<?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">ABC</journal-id><journal-title-group><journal-title>Advances in Biological Chemistry</journal-title></journal-title-group><issn pub-type="epub">2162-2183</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/abc.2020.101001</article-id><article-id pub-id-type="publisher-id">ABC-98152</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>
 
 
  DFT-Based Prediction of Bioconcentration Factors of Polychlorinated Biphenyls in Fish Species Using Molecular Descriptors
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Anil</surname><given-names>Kumar Soni</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>Pratibha</surname><given-names>Singh</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vishnu</surname><given-names>Kumar Sahu</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Department of Chemistry, Maharani Lal Kunwari Post Graduate College, Balrampur, India</addr-line></aff><aff id="aff1"><addr-line>Department of Chemistry, Shia Post Graduate College, Lucknow, India</addr-line></aff><aff id="aff2"><addr-line>Department of Chemistry, Saket Post Graduate College, Ayodhya, India</addr-line></aff><pub-date pub-type="epub"><day>05</day><month>02</month><year>2020</year></pub-date><volume>10</volume><issue>01</issue><fpage>1</fpage><lpage>15</lpage><history><date date-type="received"><day>27,</day>	<month>December</month>	<year>2019</year></date><date date-type="rev-recd"><day>3,</day>	<month>February</month>	<year>2020</year>	</date><date date-type="accepted"><day>6,</day>	<month>February</month>	<year>2020</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>
 
 
  Experimental determination of BCFs is expensive and demanding if performed correctly. Because of this, measuring the BCFs of many thousands of chemical substances that are potential regulatory interest is simply not possible. Hence, prediction of BCFs of the PCBs based on QSAR w
  ere
   made time to time to increase the probability of success and reduce the time and cost in exploring the toxicological and ecological characteristics of molecules. DFT methods are, in general, capable of generating a variety of isolated molecular descriptors as well as local reactivity descriptors quite accurately. In this work, prediction of BCFs of the fifty seven PCBs based on quantum chemical descriptors derived from DFT method using the B88-PW91 GGA energy function with the DZVP basis set ha
  ve
   been made. The study concluded that dipole moment and ionization potential are reliable descriptors for correlation of bioconcentration factors of polychlorinated biphenyls with their electronic structures. The resulted QSAR model (r<sup>2</sup> = 0.9139, 
  
   
   = 0.8986, k = 2
  , SE = 0.2668) can be useful for predicting the BCFs of compounds prior to their synthesis.
 
</p></abstract><kwd-group><kwd>PCBs</kwd><kwd> QSAR</kwd><kwd> DFT</kwd><kwd> Quantum Chemical Descriptors</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In our recent communication [<xref ref-type="bibr" rid="scirp.98152-ref1">1</xref>], we have employed atomic descriptors derived from density functional theory (DFT) based methods to predict the bioconcentration factor (BCF) of polychlorinated biphenyls (PCBs) in fish. PCBs belong to important group of environmental pollutants, which were industrially used as dielectric fluids in transformers and capacitors, as hydraulic and heat transfer fluids, and as plasticizers [<xref ref-type="bibr" rid="scirp.98152-ref2">2</xref>]. These chemicals were either washed down into the soil or into the water bodies [<xref ref-type="bibr" rid="scirp.98152-ref3">3</xref>]. From the soil, these are absorbed by the plants along with water and minerals, and from the water bodies, these are taken up by aquatic plants and animals [<xref ref-type="bibr" rid="scirp.98152-ref4">4</xref>]. This is one of the ways in which they enter the food chain [<xref ref-type="bibr" rid="scirp.98152-ref5">5</xref>]. As these chemicals are not degradable, these get accumulated progressively at each tropic level [<xref ref-type="bibr" rid="scirp.98152-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref8">8</xref>]. As human beings occupy the top level in any food chains, the maximum concentration of these chemicals gets accumulated in our bodies [<xref ref-type="bibr" rid="scirp.98152-ref9">9</xref>] - [<xref ref-type="bibr" rid="scirp.98152-ref14">14</xref>]. Fish are the principal target organisms of BCF assessment due to their relevance as food for many species including humans and the availability of standardized testing protocols [<xref ref-type="bibr" rid="scirp.98152-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref17">17</xref>]. In general, however, experimental determination of BCFs is expensive and demanding if performed correctly. Hence, a number of QSAR based study of BCFs of the PCBs were made time to time [<xref ref-type="bibr" rid="scirp.98152-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref18">18</xref>] - [<xref ref-type="bibr" rid="scirp.98152-ref34">34</xref>] because QSAR technique [<xref ref-type="bibr" rid="scirp.98152-ref35">35</xref>] increases the probability of success and reduce the time and cost in exploring the toxicological and ecological characteristics of molecules. A number of quantum chemical descriptors [<xref ref-type="bibr" rid="scirp.98152-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref38">38</xref>] have been identified in the framework of QSAR. In the present work, we present the DFT based derived quantum chemical descriptor to correlate the BCF of PCBs.</p></sec><sec id="s2"><title>2. Theory</title><p>In 1960s, Hohenberg and Khon put forward two basic theorems to which DFT is based on and its performance in the description of structure, energetic, and magnetic molecular properties has been quite substantially reviewed time to time [<xref ref-type="bibr" rid="scirp.98152-ref39">39</xref>] - [<xref ref-type="bibr" rid="scirp.98152-ref46">46</xref>]. DFT methods are, in general, capable of generating a variety of isolated molecular properties, such as dipole moment, ionization energy, electron affinity, electronegativity, hardness, softness, electrophilicity index, etc., quite accurately [<xref ref-type="bibr" rid="scirp.98152-ref47">47</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref48">48</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref49">49</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref50">50</xref>]. Here, following seven quantum chemical descriptors based on DFT method [<xref ref-type="bibr" rid="scirp.98152-ref39">39</xref>] have been tested and the final QSAR model was constructed with the help of significant descriptors. A concise description of these descriptors is as below.</p><p>The dipole moment is used to describe the polarity of the molecule [<xref ref-type="bibr" rid="scirp.98152-ref47">47</xref>] The dipole moment, μ, of a molecule is the vector sum of the dipole moments of the bonds and is calculated according to the rule of vector addition. If two bonds with the dipole moments P and Q are at an angle θ the total dipole moment is given by</p><p>μ 2 = P 2 + Q 2 + 2 P Q cos θ (1)</p><p>For instance, two identical bonds with the opposite directions (θ = 180˚) have μ = 0. For identical bonds (P = Q) Equation (1) yields</p><p>μ 2 = 2 P 2 ( 1 + cos θ ) (1a)</p><p>Ionization energy (IE), electron affinity (EA), electronegativity (χ), hardness (η) and softness (S) are defined as [<xref ref-type="bibr" rid="scirp.98152-ref48">48</xref>] [<xref ref-type="bibr" rid="scirp.98152-ref49">49</xref>]</p><p>I E = E t o t ( A + ) − E t o t ( A ) (2)</p><p>E A = E t o t ( A ) − E t o t ( A − ) (3)</p><p>χ = − μ = − ( δ E / δ N ) v ( r ) (4)</p><p>η = 1 / 2 ( δ μ / δ N ) v ( r ) = 1 / 2 ( δ 2 E / δ N 2 ) v ( r ) (5)</p><p>S = 1 / 2 η (6)</p><p>where μ is chemical potential, E is the total energy, N is number of electrons of the chemical species and v(r) the external potential. The operation definition of electronegativity, hardness and global softness are defined as:</p><p>χ = − μ = ( I P + E A ) / 2 (4a)</p><p>η = 1 / 2 ( I P − E A ) (5a)</p><p>S = 1 / ( I P − E A ) (6a)</p><p>Parr et al. introduced the global electrophilicity index [<xref ref-type="bibr" rid="scirp.98152-ref50">50</xref>], in terms of chemical potential and hardness. The electrophilicity index, ω, is a reliable property of a chemical system and its operation definition is</p><p>ω = μ 2 / 2 η (7)</p></sec><sec id="s3"><title>3. Materials and Methods</title><p>Fifty seven PCB congeners listed