<?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">AJAC</journal-id><journal-title-group><journal-title>American Journal of Analytical Chemistry</journal-title></journal-title-group><issn pub-type="epub">2156-8251</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajac.2016.71006</article-id><article-id pub-id-type="publisher-id">AJAC-62952</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>
 
 
  Theoretical and Electrochemical Characterization of &lt;i&gt;δ&lt;/i&gt;-RuCl&lt;sub&gt;2&lt;/sub&gt;(Nazpy)&lt;sub&gt;2&lt;/sub&gt;: Application to Oxidation of D-Glucose
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>awohinlin</surname><given-names>Patrice Ouattara</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>Kafoumba</surname><given-names>Bamba</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>Nahossé</surname><given-names>Ziao</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>Kouakou</surname><given-names>Nobel N’guessan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Laboratoire de Thermodynamique et de Physico-Chimie du Milieu, UFR-SFA, Université Nangui-Abrogoua, Abidjan, Cote d’Ivoire</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>bambakaf_sfa@una.edu.ci(KB)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>15</day><month>01</month><year>2016</year></pub-date><volume>07</volume><issue>01</issue><fpage>57</fpage><lpage>66</lpage><history><date date-type="received"><day>8</day>	<month>December</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>18</month>	<year>January</year>	</date><date date-type="accepted"><day>22</day>	<month>January</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 heterogenized 
  δ-RuCl
  <sub>2</sub>(Nazpy)
  <sub>2</sub> deposited on carbon toray (CT) was studied for the first time as electrochemical catalyst. Before, it was characterized by visible-ultraviolet spectra and theoretically by TDDFT method at B3LYP/Lanl2DZ level. It displayed an MLCT t
  <sub>2g</sub>e
  <sub>g</sub> → π* transition where t
  <sub>2g</sub>e
  <sub>g</sub> due to the structure of Nazpy that considerably reduces energy between d AOs of Ru represents the HOMO of the complex and π* is identified as the LUMO. Electrochemistry study shows two redox ranges in both negative and positive sides of the potential. The positive side that corresponds to the couple Ru
  <sup>IV</sup>/Ru
  <sup>III</sup> of catalyst appears to be active for oxidation of D-glucose in carbonate buffer with a high turnover. Therefore, Keto-2-gluconic and gluconic acids were the two main products obtained with respectively 80% and 17.6% of selectivity. Moreover, 
  a small amount of tartaric and glycol acids coming from the c-c bond cleavage due to non-protection of the anomeric carbon of D-glucose were also observed.
 
</p></abstract><kwd-group><kwd>DFT Calculation</kwd><kwd> HOMO-LUMO Analysis</kwd><kwd> NBO</kwd><kwd> Electrochemistry</kwd><kwd> Ruthenium Complex</kwd><kwd> D-Glucose</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Azopyridine dyes have been studied as ligands since recent years. They belong to the π-accepting ligands. They have proven to provide with tremendous results when they are binding metal [<xref ref-type="bibr" rid="scirp.62952-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.62952-ref5">5</xref>] . Besides, their performance with ruthenium as complex is more of interest of researchers since ruthenium complex displays a fascinating electron-transfer and energy transfer [<xref ref-type="bibr" rid="scirp.62952-ref6">6</xref>] . Moreover, ruthenium offers a wide range of oxidation states and its reactivities depend on the stability and inter-convertibility of these oxidation states, which in turn depend on the nature of ligands bound to the metal. The fascinating use of azo dyes is that they keep the ruthenium in low states, which increase the complex reactivity and selectivity [<xref ref-type="bibr" rid="scirp.62952-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.62952-ref8">8</xref>] .