<?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">OJCM</journal-id><journal-title-group><journal-title>Open Journal of Composite Materials</journal-title></journal-title-group><issn pub-type="epub">2164-5612</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojcm.2012.21001</article-id><article-id pub-id-type="publisher-id">OJCM-17039</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>
 
 
  Influence of Nanocrystalline ZrO&lt;sub&gt;2&lt;/sub&gt; Additives on the Fracture Toughness and Hardness of Spark Plasma Activated Sintered WC/ZrO&lt;sub&gt;2&lt;/sub&gt; Nanocomposites Obtained by Mechanical Mixing Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>Sherif El-Eskandarany</given-names></name></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hesham</surname><given-names>M. A. Soliman</given-names></name><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>M.</surname><given-names>Omoric</given-names></name></contrib></contrib-group><author-notes><corresp id="cor1">* E-mail:<email>h.soliman@mucsat.sci.eg(HMAS)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>17</day><month>01</month><year>2012</year></pub-date><volume>02</volume><issue>01</issue><fpage>1</fpage><lpage>7</lpage><history><date date-type="received"><day>October</day>	<month>11th,</month>	<year>2011</year></date><date date-type="rev-recd"><day>November</day>	<month>18th,</month>	<year>2011</year>	</date><date date-type="accepted"><day>December</day>	<month>16,</month>	<year>2011.</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 study reports the formation of ultrafine hard particles of nanocomposite WC with different additions of ZrO
  <sub>2</sub> powders (0.5 - 20 vol.%). The initial mixed powders of WC with the desired ZrO
  <sub>2</sub> concentrations were mechanically mixed for 360 ks (end-product) under argon gas atmosphere at room temperature, using high energy ball mill. The end-product consists of average grain size of about 17 nm in diameter. The obtained nanocomposite powders were consolidated into fully dense compact, using spark plasma sintering (SPS) technique in vacuum. The experimental results revealed that the consolidation step, which was conducted at 1673 K with uniaxial pressure ranging from 19.6 to 38.2 MPa for short time (0.18 ks), does not lead to dramatic grain growth in the powders so that the consolidated nanocomposite bulk objects maintain their nanocrystalline behavior, being fine grains with an average size of 63 nm in diameter. The relative densities of consolidated nanocomposite WC/ZrO
  <sub>2</sub> materials increase from 99.1% for WC-0.5% ZrO
  <sub>2</sub> to 99.93% for WC-20% ZrO
  <sub>2</sub>. The indentation fracture toughness of the composites can be tailored between 7.31 and 19.46 MPa/m
  <sup>1/2</sup> by controlling the volume fraction of ZrO
  <sub>2</sub> matrix from 0.5% to 20%. The results show that the Poisson’s ratio increased monotonically with increasing the ZrO
  <sub>2</sub> concentrations to get a maximum value of 0.268 for WC-20% ZrO
  <sub>2</sub>. In the whole range of ZrO
  <sub>2</sub> concentrations (0.5 - 20 vol.%), high hardness values (20.73 to 22.83 GPa) were achieved. The Young’s modulus tends to decrease with increasing the volume fraction of the ZrO
  <sub>2</sub> matrix to reach a minimum value of 583.2 GPa for WC-20% ZrO
  <sub>2</sub>. These hard and tough WC/ZrO
  <sub>2</sub> nanocomposites are proposed to be employed as higher abrasive-wear resistant materials.
