<?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.2016.54015</article-id><article-id pub-id-type="publisher-id">Graphene-71591</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>
 
 
  Vanadium Oxide/Graphene Nanoplatelet as a Cathode Material for Mg-Ion Battery
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>E.</surname><given-names>Sheha</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>M.</surname><given-names>H. Makled</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>Walaa</surname><given-names>M. Nouman</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>A.</surname><given-names>Bassyouni</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>S.</surname><given-names>Yaghmour</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>S.</surname><given-names>Abo-Elhassan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Physics Department, Faculty of Science, Benha University, Benha, Egypt</addr-line></aff><aff id="aff2"><addr-line>Physics Department, Faculty of Science, University of Jeddah Branch, Jeddah, KSA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>islam.shihah@fsc.bu.edu.eg(ES)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>21</day><month>09</month><year>2016</year></pub-date><volume>05</volume><issue>04</issue><fpage>178</fpage><lpage>188</lpage><history><date date-type="received"><day>September</day>	<month>16,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>October</month>	<year>25,</year>	</date><date date-type="accepted"><day>October</day>	<month>28,</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>
 
 
  The aim of the present work is to introduce a high performance cathode for magnesium-ion batteries. A simple ball mill process is employed to synthesize (V
  <sub>2</sub>O
  <sub>5</sub>)
  <sub>1-x</sub> (Graphene Nanoplatelets (GNP))
  <sub>x</sub> nanocomposite, (where x = 0, 5, 10, 15, 20 and 25 wt.% GNP). The synthesized samples are characterized using scanning electron microscope (SEM), X-ray diffraction (XRD) technique, impedance spectroscopy, cyclic voltammetry and charge-discharge test. The maximum conductivity of the investigated samples was found to be 6 &#215; 10
  <sup>-1</sup> S/cm for optimum composite film (25 wt% GNP) at room temperature. Room temperature rechargeable magnesium batteries are constructed from Mg as anode material, (V
  <sub>2</sub>O
  <sub>5</sub>)
  <sub>1-x</sub>(GNP)
  <sub>x</sub> as a cathode material and the simple non-aqueous electrolyte based MgNO
  <sub>3</sub>&#183;6H
  <sub>2</sub>O. Mg/V
  <sub>2</sub>O
  <sub>5</sub> cells employing as-prepared electrolyte exhibit initial discharge capacity ~100 mAhg
  <sup>-1</sup> while Mg/(V
  <sub>2</sub>O
  <sub>5</sub>/GNP (x = 25t.%)) cathode produces a lower initial capacity of ~90 mAhg
  <sup>-1</sup>. The high initial discharge capacity of V
  <sub>2</sub>O
  <sub>5</sub> can be attributed to the presence of a large (001) interlayer spacing (～11.53 A) for facile Mg
  <sup>+</sup> insertion/extraction.
 
</p></abstract><kwd-group><kwd>Magnesium Batteries</kwd><kwd> Vanadium Oxide</kwd><kwd> Graphene</kwd><kwd> Conductivity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Costly Cheveral phase Mo<sub>6</sub>S<sub>8</sub> cathode, and complicated electrolyte based Mg [ALCL<sub>2</sub>BuET]<sub>2</sub>/tetrahydofurane (volatile) are traditional materials in early rechargeable magnesium batteries, although, these batteries suffer from low voltage, low energy density, kinetic sluggish of Mg<sup>+2</sup> insertion/extraction [<xref ref-type="bibr" rid="scirp.71591-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.71591-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.71591-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.71591-ref4">4</xref>] . Various cathode materials for magnesium battery have been suggested in recent years, such as TiS<sub>2</sub> nanotubes [<xref ref-type="bibr" rid="scirp.71591-ref5">5</xref>] , MoS<sub>2</sub> [<xref ref-type="bibr" rid="scirp.71591-ref6">6</xref>] , GeO<sub>2</sub> [<xref ref-type="bibr" rid="scirp.71591-ref7">7</xref>] , TiS<sub>3</sub> [<xref ref-type="bibr" rid="scirp.71591-ref1">1</xref>] , V<sub>2</sub>O<sub>5</sub> [<xref ref-type="bibr" rid="scirp.71591-ref8">8</xref>] and MnO<sub>2</sub> [<xref