<?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">AMPC</journal-id><journal-title-group><journal-title>Advances in Materials Physics and Chemistry</journal-title></journal-title-group><issn pub-type="epub">2162-531X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ampc.2012.21003</article-id><article-id pub-id-type="publisher-id">AMPC-17893</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> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  TPR Study of Core-Shell Fe@Fe&lt;sub&gt;3&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt; Nanoparticles Supported on Activated Carbon and Carbon Nanotubes
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>gor</surname><given-names>Bychko</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>Yevhen</surname><given-names>Kalishyn</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>Peter</surname><given-names>Strizhak</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>L.V. Pisarzhevsky Institute of Physical Chemistry, The National Academy of Sciences of Ukraine, Kyiv, Ukraine</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>kalishyn.yevhen@gmail.com(YK)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>19</day><month>03</month><year>2012</year></pub-date><volume>02</volume><issue>01</issue><fpage>17</fpage><lpage>22</lpage><history><date date-type="received"><day>January</day>	<month>24,</month>	<year>2012</year></date><date date-type="rev-recd"><day>February</day>	<month>25,</month>	<year>2012</year>	</date><date date-type="accepted"><day>March</day>	<month>4,</month>	<year>2012</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>
 
 
  Core-shell nanoparticles Fe@Fe
  <sub>3</sub>O
  <sub>4</sub> supported on activated carbon (AC) and carbon nanotubes (CNTs) have been studied by H
  <sub>2</sub> temperature-programmed reduction (TPR). Nanoparticles with size of 6.5 nm were synthesized by iron(II) oleate thermal decomposition and were supported on activated carbon and carbon nanotubes by colloid deposition method. The nanoparticles Fe@Fe
  <sub>3</sub>O
  <sub>4</sub> are characterized by TEM and IR. Reduction of nanoparticles on AC starts at 140?C, whereas reduction of nanoparticles on CNTs starts at 200?C. Moreover, gasification of CNTs with methane releasing starts at 450?C, whereas gasification of AC is negligible at temperatures up to 800?C. All these findings illustrate a strong difference in the interaction between nanoparticles and the support material for AC and CNTs.
 
</p></abstract><kwd-group><kwd>Iron; Nanoparticles; Carbon Nanotubes; Temperature-Programmed Reduction</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Iron containing solids are often used as commercially catalysts for various processes, particularly for FischerTropsch synthesis, ammonia synthesis, etc. [1-4]. Performance of these catalysts is affected by numerous factors, one of which is the nature and structure of the support materials. Mostly studies of iron catalysts have been performed with the metal supported on SiO<sub>2</sub>, Al<sub>2</sub>O<sub>3</sub>, MgO, zeolites, and carbon [<xref ref-type="bibr" rid="scirp.17893-ref5">5</xref>]. Particularly, carbon supported iron catalysts give high selectivities to olefins in the Fisher-Tropsh reaction [<xref ref-type="bibr" rid="scirp.17893-ref6">6</xref>].</p><p>Discovery of carbon nanotubes (CNTs), followed by extensive studies of their properties, has also resulted in highlighting their catalytic properties [5,7-12]. Particularly, comparison of the catalytic activity of metal catalysts supported on various oxides, amorphous carbon, and CNTs showed that catalytic performance is generally better for CNTs. For example, a CNT-supported platinum catalyst shows superior activity in catalytic oxidation of various organic compounds [5,10]. CNT-supported metals are active in hydrogen generation from ammonia [<xref ref-type="bibr" rid="scirp.17893-ref13">13</xref>].</p><p>The main advantages of CNT supports compared to activated carbon are the high purity of the material can avoid self-poisoning, specific metal-support interaction exists that can directly affect the catalytic activity and selectivity. Unfortunately, a lack of systematic compareson with activated carbon based catalytic systems has to be noted. Particularly, it was shown that Co/CNT catalyst generates about 99% of the activity for CO conversion at 250˚C and thermally stability that is superior to Co/AC [<xref ref-type="bibr" rid="scirp.17893-ref14">14</xref>]. The effect of CNTs as cobalt support on CO conversion, product selectivity, and olefin to paraffin ratio of Fisher-Tropsh synthesis was studied and compared with AC [<xref ref-type="bibr" rid="scirp.17893-ref15">15</xref>]. The results indicated C<sub>5+</sub> selectivity enhancement was about 77% as compared to Co/AC.