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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mater.</journal-id>
<journal-title>Frontiers in Materials</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mater.</abbrev-journal-title>
<issn pub-type="epub">2296-8016</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fmats.2019.00238</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Materials</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>A Simple Flow Injection Sensing System for the Real-Time On-Line Determination of Chemical Oxygen Demand Based on 3D Au-NPs/TiO<sub>2</sub> Nanotube Arrays</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Si</surname> <given-names>Hewei</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/738589/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Zhang</surname> <given-names>Xidong</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Lin</surname> <given-names>Shiwei</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/645637/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>State Key Laboratory of Marine Resource Utilization in South China Sea, Hainan University</institution>, <addr-line>Haikou</addr-line>, <country>China</country></aff>
<aff id="aff2"><sup>2</sup><institution>School of Materials Science and Engineering, Hainan University</institution>, <addr-line>Haikou</addr-line>, <country>China</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Girish Kale, University of Leeds, United Kingdom</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Mukul Pradhan, National Institute of Technology Meghalaya, India; Ramendra Sundar Dey, Institute of Nano Science and Technology (INST), India</p></fn>
<corresp id="c001">&#x0002A;Correspondence: Shiwei Lin <email>linsw&#x00040;hainanu.edu.cn</email></corresp>
<fn fn-type="other" id="fn001"><p>This article was submitted to Functional Ceramics, a section of the journal Frontiers in Materials</p></fn></author-notes>
<pub-date pub-type="epub">
<day>04</day>
<month>10</month>
<year>2019</year>
</pub-date>
<pub-date pub-type="collection">
<year>2019</year>
</pub-date>
<volume>6</volume>
<elocation-id>238</elocation-id>
<history>
<date date-type="received">
<day>14</day>
<month>05</month>
<year>2019</year>
</date>
<date date-type="accepted">
<day>12</day>
<month>09</month>
<year>2019</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2019 Si, Zhang and Lin.</copyright-statement>
<copyright-year>2019</copyright-year>
<copyright-holder>Si, Zhang and Lin</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>3D bare TiO<sub>2</sub> nanotube arrays loaded with Au nanoparticles (3D Au-NPs/TNTAs) were prepared to effectively enhance the photoelectrocatalytic properties. A simple flow injection sensing system was proposed for the real-time on-line determination of chemical oxygen demand using the 3D Au-NPs/TNTAs electrode. The proposed photoelectrochemical oxidative degradation principle of the sensing system was analyzed and validated by the representative organic compounds with known COD values at a potential bias 1.5 V under UV illumination. A practical detection limit of the sensing system is 0.18 mg/L and the linear range is 1.92&#x02013;3,360 mg/L under the optimum conditions. In the experimental process, the sensing system exhibits long-term stability and good reproducibility.</p></abstract> <kwd-group>
<kwd>3D Au-NPs/TNTAs</kwd>
<kwd>photoelectrocatalytic</kwd>
<kwd>chemical oxygen demand (COD)</kwd>
<kwd>flow injection sensing</kwd>
<kwd>real-time on-line COD determination</kwd>
</kwd-group>
<contract-sponsor id="cn001">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content></contract-sponsor>
<counts>
<fig-count count="8"/>
<table-count count="0"/>
<equation-count count="9"/>
<ref-count count="29"/>
<page-count count="7"/>
<word-count count="4237"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>Introduction</title>
