<?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">OPJ</journal-id><journal-title-group><journal-title>Optics and Photonics Journal</journal-title></journal-title-group><issn pub-type="epub">2160-8881</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/opj.2017.78B015</article-id><article-id pub-id-type="publisher-id">OPJ-78306</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Study on the Concentration Inversion of NO &amp; NO2 Gas from the Vehicle Exhaust Based on Weighted PLS
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kai</surname><given-names>Zhang</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>Yujun</surname><given-names>Zhang</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>Kun</surname><given-names>You</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>Yibing</surname><given-names>Lu</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>Qixing</surname><given-names>Tang</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>Ying</surname><given-names>He</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>Guohua</surname><given-names>Liu</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>Boqiang</surname><given-names>Fan</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>Dongqi</surname><given-names>Yu</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>Wenqing</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei, China</addr-line></aff><pub-date pub-type="epub"><day>10</day><month>08</month><year>2017</year></pub-date><volume>07</volume><issue>08</issue><fpage>106</fpage><lpage>115</lpage><history><date date-type="received"><day>July</day>	<month>4,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>August</month>	<year>7,</year>	</date><date date-type="accepted"><day>August</day>	<month>10,</month>	<year>2017</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>
 
 
  
    It becomes a key technology to measure the concentration of the vehicle exhaust components with the absorption spectra. But because of the overlap of gas absorption bands, how to separate the absorption information of each component gas from the mixed absorption spectra has become the key point to restrict the precision of the optical detection method. In this paper, the ex-perimental platform for the absorption spectrum of vehicle exhaust components has been established. Based on the ultraviolet absorption spectra measured with the platform of exhaust gas NO &amp; NO2, the concentration regression model for the two components has been established with weighted partial least squares regression (WPLS). Finally the each spectral characteristic information of NO &amp; NO2 gas has been separated and the concentration of each corresponding component has been reversed successfully. 
  
 
</p></abstract><kwd-group><kwd>Absorption Spectra</kwd><kwd> NO &amp; NO2 Gas</kwd><kwd> Weighted Partial Least Squares  Regression</kwd><kwd> Concentration Inversion</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Nowadays the vehicle exhaust emissions have become one of the most important factors that affect the environmental air quality in our country. Therefore, it is urgent to strengthen the monitoring of vehicle exhaust emissions [<xref ref-type="bibr" rid="scirp.78306-ref1">1</xref>].</p><p>It becomes a key technology to measure the concentration of the vehicle exhaust components with the absorption spectra. But because of the overlap of gas absorption bands, how to separate the absorption information of each component gas from the mixed absorption spectra has become the key point to restrict the precision of the optical detection method [<xref ref-type="bibr" rid="scirp.78306-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.78306-ref3">3</xref>]. In this paper, based on the measured ultraviolet absorption spectra of exhaust gas NO &amp; NO<sub>2</sub>, the concentration regression models for the two components has been established with weighted partial least squares regression (WPLS). Finally the each spectral characteristic information of NO &amp; NO<sub>2</sub> gas has been separated and the concentration of each corresponding component has been reversed successfully.</p></sec><sec id="s2"><title>2. Weighted Partial Least Squares Regression: PLS</title><sec id="s2_1"><title>2.1. Partial Least Squares Regression</title><p>The partial least squares regression is multivariate statistical analysis method which is widely used. It focuses on multivariate regression modeling of multiple variables. The technology for synthesis and screening of information is used in PLS modeling process, combined with the functions of multivariate linear regression analysis, typical correlation analysis and principal component analysis [<xref ref-type="bibr" rid="scirp.78306-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.78306-ref5">5</xref>]. Then the modeling method of partial least squares regression using in the spectral analysis is introduced.</p><p>The spectral response matrix Y and its corresponding gas concentration matrix X are simultaneously decomposed into principal components, and new synthetic variables are obtained as follows:</p><disp-formula id="scirp.78306-formula73"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x2.