</p><p>In former articles, we showed that azopyridine ligands are assumed to be bidentate [<xref ref-type="bibr" rid="scirp.62952-ref9">9</xref>] . Then, the synthesis that puts together reactive RuCl<sub>3</sub>∙3H<sub>2</sub>O and the ligand in methanol gives only two C<sub>2</sub> symmetrical isomers; however the asymmetry of the ligand allows for five isomers [<xref ref-type="bibr" rid="scirp.62952-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.62952-ref11">11</xref>] . These synthesized isomers are admitted to be g-Cl and d-Cl respectively standing for g-RuCl<sub>2</sub>(L)<sub>2</sub> and d-RuCl<sub>2</sub>(L)<sub>2</sub>. L represents azopyridine ligand and the structures of both g-Cl and d-Cl mean that both ligands L are respectively in cis and trans configurations. In this report, we aim to characterize for the first time the RuCl<sub>2</sub>(Nazpy)<sub>2</sub> where Nazpy stands for 1-(2-pyridila- zo)-2-naphtol as electrochemical catalyst for the oxidation of D-glucose and by computer calculation on behalf of DFT method. Regarding its synthesis, previous works reported that the hindrance brought about by Nazpy ligand allowed for the formation of only the isomer d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> [<xref ref-type="bibr" rid="scirp.62952-ref10">10</xref>] . Before, the complex was theoretically supposed to be C<sub>2</sub> symmetrical. Here, although it displays the C<sub>2</sub> axis through Cl-Ru-Cl angle, it is discovered actually to also show a C<sub>i</sub> symmetry through Ru that represents the center of symmetry. Therefore, we can assume that d-Cl is in reality C<sub>i</sub> symmetrical. Consequently, both ligands and chloride atoms are identical by pair. Therefore, the investigation will be performed on only d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> isomer. <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) displays Nazpy ligand showing four hetero-atoms by which the bonding can be performed to ruthenium atom. However, both DFT prediction and experiment show that the most stable complex is obtained when only N<sub>py</sub> and N<sub>2</sub> are bonded to Ru [<xref ref-type="bibr" rid="scirp.62952-ref12">12</xref>] . Therefore, <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) displays isomer d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> admitted to be the lone existing complex from reaction between Nazpy and RuCl<sub>3</sub>∙3H<sub>2</sub>O.</p><p>Similar research has been undertaken before, where RuCl<sub>2</sub>(Azpy)<sub>2</sub> was the regarding complex [<xref ref-type="bibr" rid="scirp.62952-ref13">13</xref>] . Azpy stands for 2-phenylazopyridine. Therein, both isomers g-Cl and d-Cl were obviously obtained confirming that the Azpy ligand does not display any steric hindrance. Furthermore, g-Cl was discovered to be the most active complex since it provides a good yield and important quantity of electricity. Moreover, the main products yielded during electrolysis were assumed to be keto-2-gluconic and gluconic acids. However, with bare platinum as working electrode, only gluconic acid was mainly obtained when D-glucose was oxidized and the active surface was rapidly poisoned.</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> (a) 1-(2-pyridylazo)-2-naphtol(Nazpy) ligand. DFT calculation on ligand shows that the ligand necessarily binds to ruthenium by N<sub>py</sub> and N<sub>2</sub> forming then a five ring stable shell; (b) d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> indicating both ligands in trans position and both Cl atoms vertically set and opposed.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x7.png"/></fig><fig id ="fig1_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x8.png"/></fig></fig-group></sec><sec id="s2"><title>2. Methods</title><sec id="s2_1"><title>2.1. Materials</title><p>All the reagents were used as received. 1-(2-pyridylazo)-2-naphtol was bought from AVOCADO, RuCl<sub>3</sub>∙3H<sub>2</sub>O was thanks to Alfa Aeser from Johnson Mathey Company. Organics products were from Fluka, Merck and Sigma. RuCl<sub>2</sub>(Nazpy)<sub>2</sub> was synthesized by using published procedure [<xref ref-type="bibr" rid="scirp.62952-ref3">3</xref>] .</p><sec id="s2_1_1"><title>2.1.1. Experiment Measurement</title><p>Electronic spectra were recorded with an ultroscan LKB (4050/4051) in DMSO solvent. Electrochemical measurements (cyclic voltammetric, controlled potential-coulometry) were made thanks to a merger of: PC computer (commodore), a potentiostat generator (EG &amp; G, model 362), a coulometer (wenking EVI 80, bank electronic) and a recorder (Kipp &amp; Zonen, BD 90).Three electrodes that were used comprise:</p><p> The working electrode is formed with an alloy of palladium-gold wire and a carbon toray (CT). The powder of the catalyst d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> is deposited on CT after its mixture in a merger nafion-water (80 mL/80mL). 14.4 mg of the powder was deposited on CT surface that geometric area is s = 4.5 cm<sup>2</sup>).