<p>Chemical oxygen demand (COD) is the oxygen equivalent on degradation of the organic compounds, which is a significant parameter of water quality assessment (Kondo et al., <xref ref-type="bibr" rid="B7">2014</xref>). Even though potassium dichromate oxidation method is widely used, many inherent shortcomings such as time-consuming (2&#x02013;4 h) reflux process, highly toxic chemicals, corrosiveness and high cost (Ag<sub>2</sub>SO<sub>4</sub>) were existing (Allan Moore et al., <xref ref-type="bibr" rid="B1">1949</xref>; Zhang J. et al., <xref ref-type="bibr" rid="B24">2009</xref>; Zhang S. et al., <xref ref-type="bibr" rid="B26">2009</xref>). Photocatalytic methods can effectively solve these problems, but the resulting electron hole pairs are easy to recombine. Currently, an environmentally friendly and rapid photoelectrochemical COD determination way was considered a more promising approach to surmount the recombination of electron-hole pairs further to improve the degradation efficiency (Qu et al., <xref ref-type="bibr" rid="B17">2011</xref>; Li et al., <xref ref-type="bibr" rid="B9">2012</xref>).</p>
<p>However, the photoelectrocatalytic COD determination method implies a relatively narrow working range and poor reproducibility with a stop-flow operation mode in the quartz cell. Also, the shortcomings of conventional photoelectrochemical method are as follows: one is the complex three-electrode structure, the other is that it&#x00027;s hard to improve sensitivity because of inadequate degradation efficiency of working electrode (Liao et al., <xref ref-type="bibr" rid="B12">2016</xref>).</p>
<p>TiO<sub>2</sub> nanotube arrays (TNTAs) extending on the Ti foil have been used as sensing electrode to detect chemical oxygen demand (COD) in recent years, owning to its intrinsic nanotubular architecture and remarkable properties (Li et al., <xref ref-type="bibr" rid="B8">2006</xref>; Grimes, <xref ref-type="bibr" rid="B4">2007</xref>; Zheng et al., <xref ref-type="bibr" rid="B28">2008</xref>). Ti foil could be entirely transformed into nanotubes but a few micrometers thickness of nanotubes are sufficient for performing efficient photocatalysis. In addition, it is easy to have scattering effects in the liquid (Paulose et al., <xref ref-type="bibr" rid="B16">2007</xref>; Kar and Smith, <xref ref-type="bibr" rid="B6">2009</xref>). It&#x00027;s wasteful for Ti foil since it has relatively much loss of photons (Zhuang et al., <xref ref-type="bibr" rid="B29">2007</xref>; Beranek et al., <xref ref-type="bibr" rid="B2">2009</xref>). However, three-dimensional (3D) TNTAs photoelectrode extending radically on a grid of titanium wires can avoid this wastage and because of absorbing the reflected and/or refracted light (Liao et al., <xref ref-type="bibr" rid="B13">2012</xref>). Furthermore, the 3D TNTAs on Ti mesh possess larger surface area than TiO<sub>2</sub> nanotube arrays on the Ti foil which means higher photocatalytic activity. Nevertheless, TiO<sub>2</sub> nanotube arrays show shorter lifetime, poor stability, unsatisfactory photocatalytic activity in real application for COD analysis (Liang et al., <xref ref-type="bibr" rid="B11">2019</xref>). Therefore, it is important to propose a new sensor further to improve the weakness of present TiO<sub>2</sub> sensing.</p>
<p>To tackle these problems, we propose a flow injection photoelectrocatalytic COD determination method by combining continuous flow injection thin-cell reactor mode and Au nanoparticles (Au-NPs) loaded on 3D TNTAs. The influence of annealing temperature and anodizing time on the as-prepared bare 3D TNTAs were studied. The as-prepared 3D TiO<sub>2</sub> nanotube arrays were characterized via material characterizations and photoelectrochemical testing, such as FE-SEM, EDS, XRD, photocurrent-density potential characteristics and chronoamperometry experiments, to investigate their morphology, elements, structure, and photoelectrocatalytic activities. A new COD determination analytical principle was proposed, which was experimentally validated with representative organic compounds. Because of the different adsorption position on the surface of TiO<sub>2</sub>, glucose, glutamic acid and GGA (glucose: glutamic acid &#x0003D; 1:1) were chosen as the representative organic compounds (Zhang et al., <xref ref-type="bibr" rid="B25">2006</xref>; Han et al., <xref ref-type="bibr" rid="B5">2010</xref>; Liu et al., <xref ref-type="bibr" rid="B14">2014</xref>). The analytical signal generation of the proposed sensing system was optimized on the important experimental parameters such as supporting electrolyte and applied potential bias.</p>
