<?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">OJPC</journal-id><journal-title-group><journal-title>Open Journal of Physical Chemistry</journal-title></journal-title-group><issn pub-type="epub">2162-1969</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojpc.2016.64009</article-id><article-id pub-id-type="publisher-id">OJPC-71531</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>
 
 
  A Revisited Definition of the Three Solute Descriptors Related to the Van der Waals Forces in Solutions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Paul</surname><given-names>Laffort</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>B.P. 446, 64310 Ascain, France</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>10</month><year>2016</year></pub-date><volume>06</volume><issue>04</issue><fpage>86</fpage><lpage>100</lpage><history><date date-type="received"><day>August</day>	<month>22,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>October</month>	<year>24,</year>	</date><date date-type="accepted"><day>October</day>	<month>27,</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  It is currently admitted that the intermolecular forces implicated in Gas Liquid Chromatography (GLC) can be expressed as a product of parameters (or descriptors) of solutes and of parameters of solvents. The present study is limited to those of solutes, and among them the three ones 
  are 
  involved in the Van der Waals forces, whereas the two ones involved in the hydrogen bonding are left aside at this stage. These three studied parameters, 
  which 
  we call
   δ
  , 
  ω
   
  and
   
  ε
  , respectively reflect the three types of Van der Waals forces: dispersion, orientation or polarity strictly speaking, and induction-polarizability. These parameters have been experimentally obtained in previous studies for 121 Volatile Organic Compounds (VOC) via an original Multiplicative Matrix Analysis (MMA) applied to a superabundant and accurate GLC data set. Then, also in previous studies, attempts have been made to predict these parameters via a Simplified Molecular Topology procedure (SMT). Because these last published results have been somewhat disappointing, a promising new strategy of prediction is developed and detailed in the present article.
 
</p></abstract><kwd-group><kwd>Van der Waals Intermolecular Forces</kwd><kwd> Solute Descriptors</kwd><kwd> Gas Liquid Chromatography</kwd><kwd> Chemo Informatics</kwd><kwd> Multiplicative Matrix Analysis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The present study takes place at the continuation of a series of six papers started in 2005 by our group, in which we have focused our efforts on a better knowledge of the intermolecular forces involved in GLC (Gas-Liquid Chromatography) between solutes (VOC or Volatile Organic Compounds) and stationary phases [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.71531-ref6">6</xref>] . Even if it is an oversimplified view on a theoretical point of view, two types of forces are considered from an experimental approach:</p><p>・ Van der Waals, subdivided in London, Keesom, and Debye types,</p><p>・ hydrogen bonding, subdivided in proton donor and proton acceptor types.</p><p>According to Rohrschneider [<xref ref-type="bibr" rid="scirp.71531-ref7">7</xref>] , it is admitted since 1966 that the Kov&#225;ts retention indices in GLC (RI) can be expressed as a linear equation of terms, each term being a product of a solute parameter and of a solvent parameter. There is presently a general agreement to consider that five terms are necessary and sufficient. In other words, the following equation can be written:</p><disp-formula id="scirp.71531-formula116"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1230256x2.png"  xlink:type="simple"/></disp-formula><p>in which RI stands for the Kov&#225;ts retention index of the solute on the stationary phase under study, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1230256x3.png" xlink:type="simple"/></inline-formula> stands for the retention index of methane (always equals to 100). The lower case Greek letters stand for the solvation parameters of solutes, and the Latin upper case letters for the solvation parameters of stationary phases.</p><p>Among the results obtained in our series of six quoted studies, those useful for the present are summarized in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><sec id="s1_1"><title>1.1. Parameters of Solutes</title><p>The physicochemical characterization of our solute parameters is partially similar to that adopted by various authors starting with the study of Abraham et al. in 1990 [<xref ref-type="bibr" rid="scirp.71531-ref8">8</xref>] . In both cases one parameter is dependent of the molecular size, whereas the four other parameters are of polar nature in the extended meaning of the term, i.e. independent of the molecular size. We call δ (as dispersion) the apolar solute parameter and we have found that it was better identified to the molecular polarizability (or the molar refractivity) than, for example, to the molar mass, the molar volume or the partition coefficient air hexadecane.