</p><p> The auxiliary electrode is a vitreous carbonic.</p><p> The reference electrode is a reversible mercuric sulfate (MSE).</p><p>Before each experiment, the solution was bubbled with a stream of nitrogen gas (U quality from Air liquid) to get rid of oxygen and then the gas was maintained over the solution during measurements to keep it off oxygen.</p><p>Electrolysis was undertaken in a double compartments cell to separate both working and auxiliary electrodes so that we could avoid reducing oxidized compounds [<xref ref-type="bibr" rid="scirp.62952-ref14">14</xref>] . The electrolyzed products were identified by ionic chromatography (HPIC 4500i from Dionex).</p></sec><sec id="s2_1_2"><title>2.1.2. Computational Methods</title><p>All calculations were performed on the optimized geometry of the complex. The optimized geometry and all other calculations were undertaken at B3LYP/LANL2DZ level. LANL2DZ basis set is known to be an effective core potential (ECP) which is admitted to display accurate results with transition metals [<xref ref-type="bibr" rid="scirp.62952-ref15">15</xref>] . Besides, it is also suitable for any atom. NMR prediction was carried out at B3LYP/LANL2DZ level with GIAO method to confirm the C<sub>i</sub> symmetry of d-Cl. Furthermore, TD-DFT and NBO calculations were performed to figure out the electronic transition modes. Before, frequency calculation was performed on optimized molecule to find out the minima of Potential-Energy-Surface (PES) that characterizes the stable state of molecules. All the calculations were performed using Gaussian 03 program package [<xref ref-type="bibr" rid="scirp.62952-ref16">16</xref>] .</p></sec></sec></sec><sec id="s3"><title>3. Results and Discussions</title><sec id="s3_1"><title>3.1. NMR Calculation of g- and d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub></title><p><xref ref-type="fig" rid="fig1">Figure 1</xref>(a) shows the Nazpy ligand that owns all the hydrogen atoms within the complex. Therefore, <xref ref-type="table" rid="table1">Table 1</xref> displays the <sup>1</sup>H NMR recorded by theory and experiment of both isomers. The prediction was performed at B3LYP/Lanl2dz level both for the ligand and the isomers.</p><p>Through <xref ref-type="table" rid="table1">Table 1</xref>, it can be seen that d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> displays chemical shifts that match well with the experimental data. The most deshielded protons are assumed to be H<sub>α</sub>, H<sub>d</sub> and H<sub>6</sub>. Therefore, as confirmed by H NMR that RuCl<sub>2</sub>(Nazpy)<sub>2</sub> synthesized is d-Cl certainly due to the hindrance of Nazpy, we can admit that it is a C<sub>i</sub> symmetrical. Consequently, the upcoming works will be performed only on d-RuCl<sub>2</sub>(Nazpy)<sub>2 </sub>isomer.</p></sec><sec id="s3_2"><title>3.2. Characterization of d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub></title><p>Besides the NMR characterization of d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> that confirms its C<sub>i</sub> symmetry, the electronic data was studied and the spectra recorded are displayed in <xref ref-type="fig" rid="fig2">Figure 2</xref> and in <xref ref-type="table" rid="table2">Table 2</xref>. It shows the maximum wavelength recorded by experiment and theory in DMSO on both Nazpy ligand and d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>. It follows that the main data recorded by experiment is l = 590 nm. It must correspond to t<sub>2g</sub>(Ru) → π* (L) known as Metal to Ligand Charge Transfer (MLCT) transition. Moreover, the remaining three data are assumed to come from transition within ligand. Thus, the values that are l = 290, 400 and 468 nm match well with the dashed spectrum that corresponds to ligand Nazpy characterized in the same condition. The spectra are accepted to be respectively n → σ*, n → π* and π → π* or Ligand to Ligand Charge Transfer (LLCT) transitions [<xref ref-type="bibr" rid="scirp.62952-ref17">17</xref>] .