<?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">MSA</journal-id><journal-title-group><journal-title>Materials Sciences and Applications</journal-title></journal-title-group><issn pub-type="epub">2153-117X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msa.2023.148027</article-id><article-id pub-id-type="publisher-id">MSA-127074</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>
 
 
  Synthesis and Characterization of Aluminum Alloys with Metal Oxides (CuO&lt;sub&gt;2&lt;/sub&gt;) Additions as Reinforcement
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Reyna</surname><given-names>Anahí Falcón-Castrejón</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>Jose</surname><given-names>Luis Román-Zubillaga</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>Rene</surname><given-names>Guardián-Tapia</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>Lazaro</surname><given-names>Falcón-Franco</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Isaí</surname><given-names>Rosales-Cadena</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Center for Research in Engineering and Applied Sciences, Autonomous University of State of Morelos, Cuernavaca, Mexico</addr-line></aff><aff id="aff2"><addr-line>Faculty of Metallurgy, Autonomous University of Coahuila, Coahuila, Mexico</addr-line></aff><pub-date pub-type="epub"><day>09</day><month>08</month><year>2023</year></pub-date><volume>14</volume><issue>08</issue><fpage>416</fpage><lpage>425</lpage><history><date date-type="received"><day>15,</day>	<month>July</month>	<year>2023</year></date><date date-type="rev-recd"><day>15,</day>	<month>August</month>	<year>2023</year>	</date><date date-type="accepted"><day>18,</day>	<month>August</month>	<year>2023</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 this investigation, the addition of several amounts of metal oxide particles (CuO
  <sub>2</sub>) in Al matrix is carried out due to the need to improve the mechanical properties such as the ductility of aluminum for applications in the electrical sector. Samples were obtained by means of a stirring casting process. From the results of the microstructural characterization, it was observed that the metallic oxides induce the modification of the dendritic structure and grain refinement. X-ray diffraction characterization mainly shows the formation of Al
  <sub>2</sub>CuO
  <sub>4</sub>, Al
  <sub>2</sub>O
  <sub>3</sub> and CuO compounds. Mechanical properties showed that the different thermal treatments resulted in an improved hardness, from 30 kg/mm
  <sup>2</sup> for the un-reinforced sample to 90 kg/mm
  <sup>2</sup> for reinforced samples. The addition of metallic oxides in the Al matrix produces an improved electrical conductivity specifically in sample with 0.50 g of CuO
  <sub>2</sub> additions.
 
</p></abstract><kwd-group><kwd>Electrical Properties</kwd><kwd> Oxides Additions</kwd><kwd> Soft Alloys</kwd><kwd> Mechanical Properties</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In particle-reinforced materials, two groups of materials are included: The first is based on transition metal matrices and the second on soft or light alloys [<xref ref-type="bibr" rid="scirp.127074-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref2">2</xref>] . The purpose for which the composite materials were developed is to obtain enhanced properties such as: density, good tensile strength, high modulus of elasticity, low coefficient of thermal expansion, complicated to achieve with a monolithic material [<xref ref-type="bibr" rid="scirp.127074-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.127074-ref6">6</xref>] . The final result will depend on the properties of the matrix and the reinforcement, on the properties of the lightweight materials. An excellent combination can result through the combination of low melting point, good mechanical properties and low density (2.7 g/cm<sup>3</sup>) as aluminum-based alloys, these characteristics are currently needed mainly in structural applications such as aeronautics, military and transport. The addition of hard particles in a soft metallic matrix, results in a compound with combined properties, this will improve the mechanical properties of the compounds, for their different applications [<xref ref-type="bibr" rid="scirp.127074-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref7">7</xref>] . In the last decades the reinforcement of the aluminum matrix has been studied [<xref ref-type="bibr" rid="scirp.127074-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref10">10</xref>] , adding reinforcements ranging [<xref ref-type="bibr" rid="scirp.127074-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref13">13</xref>] from Nb<sub>2</sub>O<sub>5</sub>, CuO, ZnO, SnO, Cr<sub>2</sub>O<sub>3</sub>, TiO<sub>2</sub> or MgO [<xref ref-type="bibr" rid="scirp.127074-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref17">17</xref>] to unconventional reinforcements, such as quasicrystals [<xref ref-type="bibr" rid="scirp.127074-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref19">19</xref>] . All these reports show the improvement of mechanical properties. The novelty of this work is to generate information related to the addition of reinforcing oxides particles, namely CuO<sub>2</sub> into the aluminum matrix, analyzing their effect on the microstructure, mechanical and electrical properties of the resultant alloys, due to the very little information existent related to this system, due to limited information existent in the literature about this alloy and therefore the need to improve the mechanical properties such as the ductility of aluminum for applications in the electrical sector.