ref-type="bibr" rid="scirp.71591-ref9">9</xref>] . Vanadium pentaoxide (V<sub>2</sub>O<sub>5</sub>) is a semiconductor material (E<sub>g</sub> = 2.4 eV), where tuning of fermi level due to ion insertion is expected. The intercalation reaction of Mg in V<sub>2</sub>O<sub>5</sub> can be written as follows: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-2690091x2.png" xlink:type="simple"/></inline-formula>During this reaction the vanadium atoms are partially reduced from a V<sup>5+</sup> to a V<sup>+4</sup> formal oxidation state [<xref ref-type="bibr" rid="scirp.71591-ref10">10</xref>] . V<sub>2</sub>O<sub>5</sub> is belonging to the layered transition metal oxides which possess the ability to structural deformations during the insertion of Mg<sup>+2</sup> or other bivalent ions. The superior electrochemical performances of V<sub>2</sub>O<sub>5</sub> could be ascribed to the unique structure revealing the presence of a large (001) crystal planes interlayer spacing (~11.53 &#197;), which provide large interlayer spacing for facile ion insertion/extraction [<xref ref-type="bibr" rid="scirp.71591-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.71591-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.71591-ref13">13</xref>] . V<sub>2</sub>O<sub>5</sub> has been studied very intensively as a cathode material for Li-ion batteries [<xref ref-type="bibr" rid="scirp.71591-ref14">14</xref>] . Because the ionic radii of Li<sup>+</sup> and Mg<sup>2+</sup> are comparable in magnitude, 68 and 65 pm, respectively, the replacement of Li<sup>+</sup> ions by Mg<sup>2+</sup> ions in insertion compounds is possible. On the other hand, although the electrochemical performance of V<sub>2</sub>O<sub>5</sub> has shown great improvement, it suffers from its poor electronic conductivity, which may lead to both of poor capacity and the cyclic ability of V<sub>2</sub>O<sub>5</sub> electrodes. Graphene nanoplatelets represent a new class of carbon nanoparticles with multifunctional properties. Graphene nanoplatelet addition can provide barrier properties, while their pure graphitic composition makes them excellent electrical [<xref ref-type="bibr" rid="scirp.71591-ref15">15</xref>] and thermal conductors and can prevent the vanadium dissolution, and alleviate the aggregation of the particles. Since graphene, the name given to a flat monolayer of carbon atoms tightly packed into a two-dimensional (2D) honeycomb lattice, exhibits superior electrical conductivities, high surface areas and chemical tolerance intrigue, many researchers have studied the V<sub>2</sub>O<sub>5</sub>/graphene cathode [<xref ref-type="bibr" rid="scirp.71591-ref16">16</xref>] using different preparation methods to control particle size and particle shape, aiming to improve the efficiency of rechargeable batteries. In the present work we will introduce a new rechargeable magnesium battery from electrolyte system based on reaction products of MgNO<sub>3</sub>∙<sub>6</sub>H<sub>2</sub>O, succinonitril, tetraethylene glycol dimethyl ether solvent, and ((V<sub>2</sub>O<sub>5</sub>)<sub>0.75</sub>/GNP<sub>0.25</sub>) nanocomposite cathode. One of our important goals is to reduce the cost of the battery. So the starting materials will be from market and the ball mill process is the desirable one.</p></sec><sec id="s2"><title>2. Experimental</title><p>Graphene Nanoplatelets Grade M GNP was characterized by average (7 nm thickness, 10 nm particle diameter, 10<sup>7</sup> S/m Electrical conductivity and surface area ~120 - 150 m<sup>2</sup>/g) have been imported from XG Science company. Composites of V<sub>2</sub>O<sub>5</sub> and GNP were prepared by ball milling process under 4 hours’ time duration. The resulted product is designated here as (V<sub>2</sub>O<sub>5</sub>)<sub>1−x(</sub>GNP)<sub>x</sub> composites. The morphology of the nanocompsite was examined using SEM (JOEL-JSM Model 5600). The XRD patterns of the films were taken using Rigaku diffractometer type RINT-Ultima IV/S. The diffraction system based with Cu tube anode with voltage 40 KV and current 40 mA. The current?voltage characteristics of the cathodes were carried out by means of a computer controlled 2400 Keithley electrometer. For electrochemical performance testing, working electrodes (V<sub>2</sub>O<sub>5</sub> and V<sub>2</sub>O<sub>5</sub>-graphene composite powder) were prepared by mixing 85 wt.