<?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">Graphene</journal-id><journal-title-group><journal-title>Graphene</journal-title></journal-title-group><issn pub-type="epub">2169-3439</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/graphene.2022.112002</article-id><article-id pub-id-type="publisher-id">Graphene-120207</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>
 
 
  Investigation of Ceramic Based Composites by Using 2D Graphene Filler
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zeeshan</surname><given-names>Abbas</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>Rashid</surname><given-names>Jalil</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>Ibtsam</surname><given-names>Riaz</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>Muhammad</surname><given-names>Tahir</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>University of Engineering and Technology, Lahore, Pakistan</addr-line></aff><pub-date pub-type="epub"><day>29</day><month>09</month><year>2022</year></pub-date><volume>11</volume><issue>02</issue><fpage>19</fpage><lpage>29</lpage><history><date date-type="received"><day>2,</day>	<month>April</month>	<year>2022</year></date><date date-type="rev-recd"><day>26,</day>	<month>April</month>	<year>2022</year>	</date><date date-type="accepted"><day>29,</day>	<month>April</month>	<year>2022</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 ceramic composites of sodium bismuth titanate with reduce graphene oxide NBT/rGO of different compositions were fabricated by solid state sintering method and characterized. In this work, the graphene oxide (GO) and reduce graphene oxide (rGO) was successfully synthesized by Hummer’s modified method which is confirmed by FTIR and XRD results. The reduce graphene oxide used as 2D filler in piezoelectric creamic material. The crystalline structure of NBT/rGO composite was confirmed by X-ray diffraction with rhombohedral symmetry. The dispersion of rGO in the ceramic can be detect by the optical microcopy images. The electrical conductivity of sodium bismuth titanate shows increase at higher values of frequency and conductivity nanocomposites of different wt% were start decreases up to certain value of frequency. The broadening of peaks in frequency explicit plots of electrical conductivity with the help of LCR Meter (Impedance Capacitance and Resistance). The crystalline size of reduced graphene oxide and NBT is calculated by Scherrer’s formula of XRD peaks.
 
</p></abstract><kwd-group><kwd>Sodium Bismuth Titanate</kwd><kwd> Graphene Oxide</kwd><kwd> Reduce Graphene Oxide</kwd><kwd> Electrical Conductivity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The Sodium Bismuth Titanate (NBT) belongs to dielectric material family and it is new class of dielectrics. It is a lead-free piezoelectric ceramic and it is studied widely because of its high dielectric constant [<xref ref-type="bibr" rid="scirp.120207-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref2">2</xref>]. The NBT material covers large range of temperature and because of its large temperature range stability it is best suited for use in oil and gas sector, automotive and military applications. Structure of BNT is an ABO3 distorted perovskite with a rhombohedral R3c crystal symmetry at ambient temperature. The basic perovskite formula (ABO3) of NBT is ( Bi 0.5 Na 0.5 ) TiO 3 . The (ABO3) crystal structure for NBT consider as the sodium and bismuth cations are present at the corners of unit cell, cations of titanium go to center of oxygen octahedral while oxygen cations move to faces of cubic cell [<xref ref-type="bibr" rid="scirp.120207-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref4">4</xref>].</p><p>The NBT is considered as a fantastic contender of lead-free piezoelectric ceramics for it has rhombohedral symmetry with a = 3.891 A 0 and α = 89 0 36 T at normal temperature. Where NBT becomes very interesting ferroelectric material due to its large polarization P r = 38 μC / cm 2 and large coercive effect E c = 73 kV / cm . In NBT structure A-sites are occupied due to Bi<sup>3+</sup> and Na<sup>+</sup> and B-sites are occupied due to Ti 4 + [<xref ref-type="bibr" rid="scirp.120207-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref5">5</xref>].