</p></sec><sec id="s2"><title>2. Experimental Procedure</title><p>Aluminum (99.99) was used as matrix material and different concentrations of CuO<sub>2</sub> particles (0.15, 0.25 and 0.50 g) were added as reinforcing components into the liquid alloy followed by stirring with a stainless steel flat bar at 250 rpm. The resultant alloy was cast into a copper mold with a rectangular shape. To study the microstructure, 1 &#215; 1 &#215; 1 cm samples were cut, grinding with sand paper up to 600 grade and polishing with alumina paste 0.3 &#181;m and then using the Dix-Keller etching reagent to reveal its microstructure. Surfaces images were obtained using an Olympus optical microscope in dark field mode. XRD analyzes were performed in a BRUKER diffractometer to obtain identification of the phases present. The hardness Vickers tests were carried out using a Leco 300 MT equipment, average hardness values were obtained using a load of 0.1 kgf with a time of 15 s according to ASTM: E384 standard. Different heat treatments were carried out in the AR-340 FELIZA furnace, as shown in <xref ref-type="table" rid="table1">Table 1</xref>. For the study of electrical properties a RIGOL 3058E Micro-ohmmeter was employed.</p></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Microstructural Characterization</title><p>It is observed in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the microstructures for samples with Aluminum plus different CuO<sub>2</sub> additions, where in <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) it is observed a dendritic behavior with 0.15 g additions of CuO<sub>2</sub>, being the dendrite size of approximately 45 &#181;m. For the case of sample with 0.25 g of additions of CuO<sub>2</sub> in <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) it can be observed a dendritic behavior, where dendrites present an enlargement in its structure being the dendrite size of 90 &#181;m average. On the other hand for sample with 0.50 g it can be observed its microstructure in <xref ref-type="fig" rid="fig1">Figure 1</xref>(c) that exist an evolution of the dendritic structure to equiaxed grains. Hence, the effect of the oxide additions it is clearly observed for the three different compositions where copper oxides promote de grain growth [<xref ref-type="bibr" rid="scirp.127074-ref1">1</xref>] . Microstructural variations are explained considering that oxides additions may induce the modification of the dendritic structure and grain growing under the mechanism that particles during the solidification process acts as nucleation points on which the aluminum grains solidify [<xref ref-type="bibr" rid="scirp.127074-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref4">4</xref>] .</p></sec><sec id="s3_2"><title>3.2. X-Ray Diffraction Analyses</title><p>The X-Ray Diffraction patterns are presented in <xref ref-type="fig" rid="fig2">Figure 2</xref>, in it can be observed different peaks corresponding to the compounds formed during the melting process.</p><p>The proposed chemical reactions developed during the melting-casting-solidification process are as follow:</p><p>4Al + 3CuO<sub>2</sub> → 3Cu + 2Al<sub>2</sub>O<sub>3</sub> (1)</p><p>Al + 2CuO<sub>2</sub> → 2CuO + AlO<sub>2</sub> (2)</p><p>2Al + 2CuO<sub>2</sub> → Cu + Al<sub>2</sub>CuO<sub>4</sub> (3)</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Alloys designation and description of heat treatments</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Nomenclature</th><th align="center" valign="middle" >Description</th><th align="center" valign="middle" >Parameters</th></tr></thead><tr><td align="center" valign="middle" >AM</td><td align="center" valign="middle" >Aluminum Matrix</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >BA</td><td align="center" valign="middle" >As-cast alloys</td><td align="center" valign="middle" >Addition 0.15 0.25 0.50 g</td></tr><tr><td align="center" valign="middle" >AA</td><td align="center" valign="middle" >Annealed in Air</td><td align="center" valign="middle" >300˚ - 600˚C 12 h</td></tr><tr><td align="center" valign="middle" >AAA</td><td align="center" valign="middle" >Annealed in an argon atmosphere</td><td align="center" valign="middle" >600˚C 12 h</td></tr><tr><td align="center" valign="middle" >OQ</td><td align="center" valign="middle" >Oil quenched alloys</td><td align="center" valign="middle" >500˚C 1 h</td></tr><tr><td align="center" valign="middle" >BQ</td><td align="center" valign="middle" >Brine quenched alloys</td><td align="center" valign="middle" >500˚C 1 h</td></tr><tr><td align="center" valign="middle" >OQT</td><td align="center" valign="middle" >Oil-quenched + tempered</td><td align="center" valign="middle" >260˚C 