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Overview of the previous and current steps related to the present study. MMA stands for a program of Multiplicative Matrix Analysis</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1230256x4.png"/></fig><p>Three out of our four polar solute parameters are very similar to those of Abraham and co-authors: those we are calling ε, α and β. By contrast, our ω parameter (as orientation or polarity strictly speaking) is quite different of the corresponding parameter according to Abraham and co-authors (equations have however been provided to transform one system into the other one [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] ). The acronyms δ, ω, ε, α and β for the five obtained solute parameters are respectively related to the forces of:</p><p>・ dispersion (London),</p><p>・ orientation or polarity strictly speaking (Keesom),</p><p>・ polarizability-induction (Debye), (ε as electrons involvement),</p><p>・ acidity (proton donor according to Br&#248;nsted),</p><p>・ basicity (proton acceptor according to Br&#248;nsted).</p><p>Based on a strong cooperation between our group and the Kov&#225;ts group, accurate values of solute parameters have solely been established applying an original algorithm presently called MMA (as Multiplicative Matrix Analysis) to a set of retention indices of 127 compounds on 11 phases [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref4">4</xref>] .</p><p>An improvement of this step has been the reduction of the number of needed stationary phases without losing accuracy. The most satisfactory result has been obtained with two apolar phases of very different molecular weight and same structure, and three polar phases, respectively poly-fluorinated, polyether and primary mono alcoholic. Because these five phases have been synthesized by the Kov&#225;ts group and are not commercially available, a procedure has been proposed to calibrate the commercial phases using six VOC references [<xref ref-type="bibr" rid="scirp.71531-ref4">4</xref>] . Once sets of five phases from the available commercial ones would be selected as independent enough in their D, W, E, A and B values, it would be in principle easy to develop measurements of solute parameters exclusively based on experimentation, potentially more refined.</p><p>In 1982 [<xref ref-type="bibr" rid="scirp.71531-ref9">9</xref>] we tried such experimental determination 100% GLC for 240 solutes, but the set of the five chosen phases was not orthogonal enough, and we are therefore considering that study as only of a preliminary interest.</p><p>It should be relatively easy to reach the above mentioned goal using filled columns. The purpose could however be harder with open tubular columns, particularly for the proton donor phase and the two apolar phases of very different molecular weight, as suggested, for example, by the results of Poole et al. [<xref ref-type="bibr" rid="scirp.71531-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref11">11</xref>] .</p><p>The 100% GLC determination of solutes parameters not seemingly being anymore developed, an alternative way has been followed consisting in the pooling of those presently available with those published by Abraham and co-authors [<xref ref-type="bibr" rid="scirp.71531-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref13">13</xref>] . In this step the Abraham data have been suitable transformed as mentioned above, and those in gas or solid state at room temperature have been excluded. This data pool, less accurate than the previous one, was supposed to have the interest to include homogeneous values for 456 compounds of more diversified nature [<xref ref-type="bibr" rid="scirp.71531-ref3">3</xref>] .</p></sec><sec id="s1_2"><title>1.2. Solvent Parameters of Stationary Phases</title><p>In the above mentioned step, simultaneously to the solute parameters for 127 compounds, were obtained the accurate values of solvent parameters named D, W, E, A and B for 11 stationary phases.</p><p>On another hand, from the important collection of GLC retention indices published by Mc Reynolds in 1970 (207 stationary phases on 226 columns and 10 VOC) [<xref ref-type="bibr" rid="scirp.71531-ref14">14</xref>] , we identified the molecular structures of 56 of these phases and derived their solvent parameters D, W, E, A and B. Because of an abnormal behavior of the phase diglycerol, observed in various studies and seemingly due to its high surface adsorption [<xref ref-type="bibr" rid="scirp.71531-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref15">15</xref>] - [<xref ref-type="bibr" rid="scirp.71531-ref18">18</xref>] , we have discarded this phase in the present study.</p><p>As for solutes, we pooled these two data sets into a more extended data set of 66 phases (56 ? 1 + 11) [<xref ref-type="bibr" rid="scirp.71531-ref5">5</xref>] .</p><p>We added in this pooled data set, according to [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] and [<xref ref-type="bibr" rid="scirp.71531-ref14">14</xref>] , the values of the parameter called b by Mc Reynolds [<xref ref-type="bibr" rid="scirp.71531-ref14">14</xref>] , allowing to transform volumes retention Vg into Kov&#225;ts retention indices RI. Indeed, this b parameter can be considered as a fifth characteristic of phases, together with W, E, A and B, the parameter D being a constant when the GC data are expressed in relative values (which is the case for RI).