</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> <sup>1</sup>H NMR calculated at B3LYP/Lanl2dz level of both g-Cl and d-Cl isomers and ligand compared with experiment values. Both g-Cl and d-Cl are respectively C<sub>2</sub> and C<sub>i</sub> symmetrical</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  ></th><th align="center" valign="middle"  colspan="3"  >Theoretical data at B3LYP/Lanl2dz</th><th align="center" valign="middle"  colspan="2"  >Experimental [<xref ref-type="bibr" rid="scirp.62952-ref12">12</xref>] data in CDCl<sub>3</sub></th></tr></thead><tr><td align="center" valign="middle" >Ligand</td><td align="center" valign="middle" >g-Cl</td><td align="center" valign="middle" >d-Cl</td><td align="center" valign="middle" >Ligand</td><td align="center" valign="middle" >RuCl<sub>2</sub>(Nazpy)<sub>2</sub></td></tr><tr><td align="center" valign="middle" >H<sub>α</sub></td><td align="center" valign="middle" >9.23</td><td align="center" valign="middle" >9.91</td><td align="center" valign="middle" >9.59</td><td align="center" valign="middle" >8.41</td><td align="center" valign="middle" >8.87</td></tr><tr><td align="center" valign="middle" >H<sub>β</sub></td><td align="center" valign="middle" >7.66</td><td align="center" valign="middle" >8.07</td><td align="center" valign="middle" >7.76</td><td align="center" valign="middle" >7.12</td><td align="center" valign="middle" >7.72</td></tr><tr><td align="center" valign="middle" >H<sub>g</sub></td><td align="center" valign="middle" >8.26</td><td align="center" valign="middle" >8.67</td><td align="center" valign="middle" >8.50</td><td align="center" valign="middle" >7.81</td><td align="center" valign="middle" >8.43</td></tr><tr><td align="center" valign="middle" >H<sub>d</sub></td><td align="center" valign="middle" >8.41</td><td align="center" valign="middle" >8.84</td><td align="center" valign="middle" >8.91</td><td align="center" valign="middle" >7.88</td><td align="center" valign="middle" >8.44</td></tr><tr><td align="center" valign="middle" >H<sub>1</sub></td><td align="center" valign="middle" >6.86</td><td align="center" valign="middle" >6.66</td><td align="center" valign="middle" >7.94</td><td align="center" valign="middle" >6.70</td><td align="center" valign="middle" >7.11</td></tr><tr><td align="center" valign="middle" >H<sub>2</sub></td><td align="center" valign="middle" >7.88</td><td align="center" valign="middle" >7.77</td><td align="center" valign="middle" >8.27</td><td align="center" valign="middle" >7.64</td><td align="center" valign="middle" >8.32</td></tr><tr><td align="center" valign="middle" >H<sub>3</sub></td><td align="center" valign="middle" >7.72</td><td align="center" valign="middle" >7.83</td><td align="center" valign="middle" >8.03</td><td align="center" valign="middle" >7.92</td><td align="center" valign="middle" >8.08</td></tr><tr><td align="center" valign="middle" >H<sub>4</sub></td><td align="center" valign="middle" >7.67</td><td align="center" valign="middle" >7.84</td><td align="center" valign="middle" >7.87</td><td align="center" valign="middle" >7.40</td><td align="center" valign="middle" >8.01</td></tr><tr><td align="center" valign="middle" >H<sub>5</sub></td><td align="center" valign="middle" >8.00</td><td align="center" valign="middle" >7.89</td><td align="center" valign="middle" >7.89</td><td align="center" valign="middle" >7.52</td><td align="center" valign="middle" >7.90</td></tr><tr><td align="center" valign="middle" >H<sub>6</sub></td><td align="center" valign="middle" >9.62</td><td align="center" valign="middle" >8.60</td><td align="center" valign="middle" >8.72</td><td align="center" valign="middle" >8.41</td><td align="center" valign="middle" >8.85</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Second order perturbation highlighting relation between electronic transition and UV visible data. Theoretical values were determined at B3LYP/LANL2DZ with TDDFT method in DMSO phase</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Character</th><th align="center" valign="middle"  colspan="2"  >Donor&#174; Acceptor</th><th align="center" valign="middle"  colspan="2"  >Experimental data l (nm)</th><th align="center" valign="middle"  colspan="2"  >Theoretical data l (nm)</th></tr></thead><tr><td align="center" valign="middle" >Ligand (Nazpy)</td><td align="center" valign="middle" >d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub></td><td align="center" valign="middle" >Ligand</td><td align="center" valign="middle" >d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub></td><td align="center" valign="middle" >Ligand</td><td align="center" valign="middle" >d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub></td></tr><tr><td align="center" valign="middle" >LLCT</td><td align="center" valign="middle" >LP(N<sub>py</sub>) &#174; s*(C-C)</td><td align="center" valign="middle" >LP(N<sub>1</sub>) &#174; s*(N<sub>py</sub>-C)</td><td align="center" valign="middle" >290</td><td align="center" valign="middle" >290</td><td align="center" valign="middle" >293</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >LLCT</td><td