<?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">EPE</journal-id><journal-title-group><journal-title>Energy and Power Engineering</journal-title></journal-title-group><issn pub-type="epub">1949-243X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/epe.2015.79039</article-id><article-id pub-id-type="publisher-id">EPE-59063</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Hydrogen Separation Using Pt-Alumina Impregnated Membrane
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ohammed</surname><given-names>N. Kajama</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>Ngozi</surname><given-names>C. Nwogu</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>Edidiong</surname><given-names>O. Okon</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>Habiba</surname><given-names>Shehu</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>Ify</surname><given-names>Orakwe</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>Edward</surname><given-names>Gobina</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Centre for Process Integration and Membrane Technology, (CPIMT), School of Engineering, The Robert Gordon
University, Aberdeen, UK</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>e.gobina@rgu.ac.uk(EG)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>20</day><month>08</month><year>2015</year></pub-date><volume>07</volume><issue>09</issue><fpage>412</fpage><lpage>417</lpage><history><date date-type="received"><day>18</day>	<month>June</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>22</month>	<year>August</year>	</date><date date-type="accepted"><day>25</day>	<month>August</month>	<year>2015</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>
 
 
  A tubular commercial mesoporous support was used to prepare a Pt impregnated membrane using the reservoir method and tested for moderate temperature (300
  &#176;
  C) gas transport of hydrogen (H
  <sub>2</sub>
  ), helium (He) and nitrogen (N
  <sub>2</sub>
  ) gas molecules. H
  <sub>2</sub>
   and N
  <sub>2</sub>
   gas permeation of 6.1 and 4.5 l/min at 1.0 barg feed pressure and 25&#176;C respectively was obtained from the support. On the other hand, H
  <sub>2</sub>
   and N
  <sub>2</sub>
   gas permeation of 4.6 and 1.7 l/min at 1.0 barg feed pressure and 25&amp;deg;C respectively was also obtained from the Pt membrane. Selectivity of H
  <sub>2</sub>
   over He of 1.96 at 300&#176;C and 1.6 barg for the Pt membrane was obtained and found to be higher than that of the theoretical Knudsen selectivity. Also, a selectivity of H
  <sub>2</sub>
   over N
  <sub>2</sub>
   of 2.72 at 25&#176;C and 1.0 barg was obtained and found to be close to that of the theoretical Knudsen selectivity. The gas permeation and the selectivity performance of the membrane were evaluated.
 
</p></abstract><kwd-group><kwd>Tubular Support</kwd><kwd> Pt Membrane</kwd><kwd> Hydrogen Selectivity</kwd><kwd> Permeation Temperature</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Hydrogen is extensively used in the chemical, oil refining, petro-chemical and steel industries and is also projected as the clean alternative source of energy [<xref ref-type="bibr" rid="scirp.59063-ref1">1</xref>] . Almost 50% of the world’s hydrogen is produced from fossil fuels, such as natural gas and naphtha through steam reforming reaction [<xref ref-type="bibr" rid="scirp.59063-ref1">1</xref>] . Literature shows that hydrogen can actually be separated using inorganic membranes [<xref ref-type="bibr" rid="scirp.59063-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.59063-ref4">4</xref>] . Inorganic membranes derived from ceramics and metal alloys are candidates for high temperature gas separation. Palladium (Pd) [<xref ref-type="bibr" rid="scirp.59063-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.59063-ref5">5</xref>] and platinum (Pt) [<xref ref-type="bibr" rid="scirp.59063-ref5">5</xref>] alloys and metals are the ideal membranes applied for high purity hydrogen production from mixed gas streams even though these metals and their alloys are expensive. Pd-based membranes are attractive for membrane reactor applications because Pd is highly permeable to hydrogen and offer better thermal stability and selectivity than polymer and microporous membranes [<xref ref-type="bibr" rid="scirp.59063-ref5">5</xref>] . Transport of hydrogen through dense Pd membranes follows the solution diffusion mechanism where only hydrogen is transported resulting in high hydrogen purity (99.9999%), but have been limited in commercialization due to issues which include support quality, surface poisoning due to carbon species, hydride formation, and irreversible damage caused by bulk sulfide formation [<xref ref-type="bibr" rid="scirp.59063-ref5">5</xref>] -[<xref ref-type="bibr" rid="scirp.59063-ref7">7</xref>] .