</p></sec><sec id="s1_3"><title>1.3. Results Concerning the Molecular Interpretation of Solute and Solvent Parameters Get in the Previous Studies</title><sec id="s1_3_1"><title>1.3.1. On the Parameters Related to the Hydrogen Bonding Forces</title><p>The results are clear and contrasted. On one hand their identification is almost evident (to a solute proton donor property correspond a solvent proton acceptor property and reciprocally). On the other hand their values predicted on the basis of a simplified molecular topology (which is summarized in the Material and Methods section of the present paper) fail to be satisfactory each time intramolecular hydrogen forces are suspected. The solution could perhaps be to extend the molecular topology presently applied, to a larger neighboring of a given atom. However, that solution would need considerably more experimental data than the presently available ones.</p></sec><sec id="s1_3_2"><title>1.3.2. On the Parameters Related to the Van der Waals Forces</title><p>The results are more satisfactory. Out of the three molecular parameters of solutes, those of dispersion δ and of induction-polarizability ε are clearly related to equations including the molar refractivity and the Van der Waals molar volume, both being easily and accurately predictable, even for solids and gases, using a simplified molecular topology.</p><p>Similarly, out of the solvent parameters of phases, the parameters b of McReynolds and E have appeared related to equations including the Van der Waals molar volume and the PSA (polar surface area), both being easily and accurately predictable, even for solids and gases, using a simplified molecular topology. By contrast, the cases of the orientation or polarity strictly speaking parameter of solutes ω, and of its associated solvent parameter W have remained open.</p><p>The present study, therefore, is limited to intent an optimal characterization of the solute parameters related to the Van der Waals forces, those related to the hydrogen bonding forces being (temporarily?) left aside.</p></sec></sec></sec><sec id="s2"><title>2. Material and Methods</title><sec id="s2_1"><title>2.1. Statistical Tools</title><p>In addition to the Microsoft Excel Windows facilities for drawing diagrams and handling data sets, the SYSTAT 12&#174; for Windows has been applied for stepwise MLRA (Multidimensional Linear Regression Analysis).</p></sec><sec id="s2_2"><title>2.2. SMT, A Simplified Molecular Topology</title><p>The principle of this tool has already presented elsewhere [<xref ref-type="bibr" rid="scirp.71531-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref4">4</xref>] . In the version used here, it only takes into account, for each atom of a molecule, its nature and the nature of its bonds, leaving aside the nature of its first neighbors with the exception of three cases specified hereafter. Each atom is provided with an index comprising a series of digits. Their sum is at most equal to its valence. The value of the digits define the type of bonds (1 for a single, 2 for a double bond, etc.), but the bonds with hydrogen are excluded.</p><p>In addition to the 34 atom characteristics kept, we also consider three additional topological features:</p><p>・ Chlorine linked to carbon C11.</p><p>・ Amines linked to (a carbon linked to O<sub>2</sub>). This feature is present in amides.</p><p>・ A connectivity parameter due to Zamora [<xref ref-type="bibr" rid="scirp.71531-ref19">19</xref>] called the “smallest set of smallest rings” (SSSR). According to this concept, for the naphthalene for example, which contains two individual C-6 rings and one C-10 ring embracing them, only the two six numbered rings are considered. Two six numbered rings corresponding to 12 carbon atoms, the SSSR value of naphthalene is therefore be taken equal to 12.</p><p>In <xref ref-type="table" rid="table1">Table 1</xref> are summarized the topological features finally kept in the present version, concerning the atoms C, H, O, N, P, S, F, Cl, Br, I. Let us specify that the calculations using the SMT procedure have been made manually in this study, using 2D molecular drawings from Chem Spider [<xref ref-type="bibr" rid="scirp.71531-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref20">20</xref>] .</p></sec><sec id="s2_3"><title>2.3. Solute and Solvent Parameters Data</title><p>As shown in the Introduction, four sets of solvation parameters have been established along the last decade: two for VOC as solutes and two for GLC stationary phases as solvents [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.71531-ref6">6</xref>] . For solvents, both become 100% from GLC experimentation: one can be considered as accurate (11 phases), and the other one more extended (66 phases) as less precise.</p><p>For solutes, one set exclusively comes from GLC experimentation and can be considered as accurate (127 compounds), and the other one, only partially from chromatographic origin and less precise, covers a greater variety of VOC (456 compounds). Some compounds have been excluded from these two initial experimental data sets of solutes:</p><p>・ Those which include Si or Sn,</p><p>・ Those which include a given atom only linked to hydrogen (e.g. CH<sub>4</sub>, OH<sub>2</sub>, NH<sub>3</sub>, SH<sub>2</sub>),</p><p>・ Those in gas or solid state at room temperature.