</p><p>In this paper a core-shell nanoparticles Fe@Fe<sub>3</sub>O<sub>4</sub> supported on activated carbon (AC) and carbon nanotubes (CNTs) are studied by H<sub>2</sub> temperature-programmed reduction (TPR). Nanoparticles with size of 6.5 nm were synthesized by iron(II) oleate thermal decomposition and were supported on AC and CNTs by colloid deposition method. The core of nanoparticles consists of elementary Fe and shell consists of Fe<sub>2</sub>O<sub>3</sub> and Fe<sub>3</sub>O<sub>4</sub> that follows from TEM and IR studies.</p></sec><sec id="s2"><title>2. Experimental</title><p>All chemicals and solvent were of the highest purity available and were used as purchased without further purification or distillation.</p><sec id="s2_1"><title>2.1. Sample Preparation</title><p>Preparation of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles colloidal solution was performed by a modification of procedure described earlier which is based on iron(II) oleate thermal decomposition [<xref ref-type="bibr" rid="scirp.17893-ref16">16</xref>]. To synthesize Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles, 10 mL of diphenyl ether was heated under Ar atmosphere at 100˚C and appropriate amount of Fe(oleate)<sub>2</sub> was added into solution. After reflux for 2 h, the solution turned black, indicating that Fe nanoparticles were formed. The solution was then cooled to room temperature. Nanoparticles were separated and redispersed in hexane.</p><p>CNTs were synthesized by the catalytic decomposition of ethylene according to procedure described elsewhere [<xref ref-type="bibr" rid="scirp.17893-ref17">17</xref>].</p><p>Deposition of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles on CNTs was performed by mixing appropriate amounts of CNTs and colloidal solution of nanoparticles dispersed in hexane under stirring. The obtained samples were dried in air. The obtained solid Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT was found to contain 1.3% of Fe. Iron content was determined by oxygen titration method [<xref ref-type="bibr" rid="scirp.17893-ref18">18</xref>]. Synthesis of Fe@Fe<sub>3</sub>O<sub>4</sub>/AC and Fe@Fe<sub>3</sub>O<sub>4</sub>/ quartz was performed in a similar way. The obtained samples contained 1.0% of iron.</p><p>Deposition of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles on quartz was performed for studying reduction properties of pure nanoparticles.</p></sec><sec id="s2_2"><title>2.2. Sample Characterization</title><p>The average particle size was determined from transmission electron spectroscopy (TEM) images. TEM studies were carried out using PEM-125K (Selmi, Ukraine). Samples for TEM analisys were prepared by ultrasonic dispersion of catalysts in hexane, and the suspensions were dropped onto carbon-coated copper grid. At least 500 nanoparticles per sample were analyzed to determine their size and distribution.</p><p>The samples were characterized by temperature-programmed reduction (TPR) in flow system using 5% hydrogen/hellium mixture with 5˚C/min temperature ramp with a flow rate 50 mL/min. The samples were first pretreated in a helliun flow up to 350˚C and kept for 2 h to remove the adsorbed water, and then cooling to room temperature. The samples were heated from 100˚C to 800˚C.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref>(a) shows a typical TEM image of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles from a colloid solution. The presented data indicate that the nanoparticles are almost spherical. The average diameter of prepared Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles is 6.5 nm. Corresponding size distribution of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles is presented in <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) showing that size distribution is almost gaussian with standard deviation σ = 0.6 nm. Therefore the synthesized Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles are characterized by narrow size distribution.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>(c) shows the representative electron diffracttion patterns of a sample formed from colloidal solution of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles. Two different types of electron diffraction patterns could be detected depending on the position of the electron beam. The diffraction rings are attributed to iron oxides Fe<sub>3</sub>O<sub>4</sub> and γ-Fe<sub>2</sub>O<sub>3</sub> as well as to bcc-Fe.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>(d) gives IR spectrum of synthesized Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles in the range of 450 - 1000 cm<sup>–</sup><sup>1</sup>. Outside this region peaks near 3400 сm<sup>–</sup><sup>1</sup> and 1650 сm<sup>–</sup><sup>1</sup> are observed. These bands correspond to stretching and deformation vibrations of OH groups. Peaks at 797 and 690 cm<sup>–</sup><sup>1</sup> correspond to deformation vibrations of the Fe-OH bond. Peak at 891 cm<sup>–</sup><sup>1</sup> may be attributed to vibrations of the Fe-O bond for FeO(OH) whereas peaks at 481 and 605 cm<sup>–</sup><sup>1</sup> correspond to vibrations of the Fe-O bond for Fe<sub>2</sub>O<sub>3</sub>. The IR data evidently indicate existence of the surface hydroxyl groups formed by the interaction of iron with water and oxygen.