</p><p>The main characteristics of inorganic membranes are permeance and separation factor [<xref ref-type="bibr" rid="scirp.59063-ref8">8</xref>] . Permeance is a measure of the gas flow rate per unit area per unit pressure difference. Permeance is a more practical unit than permeability because the thickness of the membrane is not usually known very accurately [<xref ref-type="bibr" rid="scirp.59063-ref8">8</xref>] . Permeability is the permeance multiplied by the thickness of the membrane, and the selectivity is the ratio of the permeances.</p><p>The transport of gases through membranes is highly dependent on the pore diameter. Gas transport can also be affected by pressure and temperature. A change in temperature can affect the flow regime differently at different pore diameters. Hence, it is critically important to be able to follow the changes in the transport mechanisms of different gases during pore diameter reduction to help determine the extent to which pores have been modified [<xref ref-type="bibr" rid="scirp.59063-ref8">8</xref>] .</p><p>Here, we examine the behaviour of gas permeation on a tubular commercial support and a Pt-alumina membrane, and their corresponding selectivity at different pressures and temperatures.</p></sec><sec id="s2"><title>2. Experimental</title><p>Commercially available tubular alumina support was used. The support was a mesoporous (2 - 50 nm). The support consisted of 7 and 10 mm internal and outer diameter respectively. The support possesses a permeable length of 348 mm and a porosity of 45%. Scanning electron microscopy (Zeiss EVO LS10) image (not shown) and the energy diffraction X-ray analysis (EDAX) of the Pt membrane was obtained.</p><p>The Pt membrane was prepared using the following procedure. A solution of hexachloroplatinic acid (H<sub>2</sub>PtCl<sub>6</sub>) was used as platinum precursor. The tubular support was first dried at 65˚C. After weighing, it was dipped for 2 hours in pure water before H<sub>2</sub>PtCl<sub>6</sub> introduction. The deposition method used was based on evaporation-crystal- lisation steps using the method proposed by Uzio et al. [<xref ref-type="bibr" rid="scirp.59063-ref9">9</xref>] . The tube was first dipped for 2 hours in pure water (in our case we used deionised water) afterwards the tube was dipped for 10 hours in a 10 g/l of H<sub>2</sub>PtCl<sub>6</sub> solution. The sample was then dried at room temperature to favour evaporation from the inner side and deposition in the top layer.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> depicts the EDAX analysis of the Pt membrane. The compositional result is also shown in <xref ref-type="table" rid="table1">Table 1</xref>. After Pt impregnation, it can be seen in <xref ref-type="table" rid="table1">Table 1</xref> that a 3.52 wt% Pt is obtained.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> depicts the single gas permeation of H<sub>2</sub>, He and N<sub>2</sub> for the support. The permeation of molecules</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> EDAX analysis of the Pt membrane</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Element</th><th align="center" valign="middle" >Weight (%)</th><th align="center" valign="middle" >Atomic (%)</th></tr></thead><tr><td align="center" valign="middle" >CaCO<sub>3</sub> (C K)</td><td align="center" valign="middle" >14.41</td><td align="center" valign="middle" >19.64</td></tr><tr><td align="center" valign="middle" >SiO<sub>2</sub> (O K)</td><td align="center" valign="middle" >50.68</td><td align="center" valign="middle" >51.88</td></tr><tr><td align="center" valign="middle" >Al<sub>2</sub>O<sub>3</sub> (Al K)</td><td align="center" valign="middle" >38.52</td><td align="center" valign="middle" >23.38</td></tr><tr><td align="center" valign="middle" >SiO<sub>2</sub> (Si K)</td><td align="center" valign="middle" >0.28</td><td align="center" valign="middle" >0.16</td></tr><tr><td align="center" valign="middle" >KCl (Cl)</td><td align="center" valign="middle" >3.28</td><td align="center" valign="middle" >1.51</td></tr><tr><td align="center" valign="middle" >Wollastonite (Ca K)</td><td align="center" valign="middle" >0.32</td><td align="center" valign="middle" >0.13</td></tr><tr><td align="center" valign="middle" >Titanium (Ti K)</td><td align="center" valign="middle" >7.94</td><td align="center" valign="middle" >2.72</td></tr><tr><td align="center" valign="middle" >Zirconium (Zr L)</td><td align="center" valign="middle" >1.61</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >Platinum (Pt M)</td><td align="center" valign="middle" >3.52</td><td align="center" valign="middle" >0.30</td></tr><tr><td align="center" valign="middle" >Total</td><td align="center" valign="middle" >120.56</td><td align="center" valign="middle" >100.02</td></tr></tbody></table></table-wrap><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> EDAX of the Pt membrane showing the outer surface</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6201845x5.