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  <front>
    <journal-meta>
      <journal-id journal-id-type="publisher-id">cc</journal-id>
      <journal-title-group>
        <journal-title>Computational Chemistry</journal-title>
      </journal-title-group>
      <issn pub-type="epub">2332-5984</issn>
      <issn pub-type="ppub">2332-5968</issn>
      <publisher>
        <publisher-name>Scientific Research Publishing</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.4236/cc.2026.144008</article-id>
      <article-id pub-id-type="publisher-id">cc-154665</article-id>
      <article-categories>
        <subj-group>
          <subject>Article</subject>
        </subj-group>
        <subj-group>
          <subject>Chemistry</subject>
          <subject>Materials Science</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Design of New Anilines with Predicted Values of Their Octanol/Water Partition Coefficients</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Diarrassouba</surname>
            <given-names>Fatogoma</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
      </contrib-group>
      <aff id="aff1"><label>1</label> Laboratoire de Thermodynamique et Physico-Chimie du Milieu (LTPCM), Unité de Formation et de Recherche des Sciences Fondamentales et Appliquées (UFR-SFA), Université Nangui ABROGOUA, Abidjan, Côte d’Ivoire </aff>
      <aff id="aff2"><label>2</label> Unité de Formation et de Recherche Sciences et Technologies (UFR-ST), Université Alassane OUATTARA, Bouaké, Côte d’Ivoire </aff>
      <author-notes>
        <fn fn-type="conflict" id="fn-conflict">
          <p>The author declares no conflicts of interest regarding the publication of this paper.</p>
        </fn>
      </author-notes>
      <pub-date pub-type="epub">
        <day>08</day>
        <month>10</month>
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="collection">
        <month>10</month>
        <year>2026</year>
      </pub-date>
      <volume>14</volume>
      <issue>04</issue>
      <fpage>131</fpage>
      <lpage>147</lpage>
      <history>
        <date date-type="received">
          <day>19</day>
          <month>09</month>
          <year>2026</year>
        </date>
        <date date-type="accepted">
          <day>19</day>
          <month>10</month>
          <year>2026</year>
        </date>
        <date date-type="published">
          <day>22</day>
          <month>10</month>
          <year>2026</year>
        </date>
      </history>
      <permissions>
        <copyright-statement>© 2026 by the authors and Scientific Research Publishing Inc.</copyright-statement>
        <copyright-year>2026</copyright-year>
        <license license-type="open-access">
          <license-p> This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license ( <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link> ). </license-p>
        </license>
      </permissions>
      <self-uri content-type="doi" xlink:href="https://doi.org/10.4236/cc.2026.144008">https://doi.org/10.4236/cc.2026.144008</self-uri>
      <abstract>
        <p>In our previous work, we established a predictive QSPR (Quantitative Structure-Property Relationship) model for the octanol/water partition coefficient based on ionization energy (<italic>IE</italic>), electronic energy (<italic>E</italic><italic><sub>T</sub></italic>), and dipole moment (<italic>μ</italic>). This model has been shown to be suitable for predicting the properties of new anilines falling within its applicability domain, with a 95% confidence level. The present study, which builds upon that earlier work, aims to expand the dataset for this family of compounds by designing new anilines that fit the model’s applicability domain and predicting their octanol/water partition coefficients. In this context, we designed a series of thirty-three (33) new anilines. All these molecules were optimized at the B3LYP/6-311G (d, p) level of theory, and vibrational frequencies were calculated at the same level. The calculated octanol/water partition coefficients for these molecules indicate that they are all lipophilic. The formation reaction for these new compounds proceeds spontaneously, accompanied by heat release and a decrease in disorder.</p>
      </abstract>
      <kwd-group kwd-group-type="author-generated" xml:lang="en">
        <kwd>Design</kwd>
        <kwd>Aniline</kwd>
        <kwd>QSPR Model</kwd>
        <kwd>Octanol/Water Partition Coefficient</kwd>
        <kwd>Standard Thermodynamic Quantity of Formation</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>1. Introduction</title>
      <p>Humanity has made significant progress in numerous fields, such as agriculture, electronics, the pharmaceutical industry, and many other sectors. Chemical products play a vital role in industrial development. In general, the applications of any material depend on its characteristics and properties [<xref ref-type="bibr" rid="B1">1</xref>]. Aniline (aminobenzene) is one of the most important substances used across many industrial sectors. Due to the diversity of its applications, it has attracted the interest of many researchers. It plays a major role in multiple industrial fields, particularly in the manufacture of rubber and engine components. It is a fundamental industrial chemical, with interest in it growing following its use as an intermediate in the synthesis of numerous chemical compounds. Aniline significantly influences everyday products; notably, it is a component of many medicines. A prime example is paracetamol, a widely used drug that represents considerable production value on the market [<xref ref-type="bibr" rid="B1">1</xref>]. Aniline is a simple, well-known molecule; its octanol/water partition coefficient has been studied as a reference parameter or intermediate in broader research within toxicology, medicinal chemistry, and materials science (such as polyaniline). Understanding aniline’s lipophilicity is essential for predicting its toxicity, its ability to cross biological membranes (such as skin or cell membranes), and its environmental behavior (biodegradation and accumulation in soil). In this context, it is necessary to predict the lipophilicity of its derivatives prior to their synthesis. The general objective of this work is to utilize the QSPR (Quantitative Structure-Property Relationship) model for predicting the octanol/water partition coefficient that was developed in our previous research [<xref ref-type="bibr" rid="B2">2</xref>]. In fact, the aim is clearly to design a series of new aniline analogues falling within the model’s applicability domain and to predict their octanol/water partition coefficients using the QSPR model developed to expand the database.</p>
