<?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.2016.46031</article-id><article-id pub-id-type="publisher-id">JMMCE-72347</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>
 
 
  The Influence of Molding Density of TiO&lt;sub&gt;2&lt;/sub&gt; Varistor-Ceramic on Densification of Ceramic Body and Grain Growth
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yu</surname><given-names>Wang</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>Kemin</surname><given-names>Zhang</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>Wenge</surname><given-names>Li</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>Weihua</surname><given-names>Yao</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jinxin</surname><given-names>Ma</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>Xiaolin</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Dongguan Yilihe Electronics Co. Ltd., Dongguan, China</addr-line></aff><aff id="aff1"><addr-line>School of Materials Engineering, Shanghai University of Engineering Science, Shanghai, China</addr-line></aff><aff id="aff2"><addr-line>Merchant Marine College, Shanghai Maritime University, Shanghai, China</addr-line></aff><pub-date pub-type="epub"><day>19</day><month>10</month><year>2016</year></pub-date><volume>04</volume><issue>06</issue><fpage>380</fpage><lpage>388</lpage><history><date date-type="received"><day>October</day>	<month>28,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>November</month>	<year>26,</year>	</date><date date-type="accepted"><day>November</day>	<month>29,</month>	<year>2016</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>
 
 
  This article explored the influence of molding density of TiO
  <sub>2</sub> varistor-ceramic on densification of ceramic body and grain growth. By the main phase and second phase analysis of TiO
  <sub>2</sub> varistor-ceramic through XRD and EDAX, the effects of the second phrase on TiO
  <sub>2</sub> varistor-ceramic were studied. Grain size and its distribution were observed through scanning electron microscope and the density of porcelain body was measured. The effects of grain size, distribution and density of ceramic body on electrical property of TiO
  <sub>2</sub> varistor-ceramic were the focus issue for analysis. The increased molding density would improve the densifying of magnetic body to some extent and promote grain growth.
 
</p></abstract><kwd-group><kwd>TiO&lt;sub&gt;2&lt;/sub&gt; Varistor-Ceramic</kwd><kwd> Molding Density</kwd><kwd> Densification</kwd><kwd> Grain Size</kwd><kwd> Distribution</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Varistor-ceramic belongs to a kind of semiconductor material, which is sensitive to the variation of applied voltage. Semiconductor crystal and high barrier grain boundary can account for the microstruction revolution of the varistor-ceramic [<xref ref-type="bibr" rid="scirp.72347-ref1">1</xref>] . When the applied voltage at both ends stays in a certain range, the varistor-ceramic presents a high resistance. Otherwise, when the voltage exceeds this certain range, the resistance of the varistor-ceramic drastically decreases and the current through the varistor-ce- ramic rapidly arises. The electrical resistor in which the current and the voltage show the nonlinearity relationship is called the varistor-ceramic. Varistor-ceramic as a semiconductor material is used to protect and control the voltage surge and it has been widely applied in a variety of field, such as the aerospace, national defense, electrommunication and household appliances [<xref ref-type="bibr" rid="scirp.72347-ref2">2</xref>] .</p><p>TiO<sub>2</sub> varistor-ceramic property is determined by the performance of the crystal and the crystal boundary, which can be affected by the density of crystal and the growth process of the grain. Therefore, it is greatly important for us to research the TiO<sub>2</sub> varistor-ceramic densification and the growth process of crystal [<xref ref-type="bibr" rid="scirp.72347-ref3">3</xref>] .</p><p>In previous studies, the researchers are mainly focused on the effect of the type and composition of addition, the sintering temperature and the holding time on the electronic property and microstructure of TiO<sub>2</sub> varistor-ceramic [<xref ref-type="bibr" rid="scirp.72347-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.72347-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.72347-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.72347-ref7">7</xref>] . However, few studies were carried out about the effect of the ceramic embryo forming density on the microstructure evolution. In this investigation, on the premise of the same formula, we explore the effect of ceramic embryo forming density of TiO<sub>2</sub> varistor-ceramic on its densification and crystal growth process.