 
</p></abstract><kwd-group><kwd>Nanocomposite; Tungsten Carbide; Zirconia; Spark Plasma Sintering; Powder Metallurgy; Mechanical Alloying; Microstructure; SEM</kwd><kwd> HRTEM</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Nanotechnology is an umbrella term for a wide range of technologies concerned with structures and processes of materials that have nanometer scale. Nanocomposites are one of those advanced materials that received much attention due to their unique and unusual properties that proposing them as promising candidates for several structural and wear resistance applications [<xref ref-type="bibr" rid="scirp.17039-ref1">1</xref>]. Nanocomposite materials are formed by dispersing nanocrystalline reinforcement ceramics into metallic matrix, leading to significant improvement in the mechanical and physical properties. It has been reported that both strength and fracture toughness are increased by the order of two to four times than conventional composite materials [<xref ref-type="bibr" rid="scirp.17039-ref2">2</xref>]. Among the transitionmetal carbides, WC has excellent high temperature strength and good corrosion resistance. It shows extremely high hardness value and possesses high values of Young’s modulus [<xref ref-type="bibr" rid="scirp.17039-ref3">3</xref>]. Due to its poor fracture toughness and the difficulties in powders consolidation to obtain fully dense compacts, WC is usually mixed with metallic binders, such as Co, Fe, and Ni to form so-called cemented carbides. WC-Co cements with different Co volume fractions ranging from 4% to 14% have been widely used for cutting tools and wear resistant materials. Mechanical mixing method, using ball milling of the reinforcement materials (WC) with several concentrations of Co (metallic matrix) shows significant advantage to obtain nanocomposite WC-Co powders [4,5]. The powders were then consolidated into bulk objects, using hot pressing technique. The hot-pressed WCCo powders show remarkable increase in the fracture toughness; however the existence of the metallic binding material leads to a decrease in the hardness and elastic module values. WC-Co cements have some industrial limitations because of the presence of metallic Co matrix (binder) leads to failure at high temperature due to softening. Many efforts have been carried out to achieve superior hardness and toughness combinations through replacing the metallic Co by different types of ceramic nanocrystalline materials to form ceramic matrices (WC nanocomposites) [6-8].</p><p>The present work has been addressed in order to study the influence of nanocrystalline ZrO<sub>2</sub> additives on improving the fracture toughness and Poisson’s ratio of mechanically mixed WC-ZrO<sub>2</sub> nanocomposites. The selection of ZrO<sub>2</sub> comes from the fact that it has a high thermal stability and excellent mechanical properties such as high bending strength and excellent fracture toughness. We are also proposing a powerful tool for obtaining fully dense nano-ceramic composites, using spark plasma sintering (SPS) technique for the mechanically mixed ceramic powders of WC-ZrO<sub>2</sub>.</p></sec><sec id="s2"><title>2. Experimental</title><p>In the present study, elemental powders of WC (99.5%, 30 &#181;m) were mixed with different selected volume fractions of ZrO<sub>2</sub> (2% Y<sub>2</sub>O<sub>3</sub>) powders (99.5%, 10 &#181;m) of 0.5, 5, 10, 15 and 20 vol.%. The mixed powders of each ZrO<sub>2</sub> concentration were sealed in a cylindrical WC vial (250 ml in volume) together with fifty WC balls (10 mm in diameter) in a glove box under argon gas atmosphere. The ballto-powder weight ratio was maintained at the level of 10:1. The ball-milling experiments were carried out at room temperature, using Fritsch P5 high-energy ball mill at a rotation speed of 250 rpm. The milling experiments were interrupted at regular intervals and small amounts of the milled powders were taken out from the vial in the glove box. The powders were characterized by means of X-ray diffraction (XRD) with CuKα radiation, scanning electron microscope (SEM), transmission electron microscope (TEM) using 200 kV and/or high-resolution transmission electron microscopes (HRTEM).</p><p>The end product of the ball-milled nanocomposite powders (after 360 ks) at different ZrO<sub>2</sub> concentrations were individually consolidated into bulk samples, using spark plasma sintering (SPS) method. The consolidation procedure took place in vacuum at 1673 K with a pressure of 19.6 to 38.2 MPa. In order to avoid any undesired grain growth, the sintering process was applied for only 0.18 ks without adding any binding materials. The densities of consolidated WC/ZrO<sub>2</sub> materials were determined by Archimedes’ principle, using water immersion method. Vickers indenter with a load of 50 kg was employed to determine the hardness of the compacted samples. The size of the indentation cracks has been used to determine the fracture toughness (K<sub>c</sub>) of the sample [<xref ref-type="bibr" rid="scirp.17039-ref9">9</xref>]. The hardness and K<sub>c</sub> values reported below are averaged from at least ten indentations. The elastic properties of the bulk samples were determined by nondestructive test using pulse-echo overlap ultrasonic technique using ultrasonic detector.