    </sec>
    <sec id="sec2">
      <title>2. Material and Methods</title>
      <sec id="sec2dot1">
        <title>2.1. Material</title>
        <p>2.1.1. Reference Molecule Structure</p>
        <p>The new molecules were designed by substituting hydrogen atoms on the aniline molecule (the reference or parent molecule, sourced from the experimental database) with alkyl groups [<xref ref-type="bibr" rid="B2">2</xref>]. The two-dimensional structure of aniline is as follows (<xref ref-type="fig" rid="fig1">Figure 1</xref>):</p>
        <fig id="fig1">
          <label>Figure 1</label>
          <graphic xlink:href="https://html.scirp.org/file/1710209-rId15.jpeg?20261022091146" />
        </fig>
        <p>Figure 1. 2D structure of aniline.</p>
        <p>2.1.2. Software and Level of Theory Used</p>
        <p>GaussView 5.0 [<xref ref-type="bibr" rid="B3">3</xref>] software was used to represent the 3D structure and visualize the molecules under study. Subsequently, Gaussian 09 [<xref ref-type="bibr" rid="B4">4</xref>] software was used for geometry optimization and frequency calculations at a temperature of 298.15 K and a pressure of 1 atmosphere in the gas phase. The level of theory used to calculate the various molecular descriptors was B3LYP/6-311G (d, p). The 2D structures were generated using ChemSketch [<xref ref-type="bibr" rid="B5">5</xref>].</p>
      </sec>
      <sec id="sec2dot2">
        <title>2.2. Methods</title>
        <p>2.2.1. Domain of Applicability of a Model</p>
        <p>A QSPR/QSAR (Quantitative Structure-Property Relationship/Quantitative Structure-Activity Relationship) model cannot be considered universal, as it is developed using a limited number of compounds that do not cover the entire chemical space. Consequently, the predicted property or activity of a compound that is chemically dissimilar to the training set cannot automatically be considered reliable [<xref ref-type="bibr" rid="B6">6</xref>][<xref ref-type="bibr" rid="B7">7</xref>]. The applicability domain (AD) defines the region within which a compound’s properties can be predicted with confidence. The AD thus corresponds to the area of chemical space encompassing the training set compounds and similar compounds located nearby in that same space [<xref ref-type="bibr" rid="B8">8</xref>]. Several methods exist for determining the AD of a QSPR/QSAR model; among these is the fragment-based method [<xref ref-type="bibr" rid="B8">8</xref>]. This method assesses whether a molecule falls within a model’s AD based on the presence of specific fragments. If a new molecule contains novel fragments, it is deemed to lie outside the model’s AD. Conversely, if the new molecule presents no novel fragments, it is considered to be within the AD, and the prediction is regarded as reliable. The fragment-based method is employed in this study because it is well-suited to our simple molecules, unlike complex ones.</p>
        <p>2.2.2. QSPR Model Used to Predict the Octanol/Water Partition Coefficient of New Anilines</p>
        <p>The QSPR model used for the design of the new anilines derivatives was developed in our previous work [<xref ref-type="bibr" rid="B2">2</xref>]. The equation for this model is presented below, along with some statistical and validation parameters:</p>
        <disp-formula id="FD1">
          <label>(1)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mtext>Log</mml:mtext>
              <mml:mtext>
                 
              </mml:mtext>
              <mml:msub>
                <mml:mi>P</mml:mi>
                <mml:mrow>
                  <mml:mtext>theo</mml:mtext>
                </mml:mrow>
              </mml:msub>
              <mml:mo>=</mml:mo>
              <mml:mn>5.4544</mml:mn>
              <mml:mo>−</mml:mo>
              <mml:mn>1.8954</mml:mn>
              <mml:mtext>
                 
              </mml:mtext>
              <mml:mi>I</mml:mi>
              <mml:mi>E</mml:mi>
              <mml:mo>−</mml:mo>
              <mml:mn>0.0105</mml:mn>
              <mml:msub>
                <mml:mi>E</mml:mi>
                <mml:mi>T</mml:mi>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:mn>0.3945</mml:mn>
              <mml:mi>μ</mml:mi>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>with the ionization energy (<italic>IE</italic>) expressed in electron-volts (eV), the electronic energy (<italic>E</italic><italic><sub>T</sub></italic>) expressed in expressed in atomic units (a.u.) or Hartrees (Ha), and the dipole moment (<italic>µ</italic>) expressed in Debyes (D).</p>
        <disp-formula id="FD2">
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            <mml:mtable columnalign="left">
              <mml:mtr>
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                  <mml:mn>17</mml:mn>
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                  <mml:mi>R</mml:mi>
                  <mml:mo>=</mml:mo>
                  <mml:mn>0.9747</mml:mn>
                  <mml:mo>;</mml:mo>
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                  <mml:msup>
                    <mml:mi>R</mml:mi>
                    <mml:mn>2</mml:mn>
                  </mml:msup>
                  <mml:mo>=</mml:mo>
                  <mml:mn>0.9501</mml:mn>
                  <mml:mo>;</mml:mo>
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                  <mml:msubsup>
                    <mml:mi>R</mml:mi>
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                    </mml:mrow>
                    <mml:mn>2</mml:mn>
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                  <mml:mo>=</mml:mo>
                  <mml:mn>0.9348</mml:mn>
                  <mml:mo>;</mml:mo>
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                      </mml:mrow>
                    </mml:mrow>
                    <mml:mo stretchy="true">¯</mml:mo>
                  </mml:mover>
                  <mml:mo>=</mml:mo>
                  <mml:mn>0.9013</mml:mn>
                  <mml:mo>;</mml:mo>
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                  </mml:mtext>
                  <mml:mi>Δ</mml:mi>
                  <mml:msubsup>
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                  </mml:msubsup>
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                    </mml:mrow>