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. The Preparation of TiO<sub>2</sub> Varistor-Ceramic</title><p>The experimental raw materials were composed of industrial pure TiO<sub>2</sub> (Shanghai pengbo) and electronic grade materials (Nb<sub>2</sub>O<sub>5</sub>, SrCO<sub>3</sub> and Bi<sub>2</sub>O<sub>3</sub>). The configuration ratio is 97.9% TiO<sub>2</sub> + 1.1% Nb<sub>2</sub>O<sub>5</sub> + 0.5% SrCO<sub>3</sub> + 0.5% Bi<sub>2</sub>O<sub>3</sub> (in molar mass percent). The hybrid materials were milled for 8 h in 200 r/min with the addition of dispersant, release agent and deionized water. Then the materials were dried for 12h in 150˚C. The PVA solution (in 7 wt.%) was mixture into the materials for granulation and a circle piece can be obtained from it with a size of 13.17 in OD (outer diameter), 7.07 in ID (inside diameter) and 1.02 in height. After then, the circle piece will be sintered accompanied with the binder removal process and natural cooling. Three silver electrodes were impressed on the surface by silver ink firing and the electronic property was identified. After the sintering process, the density of porcelain body was measured. After completion of the sintering, measure the density of the porcelain body. The ceramic embryo forming density of samples were 2.35 g/cm<sup>3</sup>, 2.45 g/cm<sup>3</sup>, 2.55 g/cm<sup>3</sup>, 2.65 g/cm<sup>3</sup> and 2.75 g/cm<sup>3</sup> respectively.</p></sec><sec id="s2_2"><title>2.2. Measurement</title><p>An ZR100A ring varistors tester was used to measure the samples’ resistance: V<sub>1mA</sub> and V<sub>10mA</sub>. The nonlinear coefficients of the samples were calculated by the following formula:</p><disp-formula id="scirp.72347-formula30"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-2710475x2.png"  xlink:type="simple"/></disp-formula><p>According to the Archimedes drainage method [<xref ref-type="bibr" rid="scirp.72347-ref8">8</xref>] , the density of the TiO<sub>2</sub> varistor- ceramic can be obtained by the formula (2):</p><disp-formula id="scirp.72347-formula31"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-2710475x3.png"  xlink:type="simple"/></disp-formula><p>The densification (ρ<sub>r</sub>) of the sample is equal to the ratio of the real densification of the samples to the theoretical one, which can be calculated by the following formula:</p><disp-formula id="scirp.72347-formula32"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-2710475x4.png"  xlink:type="simple"/></disp-formula><p>where ρ<sub>1</sub> is for the TiO<sub>2</sub> samples’ theoretical density. However, the theoretical density of TiO<sub>2</sub> varistor-ceramic was ranged from the content of the addition. By calculation, in this experimental condition, the theoretical density of TiO<sub>2</sub> varistor-ceramic is 4.277 g/cm<sup>3</sup>.</p><p>The grain size and distribution were observed and analyzed by scanning electron microscope. Meantime, the average size and the distribution of grain size were obtained by using the method of linear truncation of the samples [<xref ref-type="bibr" rid="scirp.72347-ref9">9</xref>] :</p><disp-formula id="scirp.72347-formula33"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-2710475x5.png"  xlink:type="simple"/></disp-formula><p>The grain size standard deviation (σ) is obtained by the following formula:</p><disp-formula id="scirp.72347-formula34"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-2710475x6.png"  xlink:type="simple"/></disp-formula><p>The large the σ is, the more uneven the grain distribution is.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Phase Analysis</title><p>The X-ray diffraction patterns of TiO<sub>2</sub> varistor-ceramic with different ceramic embryo forming density is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Obtaining in the five samples of TiO<sub>2</sub> varistor-ceramic phase structure is rutile structure in using XRD High Score Plus auxiliary software analysis and contrasting through diffraction peak and PDF standard card. In addition to the TiO<sub>2</sub> varistor-ceramic rutile main crystal phase, also found that the existence of the second phase. As a result of the existence of second phase, the liquid</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The XRD of samples with different density</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x7.png"/></fig><p>phase can be wetting body particles and the filling the void between the particles, which also can improve the density of sample and the nonlinear coefficient of the sample. But the second phase segregation form the high resistance layer between TiO<sub>2</sub> grain crystal and make varistor voltage rasing.</p><p>Due to the five samples of the formula and The X-ray diffraction patterns of TiO<sub>2</sub> varistor-ceramic is the same, choosing a sample to analyze the composition of the second phase. <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="table" rid="table1">Table 1</xref> shows respectively the composition and content of each element of the second phase in the TiO<sub>2</sub> varistor-ceramic when the ceramic embryo forming density of sample is 2.55 g/cm<sup>3</sup>. According to these results, a preliminary decision to get the second phase is composed of Ti Sr and Nb oxide.