in <xref ref-type="fig" rid="fig1">Figure 1</xref> are the study materials for the present study. These congeners were taken from the literature with their experimental logarithmic BCF values (LogBCF<sub>exp</sub>) for several fish species (guppies, fathead minnow, rainbow trout, and bluegill sunfish) [<xref ref-type="bibr" rid="scirp.98152-ref23">23</xref>]. For BCF prediction, the 3D modeling [<xref ref-type="bibr" rid="scirp.98152-ref51">51</xref>] and geometry optimization of all the compounds have been performed on workspace program of CAChe pro software of Fujitsu [<xref ref-type="bibr" rid="scirp.98152-ref52">52</xref>] using the B88-PW91 GGA energy function with the DZVP basis set. The values of various descriptors, such as dipole moment (μ), ionization energy (IE) and electron affinity (EA) have been directly obtained from DFT calculation results and have been tabulated in <xref ref-type="table" rid="table1">Table 1</xref>. However, the values of electronegativity (χ), hardness (η), softness (S) and electrophilicity index (ω) have been calculated by solving equations given in theory and the necessary values taken from DFT calculation results and have also been tabulated in <xref ref-type="table" rid="table1">Table 1</xref>. The Project Leader program associated with CAChe has been used for multiple linear regression (MLR) analysis [<xref ref-type="bibr" rid="scirp.98152-ref53">53</xref>] using leave-out method and various regression equations have been developed for prediction of BCF (LogBCF<sub>pre</sub>).</p></sec><sec id="s4"><title>4. Results and Discussion</title><p>The assessment of BCF of a hypothetical compound is of prime interest. The QSAR method saves time and cost in determining the BCF of a series of compounds with the help of BCF of previously known compounds. The biphenyl</p><p>and its fifty seven chloro-derivatives (mono-, di-, tri, tetra-, penta-, hexa-, hepta-, nona- and decachlorobiphenyl are one, eight, four, ten, nine, twelve, six, five and one in number, respectively) and their experimental logarithmic BCF values have been taken from the literature. A number of quantum chemical descriptors have been identified which are capable of successfully correlating the activity with the structure of a chemical system. The present study is based on seven</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Values of quantum chemical descriptors, experimental BCF and predicted BCF</title></caption><table-wrap id="1_1"><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >S.N.</th><th align="center" valign="middle"  rowspan="2"  >CAS NO</th><th align="center" valign="middle"  colspan="7"  >Descriptors</th><th align="center" valign="middle"  rowspan="2"  >LogBCF<sub>exp</sub></th><th align="center" valign="middle"  colspan="7"  >LogBCF<sub>pre</sub></th></tr></thead><tr><td align="center" valign="middle" >&#181;</td><td align="center" valign="middle" >IP</td><td align="center" valign="middle" >EA</td><td align="center" valign="middle" >χ</td><td align="center" valign="middle" >η</td><td align="center" valign="middle" >S</td><td align="center" valign="middle" >ω</td><td align="center" valign="middle" >Equation (8)</td><td align="center" valign="middle" >Equation (9)</td><td align="center" valign="middle" >Equation (10)</td><td align="center" valign="middle" >Equation (11)</td><td align="center" valign="middle" >Equation (12)</td><td align="center" valign="middle" >Equation (13)</td><td align="center" valign="middle" >Equation (14)</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >92-52-4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5.557</td><td align="center" valign="middle" >1.982</td><td align="center" valign="middle" >3.770</td><td align="center" valign="middle" >1.788</td><td align="center" valign="middle" >0.280</td><td align="center" valign="middle" >3.975</td><td align="center" valign="middle" >2.64</td><td align="center" valign="middle" >2.77</td><td align="center" valign="middle" >2.74</td><td align="center" valign="middle" >2.42</td><td align="center" valign="middle" >2.47</td><td align="center" valign="middle" >2.48</td><td align="center" valign="middle" >2.55</td><td align="center" valign="middle" >2.37</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2051-62-9</td><td align="center" valign="middle" >2.005</td><td align="center" valign="middle" >5.618</td><td align="center" valign="middle" >2.184</td><td align="center" valign="middle" >3.901</td><td align="center" valign="middle" >1.717</td><td align="center" valign="middle" >0.291</td><td align="center" valign="middle" >4.432</td><td align="center" valign="middle" >2.77</td><td align="center" valign="middle" >3.00</td><td align="center" valign="middle" >3.03</td><td align="center" valign="middle" >2.80</td><td align="center" valign="middle" >2.80</td><td align="center" valign="middle" >2.82</td><td align="center" valign="middle" >2.79</td><td align="center" valign="middle" >2.71</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >13029-08-8</td><td align="center" valign="middle" >3.141</td><td align="center" valign="middle" >5.809</td><td align="center" valign="middle" >2.427</td><td align="center" valign="middle" >4.118</td><td align="center" valign="middle" >1.691</td><td align="center" valign="middle" >0.296</td><td align="center" valign="middle" >5.014</td><td align="center" valign="middle" >3.38</td><td align="center" valign="middle" >3.72</td><td align="center" valign="middle" >3.77</td><td align="center" valign="middle" >3.77</td><td align="center" valign="middle" >3.74</td><td align="center" valign="middle" >3.74</td><td align="center" valign="middle" >3.65</td><td align="center" valign="middle" >3.69</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >16605-91-7</td><td align="center" valign="middle" >2.667</td><td align="center" valign="middle" >5.863</td><td align="center" valign="middle" >2.361</td><td align="center" valign="middle" >4.112</td><td align="center" valign="middle" >1.751</td><td align="center" valign="middle" >0.286</td><td align="center" valign="middle" >4.828</td><td align="center" valign="middle" >4.11</td><td align="center" valign="middle" >3.92</td><td align="center" valign="middle" >3.95</td><td align="center" valign="middle" >3.89</td><td align="center" valign="middle" >3.86</td><td align="center" valign="middle" >3.87</td><td align="center" valign="middle" >3.86</td><td align="center" valign="middle" >3.86</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >25569-80-6</td><td align="center" valign="middle" >3.442</td><td align="center" valign="middle" >5.893</td><td align="center" valign="middle" >2.395</td><td align="center" valign="middle" >4.144</td><td align="center" valign="middle" >1.749</td><td align="center" valign="middle" >0.286</td><td align="center" valign="middle" >4.909</td><td align="center" valign="middle" >3.80</td><td align="center" valign="middle" >4.04</td><td align="center" valign="middle" >4.09</td><td align="center" valign="middle" >4.03</td><td align="center" valign="middle" >3.99</td><td align="center" valign="middle" >4.00</td><td align="center" valign="middle" >4.04</td><td align="center" valign="middle" >4.08</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >33284-50-3</td><td align="center" valign="middle" >2.076</td><td align="center" valign="middle" >5.793</td><td align="center" valign="middle" >2.363</td><td align="center" valign="middle" >4.078</td><td align="center" valign="middle" >1.715</td><td align="center" valign="middle" >0.292</td><td align="center" valign="middle" >4.848</td><td align="center" valign="middle" >3.55</td><td align="center" valign="middle" >3.66</td><td align="center" valign="middle" >3.67</td><td align="center" valign="middle" >3.64</td><td align="center" valign="middle" >3.63</td><td align="center" valign="middle" >3.64</td><td align="center" valign="middle" >3.55</td><td align="center" valign="middle" >3.52</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >34883-43-7</td><td align="center" valign="middle" >2.713</td><td align="center" valign="middle" >5.774</td><td align="center" valign="middle" >2.367</td><td align="center" valign="middle" >4.071</td><td align="center" valign="middle" >1.704</td><td align="center" valign="middle" >0.294</td><td align="center" valign="middle" >4.863</td><td align="center" valign="middle" >3.57</td><td align="center" valign="middle" >3.59</td><td align="center" valign="middle" >3.62</td><td align="center" valign="middle" >3.65</td><td align="center" valign="middle" >3.62</td><td align="center" valign="middle" >3.62</td><td