% sample as the active material, 6 wt.% conductive agent (carbon black, Super-P-Li), and 9 wt.% poly-vinylidene difluoride (PVDF) binder, N-methylpyrrolidone (Alfa) was then added to produce a viscous slurry and the resultant slurry was pasted onto copper foil. The as-prepared working electrodes were then dried in a vacuum oven at 373 K for 2 h. Electrochemical cells (CR2032 coin type) were assembled in room temperature and ambient pressure by using the working electrode, a separator (filter paper), Mg ribbon as the reference and counter electrode, and 4 gm MgNO<sub>3</sub>∙6H<sub>2</sub>O in a 2:10 (w:v) mixture of succinonitril, tetraethylene glycol dimethyl ether, respectively, as the electrolyte. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the structure scheme of MgNO<sub>3</sub>.<sub>6</sub>H<sub>2</sub>O, succinonitril and tetraethylene glycol dimethyl ether. Where MgNO<sub>3</sub>.<sub>6</sub>H<sub>2</sub>O is the Mg<sup>+2</sup> pump, tetraethylene glycol dimethyl ether is a solvent and succinonitril is a plasticizer agent to dissociate ions and improve ionic conductivity. Cyclic voltammograms (CVs) were conducted in three-electrode cell using an electrochemical instrument of CHI604E Electrochemical Workstation. The cells were charged and discharged on a multi-channel battery test system (NEWARE BTS-TC35) over the voltage range of 0 - 1.6 V versus Mg/Mg<sup>+2</sup> at constant constant current density ~40 μAcm<sup>−1</sup>.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>Figures 2(a)-(c) shows SEM images for V<sub>2</sub>O<sub>5</sub> and V<sub>2</sub>O<sub>5</sub>/GNP nanocomposites. The graphene nanoplatlets are crumpled to a curly and wavy shape. By adding GNP nanoplatlets to V<sub>2</sub>O<sub>5</sub>, the later was found to be uniformly distributed in GNP and well distributed on the 2D graphene nanoplatelets, as shown in Figures 2(a)-(c). Moreover, the graphene sheets can prevent the aggregation of V<sub>2</sub>O<sub>5</sub> particles to a certain extent, which can be of great benefit to electrochemical reactions. The XRD patterns of the synthesized (V<sub>2</sub>O<sub>5</sub>)<sub>1−x(</sub>GNP)<sub>x</sub> composites (where x = 0, 5, 10, 15, 20 and 25 %wt GNP) are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The XRD spectrum for x = 0% indicates that the V<sub>2</sub>O<sub>5</sub> composites</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Schematic illustrates the electrolyte structure</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2690091x3.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> SEM micrographs of (V<sub>2</sub>O<sub>5</sub>)<sub>1−x</sub>(GNP)<sub>x</sub> composites: (a) 0 wt% GNP; (b) 15 wt% GNP; (c) 25 wt% GNP</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2690091x4.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> XRD pattern of (V<sub>2</sub>O<sub>5</sub>)<sub>1−x(</sub>GNP)<sub>x</sub> composites</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2690091x5.png"/></fig><p>are highly crystallized in structure and the entire diffraction peaks match well with Bragg reflections of the pure orthorhombic phase of V<sub>2</sub>O<sub>5</sub> nanoparticles, which is consistent with the standard JCPDS No.41-1426 (space group Pmmn) [<xref ref-type="bibr" rid="scirp.71591-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.71591-ref18">18</xref>] . However, for x &gt; 0% an additional diffraction shoulder peak around 26.77˚, partially overlapping with the V<sub>2</sub>O<sub>5</sub> (110) peak (2θ = 26.39˚), originates from the (002) diffraction of the graphite. The intensity of the later peak increases linearly when x increases from 5 to 25% and its position corresponds to ~ 31 nm (according to the relation: λ/(2∙sinθ, θ = 26.39˚) spacing between atomic planes [<xref ref-type="bibr" rid="scirp.71591-ref19">19</xref>] . Also, the XRD spectra show a weak peak at 54.8˚ which corresponds to the (004) reflection of the graphite. It can be noticed that the graphite (002) peak position shifts to the lower angles for x = 5% and to higher angles for x = 10%. This can be related to the amount of oxygen functional groups formed between