</p></sec><sec id="s3_2"><title>3.2. Microstructure</title><p>It can be observed that the pore volume of the sample 1 is bigger and the number of pores is more from the <xref ref-type="fig" rid="fig3">Figure 3</xref>. The pore volume of the sample 2 is still bigger, but compared to sample 1, the number of pores of sample 2 is less. The pore volume of the sample 3 4 5 is smaller and with the increase of the ceramic embryo forming density have significantly reduce the numbers of stomata. Studies have shown that: due to stomatal migration to grain boundaries bring in pinning effect, improve the potential</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> EDS of second phase</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x8.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The content of second phase</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Element</th><th align="center" valign="middle" >Wt%</th><th align="center" valign="middle" >At%</th></tr></thead><tr><td align="center" valign="middle" >CK</td><td align="center" valign="middle" >08.91</td><td align="center" valign="middle" >22.42</td></tr><tr><td align="center" valign="middle" >OK</td><td align="center" valign="middle" >27.24</td><td align="center" valign="middle" >51.45</td></tr><tr><td align="center" valign="middle" >SrL</td><td align="center" valign="middle" >20.24</td><td align="center" valign="middle" >06.98</td></tr><tr><td align="center" valign="middle" >NbL</td><td align="center" valign="middle" >27.38</td><td align="center" valign="middle" >08.91</td></tr><tr><td align="center" valign="middle" >TiL</td><td align="center" valign="middle" >16.23</td><td align="center" valign="middle" >10.24</td></tr><tr><td align="center" valign="middle" >Matrix</td><td align="center" valign="middle" >Correction</td><td align="center" valign="middle" >ZAF</td></tr></tbody></table></table-wrap><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> SEM of samples with different densities under 200 times magnification; (a) ρ<sub>1</sub> = 2.35 g/cm<sup>3</sup>; (b) ρ<sub>2</sub> = 2.45 g/cm<sup>3</sup>; (c) ρ<sub>3</sub> = 2.55 g/cm<sup>3</sup>; (d) ρ<sub>4</sub> = 2.65 g/cm<sup>3</sup>; (e) ρ<sub>5</sub> =2.75 g/cm<sup>3</sup></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x9.png"/></fig><p>energy barrier, hinder the interface extension and coarsening grow up, increasing the porosity also inhibits grain growth. In the process of high temperature sintering, point defects of oxygen vacancies has a direct influence on the formation of porosity. There is a certain concentration of oxygen vacancy defects in TiO<sub>2</sub>, its shortcomings reactive as follows [<xref ref-type="bibr" rid="scirp.72347-ref10">10</xref>] :</p><disp-formula id="scirp.72347-formula35"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-2710475x10.png"  xlink:type="simple"/></disp-formula><p>In the structure of rutile TiO<sub>2</sub>, Ti<sup>4+</sup> ion coordination number is 6, the ionic radius is 68pm, and Nb<sup>5+</sup> ionic radius is 69 pm in Nb<sub>2</sub>O<sub>5</sub> is very close to Ti<sup>4+</sup> ionic radius. In the process of high temperature sintering, Nb<sup>5+</sup> solid solution in TiO<sub>2</sub> to replace Ti<sup>4+</sup> ions, but the 5 valence of Nb<sup>5+</sup> instead of 4 valence of Ti<sup>4+</sup> will generate an electrical charge compensation. Its shortcomings reactive as follows [<xref ref-type="bibr" rid="scirp.72347-ref10">10</xref>] :</p><disp-formula id="scirp.72347-formula36"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-2710475x11.png"  xlink:type="simple"/></disp-formula><p>In the process of the above defects reaction, which introduced the conduction electrons in order to grain conductivity having risen sharply and porcelain body implement semiconductor.</p><p>In <xref ref-type="fig" rid="fig4">Figure 4</xref> can be observed that the five samples all exist the second phase, which is corresponding to the results of XRD analysis. With the increase of the embryonic body forming density, the average grain size of sample rising after down.</p><p>With the average grain size is larger in TiO<sub>2</sub> varistor-ceramic, the number per unit volume of grain boundary is less, so that the total grain boundary barrier is reduced and the varistor voltage is lower.</p></sec><sec id="s3_3"><title>3.3. TiO<sub>2</sub> Varistor-Ceramic Densification Degree of Changing Rule with the Ceramic Embryo Forming Density</title><p>The densification process of porcelain body was analyzed. It has found that the ceramic density showed a trend of increases at first then decreases with the increase of the ceramic embryo forming density, as shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>. Simultaneously, its increasing</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> SEM of samples with different densities under 3000 times magnification (a) ρ<sub>1</sub> = 2.35 g/cm<sup>3</sup>; (b) ρ<sub>2</sub> = 2.45 g/cm<sup>3</sup>; (c) ρ<sub>3</sub> = 2.55 g/cm<sup>3</sup>; (d) ρ<sub>4</sub> = 2.65 g/cm<sup>3</sup>; (e) ρ<sub>5</sub> =2.75 g/cm<sup>3</sup></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x12.