</p><p>Graphene is a monoatomic layered carbon’s material that having single atomic thickness, smooth, honeycomb like structure and bound firmly. Graphene discovery had a great influence upon the research that reflected back by the published papers all over the world and still research is carried out. We may say that fullerenes (0D), nanotube (1D), and piled graphite (3D) are all the different structures of grapheme [<xref ref-type="bibr" rid="scirp.120207-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref7">7</xref>]. The simplest way to obtain graphene sheet or graphene layers is stacking method (by mechanical exfoliation method) [<xref ref-type="bibr" rid="scirp.120207-ref8">8</xref>]. Carbon has two well-known crystals diamond and graphite that are present in bulk form and shows their unique symmetry and properties like mechanical strength [<xref ref-type="bibr" rid="scirp.120207-ref9">9</xref>]. These two forms of carbon are used for different application that reflects by their bonding. In graphene carbon-carbon bonds occurs due to the positioning of electrons of 2p<sub>x</sub> and 2p<sub>y</sub> with 2s orbitals. These orbitals offer ascent to steady and localized σ bonds [<xref ref-type="bibr" rid="scirp.120207-ref10">10</xref>]. The graphene has very large electrical conductivity because its bandgap between conduction band and valence band is zero and also known as semimetal [<xref ref-type="bibr" rid="scirp.120207-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref13">13</xref>].</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. GO Synthesis</title><p>Initially 6 g graphite powder was purified. 60 ml Hydrofluoric acid (HF) was added to the 10 g graphite powder and magnetically stirred four one hour. Then deionized water (DIW) was added to it and washed until pH neutralized to 7. At 100˚C, graphite sample was dried by using magnetic stirrer. Now graphite was purified so modified hummers method could start for the synthesis of graphene oxide. 36 g of potassium permanganate (KMnO<sub>4</sub>) and 6 g of graphite powder were stirred for mix-up; for several minutes. Another solution was prepared by mixing 720 ml sulfuric acid (H<sub>2</sub>SO<sub>4</sub>) with 80 ml phosphoric acid (H<sub>3</sub>PO<sub>4</sub>) and stirred for several minutes. Now add the solution of (KMnO<sub>4</sub> + Graphite) in solution of (H<sub>2</sub>SO<sub>4</sub> + H<sub>3</sub>PO<sub>4</sub>) slowly. After stirring 12 hours the solution changes its color to dark green. Then 800 ml deionized water (DIW) and 10 ml hydrogen peroxide (H<sub>2</sub>O<sub>2</sub>) added to GO solution and stirring it 10 minutes for the removal of excess KMnO<sub>4</sub>. Now reducing the temperature of occurred exothermic reaction by ice bathing. Now for neutralization of GO solution it was washed several times with HCl and DIW. Washing of solution continue until its PH becomes 7 or neutralized. To obtain graphene oxide (GO) powder the washed graphene oxide solution was dried at 70˚C for 24 hours by using oven [<xref ref-type="bibr" rid="scirp.120207-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref16">16</xref>].</p></sec><sec id="s2_2"><title>2.2. rGO Preparation</title><p>For Reduction of graphene oxide (GO) we dispersed graphene oxide powder into DI water at the rate of 0.2 mg/ml. The solutions of graphene oxide (GO) were sonicated in an ultrasound bath for 2 hours. Then the dispersed solution of GO was placed into autoclave and heat at 180˚C for 4 hours [<xref ref-type="bibr" rid="scirp.120207-ref17">17</xref>]. The internal pressure of 400 KPa was applied into autoclave. After heating, the autoclave was cool down to ambient temperature naturally [<xref ref-type="bibr" rid="scirp.120207-ref18">18</xref>]. The sample of reduce graphene oxide was collected and washed with DI water to dry at room temperature overnight to obtain powder of reduce graphene (rGO) [<xref ref-type="bibr" rid="scirp.120207-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref19">19</xref>].