align="center" valign="middle" >3.53</td><td align="center" valign="middle" >3.57</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >34883-39-1</td><td align="center" valign="middle" >0.789</td><td align="center" valign="middle" >5.892</td><td align="center" valign="middle" >2.407</td><td align="center" valign="middle" >4.150</td><td align="center" valign="middle" >1.743</td><td align="center" valign="middle" >0.287</td><td align="center" valign="middle" >4.941</td><td align="center" valign="middle" >3.89</td><td align="center" valign="middle" >4.03</td><td align="center" valign="middle" >4.00</td><td align="center" valign="middle" >4.12</td><td align="center" valign="middle" >4.14</td><td align="center" valign="middle" >4.14</td><td align="center" valign="middle" >4.12</td><td align="center" valign="middle" >4.08</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >34883-41-5</td><td align="center" valign="middle" >2.414</td><td align="center" valign="middle" >5.951</td><td align="center" valign="middle" >2.428</td><td align="center" valign="middle" >4.190</td><td align="center" valign="middle" >1.762</td><td align="center" valign="middle" >0.284</td><td align="center" valign="middle" >4.982</td><td align="center" valign="middle" >3.78</td><td align="center" valign="middle" >4.26</td><td align="center" valign="middle" >4.27</td><td align="center" valign="middle" >4.35</td><td align="center" valign="middle" >4.33</td><td align="center" valign="middle" >4.34</td><td align="center" valign="middle" >4.37</td><td align="center" valign="middle" >4.41</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2050-68-2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5.677</td><td align="center" valign="middle" >2.369</td><td align="center" valign="middle" >4.023</td><td align="center" valign="middle" >1.654</td><td align="center" valign="middle" >0.302</td><td align="center" valign="middle" >4.893</td><td align="center" valign="middle" >3.28</td><td align="center" valign="middle" >3.22</td><td align="center" valign="middle" >3.18</td><td align="center" valign="middle" >3.23</td><td align="center" valign="middle" >3.28</td><td align="center" valign="middle" >3.28</td><td align="center" valign="middle" >3.06</td><td align="center" valign="middle" >2.95</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >37680-65-2</td><td align="center" valign="middle" >1.770</td><td align="center" valign="middle" >6.048</td><td align="center" valign="middle" >1.907</td><td align="center" valign="middle" >3.978</td><td align="center" valign="middle" >2.071</td><td align="center" valign="middle" >0.241</td><td align="center" valign="middle" >3.820</td><td align="center" valign="middle" >4.11</td><td align="center" valign="middle" >4.62</td><td align="center" valign="middle" >4.60</td><td align="center" valign="middle" >4.08</td><td align="center" valign="middle" >4.08</td><td align="center" valign="middle" >4.07</td><td align="center" valign="middle" >4.15</td><td align="center" valign="middle" >4.10</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >7012-37-5</td><td align="center" valign="middle" >1.295</td><td align="center" valign="middle" >5.828</td><td align="center" valign="middle" >2.537</td><td align="center" valign="middle" >4.183</td><td align="center" valign="middle" >1.646</td><td align="center" valign="middle" >0.304</td><td align="center" valign="middle" >5.315</td><td align="center" valign="middle" >4.20</td><td align="center" valign="middle" >3.79</td><td align="center" valign="middle" >3.78</td><td align="center" valign="middle" >4.04</td><td align="center" valign="middle" >4.05</td><td align="center" valign="middle" >4.04</td><td align="center" valign="middle" >3.84</td><td align="center" valign="middle" >3.87</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >15862-07-4</td><td align="center" valign="middle" >2.200</td><td align="center" valign="middle" >5.92</td><td align="center" valign="middle" >2.535</td><td align="center" valign="middle" >4.228</td><td align="center" valign="middle" >1.693</td><td align="center" valign="middle" >0.295</td><td align="center" valign="middle" >5.279</td><td align="center" valign="middle" >4.26</td><td align="center" valign="middle" >4.14</td><td align="center" valign="middle" >4.15</td><td align="center" valign="middle" >4.37</td><td align="center" valign="middle" >4.35</td><td align="center" valign="middle" >4.35</td><td align="center" valign="middle" >4.34</td><td align="center" valign="middle" >4.40</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >16606-02-3</td><td align="center" valign="middle" >1.168</td><td align="center" valign="middle" >5.927</td><td align="center" valign="middle" >2.581</td><td align="center" valign="middle" >4.254</td><td align="center" valign="middle" >1.673</td><td align="center" valign="middle" >0.299</td><td align="center" valign="middle" >5.409</td><td align="center" valign="middle" >4.23</td><td align="center" valign="middle" >4.17</td><td align="center" valign="middle" >4.14</td><td align="center" valign="middle" >4.37</td><td align="center" valign="middle" >4.39</td><td align="center" valign="middle" >4.39</td><td align="center" valign="middle" >4.26</td><td align="center" valign="middle" >4.27</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >38444-93-8</td><td align="center" valign="middle" >3.668</td><td align="center" valign="middle" >6.233</td><td align="center" valign="middle" >1.998</td><td align="center" valign="middle" >4.116</td><td align="center" valign="middle" >2.118</td><td align="center" valign="middle" >0.236</td><td align="center" valign="middle" >3.999</td><td align="center" valign="middle" >4.23</td><td align="center" valign="middle" >5.33<sup>a </sup></td><td align="center" valign="middle" >5.35<sup>a </sup></td><td align="center" valign="middle" >4.84</td><td align="center" valign="middle" >4.79</td><td align="center" valign="middle" >4.77</td><td align="center" valign="middle" >4.69</td><td align="center" valign="middle" >4.76<sup>a </sup></td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >41464-39-5</td><td align="center" valign="middle" >2.875</td><td align="center" valign="middle" >6.174</td><td align="center" valign="middle" >1.960</td><td align="center" valign="middle" >4.067</td><td align="center" valign="middle" >2.107</td><td align="center" valign="middle" >0.237</td><td align="center" valign="middle" >3.925</td><td align="center" valign="middle" >4.84</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >4.52</td><td align="center" valign="middle" >4.49</td><td align="center" valign="middle" >4.48</td><td align="center" valign="middle" >4.44</td><td align="center" valign="middle" >4.43</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >2437-79-8</td><td align="center" valign="middle" >2.024</td><td align="center" valign="middle" >6.138</td><td align="center" valign="middle" >2.203</td><td align="center" valign="middle" >4.171</td><td align="center" valign="middle" >1.968</td><td align="center" valign="middle" >0.254</td><td align="center" valign="middle" >4.420</td><td align="center" valign="middle" >4.85</td><td align="center" valign="middle" >4.97</td><td align="center" valign="middle" >4.94</td><td align="center" valign="middle" >4.75</td><td align="center" valign="middle" >4.74</td><td align="center" valign="middle" >4.74</td><td align="center" valign="middle" >4.80</td><td align="center" valign="middle" >4.79</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >70362-47-9</td><td align="center" valign="middle" >2.845</td><td align="center" valign="middle" >6.121</td><td align="center" valign="middle" >2.192</td><td align="center" valign="middle" >4.157</td><td align="center" valign="middle" >1.965</td><td align="center" valign="middle" >0.255</td><td align="center" valign="middle" >4.397</td><td align="center" valign="middle" >5.00</td><td align="center" valign="middle" >4.90</td><td align="center" valign="middle" >4.91</td><td align="center" valign="middle" >4.68</td><td align="center" valign="middle" >4.64</td><td align="center" valign="middle" >4.65</td><td align="center" valign="middle" >4.68</td><td align="center" valign="middle" >4.70</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >41464-40-8</td><td align="center" valign="middle" >1.376</td><td align="center" valign="middle" >6.12</td><td align="center" valign="middle" >2.189</td><td align="center" valign="middle" >4.155</td><td align="center" valign="middle" >1.966</td><td align="center" valign="middle" >0.254</td><td