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78306-formula74"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x3.png"  xlink:type="simple"/></disp-formula><p>where T &amp; U are load matrixes of X &amp; Y respectively, and P &amp; Q are scoring matrixes of X &amp; Y respectively. E &amp; F are the errors introduced by using PLS method to fit X &amp; Y respectively.</p><p>The regression model is built with PLS, which uses the characteristic spectral response matrix T and the characteristic concentration matrix U of which the vectors are orthogonal to each other.</p><disp-formula id="scirp.78306-formula75"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x4.png"  xlink:type="simple"/></disp-formula><p>The regression coefficient matrix B is as follows, which is also called the correlation matrix.</p><disp-formula id="scirp.78306-formula76"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x5.png"  xlink:type="simple"/></disp-formula><p>Therefore, the main steps of PLS include the principal component decomposition for the variable matrix Y and the corresponding independent variable matrix X, and the calculation of the correlation matrix B.</p></sec><sec id="s2_2"><title>2.2. Weighted Partial Least Squares (WPLS)</title><p>Although the PLS method has more advantages than the traditional multivariate regression method, there is still low efficiency when analyzing the absorption spectra of multi-component gas, and the accuracy of the regression results is affected by the noise and sample distribution [<xref ref-type="bibr" rid="scirp.78306-ref6">6</xref>]. In order to improve the prediction accuracy, it is necessary to assign different weights to the samples in calibration sets. By analyzing the error and recovery rate of the calibration sets, the partial least squares (PLS) method can be further improved to into the error weighted partial least squares (EWPLS) and the variance weighted partial least squares (VWPLS) [<xref ref-type="bibr" rid="scirp.78306-ref7">7</xref>].</p><p>Assume that Y<sub>c</sub> Є R<sup>M*K</sup> is the concentration matrix of the calibration set calculated by the PLS method, then the error of the recovery rate can be obtained as the following</p><disp-formula id="scirp.78306-formula77"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x6.png"  xlink:type="simple"/></disp-formula><p>where“./”represents the division between the corresponding elements of matrices. E<sub>c</sub> Є R<sup>M*K</sup> represents the recovery rate errors of K organic matters in M calibration samples. If {r<sub>1</sub>, r<sub>2</sub>, …, r<sub>M</sub>} is composed of the maximum error of the recovery rate of every row in E<sub>c</sub>, the Gauss weight corresponding to the maximum error of the recovery rate is set as follows.</p><disp-formula id="scirp.78306-formula78"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x7.png"  xlink:type="simple"/></disp-formula><p>where α is the step adjustment parameter and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x8.png" xlink:type="simple"/></inline-formula> is the weight vector of the M calibration samples. The predictive results can be improved to some extent by adjusting the maximum error of the recovery rate. In addition, the weight vector of the PLS method can also be constructed by the variance of the recovery rate. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x9.png" xlink:type="simple"/></inline-formula> represents the variance of the recovery rate in E<sub>c</sub>, then the Gauss weight is as follows.</p><disp-formula id="scirp.78306-formula79"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x10.png"  xlink:type="simple"/></disp-formula><p>where β is the step adjustment parameter and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x11.png" xlink:type="simple"/></inline-formula> is the variance weight vector of the recovery rate. Then the ﬂuorescence intensity matrix and the concentration matrix can be updated by the weight vector.</p><disp-formula id="scirp.78306-formula80"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78306x12.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x13.png" xlink:type="simple"/></inline-formula> is a diagonal matrix and the diagonal elements are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x14.png" xlink:type="simple"/></inline-formula>. And the new calibration sets X<sub>cr</sub> and Y<sub>cr</sub> are produced. Similarly, if the calibration sets are modiﬁed by the weight vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x15.png" xlink:type="simple"/></inline-formula> the new calibration sets X<sub>cv</sub> and Y<sub>cv</sub> can also be obtained. Next the EWPLS method is carried out as follows as an example.</p><p>1) Set initial vector u, calculate the weight w of X<sub>cr</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x16.png" xlink:type="simple"/></inline-formula>, calculate the score matrix t of X<sub>cr</sub>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x17.png" xlink:type="simple"/></inline-formula>.</p><p>2) calculate the weight c of Y<sub>cr</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x18.png" xlink:type="simple"/></inline-formula>, calculate the score matrix u of Y<sub>cr</sub>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x19.png" xlink:type="simple"/></inline-formula>.