</p></sec><sec id="s2_3"><title>2.3. Preparation of NBT Composites</title><p>The ceramic based composite was prepared with two different powders. The 1<sup>st</sup> one is Sodium bismuth titanate (NBT), which was added as matrix and the 2<sup>nd</sup> one was reduce graphene oxide (rGO) which used as filler in the martix. The milling of materials was done for four hours at 200 rev/mint using zirconia balls as grinding media in Teflon jars in a planetary milling. Ethanol was used as a dispersant. Ball milled powders were heated at 70˚C for one day. Drying process was done for the removal ethanol [<xref ref-type="bibr" rid="scirp.120207-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref22">22</xref>].</p><p>We prepare four sample with different weight percentage (%) of reduce graphene in NBT (0.5%, 1%, 3%, 5% in 3 g of NBT). These powders were mixed by ball milling technique. Then the powder of composite is collected by filtration [<xref ref-type="bibr" rid="scirp.120207-ref23">23</xref>].</p><p>Pressing is the technique of fabricating ceramic components by the compaction of powder in a metal die set. Then the sample were placed between the platen 1 &amp; 2 in a uniaxial hydraulic press for the formation of pellets of weight of 0.5 g [<xref ref-type="bibr" rid="scirp.120207-ref24">24</xref>]. Each sample placed under hydraulic press for 15 mints and pressure buildup of 3000-pound square per meter (PSM). Then the pellets were baked and sintered under high temperature of 1075˚C for 2 hours in a box furnace [<xref ref-type="bibr" rid="scirp.120207-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref26">26</xref>].</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Results</title><sec id="s3_1_1"><title>3.1.1. FTIR of GO and rGO</title><p>The FTIR is preferred because it provides all information about functional groups which attached with sample (<xref ref-type="fig" rid="fig1">Figure 1</xref>). We use solid samples for FTIR. The FTIR spectra show broad and deep peaks at different range. Firstly, the peaks of GO appear between 3723 - 3071 cm<sup>−</sup><sup>1</sup> that shows hydroxyl group (O-H stretching) which is due water absorption. The spectra at 1564 cm<sup>−</sup><sup>1</sup> and 1358 cm<sup>−</sup><sup>1</sup> represent C=C stretching and C-H group. The peaks at 1228 cm<sup>−</sup><sup>1</sup> and 1048 cm<sup>−</sup><sup>1</sup> represent C-O stretching and CO-O-CO stretch in anhydride. On the other hand, rGO peaks at 3833 and 3727 cm<sup>−</sup><sup>1</sup> shows O-H stretching. The spectra at 1649 cm<sup>−</sup><sup>1</sup> and 1546 cm<sup>−</sup><sup>1</sup> gives C=C stretching and N-O stretching [<xref ref-type="bibr" rid="scirp.120207-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref28">28</xref>].</p></sec><sec id="s3_1_2"><title>3.1.2. FTIR of rGO/NBT Composites</title><p>Now this given graph (<xref ref-type="fig" rid="fig2">Figure 2</xref>) belongs to NBT with different concentration 1%, 3% and 5%. The peaks of rGO in the NBT material can be easily detected. The peak at 998 cm<sup>−1</sup> shifted towards 1008 cm<sup>−1</sup> can be seen clearly as we increase</p><p>the weight percentage of rGO in the NBT. The peak at 1520 also been seen increased as the concentration of reduce graphene increased. Last peak in the graph at the range 3700 cm<sup>−1</sup> is also due to rGO which shows O-H stretching of hydroxyl group [<xref ref-type="bibr" rid="scirp.120207-ref23">23</xref>].</p></sec></sec><sec id="s3_2"><title>3.2. Optical Analysis</title><p>NBT/rGO ceramic composites were examined under optical microscopy. This technique is simplest and easy to find reduce graphene in sodium bismuth titanate structure. The dispersion of rGO in the ceramic can be detected by the optical microcopy images [<xref ref-type="bibr" rid="scirp.120207-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref29">29</xref>]. The optical images of ceramic composites are showed in the given <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref>(a) shows image of pure NBT and Figures 3(b)-(d) represent 1%, 3% and 5% concentration of reduce graphene in the NBT ceramic material at 50&#215; magnification. In images of ceramic composites, shiny material which is graphene distributed over the NBT matrix representing that the reduce graphene oxide filler was successfully dispersed in the NBT. In these optical image’s spots on the surface of NBT represent the concentration of rGO where BNT ceramic is matrix and rGO is 2D filler. We can see rGO clearly as we increase the percentage of concentration in matrix [<xref ref-type="bibr" rid="scirp.120207-ref30">30</xref>].