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Nature of atomic and structural elements used in the SMT applied procedure*</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Structural elements</th><th align="center" valign="middle" >Bonds</th><th align="center" valign="middle" >Topological features</th></tr></thead><tr><td align="center" valign="middle" >Carbon</td><td align="center" valign="middle" >≤4</td><td align="center" valign="middle" >C<sub>0</sub>, C<sub>1</sub>, C<sub>11</sub>, C<sub>111</sub>, C<sub>1111</sub>, C<sub>2</sub>, C<sub>12</sub>, C<sub>112</sub>, C<sub>22</sub>, C<sub>3</sub>, C<sub>13</sub></td></tr><tr><td align="center" valign="middle" >Oxygen</td><td align="center" valign="middle" >≤2</td><td align="center" valign="middle" >O<sub>0</sub>, O<sub>1</sub>, O<sub>11</sub>, O<sub>2</sub></td></tr><tr><td align="center" valign="middle" >Nitrogen trivalent</td><td align="center" valign="middle" >≤3</td><td align="center" valign="middle" >N<sub>0</sub>, N<sub>1</sub>, N<sub>11</sub>, N<sub>111</sub>, N<sub>12</sub>, N<sub>3</sub></td></tr><tr><td align="center" valign="middle" >Nitrogen pentavalent</td><td align="center" valign="middle" >≤5</td><td align="center" valign="middle" >N<sub>122</sub></td></tr><tr><td align="center" valign="middle" >Phosphor pentavalent</td><td align="center" valign="middle" >≤5</td><td align="center" valign="middle" >P<sub>1112</sub></td></tr><tr><td align="center" valign="middle" >Fluorine</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >F<sub>1</sub></td></tr><tr><td align="center" valign="middle" >Chlorine</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Cl<sub>1</sub></td></tr><tr><td align="center" valign="middle" >Bromine</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Br<sub>1</sub></td></tr><tr><td align="center" valign="middle" >Lodine</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >L<sub>1</sub></td></tr><tr><td align="center" valign="middle" >Sulfur divalent</td><td align="center" valign="middle" >≤2</td><td align="center" valign="middle" >S<sub>0</sub>, S<sub>1</sub>, S<sub>11</sub>, S<sub>2</sub></td></tr><tr><td align="center" valign="middle" >Sulfur hexavalent</td><td align="center" valign="middle" >≤6</td><td align="center" valign="middle" >S<sub>111111</sub>, S<sub>1122</sub></td></tr><tr><td align="center" valign="middle" >Hydrogen</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >H1 = sum (maximal bonds-explicit bonds)</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >ADDITIONAL</td></tr><tr><td align="center" valign="middle" >Cl<sub>1</sub>^C<sub>11</sub></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Chlorine linked to C11</td></tr><tr><td align="center" valign="middle" >NCO</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >N<sub>1</sub> or N<sub>11</sub> or N<sub>111</sub> linked to (a carbon linked to O<sub>2</sub>)</td></tr><tr><td align="center" valign="middle" >SSSR</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Smallest sum of the smallest rings</td></tr></tbody></table></table-wrap><p>*See explanation in the text. Italicized elements are not involved in the present study.</p><p>Finally, the number of VOC kept in these two data sets under study becomes respectively 121 for the accurate one and 447 for the extended one.</p><p>These four data sets thus specified are reported in the Supplementary Material, excluding the parameters α, β, A and B, which are involved, as we saw, in the hydrogen bonding forces.</p></sec><sec id="s2_4"><title>2.4. Polar Surface Area</title><p>The polar surface area of a molecule (PSA) is currently defined as the surface sum over all polar atoms, primarily oxygen and nitrogen, also including their attached hydrogens [<xref ref-type="bibr" rid="scirp.71531-ref21">21</xref>] . PSA has successfully been applied in 1996 and 1997 by Palm et al. to reflect the molecular transport properties of drugs, particularly blood-brain barrier (BBB) penetration and intestinal absorption [<xref ref-type="bibr" rid="scirp.71531-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref22">22</xref>] . As already pointed out in 2007 by Ertl [<xref ref-type="bibr" rid="scirp.71531-ref23">23</xref>] , the number of publications in which PSA is involved has been growing exponentially since these early publications.</p><p>These interesting results have tended to consider PSA as a strictly pharmacological property not applicable in the physicochemical field as a general criterion of polarity, since, for example, strongly polar elements such as halogens, particularly fluorine, have always been excluded of its definition. We have however recently shown that PSA, associated with the Van der Waals molecular volume Vw, appears strongly implicated in the characterization of one of the polarities observed in GLC: the McReynolds b parameter already quoted [<xref ref-type="bibr" rid="scirp.71531-ref5">5</xref>] .</p><p>Few authors also include sulphur and phosphor in an alternative definition of PSA [<xref ref-type="bibr" rid="scirp.71531-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref25">25</xref>] . We have suggested in 2013 a slight modification to the initial definition extended to O, S, N, P, with the exception of hexavalent S and pentavalent N and P [<xref ref-type="bibr" rid="scirp.71531-ref6">6</xref>] . That was based on the fact that it is difficult to consider, on a theoretical point of view, hexavalent S and pentavalent N and P as polar atoms. Indeed, in these cases, all their peripheral electrons are involved in bonds. We proposed to call PSA2 this alternative definition in 2013, and we successfully applied the corresponding molecular characteristic to an olfactory study [<xref ref-type="bibr" rid="scirp.71531-ref6">6</xref>] .