the platelets of the graphite. From the XRD measurements, no additional phases related to structural defects can be detected, while orthorhombic V<sub>2</sub>O<sub>5</sub> can be detected after ball milling of V<sub>2</sub>O<sub>5</sub> and GNP. Small shift in peak positions of V<sub>2</sub>O<sub>5</sub> after doping by GNP was observed which confirm change in (001) interlayer spacing. The crystallite size (τ) of the investigated samples (V<sub>2</sub>O<sub>5</sub>)<sub>1−x(</sub>GNP)<sub>x</sub> nano-composites (where x = 0, 5, 10, 15, 20 and 25 %wt GNP) can be calculated using the first sphere approximation of Debye-Scherrer formula [<xref ref-type="bibr" rid="scirp.71591-ref20">20</xref>] τ = K l/βcosθ, where K is the shape factor, λ is the X-ray wavelength, β is the line broadening at half the maximum intensity in radians, and θ is the Bragg angle. Using this formula, crystallite dimensions of about 30 nm could be calculated from the high intense peaks. <xref ref-type="fig" rid="fig4">Figure 4</xref>(a), shows the current voltage (I&amp;V) characteristics of (V<sub>2</sub>O<sub>5</sub>)<sub>1−x(</sub>GNP)<sub>x</sub> nano-composite. Generally, the current increases linearly with increasing voltage obeying Ohm law. The dc conductivity</p><p>was calculated using the equation: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-2690091x6.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.71591-ref21">21</xref>] , where t is the thickness of the</p><p>sample and A is the surface area of the sample. The value of the resistivity R was measured from the slopes of the straight lines in ohmic region I α V <xref ref-type="fig" rid="fig4">Figure 4</xref>(a), The effect of graphene content on the dc conductivity σ<sub>dc</sub> of (V<sub>2</sub>O<sub>5</sub>)<sub>1−x</sub>(GNP)<sub>x</sub> is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b). The dc conductivity of the composites exhibits insulator behavior for pure V<sub>2</sub>O<sub>5</sub> recording ~10 &#215; 10<sup>−6</sup> S/m, whereas semiconductor behavior for low graphene content up to x = 10 wt% was recorded. The electrical conductivity increased as the content of graphene was close to percolation threshold up to x = 5 wt%. Above the percolation threshold σ<sub>dc</sub> was found to increases exponentially before it reach to the saturated point (x = 10 wt%) which may be attributed to the formation of filler network and the composites may reach to the metallic behavior. This behavior can be described according to the percolation theory as the following power relation [<xref ref-type="bibr" rid="scirp.71591-ref22">22</xref>] ,</p><disp-formula id="scirp.71591-formula473"><graphic  xlink:href="http://html.scirp.org/file/3-2690091x7.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-2690091x8.png" xlink:type="simple"/></inline-formula> is the conductivity of conducting component, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-2690091x9.png" xlink:type="simple"/></inline-formula>is the volume fraction of Graphene, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-2690091x10.png" xlink:type="simple"/></inline-formula>is the critical volume fraction or percolation threshold, and the exponent t reflects the dimensionality of the system and has been calculated to be either 1.3 or 2.0 corresponding to two or three dimensions, respectively [<xref ref-type="bibr" rid="scirp.71591-ref23">23</xref>] . <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) (inset) shows a fitting of percolation equation for (V<sub>2</sub>O<sub>5</sub>)<sub>1−x(</sub>GNP)<sub>x</sub> composites. The exponent t was found to be about 1.4. This result confirms that the GNP nanoparticles are not located on the surface of the host material matrix particles, but it coordinated in the V<sub>2</sub>O<sub>5</sub> crystal structure and the formation of graphene three dimensional network will enhancement.