align="center" valign="middle" >LP(O) &#174; p*(C-C)</td><td align="center" valign="middle" >LP(O) &#174; p*(C-C)</td><td align="center" valign="middle" >400</td><td align="center" valign="middle" >400</td><td align="center" valign="middle" >393</td><td align="center" valign="middle" >371</td></tr><tr><td align="center" valign="middle" >LLCT</td><td align="center" valign="middle" >p(C-C) &#174; p*(C-C)</td><td align="center" valign="middle" >p(C-C) &#174; p*(C-C)</td><td align="center" valign="middle" >468</td><td align="center" valign="middle" >468</td><td align="center" valign="middle" >596</td><td align="center" valign="middle" >607</td></tr><tr><td align="center" valign="middle" >MLTC</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >LP(Ru) &#174; p*(N<sub>1</sub>-N<sub>2</sub>)</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >590</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >689</td></tr></tbody></table></table-wrap><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Electronic spectra of RuCl<sub>2</sub>(Nazpy)<sub>2</sub> and ligand Nazpy (a) recorded in DMSO solvent, solid lines represent RuCl<sub>2</sub>(Nazpy)<sub>2</sub> and dot line characterizes the ligand; (b) Electronic data predicted at B3LYP/LANL2DZ level with TDDFT method in DMSO phase. Here, dash line characterizes the ligand and solid line deals with the complex’s spectrum.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x9.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x10.png"/></fig></fig-group><p><xref ref-type="fig" rid="fig2">Figure 2</xref>(b) displays the theoretical investigation performed on both ligand and d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> in DMSO phase at B3LYP/Lanl2dz level. Regarding the ligand, it shows three bands and their wavelengths are l = 293, 393 and 596 nm. The high value of 596 nm from the experimental value (l = 468 nm) can be due to the solvent used for calculation. Concerning d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>, it shows a first band at l = 371 nm. The second band is large and includes a shoulder at l = 607 and a main band at l = 784 nm that must be the MLCT t<sub>2</sub>(Ru) → π*(L) transition. Whereas the bands at 371 and at 607 nm, they are assumed to match with transitions within the ligand Nazpy. Anyway, we can see a real shift between both experimental and theoretical data certainly due the solvent integrated in prediction. To well understand these transitions, NBO calculation was carried out. Therefore, the second-order perturbation highlighting donor-acceptor (bond-antibond) interactions exhibits the interaction LP(Ru) → *(N<sub>1</sub>-N<sub>2</sub>) that bears out the MLCT transition. <xref ref-type="table" rid="table2">Table 2</xref> summarizes all possible transitions within both the ligand and d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>.</p><p><xref ref-type="table" rid="table2">Table 2</xref> shows that oxygen is involved in the interaction within both ligand and the complex according to transition LP(O) &#174; p*(C-C). Moreover, the donor of electron through the transition regarding n → σ* can probably be explained by the value of occupancy and the availability of N atom. In the complex, as N<sub>py</sub> is involved in the bonding Ru-N<sub>py</sub>, it shares its occupancies with Ru atom instead of performing transition n → σ*. Therefore, only N<sub>1</sub> whose value of occupancy is 1.94 should necessarily be concerned by the transition n → σ* in the complex. Besides, when analyzing the HOMO-LUMO orbitals, it follows that LP(Ru) corresponds to HOMO orbital and its natural hybrid structure is h<sub>Ru</sub> = 0.46(4d<sub>xy</sub>) + 0.53(4d<sub>xz</sub>) + 0.20(4d<sub>yz</sub>) − <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2201316x11.png" xlink:type="simple"/></inline-formula> +<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2201316x12.png" xlink:type="simple"/></inline-formula>. It shows that HOMO is made of t<sub>2g</sub> orbitals that include d<sub>xy</sub>, d<sub>xz</sub> and d<sub>yz </sub>atomic orbitals. However, the hybrid also comprises two others AOs that correspond to e<sub>g</sub> MO. Therefore, that particularity of the hybrid h<sub>Ru</sub> structure where both t<sub>2g</sub> and e<sub>g</sub> MOs form the same cloud of electrons can be explained by the closeness of the energies of the five atomic d orbitals (AOs) of the metal as highlights <xref ref-type="table" rid="table3">Table 3</xref>. It shows that all