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                  </mml:mrow>
                  <mml:mo>=</mml:mo>
                  <mml:mn>0.0787</mml:mn>
                </mml:mtd>
              </mml:mtr>
            </mml:mtable>
          </mml:math>
        </disp-formula>
        <p>2.2.3. Standard Thermodynamic Quantities of Formation</p>
        <p>Quantum chemical calculations and the use of experimental data in the form of reference thermodynamic tables [<xref ref-type="bibr" rid="B9">9</xref>] allow for the determination of the standard values of the enthalpy of formation (<inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> Δ </mml:mi><mml:mi> f </mml:mi></mml:msub><mml:msup><mml:mi> H </mml:mi><mml:mn> 0 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> ), entropy of formation (<inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> Δ </mml:mi><mml:mi> f </mml:mi></mml:msub><mml:msup><mml:mi> S </mml:mi><mml:mn> 0 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> ), and Gibbs free energy of formation (<inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> Δ </mml:mi><mml:mi> f </mml:mi></mml:msub><mml:msup><mml:mi> G </mml:mi><mml:mn> 0 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> ) for the molecular system at 298.15 K and 1 atm pressure in the gas phase. The enthalpy of formation of a molecular system is calculated using the relationship proposed by J. W. Ochterski [<xref ref-type="bibr" rid="B10">10</xref>]:</p>
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                            <mml:mi>X</mml:mi>
                            <mml:mo>°</mml:mo>
                          </mml:msubsup>
                          <mml:mrow>
                            <mml:mo>(</mml:mo>
                            <mml:mrow>
                              <mml:mn>0</mml:mn>
                              <mml:mtext>
                                 
                              </mml:mtext>
                              <mml:mtext>K</mml:mtext>
                            </mml:mrow>
                            <mml:mo>)</mml:mo>
                          </mml:mrow>
                        </mml:mrow>
                        <mml:mo>)</mml:mo>
                      </mml:mrow>
                    </mml:mrow>
                  </mml:mstyle>
                </mml:mtd>
              </mml:mtr>
            </mml:mtable>
          </mml:math>
        </disp-formula>
        <p>where the last two terms of this relation are referred to as the enthalpic correction (or increment) for the molecule and the atoms, respectively. For elemental substances, this corresponds to the heat involved in heating the atoms from 0 K to 298 K. These values are obtained experimentally relative to the standard state of the elements. As for the term <inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> Δ </mml:mi><mml:mi> f </mml:mi></mml:msub><mml:msup><mml:mi> H </mml:mi><mml:mn> 0 </mml:mn></mml:msup><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> M </mml:mi><mml:mo> , </mml:mo><mml:mn> 0 </mml:mn><mml:mtext>   </mml:mtext><mml:mtext> K </mml:mtext></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> , it is determined using the following relation:</p>
        <disp-formula id="FD4">
          <label>(3)</label>
          <mml:math>
            <mml:mrow>
              <mml:msub>
                <mml:mi>Δ</mml:mi>
                <mml:mi>f</mml:mi>
              </mml:msub>
              <mml:msup>
                <mml:mi>H</mml:mi>
                <mml:mn>0</mml:mn>
              </mml:msup>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mi>M</mml:mi>
                  <mml:mo>,</mml:mo>
                  <mml:mn>0</mml:mn>
                  <mml:mtext>
                     
                  </mml:mtext>
                  <mml:mtext>K</mml:mtext>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:mstyle displaystyle="true">
                <mml:msub>
                  <mml:mo>∑</mml:mo>
                  <mml:mrow>
                    <mml:mtext>Atoms</mml:mtext>
                  </mml:mrow>
                </mml:msub>
                <mml:mrow>
                  <mml:mi>x</mml:mi>
                  <mml:msub>
                    <mml:mi>Δ</mml:mi>
                    <mml:mi>f</mml:mi>
                  </mml:msub>
                  <mml:msup>
                    <mml:mi>H</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msup>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mrow>
                      <mml:mi>X</mml:mi>
                      <mml:mo>,</mml:mo>
                      <mml:mn>0</mml:mn>
                      <mml:mtext>
                         
                      </mml:mtext>
                      <mml:mtext>K</mml:mtext>
                    </mml:mrow>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
              </mml:mstyle>
              <mml:mo>−</mml:mo>
              <mml:mo>∑</mml:mo>
              <mml:msub>
                <mml:mi>D</mml:mi>
                <mml:mn>0</mml:mn>
              </mml:msub>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mi>M</mml:mi>
                <mml:mo>)</mml:mo>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p><italic>x</italic> defines the number of atoms of species <italic>X</italic> in molecule <italic>M</italic>.</p>
        <p><inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> Δ </mml:mi><mml:mi> f </mml:mi></mml:msub><mml:msup><mml:mi> H </mml:mi><mml:mn> 0 </mml:mn></mml:msup><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> X </mml:mi><mml:mo> , </mml:mo><mml:mn> 0 </mml:mn><mml:mtext>   </mml:mtext><mml:mtext> K </mml:mtext></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> is an experimental value corresponding to the heat of formation of atom <italic>X</italic> at 0 K. The final term, <inline-formula><mml:math><mml:mrow><mml:mstyle displaystyle="true"><mml:mo> ∑ </mml:mo><mml:mrow><mml:msub><mml:mi> D </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:mrow><mml:mo> ( </mml:mo><mml:mi> M </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mstyle></mml:mrow></mml:math></inline-formula> , corresponds to the atomization energy of molecule <italic>M</italic>. This energy arises from the decomposition of one mole of the molecule into its constituent atoms. The calculation of <inline-formula><mml:math><mml:mrow><mml:mstyle displaystyle="true"><mml:mo> ∑ </mml:mo><mml:mrow><mml:msub><mml:mi> D </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:mrow><mml:mo> ( </mml:mo><mml:mi> M </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mstyle></mml:mrow></mml:math></inline-formula> is performed using the electronic energies (<italic>ε</italic>) of the constituent atoms and the molecule, as well as the internal energy at 0 K known as the Zero-Point Energy (ZPE) of the latter, according to the relation below:</p>