</p><p>Cyclic voltammetry and discharge curve</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref>(a) shows the schematic of the cell configuration of the Mg<sup>−</sup> V<sub>2</sub>O<sub>5</sub> cells in this study. The activity of V<sub>2</sub>O<sub>5</sub> and V<sub>2</sub>O<sub>5</sub>-graphene nanocomposite for hosting Mg<sup>+2</sup> ions was evaluated using cyclic voltammetry (CV) and galvanostatic discharge-charge techniques. <xref ref-type="fig" rid="fig5">Figure 5</xref>(b), shows the CV results obtained from 2.5 to 0 V using V<sub>2</sub>O<sub>5</sub> and V<sub>2</sub>O<sub>5</sub>-graphene nanocomposite as a working electrode in a three-electrode cell employing magnesium metal as the counter and reference electrode at a scan rate of 0.05 mV s<sup>−1</sup>. Although GNP succeeded to increase conductivity of V<sub>2</sub>O<sub>5</sub>, it failed to increase</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> (a) I-V curves of (V<sub>2</sub>O<sub>5</sub>)<sub>x</sub>/(GNP)<sub>1−x</sub> composites; (b) Variation of dc conductivity of (V<sub>2</sub>O<sub>5</sub>)<sub>x</sub>/(GNP)<sub>1−x</sub> composites at different grapheme concentration</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2690091x11.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> (a) Schematic illustrates Mg<sup>+2</sup> insertion/extraction within V<sub>2</sub>O<sub>5</sub>; (b) Comparison of the CV curves (at 5 mV∙s<sup>−1</sup>) for V<sub>2</sub>O<sub>5</sub> and V<sub>2</sub>O<sub>5</sub>/graphene nano-composite</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2690091x12.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Discharge-charge profiles of (a) V<sub>2</sub>O<sub>5</sub> (b) V<sub>2</sub>O<sub>5</sub>/graphene nano-composite cathodic materials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2690091x13.png"/></fig><p>the cathodic and anodic current density. This can be attributed to that the introduction of GNP in V<sub>2</sub>O<sub>5</sub> using ball mill technique can perturb the (001) interlayer spacing of V<sub>2</sub>O<sub>5</sub> and may be reduce intercalation rate. The perturbation in the interlayer spacing probably decreases the probability of Mg<sup>+2 insertion/extraction between interlayer spacing and hence decrease the specific capacity as we will see</sup>.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref>(a) &amp; <xref ref-type="fig" rid="fig6">Figure 6</xref>(b) show discharge/charge profiles of Mg/V<sub>2</sub>O<sub>5</sub> and Mg/(V<sub>2</sub>O<sub>5</sub>/GNP) coin cells, in which current density was fixed at =40 μAcm<sup>−1</sup> and the cells were discharged to 0 V and charged to 1.6 V. The initial discharge capacity of Mg/ V<sub>2</sub>O<sub>5</sub> and Mg/(V<sub>2</sub>O<sub>5</sub>/GNP) coin cells are approximately 100 and 90 mAhg<sup>−1</sup>, respectively. The combination of V<sub>2</sub>O<sub>5</sub> with GNP decrease the discharge capacity compared to pure V<sub>2</sub>O<sub>5</sub>. We could not obtain more than 2 and 4 cycles for pure and graphitized V<sub>2</sub>O<sub>5</sub>, respectively. We think the structure property of V<sub>2</sub>O<sub>5</sub> which give the advantage (001 large interlayer spacing (∼11.53 &#197;)) of facile Mg<sup>+</sup> insertion/extraction was deformed after initial cycling. The intercalation of Mg<sup>+2</sup> may perturb the bonding scheme of V<sub>2</sub>O<sub>5</sub> and losses it this property.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In summary, V<sub>2</sub>O<sub>5</sub>/GNP cathode was synthesized by a ball mill method. The integration of V<sub>2</sub>O<sub>5</sub> and graphene nanoparticles enhanced the electrical performances. This improved performance could be attributed to the formation of framework nanoscale electrode of 2D graphene decorated with well-dispersed V<sub>2</sub>O<sub>5</sub> nanoparticle. Although GNP perturbed the (001) interlayer spacing hence, it failed to enhance the electrochemical performance. As-prepared V<sub>2</sub>O<sub>5</sub> and V<sub>2</sub>O<sub>5</sub>/GNP cathodes can deliver a high capacity of 100 and 90 mAh∙g<sup>−1</sup> respectively, which provides a new direction to explore cathode materials for rechargeable Mg batteries. Further extensive investigations are required, however, to raise the performance of the magnesium-based rechargeable cells to practical levels.</p></sec><sec id="s5"><title>Cite this paper</title><p>Sheha, E., Makled, M.H., Nouman, W.M., Bassyouni, A., Yaghmour, S. and Abo-Elhassan, S. (2016) Vanadium Oxide/Graphene Nanoplatelet as a Cathode Material for Mg-Ion Battery. 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