</p></sec><sec id="s3"><title>3. Results and Discussions</title><p>XRD technique was employed to follow the structural changes that may occur during ball milling of hcp-WC with different volume fractions t-ZrO<sub>2</sub> powders and after the consolidation process that was achieved at 1673 K, using SPS technique. <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) displays the XRD pattern of ball milled WC-10% ZrO<sub>2</sub> powders after 43 ks of the milling time. The powders at this early stage of milling still consist of coarse grains, indicated by the existence of sharp Bragg-peaks which are corresponding to the matrix and reinforcement materials of t-ZrO<sub>2</sub> and hcp-WC, respectively. Contrary, the XRD pattern of the final-product <xref ref-type="fig" rid="fig1">Figure 1</xref>(b), which was obtained after longer milling time (360 ks), shows a significant broadening in the Bragg lines for both ZrO<sub>2</sub> and WC materials, suggesting the formation of nanocomposite WC-ZrO<sub>2</sub>. <xref ref-type="fig" rid="fig1">Figure 1</xref>(c) depicts the</p><p>XRD pattern of the final-product (360 ks) that was consolidated at 1673 K indicates the absence of any intermediate phase (s) other than WC and ZrO<sub>2</sub>. The absence of any reacted phases during this sintering step implies the thermodynamic compatibility of WC and ZrO<sub>2</sub> at the applied consolidation temperature. Furthermore, there is no obvious dramatic change in the grain size of both the matrix and reinforcement materials can be detected after sintering, indicating that the consolidated sample maintains its nanocrystalline properties (<xref ref-type="fig" rid="fig1">Figure 1</xref>(c)).</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the bright field image (BFI) of WC-10% ZrO<sub>2</sub> powders after ball milling for 43 ks (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)) and 360 ks (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)). The light gray region in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) shows the ZrO<sub>2</sub> matrix, whereas the dark coarse grains embedded into the matrix, present the WC grains. The WC grains that are heterogeneously distributed in the matrix have irregular shapes with a wide grain size distribution, ranging from 23 to 280 nm in diameter (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)). Obviously, the matrix material at this early stage of milling (43 ks) is either rich or poor with WC. Increasing the milling time (360 ks) leads to successive increase in the impact and shear forces that are generated by the grinding tools (balls) so that the brittle WC grains disintegrated into finer cells with an average diameter of 18 nm in diameter as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b). This dramatic disintegration causes an increase in the WC surface area, leading to the formation of nanocrystalline spherical lenses of WC, which are fairly distributed into the whole matrix material to form a homogeneous WC/ZrO<sub>2</sub> nanocomposite. The formation of these nanomaterials is attributed to the plastic deformation that is produced in the WC crystal lattice during the high-energy ball milling process and this occurs by slip and twinning in the lattice of the milled powders. Due to the successive accumulations of the dislocations density, the crystals are disintegrated into sub-grains that are initially separated by low angle grain boundaries. The formation of these sub grains is attributed to the decrease in the atomic level strain. Increasing the ball milling time from 43 ks to 360 ks leads to further lattice distortion and consequently to grain size reduction. Reduction in grain size is very important factor for the consolidation procedure because it increases the sinterability of the powders.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.17039-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">M. S. El-Eskandarany, “Mechanical Alloying for Fabrication of Advanced Engineering Materials,” William Andrew, New York, 2001, p. 45.</mixed-citation></ref><ref id="scirp.17039-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">T. Venkateswaran, D. Sarkar and B. 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