        <disp-formula id="FD5">
          <label>(4)</label>
          <mml:math>
            <mml:mrow>
              <mml:mstyle displaystyle="true">
                <mml:mo>∑</mml:mo>
                <mml:mrow>
                  <mml:msub>
                    <mml:mi>D</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msub>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mi>M</mml:mi>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
              </mml:mstyle>
              <mml:mo>=</mml:mo>
              <mml:mstyle displaystyle="true">
                <mml:msub>
                  <mml:mo>∑</mml:mo>
                  <mml:mrow>
                    <mml:mtext>Atoms</mml:mtext>
                  </mml:mrow>
                </mml:msub>
                <mml:mrow>
                  <mml:mi>x</mml:mi>
                  <mml:msub>
                    <mml:mi>ε</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msub>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mi>X</mml:mi>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
              </mml:mstyle>
              <mml:mo>−</mml:mo>
              <mml:mrow>
                <mml:mo>[</mml:mo>
                <mml:mrow>
                  <mml:msub>
                    <mml:mi>ε</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msub>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mi>M</mml:mi>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                  <mml:mo>+</mml:mo>
                  <mml:msub>
                    <mml:mi>ε</mml:mi>
                    <mml:mrow>
                      <mml:mi>Z</mml:mi>
                      <mml:mi>P</mml:mi>
                      <mml:mi>E</mml:mi>
                    </mml:mrow>
                  </mml:msub>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mi>M</mml:mi>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
                <mml:mo>]</mml:mo>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>The entropy of formation at 298 K, <inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> Δ </mml:mi><mml:mi> f </mml:mi></mml:msub><mml:msup><mml:mi> S </mml:mi><mml:mn> 0 </mml:mn></mml:msup><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 298 </mml:mn><mml:mtext>   </mml:mtext><mml:mtext> K </mml:mtext></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> , is determined using atomic entropy values (<inline-formula><mml:math><mml:mrow><mml:msup><mml:mi> S </mml:mi><mml:mn> 0 </mml:mn></mml:msup><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> X </mml:mi><mml:mo> , </mml:mo><mml:mn> 298 </mml:mn><mml:mtext>   </mml:mtext><mml:mtext> K </mml:mtext></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> ) from the JANAF Thermochemical Tables [<xref ref-type="bibr" rid="B9">9</xref>] and the molecular entropy obtained via quantum mechanical calculation. The relationship proposed by J. W. Ochterski [<xref ref-type="bibr" rid="B10">10</xref>] for determining the entropy of formation of a molecular system is:</p>
        <disp-formula id="FD6">
          <label>(5)</label>
          <mml:math>
            <mml:mrow>
              <mml:msub>
                <mml:mi>Δ</mml:mi>
                <mml:mi>f</mml:mi>
              </mml:msub>
              <mml:msup>
                <mml:mi>S</mml:mi>
                <mml:mn>0</mml:mn>
              </mml:msup>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mn>298</mml:mn>
                  <mml:mtext>
                     
                  </mml:mtext>
                  <mml:mtext>K</mml:mtext>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:msup>
                <mml:mi>S</mml:mi>
                <mml:mn>0</mml:mn>
              </mml:msup>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mi>M</mml:mi>
                  <mml:mo>,</mml:mo>
                  <mml:mn>298</mml:mn>
                  <mml:mtext>
                     
                  </mml:mtext>
                  <mml:mtext>K</mml:mtext>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>−</mml:mo>
              <mml:mstyle displaystyle="true">
                <mml:mo>∑</mml:mo>
                <mml:mrow>
                  <mml:mi>x</mml:mi>
                  <mml:msup>
                    <mml:mi>S</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msup>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mrow>
                      <mml:mi>X</mml:mi>
                      <mml:mo>,</mml:mo>
                      <mml:mn>298</mml:mn>
                      <mml:mtext>
                         
                      </mml:mtext>
                      <mml:mtext>K</mml:mtext>
                    </mml:mrow>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
              </mml:mstyle>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where <inline-formula><mml:math><mml:mrow><mml:msup><mml:mi> S </mml:mi><mml:mn> 0 </mml:mn></mml:msup><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> M </mml:mi><mml:mo> , </mml:mo><mml:mn> 298 </mml:mn><mml:mtext>   </mml:mtext><mml:mtext> K </mml:mtext></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi> H </mml:mi><mml:mrow><mml:mi> c </mml:mi><mml:mi> o </mml:mi><mml:mi> r </mml:mi><mml:mi> r </mml:mi></mml:mrow></mml:msub><mml:mo> − </mml:mo><mml:msub><mml:mi> G </mml:mi><mml:mrow><mml:mi> c </mml:mi><mml:mi> o </mml:mi><mml:mi> r </mml:mi><mml:mi> r </mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi> T </mml:mi></mml:mfrac></mml:mrow></mml:math></inline-formula> is the standard absolute entropy.</p>
        <p>Knowing the enthalpy of formation and the entropy of formation, the standard Gibbs free energy of formation is easily calculated using the relationship:</p>
        <disp-formula id="FD7">
          <label>(6)</label>
          <mml:math>
            <mml:mrow>
              <mml:msub>
                <mml:mi>Δ</mml:mi>
                <mml:mi>f</mml:mi>
              </mml:msub>
              <mml:msup>
                <mml:mi>G</mml:mi>
                <mml:mn>0</mml:mn>
              </mml:msup>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mn>298</mml:mn>
                  <mml:mtext>
                     
                  </mml:mtext>