</p></sec><sec id="s3_3"><title>3.3. LCR Meter Analysis</title><p>In this work sample is attached to probs of the LCR meter and placed in an electrical heater and temperature increases in discrete manners up to 500˚C. The sample is coated by silver paint and LCR is done at frequency between 100 Hz to 1 MHz at different temperature starting from 25˚C with a difference of 25˚C for each reading [<xref ref-type="bibr" rid="scirp.120207-ref10">10</xref>]. The capacitance and resistance of material are obtained by the</p><p>LCR meter [<xref ref-type="bibr" rid="scirp.120207-ref31">31</xref>]. We can calculate the conductivity with the given formula;</p><p>R = ρ L A</p><p>Now we can explain the electrical conductivity of NBT ceramic and rGO/NBT composite which is doped by reduced graphene oxide rGO with different wt% (1%, 3% &amp; 5%). As the concentration of rGO increases in the sample it shows decrease in electrical conductivity. We draw a graph of LCR meter between frequency and conductivity with sodium bismuth titanate doping by reduced graphene oxide with different weight percentage (<xref ref-type="fig" rid="fig4">Figure 4</xref>).</p><p>Firstly, we analysis electrical conductivity at (200˚C, 300˚C, 400˚C &amp; 500˚C) which shows decrease in the conductivity as temperature from 200˚C to 500˚C at different values as shown in the graphs of NBT ceramic and rGO/NBT composite of different wt% (1%, 3% &amp; 5%) [<xref ref-type="bibr" rid="scirp.120207-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.120207-ref32">32</xref>]. The impedance spectroscopy shows that conductivity of ceramic composite decreases as the concentration of rGO increases in the composite.</p><p>This shows that when rGO was added to piezoelectric ceramic, it become</p><p>semimetal composite of zero band gap [<xref ref-type="bibr" rid="scirp.120207-ref33">33</xref>]. The value of electrical conductivity of conducting composite shows decreases as wt% of filler increases in the composite in <xref ref-type="table" rid="table1">Table 1</xref>. The LCR Meter show results that conductivity of ceramic composite decreases at 1 MHz as the concentration of rGO increases in the composite. This shows that when rGO was added to NBT, it become semimetal composite of zero band gap. The electrical conductivity of conducting composite decreases at high frequency as wt% of filler increases in the composite.</p><sec id="s3_3_1"><title>3.4.1. XRD of rGO</title><p>Now XRD pattern of reduce graphene oxide is given in <xref ref-type="fig" rid="fig5">Figure 5</xref> that provides information about the planes. The main peak appears at 26.608 (a.u) where two other peaks also appear at 34.98 and 42.52 (a.u) [<xref ref-type="bibr" rid="scirp.120207-ref27">27</xref>].</p><p>The crystalline size of rGO is calculated by the Scherrrer’s formula which is given in the above <xref ref-type="table" rid="table2">Table 2</xref>. The crystalline size at 26.60 (a.u) is 14.22 nm, where the size of crystalline at 34.98 and 42.52 (a.u) are 6.26 and 3.94 nm respectively. The average crystalline size of NBT is taken as 8.14 nm [<xref ref-type="bibr" rid="scirp.120207-ref28">28</xref>].</p></sec><sec id="s3_3_2"><title>3.4.2. XRD of NBT</title><p>Now the sodium bismuth titanate (NBT) is a piezoelectric material with the help</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Calculation of electrical conductivity by LCR meter</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Temperature</th><th align="center" valign="middle" >Conductivity of NBT</th><th align="center" valign="middle" >Conductivity of 1% rGO</th><th align="center" valign="middle" >Conductivity of 3% rGO</th><th align="center" valign="middle" >Conductivity of 5% rGO</th></tr></thead><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >0.01005</td><td align="center" valign="middle" >0.00221</td><td align="center" valign="middle" >−0.00179</td><td align="center" valign="middle" >−0.00317</td></tr><tr><td align="center" valign="middle" >300</td><td align="center" valign="middle" >0.0116</td><td