1h</td></tr><tr><td align="center" valign="middle" >BQT</td><td align="center" valign="middle" >Brine-quenched + tempered</td><td align="center" valign="middle" >260˚C 1h</td></tr></tbody></table></table-wrap><p>It can be observed in the three possible reactions that Al and copper oxide produces the aluminum oxide plus copper, due to the dissociation of the oxygen present in the CuO<sub>2</sub>. The proposed reaction mechanism of formation is the interfacial reaction of the oxygen of the CuO<sub>2</sub> with the liquid aluminum [<xref ref-type="bibr" rid="scirp.127074-ref6">6</xref>] . It is noticeable that the aluminum oxide (Al<sub>2</sub>CuO<sub>4</sub>) in Equation (3) is product of an overheating in the system and the agitation produced by the stirring process that permit a constant external detachment of the superficial layer of the CuO<sub>2</sub> particles.</p><p>In <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) it is observed the diffraction peaks for samples with different CuO<sub>2</sub> particles additions without heat treatment, where is observed that that during the melting process are generated mainly two types of oxides; CuO and AlO<sub>2</sub>. On the other hand, when alloys with different CuO<sub>2</sub> particles are exposed to annealing treatment (see <xref ref-type="fig" rid="fig2">Figure 2</xref>(b)), predominantly Al<sub>2</sub>CuO<sub>4</sub> is generated. Finally, as can be seen in <xref ref-type="fig" rid="fig2">Figure 2</xref>(c) the change of atmosphere of heat treatments allows the creation of new metal oxides in very small quantities such as AlO<sub>3</sub> and Al<sub>2</sub>O<sub>3</sub>, this effect is attributed to an absence of oxygen in the furnace chamber [<xref ref-type="bibr" rid="scirp.127074-ref3">3</xref>] .</p><p>The particles size obtained from the X-ray diffraction spectrum was determined by measuring the average percentage of the width at half height (FWHM) of the characteristic peaks, for each of the alloys reinforced with different CuO<sub>2</sub> additions and with different heat treatments. <xref ref-type="fig" rid="fig3">Figure 3</xref> shows the percentage of the width of the peaks corresponding to each of the alloys; for as-cast alloys (BA) it was observed that the higher the amount of oxide additions, the higher the amounts of resultant aluminum and copper oxides.</p><p>After annealing for 12 h, the oxides maintain the same behavior and in the sample AA 0.50 a lower amount of AlO<sub>2</sub> is generated, but a peak corresponding to copper and Al<sub>2</sub>CuO<sub>4</sub> is shown with a width of 2.10% which is attributed to be affected by the amount of CuO<sub>2</sub> existing in the alloy [<xref ref-type="bibr" rid="scirp.127074-ref7">7</xref>] . Annealing in an argon atmosphere reduces the creation of different oxides in all alloys; Compared to BA, CuO<sub>2</sub> decreased for the alloy AAA 0.15 by 40.33%, AAA 0.25 by 58.94% and AAA 0.50 by 54.28% and for AlO<sub>2</sub> 90.08%, 75.32% and 79.41% respectively. The</p><p>previous data, allowed us to obtain as a result the average crystallite sizes calculated for each alloy, supposing that the fluctuation in hardness is inversely proportional to the average crystal size.</p></sec><sec id="s3_3"><title>3.3. Mechanical Characterization</title><sec id="s3_3_1"><title>3.3.1. Vickers Hardness</title><p>For soft matrix composite materials particles reinforced, the selection of the region in the sample where the hardness is evaluated is critical as the reinforcement phase should be considered. In <xref ref-type="fig" rid="fig4">Figure 4</xref> it is observed the plot of the hardness results AM equal to 30 kg/mm<sup>2</sup> while BM25 alloy possesses a hardness value close to 80 kg/mm<sup>2</sup>.</p><p>The Bouvard [<xref ref-type="bibr" rid="scirp.127074-ref20">20</xref>] postulation stablish that small amounts of fine reinforcing particles cover the surface of coarse metal powders; this may be the reason for the increased hardness sample; as well as the combined effects of the distribution of oxide particles that act as obstacles in the dislocations movement, in addition the localized deformation of the materials take into account the presence of intrinsic porosity in the materials [<xref ref-type="bibr" rid="scirp.127074-ref20">20</xref>] . Therefore, the elevated hardness it is attributed to a reduced grain size [<xref ref-type="bibr" rid="scirp.127074-ref14">14</xref>] , as shown in the plot. However, in samples BA50 the hardness slightly decreases, this is attributed to the dispersion of particles, creating a solid solution with uniform granular structure and average grain size of 25 &#181;m, allowing an increment in plastic deformation.</p></sec><sec id="s3_3_2"><title>3.3.2. Vickers Hardness Variation in Annealing Condition</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the plot of the hardness of samples at the three different compositions of CuO<sub>2</sub> additions against of annealing at four different temperatures, in it can be observed that the higher the temperature, the greater the plastic deformation for all the alloys, in other words a decrement in hardness is observed, reaching a state of equilibrium from 500˚C. Samples AA 0.15 and AA 0.25 obtain their maximum hardness at 300˚C above the initial hardness of the AM, unlike the sample AA 0.50 where the hardness value is lower at this temperature.