align="center" valign="middle" >4.391</td><td align="center" valign="middle" >4.84</td><td align="center" valign="middle" >4.90</td><td align="center" valign="middle" >4.86</td><td align="center" valign="middle" >4.67</td><td align="center" valign="middle" >4.68</td><td align="center" valign="middle" >4.68</td><td align="center" valign="middle" >4.76</td><td align="center" valign="middle" >4.72</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >35693-99-3</td><td align="center" valign="middle" >0.409</td><td align="center" valign="middle" >6.122</td><td align="center" valign="middle" >2.265</td><td align="center" valign="middle" >4.194</td><td align="center" valign="middle" >1.929</td><td align="center" valign="middle" >0.259</td><td align="center" valign="middle" >4.559</td><td align="center" valign="middle" >4.63</td><td align="center" valign="middle" >4.91</td><td align="center" valign="middle" >4.83</td><td align="center" valign="middle" >4.77</td><td align="center" valign="middle" >4.80</td><td align="center" valign="middle" >4.81</td><td align="center" valign="middle" >4.86</td><td align="center" valign="middle" >4.79</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >15968-05-5</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >6.194</td><td align="center" valign="middle" >1.812</td><td align="center" valign="middle" >4.003</td><td align="center" valign="middle" >2.191</td><td align="center" valign="middle" >0.228</td><td align="center" valign="middle" >3.657</td><td align="center" valign="middle" >3.85</td><td align="center" valign="middle" >5.18<sup>a </sup></td><td align="center" valign="middle" >5.08<sup>a </sup></td><td align="center" valign="middle" >4.41</td><td align="center" valign="middle" >4.46</td><td align="center" valign="middle" >4.42</td><td align="center" valign="middle" >4.19</td><td align="center" valign="middle" >4.08</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >52663-58-8</td><td align="center" valign="middle" >2.050</td><td align="center" valign="middle" >6.072</td><td align="center" valign="middle" >2.295</td><td align="center" valign="middle" >4.184</td><td align="center" valign="middle" >1.889</td><td align="center" valign="middle" >0.265</td><td align="center" valign="middle" >4.634</td><td align="center" valign="middle" >4.60</td><td align="center" valign="middle" >4.72</td><td align="center" valign="middle" >4.70</td><td align="center" valign="middle" >4.62</td><td align="center" valign="middle" >4.61</td><td align="center" valign="middle" >4.62</td><td align="center" valign="middle" >4.69</td><td align="center" valign="middle" >4.69</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >32598-11-1</td><td align="center" valign="middle" >2.204</td><td align="center" valign="middle" >6.039</td><td align="center" valign="middle" >2.727</td><td align="center" valign="middle" >4.383</td><td align="center" valign="middle" >1.656</td><td align="center" valign="middle" >0.302</td><td align="center" valign="middle" >5.800</td><td align="center" valign="middle" >4.77</td><td align="center" valign="middle" >4.59</td><td align="center" valign="middle" >4.58</td><td align="center" valign="middle" >4.95</td><td align="center" valign="middle" >4.93</td><td align="center" valign="middle" >4.93</td><td align="center" valign="middle" >4.86</td><td align="center" valign="middle" >4.97</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >32598-13-1</td><td align="center" valign="middle" >2.542</td><td align="center" valign="middle" >5.937</td><td align="center" valign="middle" >2.687</td><td align="center" valign="middle" >4.312</td><td align="center" valign="middle" >1.625</td><td align="center" valign="middle" >0.308</td><td align="center" valign="middle" >5.721</td><td align="center" valign="middle" >4.59</td><td align="center" valign="middle" >4.20</td><td align="center" valign="middle" >4.22</td><td align="center" valign="middle" >4.54</td><td align="center" valign="middle" >4.51</td><td align="center" valign="middle" >4.50</td><td align="center" valign="middle" >4.32</td><td align="center" valign="middle" >4.43</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >38380-02-8</td><td align="center" valign="middle" >2.311</td><td align="center" valign="middle" >6.164</td><td align="center" valign="middle" >2.363</td><td align="center" valign="middle" >4.264</td><td align="center" valign="middle" >1.901</td><td align="center" valign="middle" >0.263</td><td align="center" valign="middle" >4.782</td><td align="center" valign="middle" >5.38</td><td align="center" valign="middle" >5.06</td><td align="center" valign="middle" >5.05</td><td align="center" valign="middle" >5.03</td><td align="center" valign="middle" >5.01</td><td align="center" valign="middle" >5.02</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >5.13</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >68194-07-0</td><td align="center" valign="middle" >1.611</td><td align="center" valign="middle" >6.266</td><td align="center" valign="middle" >2.266</td><td align="center" valign="middle" >4.266</td><td align="center" valign="middle" >2.000</td><td align="center" valign="middle" >0.250</td><td align="center" valign="middle" >4.550</td><td align="center" valign="middle" >5.00</td><td align="center" valign="middle" >5.45</td><td align="center" valign="middle" >5.40</td><td align="center" valign="middle" >5.21</td><td align="center" valign="middle" >5.21</td><td align="center" valign="middle" >5.22</td><td align="center" valign="middle" >5.17</td><td align="center" valign="middle" >5.14</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >41464-51-1</td><td align="center" valign="middle" >2.648</td><td align="center" valign="middle" >6.216</td><td align="center" valign="middle" >2.334</td><td align="center" valign="middle" >4.275</td><td align="center" valign="middle" >1.941</td><td align="center" valign="middle" >0.258</td><td align="center" valign="middle" >4.708</td><td align="center" valign="middle" >5.43</td><td align="center" valign="middle" >5.26</td><td align="center" valign="middle" >5.25</td><td align="center" valign="middle" >5.11</td><td align="center" valign="middle" >5.09</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >5.12</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >38380-01-7</td><td align="center" valign="middle" >1.309</td><td align="center" valign="middle" >6.194</td><td align="center" valign="middle" >2.350</td><td align="center" valign="middle" >4.272</td><td align="center" valign="middle" >1.922</td><td align="center" valign="middle" >0.260</td><td align="center" valign="middle" >4.748</td><td align="center" valign="middle" >5.00</td><td align="center" valign="middle" >5.18</td><td align="center" valign="middle" >5.13</td><td align="center" valign="middle" >5.05</td><td align="center" valign="middle" >5.06</td><td align="center" valign="middle" >5.08</td><td align="center" valign="middle" >5.11</td><td align="center" valign="middle" >5.07</td></tr><tr><td align="center" valign="middle" >29</td><td align="center" valign="middle" >37680-73-2</td><td align="center" valign="middle" >1.437</td><td align="center" valign="middle" >5.971</td><td align="center" valign="middle" >2.084</td><td align="center" valign="middle" >4.028</td><td align="center" valign="middle" >1.944</td><td align="center" valign="middle" >0.257</td><td align="center" valign="middle" >4.173</td><td align="center" valign="middle" >5.40</td><td align="center" valign="middle" >4.33</td><td align="center" valign="middle" >4.31<sup>a </sup></td><td align="center" valign="middle" >4.01<sup>a </sup></td><td align="center" valign="middle" >4.02<sup>a </sup></td><td align="center" valign="middle" >4.03<sup>a </sup></td><td align="center" valign="middle" >4.16<sup>a </sup></td><td align="center" valign="middle" >4.10<sup>a </sup></td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >32598-14-4</td><td align="center" valign="middle" >3.152</td><td align="center" valign="middle" >6.025</td><td align="center" valign="middle" >2.801</td><td align="center" valign="middle" >4.413</td><td align="center" valign="middle" >1.612</td><td align="center" valign="middle" >0.310</td><td align="center" valign="middle" >6.041</td><td align="center" valign="middle" >5.00</td><td align="center" valign="middle" >4.54<sup>a </sup></td><td align="center" valign="middle" >4.56</td><td align="center" valign="middle" >4.98</td><td align="center" valign="middle" >4.95</td><td align="center" valign="middle" >4.93</td><td align="center" valign="middle" >4.84</td><td align="center" valign="middle" >5.02</td></tr><tr><td