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The change of density of porcelain body with the ceramic embryo forming density</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x13.png"/></fig><p>degree of ceramic embryo forming density is greater than that of the ceramic density as there are various pores in the porcelain body, mainly are closed pores and open pores. And the increase of the porcelain body density has a maximum value. When the value becomes too large, it will hinder the densification process of porcelain body and make porcelain body density decreased.</p></sec><sec id="s3_4"><title>3.4. TiO<sub>2</sub> Varistor-Ceramic Grain Size and Density Distribution with the Embryonic Body Molding Change Rule</title><p>Using scanning electron microscope and carries on the analysis of grain size and distribution, which obtains the average size of TiO<sub>2</sub> varistor-ceramic porcelain (dg) along with the increase of the ceramic embryo forming density first increases then decrea- ses, grain size standard deviation (σ) along with the augment of ceramic embryo forming density first increase then decrease. In <xref ref-type="fig" rid="fig6">Figure 6</xref>, grain size and grain size standard deviation have peak, when the ceramic embryo forming density is 2.55 g/cm<sup>3</sup>, the average grain size is 5.911 μm and grain size of the standard deviation sigma is 0.853 μm, it has the biggest size and best uniform distribution, the microstructure is better.</p></sec><sec id="s3_5"><title>3.5. Embryo Volume Density of TiO<sub>2</sub> Varistor-Ceramic Performance Influence</title><p><xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref>, respectively describes the varistor voltage and nonlinear coeffi- cient changing with ceramic embryo forming density curve. From the figure, the ceramic embryo forming density performance have a significant impact on TiO<sub>2</sub> varistor-ceramic electrical property. <xref ref-type="fig" rid="fig7">Figure 7</xref> shows that varistor-ceramic voltage V<sub>1mA</sub> with the increase of sample ceramic embryo forming density increase with the decrease of the first, the nonlinear coefficient α increased with the increase of sample ceramic embryo forming density first decreases then increases slightly. Due to the varistor voltage is the superposition of polycrystalline ceramics intergranular voltage, as shown in <xref ref-type="fig" rid="fig6">Figure 6</xref> as the grain size decreases after increasing first, unit volume increase with the decrease of after the first number of grain boundary, therefore, varistor voltage increase with the decrease of the first. Ceramic embryo forming density also have an impact on nonlinear coefficient α, but different from the effects of doping, when the grain growth, grain boundary number less, nonlinear coefficient showed a trend of decline to a certain degree.</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> The change of grain size and its distribution in TiO<sub>2</sub> ceramic embryo forming density</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x14.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> The change of varistor voltage with ceramic embryo forming density</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x15.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> The change of α with. ceramic embryo forming density</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-2710475x16.png"/></fig></sec></sec><sec id="s4"><title>4. Conclusions</title><p>1) Ceramic embryo forming density on the microstructure and electrical properties of TiO<sub>2</sub> varistor-ceramic has a great influence.</p><p>2) When the ceramic embryo forming density is 2.55 g/cm<sup>3</sup>, the average grain size is 5.911 μm and grain size of the standard deviation sigma is 0.853 μm, it has the biggest size and best uniform distribution, the microstructure is better.</p><p>3) Improving the ceramic embryo forming density of TiO<sub>2</sub> varistor-ceramic can accelerate the densification process to a certain degree, at the same time can promote grain growing up. The best ceramic embryo forming density related to the samples of the formula and the granularity of raw material, which requires specific test many times.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors acknowledge the financial support from Shanghai outstanding technical leaders plan (14XD1425400).</p></sec><sec id="s6"><title>Cite this paper</title><p>Wang, Y., Zhang, K.M., Li, W.G., Yao, W.H., Ma, J.X. and Zhang, X.L. (2016) The Influence of Molding Density of TiO<sub>2</sub> Varistor-Ceramic on Densification of Ceramic Body and Grain Growth. Journal of Minerals and Materials Characterization and Engineering, 4, 380-388. http://dx.doi.org/10.4236/jmmce.2016.46031</p></sec></body><back><ref-list><title>References</title><ref id="scirp.72347-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Yuan, M.J., Cui, W.Q., Li, P., et al. (2008) The Research and Application of Tio2 Varis-tor-Ceramic. 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