</p><p>A second purpose of the present study is therefore an attempt to elucidate what appears, at the first view, as a contradiction: is it PSA a pharmacological property strictly speaking or a more general tool characterizing the molecular polarity? That involves a clarification, on experimental basis, about its most suitable definition among the various ones already proposed: is it or not a unique one valid in all circumstances?</p><p>In their early applications [<xref ref-type="bibr" rid="scirp.71531-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref22">22</xref>] , PSA values have been established using sophisticated programs taking into account the molecular three-dimensional shape and its flexibility. However, a very simple topological method using summation of surface contributions of polar fragments (termed TPSA) has been applied by Ertl et al. [<xref ref-type="bibr" rid="scirp.71531-ref25">25</xref>] , exhibiting an excellent correlation with theoretical PSA values (r = 0.991, N = 34,810 substances).</p><p>In the present study, the TPSA values have been collected, for the extended set of 447 VOC, from Molinspiration [<xref ref-type="bibr" rid="scirp.71531-ref26">26</xref>] . For the stationary phases we adopted the atomic parameters according to Laffort [<xref ref-type="bibr" rid="scirp.71531-ref5">5</xref>] .</p></sec><sec id="s2_5"><title>2.5. Additional Molecular Properties Well Established</title><sec id="s2_5_1"><title>2.5.1. Molar and Molecular Volumes</title><p>The various expressions supposed to be reflecting the “intrinsic molecular volume” or the “Van der Waals molecular volume” are all additive properties (which it is not the case for the ratio molar mass/density at 20˚C). We have selected among then in the present study, the values of molecular volumes (expressed in cubic angstroms) proposed by the freely interactive calculator of Molinspiration [<xref ref-type="bibr" rid="scirp.71531-ref26">26</xref>] . The authors of this calculator have used, in a first step, a semi-empirical quantum chemistry method to build 3D molecular geometries for a training set of about 12,000 molecules. In a second step, they have fitted sum of fragment contributions to the supposed real volumes of the training set. We name this expression Vw (as Van der Waals volume).</p></sec><sec id="s2_5_2"><title>2.5.2. Molar Refractivity (MR and MR<sub>W</sub>)</title><p>These properties are the measure of the total polarizability of one mole of a given compound. According to the Lorentz and Lorenz equation, MR can be determined as follows:</p><disp-formula id="scirp.71531-formula117"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1230256x5.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.71531-formula118"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1230256x6.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.71531-formula119"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1230256x7.png"  xlink:type="simple"/></disp-formula><p>in which M, d and n stand respectively for the molar mass, the density at 20˚C and the refractive index at 20˚C. Initiated by Abraham et al. [<xref ref-type="bibr" rid="scirp.71531-ref8">8</xref>] , a modified expression of the molar refractivity can be obtained replacing V<sub>20</sub> in equation 2 by one or another expression supposed to be reflecting the “intrinsic molecular volume” or the “Van der Waals molecular volume”. We found in 2005 [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] that this modified expression of the molecular refractivity is the more suitable to reflect the apolar solubility parameter of solutes δ in GLC. As shown in Equation (5), we have here chosen V<sub>W</sub> for that, and called MR<sub>W</sub> the modified molar refractivity:</p><disp-formula id="scirp.71531-formula120"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1230256x8.png"  xlink:type="simple"/></disp-formula><p>The molar refractivity values are generally expressed in ml∙mol<sup>−</sup><sup>1</sup>.</p></sec></sec></sec><sec id="s3"><title>3. Results</title><sec id="s3_1"><title>3.1. The Solute Parameter of Orientation or Polarity Strictly Speaking</title><p>Applying a multiple linear regression analysis (MLRA) to the ω values of the 121 VOC data set, as possible functions of the molecular features of <xref ref-type="table" rid="table1">Table 1</xref>, produces the predictive model reported on the left of <xref ref-type="fig" rid="fig2">Figure 2</xref> and the corresponding correlogram on the right one. By contrast, a similar attempt with the extended data set of 447 VOC was so disappointing than those already published [<xref ref-type="bibr" rid="scirp.71531-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref3">3</xref>] .