align="center" valign="middle" >31</td><td align="center" valign="middle" >74472-35-8</td><td align="center" valign="middle" >1.993</td><td align="center" valign="middle" >6.222</td><td align="center" valign="middle" >2.395</td><td align="center" valign="middle" >4.309</td><td align="center" valign="middle" >1.914</td><td align="center" valign="middle" >0.261</td><td align="center" valign="middle" >4.850</td><td align="center" valign="middle" >5.00</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >5.25</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >5.27</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >5.35</td><td align="center" valign="middle" >5.38</td></tr><tr><td align="center" valign="middle" >32</td><td align="center" valign="middle" >31508-00-6</td><td align="center" valign="middle" >1.282</td><td align="center" valign="middle" >6.148</td><td align="center" valign="middle" >2.504</td><td align="center" valign="middle" >4.326</td><td align="center" valign="middle" >1.822</td><td align="center" valign="middle" >0.274</td><td align="center" valign="middle" >5.136</td><td align="center" valign="middle" >5.00</td><td align="center" valign="middle" >5.00</td><td align="center" valign="middle" >4.96</td><td align="center" valign="middle" >5.07</td><td align="center" valign="middle" >5.08</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >5.19</td><td align="center" valign="middle" >5.17</td></tr><tr><td align="center" valign="middle" >33</td><td align="center" valign="middle" >57465-28-8</td><td align="center" valign="middle" >1.412</td><td align="center" valign="middle" >6.062</td><td align="center" valign="middle" >2.826</td><td align="center" valign="middle" >4.444</td><td align="center" valign="middle" >1.618</td><td align="center" valign="middle" >0.309</td><td align="center" valign="middle" >6.103</td><td align="center" valign="middle" >5.81</td><td align="center" valign="middle" >4.68<sup>a </sup></td><td align="center" valign="middle" >4.64<sup>a </sup></td><td align="center" valign="middle" >5.15</td><td align="center" valign="middle" >5.15</td><td align="center" valign="middle" >5.13</td><td align="center" valign="middle" >5.02<sup>a </sup></td><td align="center" valign="middle" >5.14<sup>a </sup></td></tr><tr><td align="center" valign="middle" >34</td><td align="center" valign="middle" >38380-07-3</td><td align="center" valign="middle" >3.269</td><td align="center" valign="middle" >6.309</td><td align="center" valign="middle" >2.429</td><td align="center" valign="middle" >4.369</td><td align="center" valign="middle" >1.940</td><td align="center" valign="middle" >0.258</td><td align="center" valign="middle" >4.920</td><td align="center" valign="middle" >5.77</td><td align="center" valign="middle" >5.61</td><td align="center" valign="middle" >5.61</td><td align="center" valign="middle" >5.55</td><td align="center" valign="middle" >5.51</td><td align="center" valign="middle" >5.52</td><td align="center" valign="middle" >5.54</td><td align="center" valign="middle" >5.60</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >38411-22-2</td><td align="center" valign="middle" >1.453</td><td align="center" valign="middle" >6.222</td><td align="center" valign="middle" >2.130</td><td align="center" valign="middle" >4.176</td><td align="center" valign="middle" >2.046</td><td align="center" valign="middle" >0.244</td><td align="center" valign="middle" >4.262</td><td align="center" valign="middle" >5.43</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >5.23</td><td align="center" valign="middle" >4.89</td><td align="center" valign="middle" >4.90</td><td align="center" valign="middle" >4.90</td><td align="center" valign="middle" >4.86</td><td align="center" valign="middle" >4.80</td></tr><tr><td align="center" valign="middle" >36</td><td align="center" valign="middle" >35694-06-5</td><td align="center" valign="middle" >1.928</td><td align="center" valign="middle" >6.331</td><td align="center" valign="middle" >2.360</td><td align="center" valign="middle" >4.346</td><td align="center" valign="middle" >1.986</td><td align="center" valign="middle" >0.252</td><td align="center" valign="middle" >4.755</td><td align="center" valign="middle" >5.88</td><td align="center" valign="middle" >5.70</td><td align="center" valign="middle" >5.65</td><td align="center" valign="middle" >5.62</td><td align="center" valign="middle" >5.61</td><td align="center" valign="middle" >5.61</td><td align="center" valign="middle" >5.56</td><td align="center" valign="middle" >5.59</td></tr><tr><td align="center" valign="middle" >37</td><td align="center" valign="middle" >35065-28-2</td><td align="center" valign="middle" >1.997</td><td align="center" valign="middle" >6.325</td><td align="center" valign="middle" >2.260</td><td align="center" valign="middle" >4.293</td><td align="center" valign="middle" >2.033</td><td align="center" valign="middle" >0.246</td><td align="center" valign="middle" >4.533</td><td align="center" valign="middle" >5.39</td><td align="center" valign="middle" >5.67</td><td align="center" valign="middle" >5.63</td><td align="center" valign="middle" >5.48</td><td align="center" valign="middle" >5.47</td><td align="center" valign="middle" >5.46</td><td align="center" valign="middle" >5.38</td><td align="center" valign="middle" >5.40</td></tr><tr><td align="center" valign="middle" >38</td><td align="center" valign="middle" >52712-04-6</td><td align="center" valign="middle" >2.049</td><td align="center" valign="middle" >6.256</td><td align="center" valign="middle" >2.455</td><td align="center" valign="middle" >4.356</td><td align="center" valign="middle" >1.901</td><td align="center" valign="middle" >0.263</td><td align="center" valign="middle" >4.991</td><td align="center" valign="middle" >5.81</td><td align="center" valign="middle" >5.41</td><td align="center" valign="middle" >5.38</td><td align="center" valign="middle" >5.47</td><td align="center" valign="middle" >5.46</td><td align="center" valign="middle" >5.46</td><td align="center" valign="middle" >5.53</td><td align="center" valign="middle" >5.57</td></tr></tbody></table></table-wrap><table-wrap id="1_2"><table><tbody><thead><tr><th align="center" valign="middle" >39</th><th align="center" valign="middle" >74472-41-6</th><th align="center" valign="middle" >1.073</th><th align="center" valign="middle" >6.284</th><th align="center" valign="middle" >2.243</th><th align="center" valign="middle" >4.264</th><th align="center" valign="middle" >2.021</th><th align="center" valign="middle" >0.247</th><th align="center" valign="middle" >4.498</th><th align="center" valign="middle" >5.39</th><th align="center" valign="middle" >5.52</th><th align="center" valign="middle" >5.45</th><th align="center" valign="middle" >5.32</th><th align="center" valign="middle" >5.33</th><th align="center" valign="middle" >5.33</th><th align="center" valign="middle" >5.29</th><th align="center" valign="middle" >5.27</th></tr></thead><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >52663-63-5</td><td align="center" valign="middle" >0.472</td><td align="center" valign="middle" >6.221</td><td align="center" valign="middle" >2.302</td><td align="center" valign="middle" >4.262</td><td align="center" valign="middle" >1.960</td><td align="center" valign="middle" >0.255</td><td align="center" valign="middle" >4.634</td><td align="center" valign="middle" >5.54</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >5.20</td><td align="center" valign="middle" >5.16</td><td align="center" valign="middle" >5.19</td><td align="center" valign="middle" >5.20</td><td align="center" valign="middle" >5.19</td><td align="center" valign="middle" >5.14</td></tr><tr><td align="center" valign="middle" >41</td><td align="center" valign="middle" >35065-27-1</td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >6.257</td><td align="center" valign="middle" >2.493</td><td align="center" valign="middle" >4.375</td><td align="center" valign="middle" >1.882</td><td align="center" valign="middle" >0.266</td><td align="center" valign="middle" >5.085</td><td align="center" valign="middle" >5.65</td><td align="center" valign="middle" >5.42</td><td align="center" valign="middle" >5.32</td><td align="center" valign="middle" >5.44</td><td align="center" valign="middle" >5.49</td><td align="center" valign="middle" >5.50</td><td align="center" valign="middle" >5.47</td><td align="center" valign="middle" >5.42</td></tr><tr><td align="center" valign="middle" >42</td><td align="center" valign="middle" >33979-03-2</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >6.535</td><td