</sec>
<sec id="s2">
<title>Experimental Section</title>
<sec>
<title>Preparation of 3D Au-NPs/TNTAs/Ti</title>
<p>The working electrode was prepared by following steps. Firstly, titanium mesh (&#x0003E;99% purity, 50 meshes) was sliced rectangle pieces of 30 &#x000D7; 70 mm, which were fixed by titanium wire. Above treated titanium meshes were dipped into the mixture solution (HF: HNO<sub>3</sub>: H<sub>2</sub>O &#x0003D; 1:4:5 in v/v) about 30 s to polish, then treated with acetone, ethanol and ultrapure water by ultra-sonication in order. Subsequently, dried in air. Secondly, the treated titanium mesh was electrochemical anodization in ethylene glycol electrolyte solution (2 wt% H<sub>2</sub>O and 0.3 wt% NH<sub>4</sub>F) by two electrode configurations in different anodization time 10, 20, 30, and 60 min. With the rate of heating 2&#x000B0;C min<sup>&#x02212;1</sup>, the obtained samples were calcinated at 350, 450, 550, and 650&#x000B0;C for 3 h in muffle furnace, respectively. Among them, the electrode material with the best oxidation ability was selected as the as-prepared working electrode. Thirdly, to improve photocatalytic activity and stability of the as-prepared working electrode, Au nanoparticles were deposited on the bare 3D TNTAs by the photo-reduction method. The as-prepared working electrode was dipped into the electrolyte consisted of mixture (HAuCl<sub>4</sub> (0.1g/L): HCHO &#x0003D; 100:1 in v/v) in the quartz cell under UV irradiation for 40 s. Then the electrode was washed with ethanol, deionized water and dried in the air, which then was used as the working electrode. As for the counter electrode, Pt nanoparticles were electrodeposited on the titanium mesh treated above at &#x02212;0.3V for 3 min in the mixed solution (H<sub>2</sub>PtCl<sub>6</sub> (0.2g/L): HCHO &#x0003D; 100:1 in v/v) (Si et al., <xref ref-type="bibr" rid="B20">2019</xref>).</p>
</sec>
<sec>
<title>Characterization</title>
<p>The morphologies and microstructure of the electrode material were studied by scanning electron microscopy (FE-SEM) equipped with an energy-dispersive spectrometer (EDS). Crystal phase of the working electrode was analyzed by X-ray diffraction (XRD, Bruker D8) with Cu K&#x003B1; radiation. To choose a 3D TNTAs electrode material with best oxidation ability, linear sweep voltammetry (LSV) was performed in cube quartz reactor (50 &#x000D7; 50 &#x000D7; 50 mm) at room temperature using saturated Ag/AgCl (KCl) reference electrode, platinum foil counter electrode and the as-prepared 3D TiO<sub>2</sub> nanotube arrays working electrode in all the experiments.</p>
</sec>
<sec>
<title>Fabrication of Flow Injection Sensing System and Measurement of Their Photoelectrocatalytic Real-Time On-Line COD Sensing Properties</title>
<p>Au modified 3D TiO<sub>2</sub> Nanotube Arrays as sensing electrode was used for real-time on-line COD determination in our proposed thin-cell reactor which can be seen from our previous work (Si et al., <xref ref-type="bibr" rid="B20">2019</xref>). The schematic diagram and digital image of the real-time on-line thin-cell reactor was shown in <xref ref-type="supplementary-material" rid="SM1">Figure S1</xref>. The application potential bias and the recording of response current signal were supplied by the electrochemical workstation (Zahner Zennium, Germany). A 5W UV lamp was used as the UV source in the experiment. A 0.2 mM Na<sub>2</sub>SO<sub>4</sub> solution was as the supporting electrolyte in the photoelectrochemical measurements.</p>
</sec>
</sec>
<sec id="s3">
<title>Results and Discussion</title>
<sec>
<title>Characterization of the Electrode Materials</title>