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Gas permeation and mean pressure relationship at 25˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6201845x6.png"/></fig><p>with the smaller molecular weight such as H<sub>2</sub> = 2 g/mol and He = 4 g/mol diffuses faster with pressure whilst the larger molecular weight N<sub>2</sub> = 28 g/mol had low permeation. These results are indicative of Knudsen diffusion transport mechanism which states that the permeation flux is directly proportional to the inverse square root of the molecular weights of gases.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> depicts the permeation H<sub>2</sub> on the support and Pt membrane against feed pressure between 0.1 up to 1.0 barg. The results show a higher H<sub>2</sub> permeation with respect to the support.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> depicts the effect of temperature and permeation of H<sub>2</sub>, He and N<sub>2</sub> on the support at temperatures between 25˚C up to 300˚C and 1.5 barg feed pressure. The permeation of molecules with smaller molecular weight such as H<sub>2</sub> and He increase with temperature whilst the flux of larger molecule like N<sub>2</sub> is independent of temperature. These results are indicative of Knudsen diffusion transport mechanism. Gopalakrishnan and Diniz da Costa [<xref ref-type="bibr" rid="scirp.59063-ref10">10</xref>] also observed a higher permeation rate for He and H<sub>2</sub> at temperatures between 100˚C up to 400˚C on silica membrane.</p><p>The effect of temperature on H<sub>2</sub>/He single gas selectivity with temperatures between 25˚C up to 300˚C and 1.6 barg feed pressure on Pt membrane is depicted in <xref ref-type="fig" rid="fig5">Figure 5</xref>. H<sub>2</sub> selectivity of 1.96 over helium was obtained at 300˚C which is 2 fold to the theoretical knudsen selectivity. Also, an improvement of H<sub>2</sub> selectivity is achieved as the temperature increased from 25˚C to 300˚C. <xref ref-type="fig" rid="fig6">Figure 6</xref> depicts H<sub>2</sub>/N<sub>2</sub> selectivity and feed pressure relationship on the support and Pt membrane at 25˚C. It can be seen clearly that a selectivity of 1.36 and 2.72 were obtained from the support and Pt membrane. This result corroborates with the literature [<xref ref-type="bibr" rid="scirp.59063-ref11">11</xref>] on silica membrane. This is a clear indication that the Pt results in an activation of the hydrogen transport to enhance the selectivity of hydrogen.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Hydrogen permeation Vs feed pressure of the support and Pt membrane at 25˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6201845x7.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Gas permeation and temperature relationship @ 1.5 barg</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6201845x8.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> H<sub>2</sub>/He Selectivity and temperature relationship on Pt membrane @ 1.6 barg</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6201845x9.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> H<sub>2</sub>/N<sub>2</sub> Selectivity and feed pressure relationship on support and Pt membrane @ 25˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6201845x10.png"/></fig></sec><sec id="s4"><title>4. Conclusion</title><p>Tubular commercially available support and Pt membrane were employed for H<sub>2</sub> separation. Single gas performance through the support and Pt membrane showed Knudsen diffusion transport for the smaller molecular weight gases (H<sub>2</sub> and He). On the other hand, transport of the larger molecular weight gas (N<sub>2</sub>) was independent on temperature. The single gas permeation of H<sub>2</sub> increased from 4.6 to 6.0 l/min in the temperature range 25˚C to 300˚C, whilst the selectivity of H<sub>2</sub>/He and H<sub>2</sub>/N<sub>2</sub> attained values of 1.96 at 300˚C and 2.72 at 25˚C. High temperature also favoured H<sub>2</sub> diffusion as the H<sub>2</sub> selectivity increased by almost 2 folds as compared with the theoretical Knudsen selectivity.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors gratefully acknowledge Petroleum Technology Development Fund (PTDF) Nigeria for funding this research, and School of Pharmacy &amp; Life Sciences RGU Aberdeen for the SEM and EDXA results.</p></sec><sec id="s6"><title>Cite this paper</title><p>Mohammed N.Kajama,Ngozi C.Nwogu,Edidiong O.Okon,HabibaShehu,IfyOrakwe,EdwardGobina, (2015) Hydrogen Separation Using Pt-Alumina Impregnated Membrane. Energy and Power Engineering,07,412-417. doi: 10.4236/epe.2015.79039</p></sec></body><back><ref-list><title>References</title><ref id="scirp.59063-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kanezashi, M. and Asaeda, M. 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