In this quaternary system the phase diagram of Y<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> subsystem has been identified to form two Y<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> and Y<sub>2</sub>SiO<sub>5</sub> compounds [<xref ref-type="bibr" rid="scirp.57686-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.57686-ref10">10</xref>]. The phase relations of binary Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub> subsystem have also been reported, in which three compounds Y<sub>4</sub>Al<sub>2</sub>O<sub>9</sub> (YAM), YAlO<sub>3</sub> (YAP) and Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> (YAG) were confirmed [<xref ref-type="bibr" rid="scirp.57686-ref11">11</xref>]-[<xref ref-type="bibr" rid="scirp.57686-ref13">13</xref>]. The phase diagram of Al<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> subsystem has also been reported to form Al<sub>6</sub>Si<sub>2</sub>O<sub>13</sub> (Mullite), and is used in ceramic manufacture [<xref ref-type="bibr" rid="scirp.57686-ref14">14</xref>]. SiC is difficult to react with others oxides. SiC-SiO<sub>2</sub> has a simple binary phase diagram [<xref ref-type="bibr" rid="scirp.57686-ref15">15</xref>], but the SiC-Al<sub>2</sub>O<sub>3</sub> phase relation remains unclear [<xref ref-type="bibr" rid="scirp.57686-ref16">16</xref>]. The phase relations of binary Y<sub>2</sub>O<sub>3</sub>-SiC subsystem has been identified that no any compound was formed [<xref ref-type="bibr" rid="scirp.57686-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.57686-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.57686-ref17">17</xref>]. Knowing the phase relations of Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> quaternary system will provide help to design and manufacture of SiC ceramic. It will also provide strong evidence to know the factors of controlling the equilibrium of Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub>system.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Materials</title><p>The starting powders used for the experiments were β-SiC with 0.5% O<sub>2</sub> (mass ratio, the same below) (BF 12-A, H.C. Starck), Al<sub>2</sub>O<sub>3</sub> purity ≥ 99.99%, (Xuan Cheng Jing Rui New Material Co., Ltd., China), Y<sub>2</sub>O<sub>3</sub> &gt; 99.99% purity (Baotou Research Institute of Rare Earth), SiO<sub>2</sub> (Tianjing Fuchen Chemical Reagents factory, China) respectively. Y<sub>2</sub>O<sub>3</sub> and Al<sub>2</sub>O<sub>3</sub> powders were calcined at 1100˚C in air for 2 hr to remove their hydrates before being used.</p></sec><sec id="s2_2"><title>2.2. Experimental Procedure</title><p>Selected compositions were marked as YASS in order of Y<sub>2</sub>O<sub>3</sub>/Al<sub>2</sub>O<sub>3</sub>/SiC/SiO<sub>2</sub>. For example, YASS 1422 represents as the sample with composition of Y<sub>2</sub>O<sub>3</sub>/Al<sub>2</sub>O<sub>3</sub>/SiC/SiO<sub>2</sub> = 1/4/2/2 (molar ratio). The details are shown in <xref ref-type="table" rid="table1">Table 1</xref>. The 20 g powder mixture was mixed and ground in an agate mortar for 1.5 - 2 hrs by adding alcohol (analytical reagent, 99.9% purity). After dried up, the prepared powders were cold isostatic pressed under 250 MPa. The conditions used for solid-state reaction were: in Ar atmosphere, at temperature of 1450˚C - 1600˚C, holding 2 hrs, and then cooling down to room temperature freely. In order to achieve the reaction equilibrium, the holding time prolonged. None of noticeable phase composition change is observed could be the judgment of whether the system equilibrium is achieved. The phase compositions of the sintered samples were analyzed by X-ray diffraction (XRD) using equipment SHIMADZU XRD-6000 with CuKα radiation in 0.2˚ scan step, 2˚∙min<sup>−1</sup>. The experimental and the analysis method of phase compositions for samples are similar with our previous papers [<xref ref-type="bibr" rid="scirp.57686-ref6">6</xref>]-[<xref ref-type="bibr" rid="scirp.57686-ref8">8</xref>].</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>XRD analysis results of sintered samples are shown in <xref ref-type="table" rid="table1">Table 1</xref>. The effect of SiO<sub>2</sub> impurity on the phase relations in SiC ceramic system is paid close attention. However in our previous work of the phase relations of SiC- Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub> system [<xref ref-type="bibr" rid="scirp.57686-ref6">6</xref>], seemingly no such effect was found (see <xref ref-type="fig" rid="fig1">Figure 1</xref>). In order to identify SiO<sub>2</sub> caused by oxidation of SiC at high temperature, the SiC powder was heated to 1450˚C, hold 2 hours in Ar. <xref ref-type="fig" rid="fig2">Figure 2</xref> is XRD pattern of β-SiC starting powder after heating at 1450˚C, showing no trace of SiO<sub>2</sub> could be found. The experimental results also indicated that SiO<sub>2</sub> impurity on the surface of SiC did not participated in the reaction with other oxides in system [<xref ref-type="bibr" rid="scirp.57686-ref6">6</xref>]. There might be too little amount of SiO<sub>2</sub> to detect or the SiO<sub>2</sub> and other components might form a few of liquid at the grain-boundaries, because the eutectic temperature of Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub></p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> XRD analyses of sintered samples of Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample</th><th align="center" valign="middle"  colspan="4"  >Compositions (mol.)