<p>The effect of preparation parameters of anodic time and calcination temperature on the saturated photocurrent density of the as-prepared electrodes was obtained in LSV under the UV illumination (Zhang J. et al., <xref ref-type="bibr" rid="B24">2009</xref>). As shown in <xref ref-type="supplementary-material" rid="SM1">Table S1</xref>, the electrode with anodic oxidation for 10 min and calcination temperature at 450&#x000B0;C possess the highest saturated photocurrent density. Therefore, the electrode which is prepared at 60 V for anodic time 10 min and calcination temperature at 450&#x000B0;C for 3 h (No. 2 in <xref ref-type="supplementary-material" rid="SM1">Table S1</xref>) was selected as the as-prepared working electrode in our proposed flow injection sensing system.</p>
<p><xref ref-type="fig" rid="F1">Figure 1</xref> shows the surface morphology of the working electrode material where highly-ordered TNTAs are distributed uniformly and aligned vertically on the Ti meshes (Liao et al., <xref ref-type="bibr" rid="B13">2012</xref>). The average inner diameter of the 3D TNTAs is 65 nm with length of 3 um, as depicted in <xref ref-type="fig" rid="F1">Figures 1B,C</xref>. <xref ref-type="fig" rid="F1">Figure 1D</xref> displays Au-NPs loaded on the 3D TNTAs and the EDS spectrum further identify the presence of Au-NPs on the bare 3D TNTAs where the weight of Au is 0.48% (<xref ref-type="supplementary-material" rid="SM1">Figure S2</xref>). The XPS results show the coexistence of Ti, O and Au elements in the prepared nanocomposite, as shown in <xref ref-type="supplementary-material" rid="SM1">Figure S3</xref>. From the XPS spectra, Ti 2p1/2 and Ti 2p3/2 were obtained at 464 eV and 458 eV while O 1s was at 530 eV, which are all consistent with the literature reports (Luo et al., <xref ref-type="bibr" rid="B15">2016</xref>; Siavash et al., <xref ref-type="bibr" rid="B21">2017</xref>). Furthermore, the existence of Au in the nanocomposite is confirmed by the Au 4f7/2 and Au 4f5/2 peaks at 83 and 86.7 eV, respectively. The role of Au in the Au/TiO<sub>2</sub> composite enhances the electrical conductivity and raises the optical conductivity further to improve the photoelectrocatalytic properties (Rudra et al., <xref ref-type="bibr" rid="B18">2018a</xref>,<xref ref-type="bibr" rid="B19">b</xref>).</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>SEM images: <bold>(A)</bold> Ti meshes, <bold>(B)</bold> side view and <bold>(C)</bold> top view of the bare 3D TNTAs, <bold>(D)</bold> Au-NPs on the bare 3D TNTAs.</p></caption>
<graphic xlink:href="fmats-06-00238-g0001.tif"/>
</fig>
<p><xref ref-type="fig" rid="F2">Figure 2</xref> shows the XRD patterns of the 3D TNTAs before, and after calcinated. The diffraction peaks attributed to the formation of anatase TiO<sub>2</sub> structure after annealing, which has higher photocatalytic activity (Zhang et al., <xref ref-type="bibr" rid="B27">2016</xref>). There appears rutile when the annealing temperature reaches to 650&#x000B0;C. Furthermore, the photocurrent response of the samples annealed at different temperatures were measured in comparation to that of Au nanoparticles modified TiO<sub>2</sub> nanotube arrays, as depicted in <xref ref-type="supplementary-material" rid="SM1">Figure S4</xref>. Among them, the sample annealed at 450&#x000B0;C has the optimal photocurrent density. The obtained working electrode possess the higher photocurrent density compared to pure TiO<sub>2</sub> nanotube arrays, indicating the existence of Au nanoparticles can improve the sensing property.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>XRD patterns of the reduced at 350, 450, 550, and 650&#x000B0;C, respectively and non-reduced as-prepared 3D TNTAs electrode.</p></caption>
<graphic xlink:href="fmats-06-00238-g0002.tif"/>
</fig>
</sec>
<sec>
<title>The Photoelectrocatalytic Properties of the Sensing System</title>