AOs in the complex have almost the same energy and therefore, they must all be involved in the hybridization. In the contrary, Ru atom displays AOs whose energy are actually different and the occupancies are distributed according to energy values indicates a significant discrepancy between t<sub>2g</sub> and e<sub>g</sub> orbitals. Thus, we can assume that the ligand Nazpy induces a weak field [<xref ref-type="bibr" rid="scirp.62952-ref18">18</xref>] . Otherwise, the stabilization energy of the ligands field is assumed to be shallow allowing all the five AOs to share the d electrons 7.16 occupancies as indicates the electron configuration of Ru according to NBO analysis: [core]5s(0.27)4d(7.16)5p(0.01)5d(0.03)6p(0.02).</p><p>Therefore, we can conclude anyway that the HOMO is exclusively made of metallic orbital d of the ruthenium. So the electronic transition must be written as t<sub>2g</sub>e<sub>g</sub>(Ru)&#174;p*(N<sub>1</sub> − N<sub>2</sub>). Regarding LUMO orbital, it corresponds to p*(N<sub>1</sub> − N<sub>2</sub>) which natural hybrid structure for N<sub>2</sub> atom is h<sub>N</sub> = 0.99(2p<sub>x</sub>) − 0.12(2p<sub>y</sub>) and the overlap of both atomic obitals (AOs) that confirms the p character of the molecular orbital is written as follow:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2201316x13.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3_3"><title>3.3. Electrochemical Characterization</title><p>Cyclic voltammetry is assumed to be the most versatile electroanalytical technique for the study of species. It permits to rapidly observe redox behavior over a wide range of potential [<xref ref-type="bibr" rid="scirp.62952-ref19">19</xref>] . <xref ref-type="fig" rid="fig3">Figure 3</xref> displays two voltammograms of d-RuCl<sub>2</sub>(Nazpy)<sub>2 </sub>recorded in carbonate buffer (0,1 M Na<sub>2</sub>CO<sub>3</sub>/NaHCO<sub>3</sub>).</p><p>The voltammogram of <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) has been recorded in the negative range of the potential from −950 mV to −450 mV/MSE. During the positive sweep, an oxidative peak can be observed at −486 mV/MSE. Regarding the reductive peak, it is observed at −616 mV/MSE during the negative sweep of the rate. Therefore, The peak-to- peak DE = 130 mV shows that the system is quasi-reversible and it is assigned to the couple Ru(III)/Ru(II). The second voltammogram regarding <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) is attributed to the couple Ru(IV)/Ru(III). Herein, the positive sweep of the rate indicates an oxidation peak at 323 mV/MSE corresponding to Equation (1).</p><disp-formula id="scirp.62952-formula814"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2201316x14.png"  xlink:type="simple"/></disp-formula><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Populations and energy (a.u.) of d AOs of both Ru atom and Ru in d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub></title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Ru (in)</th><th align="center" valign="middle"  colspan="2"  >d<sub>xy</sub></th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >d<sub>yz</sub></th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >d<sub>xz</sub></th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2201316x15.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >d<sub>z&#178;</sub></th></tr></thead><tr><td align="center" valign="middle" >Population</td><td align="center" valign="middle" >Energy</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Population</td><td align="center" valign="middle" >Energy</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Population</td><td align="center" valign="middle" >Energy</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Population</td><td align="center" valign="middle" >Energy</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Population</td><td align="center" valign="middle" >Energy</td></tr><tr><td align="center" valign="middle" >d-Cl</td><td align="center" valign="middle" >1.48</td><td align="center" valign="middle" >−0.22</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.63</td><td align="center" valign="middle" >−0.22</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.56</td><td align="center" valign="middle" >−0.23</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.29</td><td align="center" valign="middle" >−0.21</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.20</td><td align="center" valign="middle" >−0.2</td></tr><tr><td