                  <mml:mtext>K</mml:mtext>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:msub>
                <mml:mi>Δ</mml:mi>
                <mml:mi>f</mml:mi>
              </mml:msub>
              <mml:msup>
                <mml:mi>H</mml:mi>
                <mml:mn>0</mml:mn>
              </mml:msup>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mn>298</mml:mn>
                  <mml:mtext>
                     
                  </mml:mtext>
                  <mml:mtext>K</mml:mtext>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>−</mml:mo>
              <mml:mi>T</mml:mi>
              <mml:msub>
                <mml:mi>Δ</mml:mi>
                <mml:mi>f</mml:mi>
              </mml:msub>
              <mml:msup>
                <mml:mi>S</mml:mi>
                <mml:mn>0</mml:mn>
              </mml:msup>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mn>298</mml:mn>
                  <mml:mtext>
                     
                  </mml:mtext>
                  <mml:mtext>K</mml:mtext>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <disp-formula id="FD8">
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>T</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mn>298.15</mml:mn>
              <mml:mtext>
                 
              </mml:mtext>
              <mml:mtext>K</mml:mtext>
            </mml:mrow>
          </mml:math>
        </disp-formula>
      </sec>
    </sec>
    <sec id="sec3">
      <title>3. Results and Discussion</title>
      <sec id="sec3dot1">
        <title>3.1. Design of Novel Aniline-Based Compounds</title>
        <p>A series of thirty-three (33) molecules was designed by substituting hydrogen atoms of aniline (the parent molecule) with alkyl groups. The molecules were designated AN_<italic>i</italic> (1 ≤ <italic>i</italic> ≤ 33). The developed QSPR model was used to predict the octanol/water partition coefficient for this series. The 2D structures, molecular descriptor values, and theoretical octanol/water partition coefficient values are summarized in <bold>Table 1</bold>.</p>
        <p><bold>Table 1</bold><bold>.</bold> 2D structures of the designed molecules, molecular descriptor values, and theoretical octanol/water partition coefficient values obtained using the QSPR model.</p>
        <table-wrap id="tbl1">
          <label>Table 1</label>
          <table>
            <tbody>
              <tr>
                <td>
                  <bold>Compound</bold>
                </td>
                <td>
                  <bold>2D structure</bold>
                </td>
                <td>
                  <italic>
                    <bold>IE</bold>
                  </italic>
                  <bold>(eV)</bold>
                </td>
                <td>
                  <italic>
                    <bold>E</bold>
                  </italic>
                  <italic>
                    <bold>
                      <sub>T</sub>
                    </bold>
                  </italic>
                  <bold>(u.a.)</bold>
                </td>
                <td>
                  <italic>
                    <bold>μ</bold>
                  </italic>
                  <bold>(D)</bold>
                </td>
                <td>
                  <bold>Log</bold>
                  <italic>
                    <bold>P</bold>
                  </italic>
                  <bold>
                    <sub>theo</sub>
                  </bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_1</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId52.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2835</td>
                <td>−405.6567</td>
                <td>1.6054</td>
                <td>
                  <bold>2.23</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_2</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId54.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2141</td>
                <td>−405.6598</td>
                <td>1.5990</td>
                <td>
                  <bold>2.36</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_3</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId56.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2755</td>
                <td>−405.6605</td>
                <td>1.6079</td>
                <td>
                  <bold>2.24</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_4</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId58.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2468</td>
                <td>−405.6581</td>
                <td>1.8052</td>
                <td>
                  <bold>2.38</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_5</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId60.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2763</td>
                <td>−444.9792</td>
                <td>1.5376</td>
                <td>
                  <bold>2.63</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_6</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId62.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2091</td>
                <td>−444.9843</td>
                <td>1.5732</td>
                <td>
                  <bold>2.77</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_7</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId64.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2712</td>
                <td>−444.9850</td>
                <td>1.5664</td>
                <td>
                  <bold>2.65</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_8</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId66.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2436</td>
                <td>−444.9821</td>
                <td>1.7273</td>
                <td>
                  <bold>2.76</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_9</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId68.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2750</td>
                <td>−484.3034</td>
                <td>1.5699</td>
                <td>
                  <bold>3.06</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_10</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId70.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2059</td>
                <td>−484.3084</td>
                <td>1.5696</td>
                <td>
                  <bold>3.19</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_11</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId72.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2899</td>