<p><xref ref-type="fig" rid="F3">Figure 3</xref> shows photocurrent response of the sensing system as a function of time at the repeated on/off cycles with applied potential 1.5 V under UV illumination. The 0.2 mM Na<sub>2</sub>SO<sub>4</sub> solution is as the supporting electrolyte. The photocurrent density of non-reduced bare 3D TNTAs was measured nearly to be 0 mA without UV light, but a significant increasing in current value was seen under UV illumination. The non-light current was measured to be low upon switch off the light, but the current quickly increased when turned on the UV light, indicating the sensing system responds quickly to UV source.</p>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Photocurrent responses of the sensing system as a function of time at the repeated on/off cycles with an applied potential 1.5 V under UV illumination. 0.2 mM Na<sub>2</sub>SO<sub>4</sub> solution as the supporting electrolyte.</p></caption>
<graphic xlink:href="fmats-06-00238-g0003.tif"/>
</fig>
<p><xref ref-type="fig" rid="F4">Figure 4</xref> shows linear sweep voltammograms of the Au-NPs/3D TNTAs electrode in 0.2 mM Na<sub>2</sub>SO<sub>4</sub> and 1 mM glucose in 0.2 mM Na<sub>2</sub>SO<sub>4</sub> solution with and without UV irradiation, respectively, in order to investigate the response of oxidation current produced by degradation of organic compounds. As we can see from <xref ref-type="fig" rid="F4">Figure 4</xref>, there was almost no response to oxidation current when glucose was added in the non-UV light (<xref ref-type="fig" rid="F4">Figure 4A</xref>). However, a significant oxidation current appears when ultraviolet light was applied (<xref ref-type="fig" rid="F4">Figure 4B</xref>).</p>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Linear voltammograms of the sensing system: (a) 0.2 mM Na<sub>2</sub>SO<sub>4</sub> and (b) 0.2 mM Na<sub>2</sub>SO<sub>4</sub> containing glucose organic using 3D Au-NPs/TNTAs sensing electrode at the potential scan rate of 10 mVs<sup>&#x02212;1</sup> without <bold>(A)</bold> and with <bold>(B)</bold> UV illumination.</p></caption>
<graphic xlink:href="fmats-06-00238-g0004.tif"/>
</fig>
</sec>
<sec>
<title>COD Sensing Mechanism</title>
<p>A new detection principle was proposed based on the postulate that the potential of the counter electrode</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M1"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x003C6;</mml:mi></mml:mrow><mml:mrow><mml:mtext mathvariant="normal">counter</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>0</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>The analog circuit diagram of the proposed COD sensor is as follows <xref ref-type="fig" rid="F5">Figure 5</xref>:</p>
<p>According to the &#x0201C;Closed Circuit Ohm Law,&#x0201D; for the proposed COD sensor</p>
<disp-formula id="E2"><label>(2)</label><mml:math id="M2"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mtext mathvariant="normal">v</mml:mtext></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:mi>I</mml:mi><mml:mi>R</mml:mi></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Where <italic>E</italic> is the applied voltage; v<sub>reactor</sub> is the voltage on the photoelectrochemical reactor; <italic>I</italic> is the current in the closed circuit; <italic>R</italic> is the resistance of the closed circuit except reactor.</p>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>Internal circuit diagram of the proposed real-time on-line sensing system.</p></caption>
<graphic xlink:href="fmats-06-00238-g0005.tif"/>
</fig>
<p>When ultraviolet light irradiates the sensing electrode, photoholes possess strong oxidizing capacities which can mineralize organic compounds. Assuming that the organic compounds are stoichiometrically mineralized on surface of the sensing electrode, the potential of sensing electrode can be given by Nernst equation</p>
<disp-formula id="E3"><label>(3)</label><mml:math id="M3"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>&#x003C6;</mml:mi></mml:mrow><mml:mrow><mml:mtext mathvariant="normal">working</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn>2</mml:mn><mml:mo>.</mml:mo><mml:mn>30</mml:mn><mml:mfrac><mml:mrow><mml:mi>k</mml:mi><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mi>q</mml:mi></mml:mrow></mml:mfrac><mml:mo>log</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>A</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Where <italic>C</italic><sub><italic>m</italic></sub>, <italic>T, k, n, A</italic> are the molar concentration, temperature, Boltzmann constant, the electron transfer number of the individual organic compound and constant, respectively.</p>