align="center" valign="middle" >atom</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−0.2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−0.18</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−0.18</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >−0.15</td></tr></tbody></table></table-wrap><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Cyclic voltammogram of d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>/nafion-water-C<sub>t</sub> in NaHCO<sub>3</sub>/Na<sub>2</sub>CO<sub>3</sub> 0,1 M at a scan rate of 50 mV/S and at 298.15 K: (a) Potential range regards Ru<sup>III</sup>/Ru<sup>II</sup>; (b) Potential range concerns Ru<sup>IV</sup>/Ru<sup>III</sup>. i<sub>pa</sub> and i<sub>pc</sub> stands respectively for anodic and cathodic peaks currents.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x16.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x17.png"/></fig></fig-group><p>Besides, the reductive peak recorded during the reverse sweep of the rate is at 277 mV/MSE and the regarding reaction is characterized by Equation (2).</p><disp-formula id="scirp.62952-formula815"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2201316x18.png"  xlink:type="simple"/></disp-formula><p>Therefore, the peak-to-peak separation DE = 46 mV/MSE indicates a reversible system and this reversibility was borne out by the ratio peaks currents</p><disp-formula id="scirp.62952-formula816"><label>. (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2201316x19.png"  xlink:type="simple"/></disp-formula><p>Moreover, the number of electrons transferred in the electrode reaction for the couple is obtained by Equation (4).</p><disp-formula id="scirp.62952-formula817"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2201316x20.png"  xlink:type="simple"/></disp-formula><p>It follows that both systems are consistent with the literature since it has been assumed that electron exchange comes exclusively from ruthenium atom. Thus, the ligands are merely concerned by rendering the Ru atom more selective [<xref ref-type="bibr" rid="scirp.62952-ref8">8</xref>] . Moreover, electrochemical characterization of RuCl<sub>3</sub>∙3H<sub>2</sub>O performed in previous paper shows well the difference between both catalysts [<xref ref-type="bibr" rid="scirp.62952-ref13">13</xref>] . This discrepancy is due to ligand lowering the redox values in the complex. Furthermore, we calculated the quantity of electricity by integration of the surfaces of both positive and negative peaks of the latter voltammogram though the potential range fits well with oxidation potential of carbohydrate molecules. Therefore, as indicated in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b), Q<sub>1</sub> and Q<sub>2</sub> are equal confirming the reversible state of the system. So, the quantity of electricity calculated was as well for the oxidation as for the reduction surfaces Q = 263 &#181;C.</p></sec><sec id="s3_4"><title>3.4. Electrolysis Study of D-Glucose</title><p>D-glucose was oxidized over a working electrode d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>/CT. The reaction last out 48 h. Before, <xref ref-type="fig" rid="fig4">Figure 4</xref> displays voltammogram recorded over 50 mmol∙L<sup>−1</sup> of D-glucose compared with that recorded in supporting electrolyte alone. In presence of D-glucose, a reductive peak was absent confirming the fast reaction between Ru<sup>IV</sup> and the sample. This voltammogram was recorded at the beginning of the electrolysis to find out the best potential to be fixed up for oxidation of D-glucose. Therefore, the accepted potential which current was the most important was 600 mV/MSE. In consequence, the prolonged electrolysis was then performed by setting the electrolysis potential at 600 mV/MSE to renew the oxidation state of Ru.</p><p>The density current observed at the beginning was j = 49 &#181;A∙mg<sup>−1</sup>. This value decreased during 15 hours and stabilized at j = 16 &#181;A∙mg<sup>−1</sup>. At the end, the current was however 14 μA∙mg<sup>−1</sup> and the quantity of electricity was 45.1C with a yield of 20.5% of D-glucose. <xref ref-type="fig" rid="fig5">Figure 5</xref> presents the evolution of both quantity of current and the density of electricity recorded during the prolonged electrolysis.