                <td>−444.9782</td>
                <td>1.6359</td>
                <td>
                  <bold>2.64</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_12</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId74.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2175</td>
                <td>−444.9833</td>
                <td>1.6297</td>
                <td>
                  <bold>2.78</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_13</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId76.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2663</td>
                <td>−444.984</td>
                <td>1.6670</td>
                <td>
                  <bold>2.70</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_14</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId78.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2727</td>
                <td>−444.9811</td>
                <td>1.7300</td>
                <td>
                  <bold>2.71</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_15</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId80.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2916</td>
                <td>−484.3016</td>
                <td>1.6309</td>
                <td>
                  <bold>3.05</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_16</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId82.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2228</td>
                <td>−484.3071</td>
                <td>1.6807</td>
                <td>
                  <bold>3.20</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_17</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId84.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2725</td>
                <td>−484.3077</td>
                <td>1.6608</td>
                <td>
                  <bold>3.10</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_18</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId86.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2668</td>
                <td>−484.3038</td>
                <td>1.6640</td>
                <td>
                  <bold>3.11</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_19</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId88.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.2120</td>
                <td>−484.3052</td>
                <td>1.6905</td>
                <td>
                  <bold>3.22</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_20</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId90.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.1592</td>
                <td>−484.3103</td>
                <td>1.6936</td>
                <td>
                  <bold>3.32</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_21</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId92.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.4802</td>
                <td>−444.9665</td>
                <td>0.9547</td>
                <td>
                  <bold>2.01</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_22</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId94.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.3898</td>
                <td>−444.9694</td>
                <td>0.9662</td>
                <td>
                  <bold>2.19</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_23</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId96.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.1259</td>
                <td>−444.9753</td>
                <td>1.7789</td>
                <td>
                  <bold>3.01</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_24</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId98.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.4622</td>
                <td>−444.9658</td>
                <td>1.3539</td>
                <td>
                  <bold>2.20</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_25</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId100.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.1312</td>
                <td>−484.2958</td>
                <td>1.7410</td>
                <td>
                  <bold>3.40</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_26</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId102.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.0690</td>
                <td>−484.2992</td>
                <td>1.7488</td>
                <td>
                  <bold>3.52</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_27</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId104.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.1371</td>
                <td>−484.2989</td>
                <td>1.8597</td>
                <td>
                  <bold>3.43</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_28</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId106.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.4630</td>
                <td>−484.2900</td>
                <td>1.2892</td>
                <td>
                  <bold>2.59</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_29</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId108.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.3107</td>
                <td>−484.2742</td>
                <td>0.7854</td>
                <td>
                  <bold>2.68</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_30</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId110.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.3310</td>
                <td>−484.2781</td>
                <td>0.6134</td>
                <td>
                  <bold>2.57</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_31</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId112.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.3391</td>
                <td>−484.2782</td>
                <td>0.4777</td>
                <td>
                  <bold>2.50</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_32</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId114.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.3665</td>
                <td>−484.2750</td>
                <td>0.8021</td>
                <td>
                  <bold>2.58</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_33</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId116.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>4.3752</td>
                <td>−523.5974</td>