<p>Therefore, the applied voltage on the reactor can be given as follows:</p>
<disp-formula id="E4"><label>(4)</label><mml:math id="M4"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn>2</mml:mn><mml:mo>.</mml:mo><mml:mn>30</mml:mn><mml:mfrac><mml:mrow><mml:mi>k</mml:mi><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mi>q</mml:mi></mml:mrow></mml:mfrac><mml:mo>log</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>A</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>According to the relationship between molar concentration (<italic>C</italic><sub>m</sub>) and COD concentration [COD] &#x0003D; 8000 <italic>nC</italic><sub><italic>m</italic></sub> (Wang et al., <xref ref-type="bibr" rid="B22">2013</xref>), then Equation (4) can be given by:</p>
<disp-formula id="E5"><label>(5)</label><mml:math id="M5"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mi>t</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn>2</mml:mn><mml:mo>.</mml:mo><mml:mn>30</mml:mn><mml:mfrac><mml:mrow><mml:mi>k</mml:mi><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mi>q</mml:mi></mml:mrow></mml:mfrac><mml:mo>log</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>C</mml:mi><mml:mi>O</mml:mi><mml:mi>D</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>A</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p><xref ref-type="fig" rid="F6">Figure 6</xref> shows the photocurrent-time profiles with the absence (i<sub>blank</sub>) and existence (i<sub>total</sub>) of organic compounds using the proposed sensing system. When the sensing electrode is illuminated with UV light, i<sub>blank</sub> obtained in the supporting electrolyte mainly from the oxidation of water, while the observed photocurrent (i<sub>total</sub>) in the sample organic solution originates from both the oxidation of water and the photoelectrocatalytic oxidation of organic compounds. As we know, i<sub>net</sub> (net steady state current) originates from i<sub>total</sub> via subtracting the i<sub>blank</sub>, which is the step between the blank photocurrent and the total photocurrent in <xref ref-type="fig" rid="F6">Figure 6</xref> (Chen et al., <xref ref-type="bibr" rid="B3">2012</xref>).</p>
<disp-formula id="E6"><label>(6)</label><mml:math id="M6"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mtext mathvariant="normal">I</mml:mtext></mml:mrow><mml:mrow><mml:mtext mathvariant="normal">net</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mtext mathvariant="normal">i</mml:mtext></mml:mrow><mml:mrow><mml:mtext mathvariant="normal">total</mml:mtext></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mtext mathvariant="normal">i</mml:mtext></mml:mrow><mml:mrow><mml:mtext mathvariant="normal">blank</mml:mtext></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>I<sub>net</sub> can be transformed into the equivalent COD values according to Faraday&#x00027;s law.</p>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>Photocurrent response of a 0.2 mM Na<sub>2</sub>SO<sub>4</sub> blank solution (i<sub>blank</sub>) and the 0.2 mM Na<sub>2</sub>SO<sub>4</sub> solution containing organic compounds (i<sub>total</sub>). The step originates from the oxidation of the organic compounds.</p></caption>
<graphic xlink:href="fmats-06-00238-g0006.tif"/>
</fig>
<p>According to Equations (2), (5), and (6), I<sub>net</sub> can be given by:</p>
<disp-formula id="E7"><label>(7)</label><mml:math id="M7"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mtext mathvariant="normal">I</mml:mtext></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mi>e</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>2</mml:mn><mml:mo>.</mml:mo><mml:mn>30</mml:mn><mml:mfrac><mml:mrow><mml:mi>k</mml:mi><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mi>q</mml:mi></mml:mrow></mml:mfrac><mml:mo>log</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>C</mml:mi><mml:mi>O</mml:mi><mml:mi>D</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>A</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>&#x0002B;</mml:mo><mml:msub><mml:mrow><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mtext mathvariant="normal">blank</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>R</mml:mi></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<disp-formula id="E8"><label>(8)</label><mml:math id="M8"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:mo>=</mml:mo></mml:mtd><mml:mtd><mml:mfrac><mml:mrow><mml:mn>2</mml:mn><mml:mo>.