</p><p>As a reminder, F ratio value can be obtained from the correlation coefficient r, the number of observations N (here the number of VOC) and the number of independent variables, according to Abdi [<xref ref-type="bibr" rid="scirp.71531-ref27">27</xref>] :</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> A simplified molecular topology (SMT) applied to the set of 121 ω experimental values from [<xref ref-type="bibr" rid="scirp.71531-ref4">4</xref>] and reported in the Supplementary Material. Out of the 37 molecular features of <xref ref-type="table" rid="table1">Table 1</xref>, 11 have been selected using MLRA (partial F ratio &gt; 20). On the right: the corresponding correlogram for these 121 VOC values. We propose to call ω<sub>2016</sub> the values obtained according to the above SMT model. See details on the molecular feature [NCO] in the text</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1230256x9.png"/></fig><disp-formula id="scirp.71531-formula121"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1230256x10.png"  xlink:type="simple"/></disp-formula><p>Obviously, the quality of the prediction differs according to the considered statistical test; r or F (both statistical tests are supposed to be as high as possible).</p><p>Most statisticians often prefer the second criterion, particularly when the number of independent variables increases in large proportion relatively to the number of observations.</p><p>As a result, we consider for further uses, and perhaps as a first approach, the SMT model reported in <xref ref-type="fig" rid="fig2">Figure 2</xref> as a definition of the ω parameter (which we will call ω<sub>2016</sub>) in spite of the smaller diversity of molecular functions involved included in its definition (more precisely, ω<sub>2016</sub> = 100 times the SMT predicted values of experimental ω values).</p><p>An interesting observation is the discarding of the molecular feature N122 (present in nitrates) by the MLRA program, confirming our previous hypothesis that the pentavalent N is non polar [<xref ref-type="bibr" rid="scirp.71531-ref6">6</xref>] .</p><p>Let us specify that in <xref ref-type="fig" rid="fig2">Figure 2</xref>, the [NCO] molecular feature is not present in any of the 121 VOCs under study. It has however been added (between brackets), because when the MLRA is applied to the less precise data set of 447 VOC using as independent variables the same 37 features of <xref ref-type="table" rid="table1">Table 1</xref> plus the predicted ω according to the initial model of <xref ref-type="fig" rid="fig2">Figure 2</xref>, the unique feature added by the MLRA with a partial F ratio &gt;20, is NCO.</p></sec><sec id="s3_2"><title>3.2. Short Recalling and Updating of the Well Established Characterization of the Solute Parameters δ and ε</title><p>The best molecular property well established, related to the solute parameter of dispersion δ obtained via an experimental GLC, has been found to be the molar refractivity we have named MR<sub>w</sub> in Equation (5) [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] . Because the refractive index is not always available in liquid state, we propose to call henceforward δ<sub>2016</sub>, the values obtained using the SMT model of <xref ref-type="fig" rid="fig3">Figure 3</xref>, which will be valid whatever the states of VOCs under study at room temperature are. More precisely:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1230256x11.png" xlink:type="simple"/></inline-formula>from SMT up <xref ref-type="fig" rid="fig3">Figure 3</xref> (7)</p><p>The theoretical induction-polarizability parameter ε<sub>theoret</sub> is obtained via a bilinear relationship between the molar refractivity and the molar volume, such as its values equals zero for n-alkanes, according to the following equation:</p><disp-formula id="scirp.71531-formula122"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1230256x12.png"  xlink:type="simple"/></disp-formula><p>In order to express it in a similar scale of sizes than δ<sub>2016</sub> and ω<sub>2016</sub>, we define henceforward ε<sub>2016</sub> as follows:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1230256x13.png" xlink:type="simple"/></inline-formula>from SMT down <xref ref-type="fig" rid="fig3">Figure 3</xref> (9)</p></sec><sec id="s3_3"><title>3.3. The Solvent Parameters McR b, W and E Equations</title><p>No significant improvements have been found in the present study, comparatively to</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> SMT definitions models for the parameters of dispersion (δ<sub>2016</sub>) and induction-pola- rizability (ε<sub>2016</sub>), validated by the two correlograms on the right for the set of 447 compounds reported in the Supplementary Material.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1230256x14.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1230256x15.png"/></fig></fig-group><p>[<xref ref-type="bibr" rid="scirp.71531-ref5">5</xref>] , in the characterization of these three parameters using well established molecular properties or/and the SMT procedure. We can therefore consider as temporary valid the observations mentioned in this previous paper, which can be summarized as follows:</p><p>・ the three parameters appear partially related, in addition to other molecular features, to PSA,</p><p>・ each molecular feature concerned, including PSA, appears involved in a ratio of this feature to the molar volume V<sub>w</sub>, on the contrary of what is observed for solute parameters. In other words, the various types of solvent polarities appear in some way, as densities of polarity,</p><p>・ more precisely, the parameters McR b and E can be expressed via two different equations including both PSA/V<sub>W</sub> and 1/V<sub>W</sub>.