align="center" valign="middle" >2.153</td><td align="center" valign="middle" >4.344</td><td align="center" valign="middle" >2.191</td><td align="center" valign="middle" >0.228</td><td align="center" valign="middle" >4.306</td><td align="center" valign="middle" >4.93</td><td align="center" valign="middle" >6.47<sup>a </sup></td><td align="center" valign="middle" >6.34<sup>a </sup></td><td align="center" valign="middle" >6.03<sup>a </sup></td><td align="center" valign="middle" >6.08<sup>a </sup></td><td align="center" valign="middle" >6.03<sup>a </sup></td><td align="center" valign="middle" >5.54</td><td align="center" valign="middle" >5.48</td></tr><tr><td align="center" valign="middle" >43</td><td align="center" valign="middle" >38380-08-4</td><td align="center" valign="middle" >1.712</td><td align="center" valign="middle" >6.221</td><td align="center" valign="middle" >2.629</td><td align="center" valign="middle" >4.425</td><td align="center" valign="middle" >1.796</td><td align="center" valign="middle" >0.278</td><td align="center" valign="middle" >5.451</td><td align="center" valign="middle" >5.39</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >5.24</td><td align="center" valign="middle" >5.48</td><td align="center" valign="middle" >5.48</td><td align="center" valign="middle" >5.49</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >5.64</td></tr><tr><td align="center" valign="middle" >44</td><td align="center" valign="middle" >69782-90-7</td><td align="center" valign="middle" >2.096</td><td align="center" valign="middle" >6.158</td><td align="center" valign="middle" >2.940</td><td align="center" valign="middle" >4.549</td><td align="center" valign="middle" >1.609</td><td align="center" valign="middle" >0.311</td><td align="center" valign="middle" >6.430</td><td align="center" valign="middle" >5.39</td><td align="center" valign="middle" >5.04</td><td align="center" valign="middle" >5.02</td><td align="center" valign="middle" >5.62</td><td align="center" valign="middle" >5.61</td><td align="center" valign="middle" >5.59</td><td align="center" valign="middle" >5.53</td><td align="center" valign="middle" >5.73</td></tr><tr><td align="center" valign="middle" >45</td><td align="center" valign="middle" >32774-16-6</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >6.178</td><td align="center" valign="middle" >2.960</td><td align="center" valign="middle" >4.569</td><td align="center" valign="middle" >1.609</td><td align="center" valign="middle" >0.311</td><td align="center" valign="middle" >6.487</td><td align="center" valign="middle" >5.97</td><td align="center" valign="middle" >5.12</td><td align="center" valign="middle" >5.03<sup>a </sup></td><td align="center" valign="middle" >5.72</td><td align="center" valign="middle" >5.76</td><td align="center" valign="middle" >5.73</td><td align="center" valign="middle" >5.65</td><td align="center" valign="middle" >5.76</td></tr><tr><td align="center" valign="middle" >46</td><td align="center" valign="middle" >38411-25-5</td><td align="center" valign="middle" >2.751</td><td align="center" valign="middle" >6.351</td><td align="center" valign="middle" >2.291</td><td align="center" valign="middle" >4.321</td><td align="center" valign="middle" >2.030</td><td align="center" valign="middle" >0.246</td><td align="center" valign="middle" >4.599</td><td align="center" valign="middle" >5.80</td><td align="center" valign="middle" >5.77</td><td align="center" valign="middle" >5.75</td><td align="center" valign="middle" >5.54</td><td align="center" valign="middle" >5.51</td><td align="center" valign="middle" >5.51</td><td align="center" valign="middle" >5.46</td><td align="center" valign="middle" >5.49</td></tr><tr><td align="center" valign="middle" >47</td><td align="center" valign="middle" >35065-29-3</td><td align="center" valign="middle" >0.839</td><td align="center" valign="middle" >6.340</td><td align="center" valign="middle" >2.558</td><td align="center" valign="middle" >4.449</td><td align="center" valign="middle" >1.891</td><td align="center" valign="middle" >0.264</td><td align="center" valign="middle" >5.234</td><td align="center" valign="middle" >5.80</td><td align="center" valign="middle" >5.73</td><td align="center" valign="middle" >5.65</td><td align="center" valign="middle" >5.82</td><td align="center" valign="middle" >5.84</td><td align="center" valign="middle" >5.86</td><td align="center" valign="middle" >5.91</td><td align="center" valign="middle" >5.90</td></tr><tr><td align="center" valign="middle" >48</td><td align="center" valign="middle" >60145-23-5</td><td align="center" valign="middle" >1.823</td><td align="center" valign="middle" >6.376</td><td align="center" valign="middle" >2.319</td><td align="center" valign="middle" >4.348</td><td align="center" valign="middle" >2.029</td><td align="center" valign="middle" >0.246</td><td align="center" valign="middle" >4.659</td><td align="center" valign="middle" >5.80</td><td align="center" valign="middle" >5.87</td><td align="center" valign="middle" >5.81</td><td align="center" valign="middle" >5.73</td><td align="center" valign="middle" >5.73</td><td align="center" valign="middle" >5.72</td><td align="center" valign="middle" >5.67</td><td align="center" valign="middle" >5.69</td></tr><tr><td align="center" valign="middle" >49</td><td align="center" valign="middle" >52663-69-1</td><td align="center" valign="middle" >0.933</td><td align="center" valign="middle" >6.329</td><td align="center" valign="middle" >2.388</td><td align="center" valign="middle" >4.359</td><td align="center" valign="middle" >1.971</td><td align="center" valign="middle" >0.254</td><td align="center" valign="middle" >4.820</td><td align="center" valign="middle" >5.84</td><td align="center" valign="middle" >5.69</td><td align="center" valign="middle" >5.61</td><td align="center" valign="middle" >5.65</td><td align="center" valign="middle" >5.67</td><td align="center" valign="middle" >5.66</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >5.59</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >52663-68-0</td><td align="center" valign="middle" >2.193</td><td align="center" valign="middle" >6.441</td><td align="center" valign="middle" >2.327</td><td align="center" valign="middle" >4.384</td><td align="center" valign="middle" >2.057</td><td align="center" valign="middle" >0.243</td><td align="center" valign="middle" >4.672</td><td align="center" valign="middle" >5.80</td><td align="center" valign="middle" >6.11</td><td align="center" valign="middle" >6.06</td><td align="center" valign="middle" >5.90</td><td align="center" valign="middle" >5.89</td><td align="center" valign="middle" >5.88</td><td align="center" valign="middle" >5.72</td><td align="center" valign="middle" >5.74</td></tr><tr><td align="center" valign="middle" >51</td><td align="center" valign="middle" >74472-50-7</td><td align="center" valign="middle" >1.833</td><td align="center" valign="middle" >6.373</td><td align="center" valign="middle" >2.620</td><td align="center" valign="middle" >4.497</td><td align="center" valign="middle" >1.877</td><td align="center" valign="middle" >0.266</td><td align="center" valign="middle" >5.387</td><td align="center" valign="middle" >5.84</td><td align="center" valign="middle" >5.86</td><td align="center" valign="middle" >5.80</td><td align="center" valign="middle" >6.08</td><td align="center" valign="middle" >6.07</td><td align="center" valign="middle" >6.08</td><td align="center" valign="middle" >6.19</td><td align="center" valign="middle" >6.27</td></tr><tr><td align="center" valign="middle" >52</td><td align="center" valign="middle" >35694-08-7</td><td align="center" valign="middle" >1.101</td><td align="center" valign="middle" >6.419</td><td align="center" valign="middle" >2.675</td><td align="center" valign="middle" >4.547</td><td align="center" valign="middle" >1.872</td><td align="center" valign="middle" >0.267</td><td align="center" valign="middle" >5.522</td><td align="center" valign="middle" >5.81</td><td align="center" valign="middle" >6.03</td><td align="center" valign="middle" >5.95</td><td align="center" valign="middle" >6.24</td><td align="center" valign="middle" >6.25</td><td align="center" valign="middle" >6.27</td><td align="center" valign="middle" >6.32</td><td align="center" valign="middle" >6.36</td></tr><tr><td align="center" valign="middle" >53</td><td align="center" valign="middle" >52663-78-2</td><td align="center" valign="middle" >1.956</td><td align="center" valign="middle" >6.46</td><td