</p><p>3) If the convergence<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x20.png" xlink:type="simple"/></inline-formula>, has not reached, return to Steps 1 and 2, and otherwise continue with Step 4;</p><p>4) Remove the calculated components from X<sub>cr</sub>, Y<sub>cr</sub>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x21.png" xlink:type="simple"/></inline-formula>.</p><p>5) Return to Step 1, until all the components are extracted.</p><p>6) According to Equation (4), calculate the regression factor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x22.png" xlink:type="simple"/></inline-formula>, then calculate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x23.png" xlink:type="simple"/></inline-formula>.</p><p>7) If the convergence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x24.png" xlink:type="simple"/></inline-formula> has not reached, calculate W<sub>r</sub>, X<sub>cr</sub>, Y<sub>cr</sub>, return to Step 1, Otherwise continue with Step 8.</p><p>8) calculate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78306x25.png" xlink:type="simple"/></inline-formula>.</p></sec></sec><sec id="s3"><title>3. NO and NO<sub>2</sub> Feature Extraction and Concentration Inversion Experiments Based on WPLS</title><p>The UV absorption cross-sections of NO and NO<sub>2</sub> gas within the 180 nm - 400 nm band are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. It shows a single peak absorption phenomenon of NO gas, which has a strong absorption peak at 205 nm, 215 nm and 225 nm. NO’s absorption cross-section is at 10<sup>−19</sup> magnitude orders. While it shows a continuous absorption phenomenon of NO<sub>2</sub> within 200 nm - 225 nm and 350 nm - 430 nm band, and the absorption cross-section magnitude is the same as NO. This will directly lead to the overlapping absorption of the two components and affect the concentration inversion of each single component seriously. So in this paper WPLS algorithm has been used to establish regression models to eliminate the interference and separate the independent components accurately.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Absorption cross-sections of NO &amp; NO<sub>2</sub> in the near UV band</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x26.png"/></fig><sec id="s3_1"><title>3.1. Acquisition of NO &amp; NO<sub>2</sub> Absorption Spectra from the Vehicle Exhaust</title><p>As shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>, the experimental platform for absorption spectra acquisition of NO<sub>X</sub> from the vehicle exhaust has been built. It’s composed of a gas distribution unit and a measuring unit. The gas distribution unit can mix two gases of different concentrations with a precision of 1%. And the measuring unit consists of a flashing xenon lamp, an ultraviolet spectrometer, a sample gas chamber and a data processing terminal and so on, which can measure the ultraviolet spectrum data of the sample gas effectively at a certain temperature and pressure.</p><p>In order to avoid multicollinearity, the orthogonal principle is followed in the sample concentration design for NO &amp; NO<sub>2</sub>. Samples of different concentration are designed as shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Then a series of designed NO or NO<sub>2</sub> UV absorption spectra (200 nm - 440 nm) of different concentrations have been obtained with the platform, also with their mixture absorption spectra. The NO absorption spectra of different concentrations are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a), meanwhile the NO<sub>2</sub> absorption spectra of different concentrations are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(c) also with a series of their mixture absorption spectra in <xref ref-type="fig" rid="fig3">Figure 3</xref>(d).</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Designed concentration of NO and NO<sub>2</sub> sample gas</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Single NO<sub>2</sub></th><th align="center" valign="middle" >Single NO</th><th align="center" valign="middle" >Single NO</th><th align="center" valign="middle"  colspan="2"  >Mixed NO &amp; NO<sub>2</sub></th></tr></thead><tr><td align="center" valign="middle" >608</td><td align="center" valign="middle" >308</td><td align="center" valign="middle" >2549</td><td align="center" valign="middle" >1022</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >547.2</td><td align="center" valign="middle" >277.2</td><td align="center" valign="middle" >2294.1</td><td align="center" valign="middle" >919.8</td><td align="center" valign="middle" >254.9</td></tr><tr><td align="center" valign="middle" >516.8</td><td align="center" valign="middle" >261.8</td><td align="center" valign="middle" >2166.65</td><td align="center" valign="middle" >868.7</td><td align="center" valign="middle" >382.35</td></tr><tr><td align="center" valign="middle" >486.4</td><td align="center" valign="middle" >246.4</td><td align="center" valign="middle" >2039.2</td><td align="center" valign="middle" >817.6</td><td align="center" valign="middle" >509.8</td></tr><tr><td align="center" valign="middle" >456</td><td align="center" valign="middle" >231</td><td align="center" valign="middle" >1911.75</td><td align="center" valign="middle" >766.5</td><td align="center" valign="middle" >637.25</td></tr><tr><td align="center" valign="middle" >425.6</td><td align="center" valign="middle" >215.6</td><td align="center" valign="middle" >1784.3</td><td