                <td>0.9235</td>
                <td>
                  <bold>3.02</bold>
                </td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p><bold>Table 1</bold> shows variations in each determined parameter from one molecule to another. The data indicate that the octanol/water partition coefficient values are all positive, revealing that the designed molecules are lipophilic (hydrophobic). Consequently, these compounds are soluble in fatty substances but insoluble in polar solvents such as water. This lipophilic nature stems from the substitution of hydrogen atoms on the aromatic ring or nitrogen atom with alkyl groups, which are lipophilic moieties. Molecules with a LogP value between 0 and 3 are moderately lipophilic, whereas those with a LogP greater than 3 are highly lipophilic. Furthermore, the hydrophobicity of the molecules increases with the length of the substituent’s carbon chain. For instance, a compound with a methyl group (-CH<sub>3</sub>) on the ring is less lipophilic than one with an ethyl group (-C<sub>2</sub>H<sub>5</sub>); similarly, a compound with an ethyl group is less lipophilic than one with a propyl group (-C<sub>3</sub>H<sub>7</sub>). Positional isomers exhibit virtually identical octanol/water partition coefficient values, implying they possess essentially the same degree of hydrophobicity. Generally, for a given total number of carbon atoms, a molecule with a branched alkyl group (e.g., isopropyl) shows a slightly lower lipophilicity parameter than one with a linear chain (e.g., propyl) due to differences in steric hindrance. Overall, the hydrophobicity of the molecules varies with the dipole moment. Indeed, as the dipole moment increases, hydrophobic character increases. Conversely, a decrease in hydrophobic character is observed when the dipole moment decreases. For aniline (the parent molecule), the experimental value of the octanol/water partition coefficient is 0.90 (±0.05) [<xref ref-type="bibr" rid="B2">2</xref>]. This positive value clearly indicates that aniline is also lipophilic. The lipophilicity of aniline derivatives varies predictably depending on whether the aniline is primary, secondary, or tertiary, as well as on the nature of the substituents attached to the nitrogen atom or the aromatic ring. Overall, lipophilicity increases with the degree of substitution (from primary to tertiary aniline) and with the length or volume of the alkyl groups. However, ideally, experimental octanol/water partition coefficient values for these new molecules should be obtained.</p>
      </sec>
      <sec id="sec3dot2">
        <title>3.2. Standard Thermodynamic Quantities of Formation of the Molecules</title>
        <p>The thermodynamic quantities of formation were determined in order to study the thermodynamic stability and characteristics of the formation reactions of the designed molecules.</p>
        <p><bold>Table 2.</bold> Structures of the designed molecules and values of formation quantities (in kcal/mol), except for entropy of formation (in cal/mol·K) (<italic>T</italic> = 298.15 K, <italic>P</italic> = 1 atm, gas phase).</p>
        <table-wrap id="tbl2">
          <label>Table 2</label>
          <table>
            <tbody>
              <tr>
                <td>
                  <bold>Compound</bold>
                </td>
                <td>
                  <bold>2D structure</bold>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>Δ</mml:mi>
                          <mml:mi>f</mml:mi>
                        </mml:msub>
                        <mml:msubsup>
                          <mml:mstyle mathvariant="bold" mathsize="normal">
                            <mml:mi>H</mml:mi>
                          </mml:mstyle>
                          <mml:mrow>
                            <mml:mn>2</mml:mn>
                            <mml:mn>9</mml:mn>
                            <mml:mn>8</mml:mn>
                          </mml:mrow>
                          <mml:mn>0</mml:mn>
                        </mml:msubsup>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>Δ</mml:mi>
                          <mml:mi>f</mml:mi>
                        </mml:msub>
                        <mml:msubsup>
                          <mml:mstyle mathvariant="bold" mathsize="normal">
                            <mml:mi>S</mml:mi>
                          </mml:mstyle>
                          <mml:mrow>
                            <mml:mn>2</mml:mn>
                            <mml:mn>9</mml:mn>
                            <mml:mn>8</mml:mn>
                          </mml:mrow>
                          <mml:mn>0</mml:mn>
                        </mml:msubsup>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
                <td>
                  <inline-formula>
                    <mml:math display="inline">
                      <mml:mrow>
                        <mml:msub>
                          <mml:mi>Δ</mml:mi>
                          <mml:mi>f</mml:mi>
                        </mml:msub>
                        <mml:msubsup>
                          <mml:mstyle mathvariant="bold" mathsize="normal">
                            <mml:mi>G</mml:mi>
                          </mml:mstyle>
                          <mml:mrow>
                            <mml:mn>2</mml:mn>
                            <mml:mn>9</mml:mn>
                            <mml:mn>8</mml:mn>
                          </mml:mrow>
                          <mml:mn>0</mml:mn>
                        </mml:msubsup>
                      </mml:mrow>
                    </mml:math>
                  </inline-formula>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>AN_1</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId124.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−413.8600</td>
                <td>−636.6470</td>
                <td>−224.0437</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_2</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId54.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−415.9772</td>
                <td>−634.0562</td>
                <td>−226.9334</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_3</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId56.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−416.4139</td>
                <td>−634.5171</td>
                <td>−227.2327</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_4</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId58.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−414.7542</td>