</p><p>For annealing in an argon atmosphere, a rectangular of steel chamber was manufactured and designed, which was adapted to the furnace where the Argon was recirculated during the 12 h of annealing at 600˚C. In <xref ref-type="fig" rid="fig6">Figure 6</xref> is presented</p><p>the hardness variations of the AA samples under annealing with different atmosphere at a temperature of 600˚C. Annealed alloys maintain the same behavior as samples annealed in an argon atmosphere, but their hardness is lower, this is attributed to the amount of the new oxides generated during heat treatment.</p></sec></sec><sec id="s3_4"><title>3.4. Electrical Characterization</title><p>It is well known that electrical resistance of a material is proportional to the electrical resistivity and is inversely proportional to the electrical conductivity [<xref ref-type="bibr" rid="scirp.127074-ref21">21</xref>] . In plot of <xref ref-type="fig" rid="fig7">Figure 7</xref> it can be observed a horizontal line that denotes value of the electrical conductivity of aluminum, this resulted 3.5 S/m at 20˚C, taking this value as a reference, it can be observed that copper dioxide addition in combination with the different heat treatments tends to increase the electrical conductivity. As it is well known, copper oxides are included in the family of superconductors [<xref ref-type="bibr" rid="scirp.127074-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref23">23</xref>] and are called high temperature superconductors since they exhibit superconductivity at approximately 195˚C. For the OQ samples with 0.15g CuO<sub>2</sub> addition oil tempered it is observed that it keep the electrical conductivity close to the value of unalloyed aluminum. The decrease in electrical conductivity for the rest of the samples with this addition has been attributed as a result of the gradual increase in the number and size of particles of CuO<sub>2</sub>, which leads to a decrease in the conductivity of the composite material due to the electrons dispersion; this effect has been correlated with impurities in aluminum matrix [<xref ref-type="bibr" rid="scirp.127074-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref22">22</xref>] .</p><p>For the samples with the addition of 0.25 and 0.50, it is observed that the AA, AAA and OQT samples the conductivity increases, this is attributed to the low index of precipitates in the surface area that which produces a partially freeway effect on the matrix [<xref ref-type="bibr" rid="scirp.127074-ref22">22</xref>] , for consequence this phenomena generates an increment in electrical conductivity values.</p><p>On the other hand, the non-linear correlation of the electrical conductivity with the hardness perhaps is the result of the differences in response of the hardness with the thermal treatments, which has been affected via generation of copper and aluminum precipitates with different size and randomly dispersed, created during the different aging stages [<xref ref-type="bibr" rid="scirp.127074-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.127074-ref23">23</xref>] .</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>Aluminum alloys with CuO<sub>2</sub> particulates were obtained successfully by melt stirring process. A dendritic structure from fine to coarse was obtained depending of the amount of copper oxides added. Particularly, addition of 15 g of CuO<sub>2</sub> increases the hardness of the aluminum accompanied with a heat treatment of 300˚C for 12 h reaching values of 90 kg/mm<sup>2</sup> approximately. Heat treatment with Ar atmosphere decreases the amounts of metal oxides formed. The quenching and tempering treatments affect positively the alloys hardness. The addition of metal oxide particles increases the electrical conductivity specifically in samples with 0.50 g of CuO<sub>2</sub> additions reaching average values on the order of 4.3 &#215; 10<sup>7</sup> S/m. Obtained results indicate the possibility to use the alloys for fabrication of electrical conduction wires.</p></sec><sec id="s5"><title>Acknowledgements</title><p>Authors are thankful with A. Aguilar and J. Macedonio for important technical support in mechanical characterization. This project was supported by CONAHCYT and PRODEP under grant UAEM/ PTC-00074</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Falc&#243;n-Castrej&#243;n, R.A., Rom&#225;n-Zubillaga, J.L., Guardi&#225;n-Tapia, R., Falc&#243;n-Franco, L. and Rosales-Cadena, I. (2023) Synthesis and Characterization of Aluminum Alloys with Metal Oxides (CuO<sub>2</sub>) Additions as Reinforcement. Materials Sciences and Applications, 14, 416-425. https://doi.org/10.4236/msa.2023.148027</p></sec></body><back><ref-list><title>References</title><ref id="scirp.127074-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Chen, G., Sun, G. and Zhu, Z. (1998) On the Chemical Reactions to Process Particle Reinforced Al-Cu Alloy Matrix Composites. 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