align="center" valign="middle" >715.4</td><td align="center" valign="middle" >764.7</td></tr><tr><td align="center" valign="middle" >395.2</td><td align="center" valign="middle" >200.2</td><td align="center" valign="middle" >1656.85</td><td align="center" valign="middle" >664.3</td><td align="center" valign="middle" >892.15</td></tr><tr><td align="center" valign="middle" >364.8</td><td align="center" valign="middle" >184.8</td><td align="center" valign="middle" >1529.4</td><td align="center" valign="middle" >613.2</td><td align="center" valign="middle" >1019.6</td></tr><tr><td align="center" valign="middle" >334.4</td><td align="center" valign="middle" >169.4</td><td align="center" valign="middle" >1401.95</td><td align="center" valign="middle" >562.1</td><td align="center" valign="middle" >1147.05</td></tr><tr><td align="center" valign="middle" >304</td><td align="center" valign="middle" >154</td><td align="center" valign="middle" >1274.5</td><td align="center" valign="middle" >511</td><td align="center" valign="middle" >1274.5</td></tr><tr><td align="center" valign="middle" >273.6</td><td align="center" valign="middle" >138.6</td><td align="center" valign="middle" >1147.05</td><td align="center" valign="middle" >459.9</td><td align="center" valign="middle" >1401.95</td></tr><tr><td align="center" valign="middle" >243.2</td><td align="center" valign="middle" >123.2</td><td align="center" valign="middle" >1019.6</td><td align="center" valign="middle" >408.8</td><td align="center" valign="middle" >1529.4</td></tr><tr><td align="center" valign="middle" >212.8</td><td align="center" valign="middle" >107.8</td><td align="center" valign="middle" >892.15</td><td align="center" valign="middle" >357.7</td><td align="center" valign="middle" >1656.85</td></tr><tr><td align="center" valign="middle" >182.4</td><td align="center" valign="middle" >92.4</td><td align="center" valign="middle" >764.7</td><td align="center" valign="middle" >306.6</td><td align="center" valign="middle" >1784.3</td></tr><tr><td align="center" valign="middle" >152</td><td align="center" valign="middle" >77</td><td align="center" valign="middle" >637.25</td><td align="center" valign="middle" >255.5</td><td align="center" valign="middle" >1911.75</td></tr><tr><td align="center" valign="middle" >121.6</td><td align="center" valign="middle" >61.6</td><td align="center" valign="middle" >509.8</td><td align="center" valign="middle" >204.4</td><td align="center" valign="middle" >2039.2</td></tr><tr><td align="center" valign="middle" >91.2</td><td align="center" valign="middle" >46.2</td><td align="center" valign="middle" >382.35</td><td align="center" valign="middle" >153.3</td><td align="center" valign="middle" >2166.65</td></tr><tr><td align="center" valign="middle" >60.8</td><td align="center" valign="middle" >30.8</td><td align="center" valign="middle" >254.9</td><td align="center" valign="middle" >102.2</td><td align="center" valign="middle" >2294.1</td></tr></tbody></table></table-wrap><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Schematic diagram of the experimental platform for NO<sub>X</sub> spectra acquisition</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x27.png"/></fig><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Absorption spectra of NO &amp; NO<sub>2</sub> at different concentrations. (a) NO absorption spectra (29 samples); (b) NO<sub>2</sub> absorption spectra (20 samples, 198 - 229 nm); (c) NO<sub>2</sub> absorption spectra (20 samples, 299 - 439 nm); (d) mixed absorption spectra.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x28.png"/></fig><fig id ="fig3_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x29.png"/></fig><fig id ="fig3_3"><label> (d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x30.png"/></fig><fig id ="fig3_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x31.png"/></fig></fig-group></sec><sec id="s3_2"><title>3.2. Experiments and Result Analysis</title><p>Here, the concentration inversion of NO and NO<sub>2</sub> components from the vehicle exhaust with ultraviolet absorption spectrum based on WPLS is actually a partial least squares regression problem with three independent variables and two dependent variables, as shown in <xref ref-type="table" rid="table2">Table 2</xref>. The regression equation of Y<sub>1</sub> - Y<sub>2</sub> for X<sub>1</sub> - X<sub>3</sub> should be established to determine the relationship between the concentration of the two components gas, Y and their absorbance, X.</p><p>According to Steps 1-8 in 2.2, a data processing program has been compiled with MATLAB, and then the regression models have been established with the obtained spectral sample data from which one spectral data has been selected and taken out, then the concentration have been inversed by put the selected spectral data into the model. That’s the same with every concentration. Finally the experimental results are shown in Figures 4-9.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Experimental results of pure NO spectra (28 samples for modeling and 1 sample for prediction)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x32.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Experimental results of pure NO<sub>2</sub> spectra (19 samples for modeling and 1 sample for prediction)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x33.