align="center" valign="middle" >2.465</td><td align="center" valign="middle" >4.463</td><td align="center" valign="middle" >1.998</td><td align="center" valign="middle" >0.250</td><td align="center" valign="middle" >4.984</td><td align="center" valign="middle" >5.92</td><td align="center" valign="middle" >6.18</td><td align="center" valign="middle" >6.13</td><td align="center" valign="middle" >6.21</td><td align="center" valign="middle" >6.20</td><td align="center" valign="middle" >6.19</td><td align="center" valign="middle" >6.14</td><td align="center" valign="middle" >6.20</td></tr><tr><td align="center" valign="middle" >54</td><td align="center" valign="middle" >42740-50-1</td><td align="center" valign="middle" >1.529</td><td align="center" valign="middle" >6.421</td><td align="center" valign="middle" >2.460</td><td align="center" valign="middle" >4.441</td><td align="center" valign="middle" >1.981</td><td align="center" valign="middle" >0.252</td><td align="center" valign="middle" >4.978</td><td align="center" valign="middle" >5.92</td><td align="center" valign="middle" >6.04</td><td align="center" valign="middle" >5.97</td><td align="center" valign="middle" >6.06</td><td align="center" valign="middle" >6.06</td><td align="center" valign="middle" >6.06</td><td align="center" valign="middle" >6.05</td><td align="center" valign="middle" >6.08</td></tr><tr><td align="center" valign="middle" >55</td><td align="center" valign="middle" >68194-17-2</td><td align="center" valign="middle" >0.875</td><td align="center" valign="middle" >6.369</td><td align="center" valign="middle" >2.587</td><td align="center" valign="middle" >4.478</td><td align="center" valign="middle" >1.891</td><td align="center" valign="middle" >0.264</td><td align="center" valign="middle" >5.302</td><td align="center" valign="middle" >5.88</td><td align="center" valign="middle" >5.84</td><td align="center" valign="middle" >5.76</td><td align="center" valign="middle" >5.95</td><td align="center" valign="middle" >5.98</td><td align="center" valign="middle" >5.99</td><td align="center" valign="middle" >6.05</td><td align="center" valign="middle" >6.05</td></tr><tr><td align="center" valign="middle" >56</td><td align="center" valign="middle" >2136-99-4</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >6.34</td><td align="center" valign="middle" >2.403</td><td align="center" valign="middle" >4.372</td><td align="center" valign="middle" >1.969</td><td align="center" valign="middle" >0.254</td><td align="center" valign="middle" >4.854</td><td align="center" valign="middle" >5.82</td><td align="center" valign="middle" >5.73</td><td align="center" valign="middle" >5.62</td><td align="center" valign="middle" >5.71</td><td align="center" valign="middle" >5.75</td><td align="center" valign="middle" >5.75</td><td align="center" valign="middle" >5.68</td><td align="center" valign="middle" >5.64</td></tr><tr><td align="center" valign="middle" >57</td><td align="center" valign="middle" >52663-77-1</td><td align="center" valign="middle" >0.915</td><td align="center" valign="middle" >6.387</td><td align="center" valign="middle" >2.521</td><td align="center" valign="middle" >4.454</td><td align="center" valign="middle" >1.933</td><td align="center" valign="middle" >0.259</td><td align="center" valign="middle" >5.131</td><td align="center" valign="middle" >5.71</td><td align="center" valign="middle" >5.91</td><td align="center" valign="middle" >5.82</td><td align="center" valign="middle" >5.94</td><td align="center" valign="middle" >5.96</td><td align="center" valign="middle" >5.97</td><td align="center" valign="middle" >5.91</td><td align="center" valign="middle" >5.90</td></tr><tr><td align="center" valign="middle" >58</td><td align="center" valign="middle" >2051-24-3</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >6.486</td><td align="center" valign="middle" >2.695</td><td align="center" valign="middle" >4.591</td><td align="center" valign="middle" >1.896</td><td align="center" valign="middle" >0.264</td><td align="center" valign="middle" >5.558</td><td align="center" valign="middle" >5.44</td><td align="center" valign="middle" >6.28<sup>a </sup></td><td align="center" valign="middle" >6.16<sup> </sup></td><td align="center" valign="middle" >6.57<sup>a </sup></td><td align="center" valign="middle" >6.61<sup>a </sup></td><td align="center" valign="middle" >6.61<sup>a </sup></td><td align="center" valign="middle" >6.61<sup>a </sup></td><td align="center" valign="middle" >6.64<sup>a </sup></td></tr></tbody></table></table-wrap></table-wrap-group><p><sup>a</sup>data point not used in the model, &#181; is the dipole moment in debye, IP is the ionization energy in eV, EA is the electron affinity in eV, χ is the electronegativity in eV, η is the absolute hardness in eV, S is the global softness and ω is the electrophilicity of the molecule.</p><p>quantum chemical reactivity descriptors: dipole moment, ionization potential, electron affinity, electronegativity, hardness, softness and electrophilicity index. Dipole moment (μ) gives valuable information regarding the symmetry of molecule. It also helps in explaining the solubility of substances. The computational result of dipole moment of the compounds (<xref ref-type="table" rid="table1">Table 1</xref>) show that all the compounds have definite dipole moment, except compound no. 1 and 10. Thus, both of these compounds are symmetrical. The range of dipole moment is 0.002 - 0.011D (5), 0.156 - 0.933D (8), 1.073 - 1.997D (20), 2.005 - 2.875D (18) and 3.141 - 3.668D (5). Ionization potential (IP) of a molecule is the minimal energy needed for the detachment of an electron for a molecule. According to Koopman’s theorem the IE is simply the eigenvalue of HOMO with change in sign and characterizes the susceptibility of the molecule toward attack by electrophiles. IP value as included in <xref ref-type="table" rid="table1">Table 1</xref> shows that fifteen compounds have their IP in the range of 5.557 - 5.971 eV and the rest forty five in the range of 6.028 - 6.535 eV. Electron affinity (EA) is the energy difference between an uncharged species and its negative ion. It is an important property of atoms and molecules. According to Koopman’s theorem [<xref ref-type="bibr" rid="scirp.98152-ref54">54</xref>] the EA is simply the eigenvalue of LUMO with change in sign and characterizes the susceptibility of the molecule toward attack by nucleophiles. The experimental and/or theoretical determination of this quantity is an important task. A close look at <xref ref-type="table" rid="table1">Table 1</xref>, shows all the compounds have definite value of electron affinity (1.812 to 1.998 eV (5) and 2.084 - 2.960 eV (53). Electronegativity (χ) measures the ability to attract electron itself. Large χ values characterize acids and small χ values are found for bases. If two molecules are brought together, electrons will flow from the one of lower χ to that of higher χ. All the compounds have definite value of χ ranging from 4.003 to 4.591 eV, except three compounds (1, 2 and 11) have χ value lower than 4.0 eV. The parameter hardness (η) is interpreted as the resistance of the chemical potential to change in the number of electrons or resistance to deformation or change. All the compounds have definite value of η in the range 1.609 - 1.998 eV (46) and 2.0 - 2.191 eV (12). The minimum value of hardness is zero and it corresponds to the maximum softness (S). The ranges of softness values are 0.228 - 0.299 (50) and 0.302 - 0.311 (8). Electrophilicity index (ω) measures the stabilization in energy when the system acquires an additional electronic charge from the environment. The electrophilicity index is positive, definite quantity and the direction of the charge is completely determined by the electronic chemical potential (μ = −χ) of the molecule because an electrophile is a chemical species capable of accepting electrons from the environment and its energy must decrease upon accepting electronic charge. All the compounds have definite value of ω included in <xref ref-type="table" rid="table1">Table 1</xref>. The range of ω is 3.657 - 3.999 (5), 4.179 - 4.991 (34), 5.014 - 5.8 (15) and 6.041 - 6.487 (4).</p><p>Multiple linear regression analyses were employed to developed reliable models for the prediction of BCF. For MLR analysis, above descriptors (<xref ref-type="table" rid="table1">Table 1</xref>) were used as independent variables and the experimental logarithmic BCF values as dependent variable. MLR analysis has been made by Project Leader software associated with CAChe, using the descriptors in various combinations. The best seven models (for k = 1, 2, 3, 4, 5, 6 and 7) are presented here.