</p><p>Furthermore, the electrolyzed products were analyzed thanks to ionic chromatography. Herein, new more products were obtained that have never been yielded since the recognized most active catalysts as platinum and gold were used [<xref ref-type="bibr" rid="scirp.62952-ref20">20</xref>] - [<xref ref-type="bibr" rid="scirp.62952-ref23">23</xref>] . Keto-2-gluconic and gluconic acids were obtained respectively with 80% and 17.6% of selectivity. Besides, small amounts of products like tartaric and oxalic acids coming from C-C cleavage were also observed. The particularity of the catalyst is that it has been used for many times, and it did not suffer from any damage. <xref ref-type="fig" rid="fig6">Figure 6</xref> summarizes the evolution of transformation of D-glucose into the main products aforementioned.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Voltammograms of d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>/CT recorded in NaHCO<sub>3</sub>- Na<sub>2</sub>CO<sub>3</sub> 0.1 mol∙L<sup>−1</sup>, at 50 mV∙s<sup>−1</sup> and at 25˚C. (---) supporting electrolyte alone; (&#190;) in presence of 50 mmol∙L<sup>−1</sup> of D-glucose</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x21.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Evolution of current density (&#161;) and quantity of electricity (&#161;) versus time during the electrolysis of D-glucose over d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>/CT</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x22.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Evolution of concentrations of D-glucose (&#161;) and the main products during prolonged electrolysis over d-RuCl<sub>2</sub>(nazpy)<sub>2</sub>. (&#161;) keto-2-gluconic acid, (p) gluconic acid</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2201316x23.png"/></fig></sec></sec><sec id="s4"><title>4. Conclusions</title><p>C<sub>i</sub> symmetrical d-RuCl<sub>2</sub>(Nazpy)<sub>2</sub> was studied for the first time as working electrode for oxidation of D-glucose. Before, its characterization by UV visible technique and TDDFT method at B3LYP/LANL2DZ level was carried out in DMSO phase. A MLCT and three LLCT transitions were obtained. The MLCT is assumed to be t<sub>2g</sub>e<sub>g</sub> &#174; p* transition, though the HOMO is a linear combination of the five atomic d orbitals as their energies are very close. The regarding hybridization according to NBO analysis is: h<sub>Ru</sub> = 0.46(4d<sub>xy</sub>) + 0.53(4d<sub>xz</sub>) + 0.20(4d<sub>yz</sub>) − <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2201316x24.png" xlink:type="simple"/></inline-formula> +<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2201316x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2201316x25.png" xlink:type="simple"/></inline-formula>. Nazpy is therefore assumed to reduce energy gap between the five AOs d of Ru on the benefit of the well sharing electrons.</p><p>Besides, cyclic voltammetry performed on the heterogeneous catalyst displayed two redox couples. The first couple that was discovered in negative range of potential was Ru<sup>+III</sup>/Ru<sup>+II</sup>. This process was irreversible though the peak-to-peak separated potential was DE = 130 mV/MSE. The second range was recorded in positive range of the potential between 0 and 600 mV/MSE. The peak-to-peak separated potential DE = 46 mV indicated a reversible system, and the regarding redox couple was assumed to be Ru<sup>+IV</sup>/Ru<sup>+III</sup>. The electro-oxidation of D- glucose was undertaken at 600 mV/MSE as this potential was the convenient one to renew the Ru<sup>+IV</sup> state. Therefore, keto-2-gluconic and gluconic acids were both the main products yielded with respectively 80% and 17.6% amounts of selectivity. These products were the same obtained when RuCl<sub>2</sub>(Azpy)<sub>2</sub> was studied as mediators where the current produced was unfortunately feeble. Comparatively to platinum that is up to now recognized to be the best active catalyst, however its active sites are rapidly poisoned; the azopyridine complex of ruthenium is assumed to be more selective.</p></sec><sec id="s5"><title>Cite this paper</title><p>Wawohinlin PatriceOuattara,KafoumbaBamba,Nahoss&#233;Ziao,Kouakou NobelN’guessan, (2016) Theoretical and Electrochemical Characterization of δ-RuCl<sub>2</sub>(Nazpy)<sub>2</sub>: Application to Oxidation of D-Glucose. American Journal of Analytical Chemistry,07,57-66. doi: 10.4236/ajac.2016.71006</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.62952-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Krause, R. and Krause, K. (1982) Chemistry of Bipyridyl Like Ligands. 2. Mixed Complexes of Ruthenium(II) with 2-(Phenylazo)pyridine: A New .pi.-Bonding Probe. 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