align="center" valign="middle" >0.00168</td><td align="center" valign="middle" >−0.00180</td><td align="center" valign="middle" >−0.00321</td></tr><tr><td align="center" valign="middle" >400</td><td align="center" valign="middle" >0.0174</td><td align="center" valign="middle" >0.00168</td><td align="center" valign="middle" >−0.00188</td><td align="center" valign="middle" >−0.00311</td></tr><tr><td align="center" valign="middle" >500</td><td align="center" valign="middle" >0.01928</td><td align="center" valign="middle" >0.00168</td><td align="center" valign="middle" >−0.00191</td><td align="center" valign="middle" >−0.00226</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Calculation of crystalline size of rGO by Scherrer’s formula</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Peak position</th><th align="center" valign="middle" >FWHM</th><th align="center" valign="middle" >Crystallite size</th><th align="center" valign="middle" >Average size</th></tr></thead><tr><td align="center" valign="middle" >26.60</td><td align="center" valign="middle" >0.6080</td><td align="center" valign="middle" >14.22</td><td align="center" valign="middle"  rowspan="3"  >8.14 nm</td></tr><tr><td align="center" valign="middle" >34.98</td><td align="center" valign="middle" >1.3937</td><td align="center" valign="middle" >6.26</td></tr><tr><td align="center" valign="middle" >42.52</td><td align="center" valign="middle" >2.267</td><td align="center" valign="middle" >3.94</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Calculation of crystalline size of NBT by Scherrer’s formula</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Peak position</th><th align="center" valign="middle" >FWHW</th><th align="center" valign="middle" >Crystallite size</th><th align="center" valign="middle" >Average Crystallite size</th></tr></thead><tr><td align="center" valign="middle" >32.98</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >41.22 nm</td><td align="center" valign="middle"  rowspan="3"  >31.91 nm</td></tr><tr><td align="center" valign="middle" >47.34</td><td align="center" valign="middle" >0.28</td><td align="center" valign="middle" >32.37 nm</td></tr><tr><td align="center" valign="middle" >58.81</td><td align="center" valign="middle" >0.43</td><td align="center" valign="middle" >22.16 nm</td></tr></tbody></table></table-wrap><p>of XRD results we can analysis the plane and peaks (<xref ref-type="fig" rid="fig6">Figure 6</xref>). The results show three peaks at different positions. The intensity of major peak is 32.98 (a.u) in theses peaks two other peaks are NBT material are 47.34 and 58.81 (a.u) [<xref ref-type="bibr" rid="scirp.120207-ref34">34</xref>].</p><p>The crystalline size of NBT is calculated by the Scherrrer’s formula which is given in <xref ref-type="table" rid="table3">Table 3</xref>. The crystalline size at 32.98 (a.u) is 41.22 nm, where the size of crystalline at 47.34 and 58.81 (a.u) are 32.37 and 22.16 nm respectively. The average crystalline size of NBT is taken as 31.91 nm.</p></sec></sec></sec><sec id="s4"><title>4. Conclusion</title><p>The conclusion of this research work is synthesis graphene oxide by graphite powder by using improved Hummer’s method without using NaNO<sub>3</sub>. Without using NaNO<sub>3</sub> still produce same characteristic of GO. By the help of auto clave GO is thermally reduced to rGO after heating at 160˚C for 6 hours. Taking sodium bismuth titanate powder (NBT) to prepare rGO/NBT composites, now use different weight percentage (1%, 3% &amp; 5%) of rGO in NBT. The composites were synthesis by ball milling and pressing under 3 MPa pressure and sintered at 1075˚C. FTIR results shows that different functional group attached with GO, rGO and composite of different concentration. Optical Microscopy images shows dispersion of rGO in NBT ceramic. With the help of LCR Meter, we measure decrease in electrical conductivity of composites (1%, 3%, 5%) at 200˚C (σNBT = 0.01005, σ 1% = 0.00221, σ 3% = −0.00179, σ 5% = −0.00317). By using XRD results calculate crystalline size of the sample by Scherrer’s formula.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Abbas, Z., Jalil, R., Riaz, I. and Tahir, M. 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