</p><p>When, k = 1, single descriptor has been used as independent variable, then with respect to each descriptor seven equations were made and the best-fitted equation of this class is Equation (8), where IP is the ionization potential of the molecule and, it has a positive descriptor coefficient magnitude that shows that its direct relationship with the BCF.</p><p>L o g B C F p r e = 3.7854 &#215; I P − 18.2697 r 2 = 0.9118 , r C V 2 = 0.8953 , S E = 0.2698 (8)</p><p>The predicted logarithmic BCF values from Equation (8) are also given in <xref ref-type="table" rid="table1">Table 1</xref>. The statistical quality of the equation is good as is evident from its correlation coefficient r<sup>2</sup> value = 0.9118 and a cross-validated coefficient r C V 2 = 0.8953. The predicted BCF is reliable as is evident from its standard error (SE) value. The trend of the experimental and predicted BCFs is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) which shows that there is little difference between experimental and predicted BCFs.</p><p>For k = 2, the best-fitted equation is Equation (9), where &#181; and IP is the dipole moment and ionization potential of the molecule, respectively. Both, &#181; and</p><p>IP have positive descriptor coefficient magnitudes that show direct relationships with the BCF.</p><p>L o g B C F p r e = 0.0319265 &#215; μ + 3.68314 &#215; I P − 17.7294 r 2 = 0.9139 , r C V 2 = 0.8986 , S E = 0.2668 (9)</p><p>The predicted logarithmic BCF values from Equation (9) are also given in <xref ref-type="table" rid="table1">Table 1</xref>. The statistical quality of the equation is more reliable than Equation (8) as is evident from its correlation coefficient r<sup>2</sup> value = 0.91389 and a cross-validated coefficient r C V 2 = 0.8986. The predicted BCF is reliable as is evident from its standard error (SE) value. The trend of the experimental and predicted BCFs is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b).</p><p>For k = 3, the best-fitted equation is Equation (10), where IP, EA and χ is the ionization potential, electron affinity and of the molecule, respectively.</p><p>L o g B C F p r e = − 68.2118 &#215; I P − 70.5862 &#215; E A + 143.542 &#215; χ − 19.7812 r 2 = 0.9102 , r C V 2 = 0.8946 , S E = 0.2775 (10)</p><p>Both, IP and EA have negative descriptor coefficient magnitudes that show indirect relationships with the BCF, while the third descriptor, χ, has a positive magnitude i.e., direct relationship. The statistical quality of the equation is r<sup>2</sup> = 0.9102, r C V 2 = 0.8946 and SE = 0.2775. The predicted logarithmic BCF values as obtained from this model are also given in <xref ref-type="table" rid="table1">Table 1</xref>. The trend of the experimental and predicted BCFs is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(c).</p><p>For k = 4, the best-fitted equation is Equation (11). The variables of this model are dipole moment, ionization potential, electron affinity and electronegativity, all with negative descriptor coefficient magnitudes except the electronegativity.</p><p>L o g B C F p r e = − 0.0271479 &#215; μ − 65.5176 &#215; I P − 67.889 &#215; E A + 138.139 &#215; χ − 19.6776 r 2 = 0.9110 , r C V 2 = 0.8887 , S E = 0.2779 (11)</p><p>The predicted logarithmic BCF values as obtained from this model are also given in <xref ref-type="table" rid="table1">Table 1</xref>. The trend of the experimental and predicted BCFs is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(d).</p><p>For k = 5, the best-fitted equation is the Equation (12). The variables of this model are dipole moment, ionization potential, electron affinity, electronegativity and softness all with negative descriptor coefficient magnitudes except the electronegativity.</p><p>L o g B C F p r e = − 0.0261386 &#215; μ − 58.9446 &#215; I P − 60.2176 &#215; E A + 123.883 &#215; χ − 7.45897 &#215; S − 15.5638 r 2 = 0.9112 , r C V 2 = 0.8630 , S E = 0.2815 (12)</p><p>The predicted logarithmic BCF values as obtained from this model are also given in <xref ref-type="table" rid="table1">Table 1</xref>. The trend of the experimental and predicted BCFs is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(e).</p><p>For k = 6, the best-fitted equation is the Equation (13). The variables of this model are ionization potential, electron affinity, electronegativity, hardness, softness and electronegativity index.</p><p>L o g B C F p r e = − 77.8689 &#215; I P − 5.08309 &#215; E A + 83.4781 &#215; χ + 65.3488 &#215; η − 99.3578 &#215; S + 1.79358 &#215; ω + 34.4746 r 2 = 0.9077 , r C V 2 = 0.6856 , S E = 0.2874 (13)</p><p>The predicted logarithmic BCF values as obtained from this model are also given in <xref ref-type="table" rid="table1">Table 1</xref>. The trend of the experimental and predicted BCFs is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(f).</p><p>For k = 7, seven descriptors have been used as independent variables and the resulted equation is Equation (14).</p><p>L o g B C F p r e = 0.0413017 &#215; μ − 106.417 &#215; I P + 97.0787 &#215; E A + 9.55439 &#215; χ + 197.236 &#215; η − 94.8928 &#215; S + 2.04835 &#215; ω + 31.0716 r 2 = 0.9071 , r C V 2 = 0.8007 , S E = 0.2928 (14)</p><p>The predicted logarithmic BCF values as obtained from this model are also given in <xref ref-type="table" rid="table1">Table 1</xref>. The trend of the experimental and predicted BCFs is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(g).</p><p>For comparative study and selection of the reliable model among the above seven models, the regression summary is presented as below.</p><p>Regression summary of the above models</p><p>From the above summary, the reliable model is the Equation (9) as it has higher value of r<sup>2</sup> and r C V 2 , lower values of “k” and SE than other models. The current study accounts for previous findings in most easier and convenient way. Ivanciuc et al., for the first time made QSAR study on these compounds aggregated from various literature reports. Predictive ability of their models was “r” between 0.903 and 0.935 for splinoid QSSAR and “r” between 0.745 and 0.887 for cluster-expansion [<xref ref-type="bibr" rid="scirp.98152-ref23">23</xref>]. In continuation to this Katritzky et al., reported QSAR results of the same data sets based on 486 constitutional, topological, geometrical, electrostatic, quantum chemical and thermodynamic descriptors derived solely from molecular structure using CODESSA Pro software and proposed that two-parameter model satisfactorily describes the relationship between observed and calculated values in terms of statistical parameters [<xref ref-type="bibr" rid="scirp.98152-ref18">18</xref>]. E.B. de Melo reported QSAR results based on E-state and topological descriptors using SMILE software and the best model present five descriptors (one E-state index and four topological descriptors) [<xref ref-type="bibr" rid="scirp.98152-ref55">55</xref>]. Liu et al. made QSAR studies of BCFs of PCBs using DFT, PCS and CoMFA, and their result show that the electrostatic descriptors (R<sup>2</sup> = 0.926; Q<sup>2</sup> = 0.821; RMSE = 0.235) play a more significant role in BCFs of PCBs [<xref ref-type="bibr" rid="scirp.98152-ref56">56</xref>]. Using deep belief network QSPR models for predicting the physicochemical properties of PCBs were also made by Safder et al. [<xref ref-type="bibr" rid="scirp.98152-ref57">57</xref>].</p></sec><sec id="s5"><title>5. Conclusions</title><p>On the basis of present study, it has been concluded that DFT-based quantum chemical descriptors have sufficient reliability to relate the bioconcentration factors of polychlorinated biphenyls with their electronic structures. The QSAR model, “LogBCF<sub>pre</sub> = 0.0319265 &#215; &#181; +3.68314 &#215; IP − 17.7294”, can be useful for predicting the BCF of compounds prior to their synthesis and dipole moment and ionization potential are reliable descriptors for predicting BCF, and Both dipole moment and ionization potential have direct relationship with log BCF.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors are thankful to Principal M.L.K. (P.G.) College; Balrampur, for providing the laboratory facilities to conduct the calculation.</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Soni, A.K., Singh, P. and Sahu, V.K. (2020) DFT-Based Prediction of Bioconcentration Factors of Polychlorinated Biphenyls in Fish Species Using Molecular Descriptors. 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