</p><p>At this stage, there is no new argument concerning the inclusion or not of other polar elements than N and O in the definition of PSA. By contrast, the observation already made [<xref ref-type="bibr" rid="scirp.71531-ref6">6</xref>] that the pentavalent N does not seem to be a polar feature is confirmed in the present study.</p></sec></sec><sec id="s4"><title>4. Discussion-Conclusion</title><sec id="s4_1"><title>4.1. Solute Parameters</title><p>The results on solute parameters presented here, compared to those previously published on the same topic, show real improvements, as summarized in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>Let us recall that the difference in the N values between 2008 and the present study for δ and ε not at all results from an elimination of outliers in the MLRA of data, but from objective facts detailed in the Materials and Methods section. Concerning ω, the important difference value of N is principally interpreted as a lack of accuracy in the more extended data set, as we already saw.</p><p>The improvements observed in the present study are principally due to a pragmatic approach summarized in <xref ref-type="fig" rid="fig1">Figure 1</xref>:</p><p>・ starting with only accurate and superabundant experimental data submitted to an MMA;</p><p>・ physicochemical characterization when possible, with molecular properties well established for a large amount of compounds, as it is the case, for example, for V<sub>W</sub>, MR<sub>W</sub> and PSA;</p><p>・ if it is successful, applying SMT to these well established properties, in order to overcome some inappropriate situations (e.g. refraction index for solids and gases); this step has been applied to δ<sub>2016</sub> and ε<sub>2016</sub>;</p><p>・ if it is unsuccessful, applying SMT to chromatographic accurate and less numerous data (this step has been applied to ω<sub>2016</sub>).</p><p>It should be of interest to note the high mutual independence of these parameters, as it can be seen in <xref ref-type="fig" rid="fig4">Figure 4</xref>, and similarly previously observed for the initial data set of 125 solute parameters of 100% experimental GLC origin [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] .</p></sec><sec id="s4_2"><title>4.2. Solvent Parameters</title><p>The absence of improvements for solvent parameters is very probably due to a too small amount of accurate and superabundant chromatographic measurements. One of the consequences is the uncertainty about possible presence of polar elements in the definition of PSA, other than N and O. The only conclusive fact seems to be the absence</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Compared values of statistical tests get for some predicted values of solute parameters involved in the Van der Waals intermolecular forces of solutions. The correlation coefficient, the number of VOC and the partial F ratio are respectively represented by r, N and F</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" >r</th><th align="center" valign="middle" >N</th><th align="center" valign="middle" >F</th></tr></thead><tr><td align="center" valign="middle" >δ</td><td align="center" valign="middle" >2008 (ref. [<xref ref-type="bibr" rid="scirp.71531-ref3">3</xref>] )</td><td align="center" valign="middle" >0.981</td><td align="center" valign="middle" >456</td><td align="center" valign="middle" >944</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >present study</td><td align="center" valign="middle" >0.997</td><td align="center" valign="middle" >447</td><td align="center" valign="middle" >6136</td></tr><tr><td align="center" valign="middle" >ω</td><td align="center" valign="middle" >2008 (ref. [<xref ref-type="bibr" rid="scirp.71531-ref3">3</xref>] )</td><td align="center" valign="middle" >0.861</td><td align="center" valign="middle" >456</td><td align="center" valign="middle" >145</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >present study</td><td align="center" valign="middle" >0.976</td><td align="center" valign="middle" >121</td><td align="center" valign="middle" >197</td></tr><tr><td align="center" valign="middle" >ε</td><td align="center" valign="middle" >2008 (ref. [<xref ref-type="bibr" rid="scirp.71531-ref3">3</xref>] )</td><td align="center" valign="middle" >0.954</td><td align="center" valign="middle" >456</td><td align="center" valign="middle" >351</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >present study</td><td align="center" valign="middle" >0.978</td><td align="center" valign="middle" >447</td><td align="center" valign="middle" >691</td></tr></tbody></table></table-wrap><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Mutual correlation coefficients between the three solute parameters defined in the present study as involved in the Van der Waals molecular forces of solutions, for 447 solutes</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1230256x16.png"/></fig><p>of pentavalent N and P and of hexavalent S.