</th><th align="center" valign="middle"  rowspan="2"  >Temp (˚C)</th><th align="center" valign="middle"  rowspan="2"  >Phases identified in sintered bodies&#169;</th></tr></thead><tr><td align="center" valign="middle" >Y<sub>2</sub>O<sub>3</sub></td><td align="center" valign="middle" >Al<sub>2</sub>O<sub>3</sub></td><td align="center" valign="middle" >SiC</td><td align="center" valign="middle" >SiO<sub>2</sub></td></tr><tr><td align="center" valign="middle" >YASS0133</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1550</td><td align="center" valign="middle" >SiO<sub>2(VS)</sub>, SiC<sub>(S)</sub>, Al<sub>6</sub>Si<sub>2</sub>O<sub>13(M)</sub></td></tr><tr><td align="center" valign="middle" >YASS0421</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1550</td><td align="center" valign="middle" >Al<sub>2</sub>O<sub>3(S)</sub>, SiC<sub>(S)</sub>, Al<sub>6</sub>Si<sub>2</sub>O<sub>13(M)</sub></td></tr><tr><td align="center" valign="middle" >YASS1422</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1550</td><td align="center" valign="middle" >YAG<sub>(S)</sub>, Al<sub>2</sub>O<sub>3(M)</sub>, Y<sub>2</sub>Si<sub>2</sub>O<sub>7(M)</sub>, SiC<sub>(W)</sub></td></tr><tr><td align="center" valign="middle" >YASS3211</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1550</td><td align="center" valign="middle" >YAP<sub>(VS)</sub>, YAM<sub>(S)</sub>, SiC<sub>(W)</sub>, Y<sub>2</sub>SiO<sub>5(W)</sub></td></tr><tr><td align="center" valign="middle" >YASS1414</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1500</td><td align="center" valign="middle" >Y<sub>2</sub>Si<sub>2</sub>O<sub>7(VS)</sub>, SiC<sub>(M)</sub>, Al<sub>6</sub>Si<sub>2</sub>O<sub>13(M)</sub>, Al<sub>2</sub>O<sub>3(W)</sub></td></tr><tr><td align="center" valign="middle" >YASS1315</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1500</td><td align="center" valign="middle" >Y<sub>2</sub>Si<sub>2</sub>O<sub>7(VS)</sub>，SiC<sub>(M)</sub>, Al<sub>6</sub>Si<sub>2</sub>O<sub>13(M)</sub>, SiO<sub>2(M)</sub></td></tr></tbody></table></table-wrap><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title>Phase relations of SiC-Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub> system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57686x4.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> XRD pattern of starting powder β-SiC at 1450<sup>˚</sup>C/2 hrs in Ar</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57686x5.png"/></fig><p>system is very low (1370˚C) [<xref ref-type="bibr" rid="scirp.57686-ref18">18</xref>]. Even so, understanding the high temperature react behavior of SiO<sub>2</sub> and its effect on the phase relations in the present system, as well as, further on the manufacture of SiC ceramic is required. For this reason, SiO<sub>2</sub> was chosen as a member of the quaternary Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system. Samples were sintered at 1500˚C - 1600˚C/2 hrs in Ar. <xref ref-type="fig" rid="fig3">Figure 3</xref> is XRD patterns of YASS0133 and YASS0421 sintered samples. From <xref ref-type="fig" rid="fig3">Figure 3</xref>, it could be found that both samples have Al<sub>6</sub>Si<sub>2</sub>O<sub>13</sub> (mullite) and SiC formed. The different is YASS0133 contains SiO<sub>2,</sub> butYASS0421 contains Al<sub>2</sub>O<sub>3</sub>. It can be confirmed that SiC can form a tie- line with mullite. Three phases could be identified in YASS0133 as SiC, SiO<sub>2</sub> and mullite. While in YASS0421 three phase coexistence of SiC, Al<sub>2</sub>O<sub>3</sub> andAl<sub>6</sub>Si<sub>2</sub>O<sub>13</sub> could be found. Therefore the subsolidus phase diagram of Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system can be presented as <xref ref-type="fig" rid="fig4">Figure 4</xref>. <xref ref-type="fig" rid="fig5">Figure 5</xref> is XRD patterns of specimens of YASS 1422 and YASS 3211. In <xref ref-type="fig" rid="fig5">Figure 5</xref> it was found that the two samples both have SiC and yttrium silicates phases. The different is YASS1422 have Al<sub>2</sub>O<sub>3</sub> and YAG (Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>), while YASS3211 have YAM (Y<sub>4</sub>Al<sub>2</sub>O<sub>9</sub>) and YAP (YAlO<sub>3</sub>). It indicates two points, one is mulite can not has a tie-line with SiC. The other is SiO<sub>2</sub> was almost used up to form yttrium silicates. Four phases could be identified as YAG, Al<sub>2</sub>O<sub>3</sub>, SiC and Y<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> in YASS1422. And four phases of YAM, YAP, SiC and Y<sub>2</sub>SiO<sub>5</sub> were found in YASS3211 specimen. <xref ref-type="fig" rid="fig6">Figure 6</xref> is XRD patterns</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> XRD patterns ofYASS0421 (a) and YASS0133 (b) specimens</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57686x6.