                <td>−636.9269</td>
                <td>−224.8544</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_5</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId60.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−456.3109</td>
                <td>−720.9608</td>
                <td>−241.3565</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_6</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId62.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−459.6800</td>
                <td>−719.0918</td>
                <td>−245.2828</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_7</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId64.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−460.1143</td>
                <td>−719.6201</td>
                <td>−245.5595</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_8</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId66.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−458.1244</td>
                <td>−722.0426</td>
                <td>−242.8474</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_9</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId68.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−499.7747</td>
                <td>−806.2616</td>
                <td>−259.3878</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_10</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId70.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−503.0992</td>
                <td>−804.3716</td>
                <td>−263.2758</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_11</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId72.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−455.8792</td>
                <td>−721.5816</td>
                <td>−240.7396</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_12</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId74.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−459.2828</td>
                <td>−721.1207</td>
                <td>−244.2807</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_13</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId76.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−459.7039</td>
                <td>−721.2238</td>
                <td>−244.6710</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_14</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId78.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−457.6833</td>
                <td>−723.8799</td>
                <td>−241.8585</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_15</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId80.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−498.8811</td>
                <td>−806.3794</td>
                <td>−258.4591</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_16</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId82.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−502.5018</td>
                <td>−806.2932</td>
                <td>−262.1055</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_17</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId84.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−502.8689</td>
                <td>−806.4426</td>
                <td>−262.4281</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_18</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId86.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−500.1800</td>
                <td>−808.9998</td>
                <td>−258.9768</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_19</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId88.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−501.4332</td>
                <td>−807.5770</td>
                <td>−260.6541</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_20</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId90.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−504.8186</td>
                <td>−806.4573</td>
                <td>−264.3733</td>
              </tr>
              <tr>
                <td>
                  <bold>AN_21</bold>
                </td>
                <td>
                  <inline-graphic xlink:href="https://html.scirp.org/file/1710209-rId92.jpeg?20261022091148">
                  </inline-graphic>
                </td>
                <td>−448.3114</td>
                <td>−721.8552</td>
                <td>−233.0903</td>
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                <td>−578.7444</td>
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        </table-wrap>
        <p>Variations in the determined thermodynamic quantities are also observed from one molecule to another. The values for the standard thermodynamic quantities of formation for the new anilines are all negative. Negative values for enthalpy and Gibbs free energy indicate an exothermic reaction and a spontaneous reaction, respectively. A negative entropy value indicates a decrease in disorder. Consequently, the formation of all the new anilines occurs spontaneously, accompanied by heat release and a decrease in disorder, at a temperature of 298.15 K and a pressure of 1 atm in the gas phase (<bold>Table 2</bold>). The negative value of the Gibbs free energy of formation thus reflects the existence and stability of the newly designed molecules.</p>
      </sec>
    </sec>
    <sec id="sec4">
      <title>4. Conclusion</title>
      <p>Regarding this study, which aimed to design new aniline derivatives, a key finding is that all thirty-three (33) designed molecules exhibit positive octanol/water partition coefficients, indicating that they are lipophilic. Overall, lipophilicity increases with the degree of substitution (from primary to tertiary aniline) and with the length or volume of the alkyl groups. As for the thermodynamic parameters of formation, all values are negative; this indicates that the formation of these new molecules occurs spontaneously, accompanied by heat release and a decrease in disorder. The lipophilicity of the aniline derivatives varies predictably depending on whether the aniline is primary, secondary, or tertiary, as well as on the nature of the substituents attached to the nitrogen atom or the aromatic ring. However, obtaining experimental values would be ideal, as this would allow for the confirmation or refutation of the theoretically determined molecular properties.</p>
    </sec>
  </body>
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