</p></sec><sec id="s4_3"><title>4.3. General Comments</title><p>The present study does not provide any improvements in the separation of components of solutions nor the identification of such components, both being the principal followed purposes in chromatographic sciences. On the other hand, the results obtained in this study and in some other ones we have previously conducted in a similar way, would not be reached without the strongly help of GLC experimentation. We have presently the key to determine with simplicity and a relatively not too bad accuracy, the three parameters, for solutes, of Van der Waals forces in solutions. And we strongly believe that these labile forces could be implicated in some pharmacological and chemo sensorial properties. Our next effort will be to test this hypothesis.</p><p>It should be difficult to conclude this study without quoting an important recent review on the “Determination of solute descriptors by chromatographic methods” by Poole et al. [<xref ref-type="bibr" rid="scirp.71531-ref28">28</xref>] , and regret, at this juncture, some lack of mutual understanding between the majority of the authors working in this topic and our group. That, among others, concerns the no using of MMA as an appropriate tool to process GLC superabundant data sets (with the exception of Ulrich [<xref ref-type="bibr" rid="scirp.71531-ref29">29</xref>] ). One consequence is the supposed “impossibility to reflect independently the interactions associated with induced and stables dipoles” [<xref ref-type="bibr" rid="scirp.71531-ref28">28</xref>] . In fact and in spite of a questionable letter to the editor in 2006 [<xref ref-type="bibr" rid="scirp.71531-ref30">30</xref>] (short answer in [<xref ref-type="bibr" rid="scirp.71531-ref3">3</xref>] ) and an abundant exchange of correspondence with Michael Abraham, it has been demonstrated since 2005 [<xref ref-type="bibr" rid="scirp.71531-ref1">1</xref>] that a strictly speaking polarity descriptor of solutes can be expressed on the solely basis of S, R and B, according to the acronyms and the data of Abraham and co-authors. In addition, it is proposed in the present study a definition of such polarity descriptor, termed ω<sub>2016</sub>, uniquely based on some molecular features as we saw above. The validation of one or another ways, or possible crossed ones, could be based in the future on comparative performances in QSAR and QSPR.</p><p>Concerning the possible objection against our ω<sub>2016</sub> model, because only based on 121 solutes, it should be noted that this data set includes numerous chemical functions: alcohols, aldehydes, ketones, ethers, nitro-compounds, nitriles, secondary and tertiary amines, esters, various types of halogen and sulfur compounds and hydrocarbons, both of saturated or unsaturated types, with or without mono and polycycles… are however absent (and present in the set of 447 solutes) primary amines, carboxylic acids, amides and lactones. Also, substances with more than one chemical function are sparingly represented in this 121 data set. As a conclusion, the strictly speaking polarity descriptor proposed here, of purely pragmatic and not at all of theoretical nature, could be considered as a first approach, and possibly improvable in the future with the help, among others, of semi empirical quantum chemical methods already applied in this topic (e.g. [<xref ref-type="bibr" rid="scirp.71531-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.71531-ref31">31</xref>] ).</p></sec></sec><sec id="s5"><title>Acknowledgements</title><p>The author warmly thanks David Laffort for his writing assistance. He also sincerely thanks the Royal Society of Chemistry for its free Chem Spider database of chemical structures [<xref ref-type="bibr" rid="scirp.71531-ref20">20</xref>] and the Molinspiration Company for its freely interactive calculator [<xref ref-type="bibr" rid="scirp.71531-ref26">26</xref>] . This research did not receive any specific grant from funding agencies in the public, commercial, or not-for-profit sectors.</p></sec><sec id="s6"><title>Cite this paper</title><p>Laffort, P. (2016) A Revisited Definition of the Three Solute Descriptors Related to the Van der Waals Forces in Solutions. Open Journal of Physical Chemistry, 6, 86-100. http://dx.doi.org/10.4236/ojpc.2016.64009</p></sec><sec id="s7"><title>Supplementary Material</title><p>Databases associated with this article are freely available, on request to the author:&lt;paul.laffort@sfr.fr&gt;</p><disp-formula id="scirp.71531-formula123"><graphic  xlink:href="http://html.scirp.org/file/2-1230256x17.png"  xlink:type="simple"/></disp-formula><p>Submit or recommend next manuscript to SCIRP and we will provide best service for you:</p><p>Accepting pre-submission inquiries through Email, Facebook, LinkedIn, Twitter, etc.</p><p>A wide selection of journals (inclusive of 9 subjects, more than 200 journals)</p><p>Providing 24-hour high-quality service</p><p>User-friendly online submission system</p><p>Fair and swift peer-review system</p><p>Efficient typesetting and proofreading procedure</p><p>Display of the result of downloads and visits, as well as the number of cited articles</p><p>Maximum dissemination of your research work</p><p>Submit your manuscript at: http://papersubmission.scirp.org/</p><p>Or contact ojpc@scirp.org</p></sec></body><back><ref-list><title>References</title><ref id="scirp.71531-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Laffort, P., Chauvin, F., Dallos, A., Callegari, P. and Valentin, D. 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