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Experimental results of NO &amp; NO<sub>2</sub> mixed spectra (19 samples for modeling and 1 sample for prediction)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x34.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Experimental results of pure NO and mixed spectra (48 samples for modeling and 1 sample for prediction)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x35.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Experimental results of pure NO<sub>2</sub> and mixed spectra (39 samples for modeling and 1 sample for prediction)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x36.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Experimental results of pure NO, pure NO<sub>2</sub> and their mixed spectra (68 samples for modeling and 1 sample for prediction)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78306x37.png"/></fig><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> WPLS independent and dependent variables</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >WPLS independent variable</th><th align="center" valign="middle" >X<sub>1</sub>-NO<sub>2</sub><sub> </sub> absorbance</th><th align="center" valign="middle"  colspan="2"  >X<sub>2</sub>-NO absorbance</th><th align="center" valign="middle" >X<sub>3</sub>-NO, NO<sub>2</sub><sub> </sub> Mixed absorbance</th></tr></thead><tr><td align="center" valign="middle" >WPLS dependent variable</td><td align="center" valign="middle"  colspan="2"  >Y<sub>1</sub>-NO concentration</td><td align="center" valign="middle"  colspan="2"  >Y<sub>2</sub>-NO<sub>2</sub> concentration</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>As seen from the above experimental results, using either the spectra of the individual components of NO or NO2 or mixed spectra of the two components or even all the individual and mixed spectra for the regression modeling and concentration inversion based on WPLS, the experimental results are all excellent.</p><p>The approximation between the inversion results and real sample concentration are all above 99.4%, of which the highest can reach 99.97%. So it can be concluded that with WPLS algorithm the components’ characteristics of the mixed spectral in which there’re overlapped absorption with NO &amp; NO<sub>2</sub> can be separated, and then each concentration of the samples can be inversed accurately.</p><p>In this experiment, It’s not considered that the modeling optimization [<xref ref-type="bibr" rid="scirp.78306-ref6">6</xref>], the inversion band and spectral data denoising [<xref ref-type="bibr" rid="scirp.78306-ref8">8</xref>]. The spectral data used here in WPLS are the direct output of the spectrometer, of which the band is the whole detecting range of the spectrometer (its wavelength range: 198 - 438 nm, a total of 3648 sampling points). Meanwhile in the whole mixed spectra, there’re not overlapped absorption at all sampling points, and there are also many places with zero absorbance, which will affect the accuracy of WPLS modeling.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>Be aimed at the interference caused by spectral overlap absorption in the vehicle exhaust gas concentration detection with spectra method, the experimental platform for absorption spectrum detection of exhaust gas has been built. On the basis of measuring the ultraviolet absorption spectra of exhaust components NO and NO<sub>2</sub>, the weighted partial least squares regression (WPLS) algorithm has been used and then regression models of the components’ concentration have been established, finally each NO or NO<sub>2</sub> concentration of the mixed gas samples has been inverted successfully. From the experimental results, under the condition without the original spectral denoising and WPLS modeling band optimization, the approximation of the concentration inversion results and the real samples can reach more than 99.4%.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The work is supported by the National Key Research and Development Program of China (2016YFC0201003) &amp; the 863 National High Technology Research and Development Program of China (No. 2014AA06A503).</p></sec><sec id="s6"><title>Cite this paper</title><p>Zhang, K., Zhang, Y.J., You, K., Lu, Y.B., Tang, Q.X., He, Y., Liu, G.H., Fan, B.Q., Yu, D.Q. and Liu, W.Q. (2017) Study on the Concentration Inversion of NO &amp; NO<sub>2</sub> Gas from the Vehicle Exhaust Based on Weighted PLS. Optics and Photonics Journal, 7, 106-115. https://doi.org/10.4236/opj.2017.78B015</p></sec></body><back><ref-list><title>References</title><ref id="scirp.78306-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">(2016) Environmental Status Bulletin of China in 2015 (Excerpt). Environmental Protection, No. 11, 43-51.</mixed-citation></ref><ref id="scirp.78306-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Wang, Y.J. (2016) Monitoring of Mixture Gas Concentration of SO2 and NO Based on Ultraviolet Absorption Spectroscopy. Chong-qing University, Chongqing.</mixed-citation></ref><ref id="scirp.78306-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Sun, Y.T. and Zhang, H.T. (2015) Real-Time Monitoring of the Concentration of SO2 and H2S in Mixed Gases Based on Ultraviolet Absorption Spectroscopy. 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