</p><p>TEM, electron diffraction and IR data allows one to conclude that the initially formed iron nanoparticles are partially oxidized due to contact with atmospheric oxygen and water and characterized by core-shell structure. Core of nanoparticle consists of elemental iron. The core is surrounded by iron oxide and the surface hydroxyl groups.</p><p>Figures 2(a) and (b) present TEM images of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles deposited on AC and CNT, correspondingly. Obtained solids are marked as Fe@Fe<sub>3</sub>O<sub>4</sub>/AC and Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT. Distribution of nanoparticles Fe@Fe<sub>3</sub>O<sub>4</sub> over both supports is homogeneous as it follows from the data presented in <xref ref-type="fig" rid="fig2">Figure 2</xref>. For both supports the mean diameter of supported Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles is 6.7 nm with standard deviation σ = 0.6 nm. The size of supported nanoparticles is the same as in colloid solution. Therefore, there are no changes of nanoparticles morphology or chemical composition during their deposition.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> gives the H<sub>2</sub>-TPR curves as solid lines for Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)), Fe@Fe<sub>3</sub>O<sub>4</sub>/AC (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)), and Fe@Fe<sub>3</sub>O<sub>4</sub>/quartz (<xref ref-type="fig" rid="fig3">Figure 3</xref>(c)). For comparison the H<sub>2</sub>-TPR curves of pure CNTs and AC are presented in these figures by dashed lines.</p><p>Reduction of pure CNTs starts at 450˚C. It is characterized by two well-defined peaks which correspond to the gasification of the CNTs [<xref ref-type="bibr" rid="scirp.17893-ref3">3</xref>]. Methane was detected by mass spectrometry as a single product of gasification at temperatures above 550˚C. There are two peaks (at ca. 650˚C and ca. 750˚C) for the H2-TPR profiles for pure CNT. These peaks can be assigned for gasification started as transformation of outer and inner walls of CNT. Reduction of Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT starts at 200˚C. Two small peaks near 300˚C may be attributed to the reduction of two different types of oxygen in the shell of nanoparticle. Methane is detected in products at temperatures above 450˚C. Therefore, in temperature range 200˚C - 450˚C only reduction of iron oxides takes place. At higher temperatures nanoparticles catalyze gasification of CNTs reducing temperature of the methane release to from 550˚C to 450˚C.</p><p>Similar picture is observed for the reduction of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles supported on AC at low temperatures. However, reduction starts at 140˚C. Contrary to CNTs no gasification appears for both AC and Fe@Fe<sub>3</sub>O<sub>4</sub>/AC and no methane formation was found. Therefore, broad peak at temperatures above 400˚C may be attributed to the reduction of the shell of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles.</p><p>H<sub>2</sub>-TPR curves for pure Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles are presented in <xref ref-type="fig" rid="fig3">Figure 3</xref>(c). Reduction of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles starts at 200˚C. It is characterized by four welldefined peaks at 250˚C, 400˚C, 550˚C, and 700˚C. First three peaks correspond to the stepwise reduction of iron oxides as: Fe<sub>2</sub>O<sub>3</sub> → Fe<sub>3</sub>O<sub>4</sub> → FeO → Fe [19,20]. The Fe<sub>2</sub>O<sub>3</sub> → Fe<sub>3</sub>O<sub>4</sub> peak at 250˚C demonstrates that γ-Fe<sub>2</sub>O<sub>3</sub> exists in the nanoparticles shell. However, relatively low intensity of the Fe<sub>2</sub>O<sub>3</sub> → Fe<sub>3</sub>O<sub>4</sub> peak suggests the low fraction of Fe<sub>2</sub>O<sub>3</sub> in the nanoparticles shell. Next reduction step Fe<sub>3</sub>O<sub>4</sub> → FeO is observed at 400˚C. Peak at 550˚C may be considered for conversion of the iron oxide into metallic iron. The last peak is observed at 700˚C. It may be associated with reduction of Fe carbide [<xref ref-type="bibr" rid="scirp.17893-ref21">21</xref>]. Fe carbide is formed during the interaction between iron nanoparticles and organic surfactants that stabilize nanoparticles in colloidal solution.