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Subsolidus phase diagram of Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57686x7.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> XRD patterns of YASS1422 and YASS3211 specimens</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57686x8.png"/></fig><p>of YASS1315 and YASS1414 samples. Phases identified by XRD analysis in YASS1315 are SiC, Al<sub>6</sub>Si<sub>2</sub>O<sub>13</sub>, SiO<sub>2</sub> and Y<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>, for YASS1414 they are SiC, Al<sub>2</sub>O<sub>3</sub>, Al<sub>6</sub>Si<sub>2</sub>O<sub>13</sub> and Y<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>. In <xref ref-type="fig" rid="fig6">Figure 6</xref> we found that the two samples both have Y<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>, Al<sub>6</sub>Si<sub>2</sub>O<sub>13</sub> and SiC. The different is, YASS1315 has SiO<sub>2</sub>, YASS1414 has Al<sub>2</sub>O<sub>3</sub>. It is indicated that SiO<sub>2</sub> plays the role of forming mullite and yttrium silicates and leading to establish the phase equilibria with yttrium aluminates and SiC. The formation of above several four phase coexistence involving both yttrium silicates and mullite extends the ternary system SiC-Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub> into the quaternary system included SiO<sub>2</sub>. Combing the phase diagrams of Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub>-SiC system with Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> system [<xref ref-type="bibr" rid="scirp.57686-ref18">18</xref>] the tentative phase diagram of quaternary SiC-Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> (Si-Al-Y-O-C) system can be presented as <xref ref-type="fig" rid="fig7">Figure 7</xref> which shows that the triangle equilibrium relations of SiC with three yttrium aluminates extend to the tetrahedral equilibrium relations with three yttrium silicates Y<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>, Y<sub>2</sub>SiO<sub>5</sub> and mullite, respectively. Besides, it should be indicated that the tie-line YAP-Y<sub>2</sub>SiO<sub>5</sub> in present work is better stead of YAG-YAMss tie-line in the phase diagram of Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> system [<xref ref-type="bibr" rid="scirp.57686-ref18">18</xref>]. The possible YAMss solid-solution is not measured in present work.</p></sec><sec id="s4"><title>4. Conclusion</title><p>The subsolidus phase diagram of the Al<sub>2</sub>O<sub>3</sub>-SiC-SiO<sub>2</sub> system was given. The phase relations in the SiC-Al<sub>2</sub>O<sub>3</sub>-</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> XRD patterns of YASS1414 and YASS1315 specimens</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57686x9.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Tentative phase diagram of quaternary system SiC- Al<sub>2</sub>O<sub>3</sub>-Y<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> (Si-Al-Y-O-C)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57686x10.png"/></fig><p>Y<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> system were established. The tentative phase diagram of this quaternary system was presented in which SiO<sub>2</sub> plays the role of forming mullite and yttrium silicates and leading to establish the phase equilibria of yttrium silicates with yttrium aluminates and SiC.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The present work was financially supported by National Natural Science Foundation of China, NSFC51362001.</p></sec><sec id="s6"><title>Cite this paper</title><p>Kan Wu,Laner Wu,Zhenkun Huang,Yong Jiang,Yun Ma, (2015) Phase Relations in Si-Al-Y-O-C Systems. Journal of Materials Science and Chemical Engineering,03,90-96. doi: 10.4236/msce.2015.37011</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.57686-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Chia, K.Y., Boecker, W.D.G. and Storm, R.S. (1994) Silicon Carbide Bodies Having High Toughness and Fracture Resistance and Method of Making. 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