</mml:mo><mml:mn>30</mml:mn><mml:mfrac><mml:mrow><mml:mtext mathvariant="normal">k</mml:mtext><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mtext mathvariant="normal">nq</mml:mtext></mml:mrow></mml:mfrac><mml:mo>log</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>C</mml:mi><mml:mi>O</mml:mi><mml:mi>D</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mi>R</mml:mi></mml:mrow></mml:mfrac><mml:mo>&#x0002B;</mml:mo><mml:mi>A</mml:mi></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<disp-formula id="E9"><label>(9)</label><mml:math id="M9"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:mo>=</mml:mo></mml:mtd><mml:mtd><mml:mi>&#x003B1;</mml:mi><mml:mo>log</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>C</mml:mi><mml:mi>O</mml:mi><mml:mi>D</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>&#x0002B;</mml:mo><mml:mi>A</mml:mi></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Where both &#x003B1; and A are constant. The I<sub>net</sub> possess linear relationship with the logarithm of the COD value.</p>
</sec>
<sec>
<title>COD Sensing Properties</title>
<p>Photogenerated hole is a strong oxidant for degradation of organic compounds during the process of photocatalytic oxidation. The combination of photogenerated electrons and holes often limits the degradation efficiency. However, the addition of a bias voltage can transfer photogenerated electrons to the internal circuit, thereby improving the degradation efficiency (Zheng et al., <xref ref-type="bibr" rid="B28">2008</xref>). In order to find the proper applied bias, the effect of applied bias on net current is studied under different bias conditions (Li et al., <xref ref-type="bibr" rid="B10">2014</xref>), as shown in <xref ref-type="fig" rid="F7">Figure 7A</xref>. The determined I<sub>net</sub> values are lower than that the applied bias value is above 1 V, however, the obtained I<sub>net</sub> values are not fluctuation when the applied voltages are between 1.0 and 1.5 V. In all the experiments, the applied bias 1.5 V was chosen as the proper voltage. In addition, the current signal is influenced by the large solution resistance due to the solution channel in the thin-layer reactor. The influence of supporting electrolyte concentration on the generated photocurrent is also studied. In <xref ref-type="fig" rid="F7">Figure 7B</xref>, the current rises with the increase of conductive ions at a certain concentration range. The current reaches its saturation value at higher electrolyte concentration. Thus, 0.2 mM Na<sub>2</sub>SO<sub>4</sub> was selected as the optimal supporting electrolyte concentration.</p>
<fig id="F7" position="float">
<label>Figure 7</label>
<caption><p>Optimization of the real-time on-line sensing system: effect of <bold>(A)</bold> applied voltage and <bold>(B)</bold> supporting electrolyte concentration on photocurrent.</p></caption>
<graphic xlink:href="fmats-06-00238-g0007.tif"/>
</fig>
<p>In order to validate the proposed COD analysis principle, some pure organic compounds such as glucose and sucrose and synthetic sample (GGA) were chosen as the representative organic compounds. Chronoamperometric experiments were performed via injecting various molar concentration organic compounds at a constant applied bias V &#x0003D; 1.5 V with UV light. When various concentration organic compounds were added, the rapidly raising photocurrent responses were obtained and then recorded by the electrochemical workstation (Zahner zennium, Germany). The relationship between I<sub>net</sub> and molar concentration of individual organic compounds with equal COD values of each is presented in <xref ref-type="fig" rid="F8">Figure 8A</xref>. In addition, the relationship between I<sub>net</sub> and the