</p><p>The H<sub>2</sub>-TPR curves for pure CNT and AC supports are totally different. Such difference of reduction properties of these supports is expected and agreed with literature data [4,22,23]. It was found that CH<sub>4</sub> production is not observed in the temperature until 1000˚C for activated carbon [<xref ref-type="bibr" rid="scirp.17893-ref22">22</xref>]. Contrary, methane production was detected for CNT gasification [4,23]. This difference is associated with chemical structure and properties of AC and CNT.</p><p>Comparison of reduction properties of Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT and pure Fe@Fe<sub>3</sub>O<sub>4</sub> shows similarity of reduction Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles. Reduction of Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT gives three small peaks on the H<sub>2</sub>-TPR curves (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)). Temperature of reduction of Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT corresponds to the pure nanoparticles. Therefore, in temperature range 200˚C - 450˚C only reduction of iron oxides takes place. At higher temperatures the reduction of supported nanoparticles and gasification of CNTs appears simultaneously.</p><p>Reduction properties of Fe@Fe<sub>3</sub>O<sub>4</sub>/AC and pure Fe@Fe<sub>3</sub>O<sub>4</sub> are significantly differed. Reduction of Fe@Fe<sub>3</sub>O<sub>4</sub>/AC starts at 140˚C and one well-defined peak is observed at 400˚C. It indicates that total reduction of Fe@Fe<sub>3</sub>O<sub>4</sub>/AC occurs in one stage and may be attributed to the reduction of the shell of Fe@Fe<sub>3</sub>O<sub>4</sub> nanoparticles.</p><p>Comparison of reduction properties of Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT and Fe@Fe<sub>3</sub>O<sub>4</sub>/AC indicates a huge difference in an interaction between nanoparticles and support. No gasification appears for Fe@Fe<sub>3</sub>O<sub>4</sub>/AC whereas nanoparticles catalyze reduction of CNTs for Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT. As a result, H<sub>2</sub>-TPR curve at temperatures above 400˚C for Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT is caused by a superposition of both CNTs gasification with methane formation and reduction of the nanoparticles shell. Reduction of nanoparticles shell starts at lower temperatures for AC. Differences in gasification and shell reduction suggest strong interaction between nanoparticles and support for CNTs. Possibly, it is associated with existence of semiconducting zones in CNTs resulting in a formation of Schottky barrier between CNT and nanoparticle.</p><p>Strong interaction between nanoparticles and support for CNTs could be associated with particularities of CNT structure. Tubular morphology of the graphene layers governs difference in properties of CNT and other carbonaceous supports. Exterior surface of the CNT is electron-rich, whereas the interior surface is electron-deficient. That could influence metal and metal oxide particles in contact with CNT surface [24,25]. Interaction between electronic structure of CNT and metal or metal oxide nanoparticles may drastically change properties of these nanoparticles. As a result, that enhances reduction of nanoparticles supported on CNT. Moreover it was found that metal particles supported on CNT are more catalytically active in gasification process comparing with other carbonaceous supports [<xref ref-type="bibr" rid="scirp.17893-ref25">25</xref>].</p></sec><sec id="s4"><title>4. Conclusions</title><p>In this study, nanoparticles with size of 6.5 nm were synthesized by iron(II) oleate thermal decomposition and were deposited on AC and CNTs by colloid deposition method. No agglomeration of nanoparticles on these supports was observed. TEM, electron diffraction and IR data allows one to conclude that the initially formed iron nanoparticles are partially oxidized due to contact with atmospheric oxygen and water and characterized by coreshell structure.</p><p>H<sub>2</sub>-TPR study of obtained solids has shown a difference of reduction properties for Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT and Fe@Fe<sub>3</sub>O<sub>4</sub>/AC. Reduction of shell for Fe@Fe<sub>3</sub>O<sub>4</sub>/AC starts at 140˚C and no gasification of AC occurs at temperatures up to 800˚C. Contrary, for Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT the reduction starts at 200˚C and gasification appears with methane formation. The difference in H<sub>2</sub>-TPR behavior for Fe@Fe<sub>3</sub>O<sub>4</sub>/CNT and Fe@Fe<sub>3</sub>O<sub>4</sub>/AC may indicate a possible difference in catalytic performance of these solids in various heterogeneous catalytic processes.</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>The work is supported by the grants of the National Academy of Sciences of Ukraine and the Ministry of Education and Science of Ukraine. Authors are thankful to A. I. 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