equivalent theoretical COD values converted from the molar concentrations of organic compounds ([COD] &#x0003D; 8000nC<sub>m</sub>) were deduced in <xref ref-type="fig" rid="F8">Figure 8B</xref>. In the figure, I<sub>net</sub> possess linear relationship with the logarithm of the organic compound concentrations studied in this paper. The plots display that the investigated organic compounds are fitted into a line y &#x0003D; 0.000887 log(x) &#x02013; 3.22&#x000D7;10<sup>&#x02212;4</sup> (where y represents I<sub>net</sub> obtained from organics oxidation, x represents the COD value of the organics) with <italic>R</italic><sup>2</sup> &#x0003D; 0.975, indicating the proportional relationship between the I<sub>net</sub> and the COD value for the 3D Au-NPs/TNTAs COD sensing system. Furthermore, a wide working linear range from 1.92 to 3,360 mg L<sup>&#x02212;1</sup> were obtained. The proposed COD sensing system also possess a detection limit of 0.18 mg L<sup>&#x02212;1</sup> COD (S/N&#x0003D;3).</p>
<fig id="F8" position="float">
<label>Figure 8</label>
<caption><p>Verification of analysis principle: <bold>(A)</bold> the correlation of I<sub>net</sub> and molar concentrations of selected organic compounds; <bold>(B)</bold> the relationship between I<sub>net</sub> and the theoretical COD values of the selected organic compounds.</p></caption>
<graphic xlink:href="fmats-06-00238-g0008.tif"/>
</fig>
</sec>
<sec>
<title>Reproducibility and Operational Stability of the Proposed Sensing System</title>
<p>The reproducibility of the photoelectrochemical sensor was assessed by measuring the current signal at 19.2 mg/L COD (Yao et al., <xref ref-type="bibr" rid="B23">2015</xref>). The relative standard deviation was 2.5% for 11 determinations, suggesting excellent reproducibility. To study the long-term stability about the proposed sensing system, response photocurrent to 0.1 mM glucose (theoretical COD value 19.2 mg/L) was measured during 10 days period. The RSD is 3.7%, showing good stability of the sensing system.</p>
</sec>
</sec>
<sec sec-type="conclusions" id="s4">
<title>Conclusions</title>
<p>A real-time on-line sensing system combining with 3D Au-NPs/TNTAs sensing electrode and photoelectrochemical reactor is proposed toward the determination of COD, which is on account of the relationship between the COD values and the quantity captured charge applying the photoelelctrocatalytic method. In the photoelectrochemical experiments, the optimum conditions such as applied bias and supporting electrolyte were investigated. Glucose, sucrose and GGA were chosen as the representative organic compounds to validated the proposed sensing principle. The sensing photocurrent presents a linear relationship with the logarithm of COD values. The proposed sensing system shows a detection limit of 0.18 mg/L with the linear range from 1.96 to 3,360 mg/L.</p>
</sec>
<sec sec-type="data-availability-statement" id="s5">
<title>Data Availability Statement</title>
<p>All datasets generated for this study are included in the manuscript/<xref ref-type="sec" rid="s7">Supplementary Files</xref>.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>HS designed and conducted the experiments and analyzed the results. XZ prepared the bare 3D TNTAs nanotube arrays. SL revised, read, and approved the submitted version.</p>
<sec>
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</sec>
</body>
<back>
<sec sec-type="supplementary-material" id="s7">
<title>Supplementary Material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fmats.2019.00238/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmats.2019.00238/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Data_Sheet_1.pdf" id="SM1" mimetype="application/pdf" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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<fn-group>
<fn fn-type="financial-disclosure"><p><bold>Funding.</bold> This work was supported by the National Natural Science Foundation of China (Grant No. 61764003), Major Science and Technology Planning Project of Hainan Province (ZDKJ201810).</p>
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