<?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">CC</journal-id><journal-title-group><journal-title>Computational Chemistry</journal-title></journal-title-group><issn pub-type="epub">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.2017.52006</article-id><article-id pub-id-type="publisher-id">CC-75774</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>
 
 
  Comparative Study of the Chemical Reactivity of Helical Peptide Models for Protein Glycation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Juan</surname><given-names>Frau</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Daniel</surname><given-names>Glossman-Mitnik</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Departament de Química, Universitat de les Illes Balears, Palma de Mallorca, Spain</addr-line></aff><aff id="aff2"><addr-line>Laboratorio Virtual NANOCOSMOS, Departamento de Medio Ambiente y Energía, Centro de Investigación en Materiales Avanzados, Chihuahua, Mexico</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>juan.frau@uib.es(JF)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>28</day><month>04</month><year>2017</year></pub-date><volume>05</volume><issue>02</issue><fpage>65</fpage><lpage>73</lpage><history><date date-type="received"><day>January</day>	<month>4,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>April</month>	<year>25,</year>	</date><date date-type="accepted"><day>April</day>	<month>28,</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Non-enzymatic glycation of proteins has been implicated as an important cause of the complications associated with diabetes and Alzheimer disease. It is well known that glycation involves the reactivity of, primarily, the 
  <em>ε</em>-amino group of the lysines present in the protein. The immediate chemical environment of an amino group modulates the glycation reaction. In this work, several model helical peptides for protein glycation has been studied by resorting to QM:MM calculations through the ONIOM methodology. Some Conceptual DFT descriptors have been calculated that allowed the comparison of the chemical reactivity between the different model peptides in terms of the position of the Lys group and other spatially proximate amino acid residues.
 
</p></abstract><kwd-group><kwd>Helical Model peptides</kwd><kwd> Protein Glycation</kwd><kwd> Computational Chemistry</kwd><kwd> Molecular Modeling</kwd><kwd> Conceptual DFT</kwd><kwd> Chemical Reactivity Theory</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The nonenzymatic reaction between reducing carbohydrates and the amino groups of amino acids, peptide and proteins is called glycation and through a series of chain reaction leads to the formation of Advanced Glycation End- products (AGEs). These molecules have been related to some diseases like diabetes, Alzheimer and Parkinson. Nonenzymatic glycation of proteins has been implicated as an important cause of the complications associated with diabetes and Alzheimer disease. It is well known that glycation involves the reactivity of, primarily, the ε-amino group of the lysines present in the protein.</p><p>The immediate chemical environment of an amino group modulates the glycation reaction. Some years ago, Venkatraman et al [<xref ref-type="bibr" rid="scirp.75774-ref1">1</xref>] studied several helical peptide models in order to elucidate the proximity effect in the catalysis of the Amadori rearrangement. Their conclusions were similar to those of Howard et al [<xref ref-type="bibr" rid="scirp.75774-ref2">2</xref>] and Povey et al [<xref ref-type="bibr" rid="scirp.75774-ref3">3</xref>] who found that the glycation reaction affected the helicity, charge and other properties of the resulting molecules. </p><p>Therefore, we consider that it will be of practical interest to develop a the- oretical and computational tool that could be an aid for the prediction of the preferred glycation sites for the different possible conformational structures of model peptides because they could be an aid in the development of AGE in- hibitors. </p><p>Thus, the objective of this work is to predict the preferred glycation sites of the model helical peptides proposed by Venkatraman et al [<xref ref-type="bibr" rid="scirp.75774-ref1">1</xref>] by resorting to the calculation of some Conceptual DFT descriptors like the Fukui function indexes, the condensed dual descriptor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x3.png" xlink:type="simple"/></inline-formula> and the electrophilic and nucleophilic Parr functions. As the preferred glycation sites will be the same as those for the protonation reaction, the results of the calculations will allow us to qualitatively predict the pKa’s of the different lysine residues on the light of the obtained values for the Conceptual DFT descriptors [<xref ref-type="bibr" rid="scirp.75774-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref6">6</xref>] .</p></sec><sec id="s2"><title>2. Theoretical Background</title><p>As this work is part of an ongoing project, the theoretical background is analog to that presented in previous research [<xref ref-type="bibr" rid="scirp.75774-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.75774-ref13">13</xref>] and will be shown here for the sake of completeness. As it has been described in detail before, [<xref ref-type="bibr" rid="scirp.75774-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.75774-ref13">13</xref>] within the conceptual framework of DFT, [<xref ref-type="bibr" rid="scirp.75774-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref14">14</xref>] the chemical potential m is defined as: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x4.png" xlink:type="simple"/></inline-formula>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x5.png" xlink:type="simple"/></inline-formula> is the electronegativity, while the global chemical hardness <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x6.png" xlink:type="simple"/></inline-formula> is:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x7.png" xlink:type="simple"/></inline-formula>. Using a finite difference approximation, these expressions can be written as: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x8.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x9.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x10.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x11.png" xlink:type="simple"/></inline-formula> are the vertical ionization potential and elec- tron affinity, respectively. The electrophilicity index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x12.png" xlink:type="simple"/></inline-formula> has been defined as:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x13.png" xlink:type="simple"/></inline-formula>. The electrodonating (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x14.png" xlink:type="simple"/></inline-formula>) and electroaccepting (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x15.png" xlink:type="simple"/></inline-formula>) powers have been defined as: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x16.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x17.png" xlink:type="simple"/></inline-formula>. It follows that a larger (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x18.png" xlink:type="simple"/></inline-formula>) value corresponds to a better capability of accepting charge, whereas a smaller value of (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x19.png" xlink:type="simple"/></inline-formula>) makes it a better electron donor. In order to compare (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x20.png" xlink:type="simple"/></inline-formula>) with (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x21.png" xlink:type="simple"/></inline-formula>), the following definition of net electrophilicity has been proposed:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x22.png" xlink:type="simple"/></inline-formula>, that is, the electroaccepting power relative to the electrodonating power.</p></sec><sec id="s3"><title>3. Settings and Computational Methods</title><p>Following the lines of our previous work [<xref ref-type="bibr" rid="scirp.75774-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.75774-ref13">13</xref>] , the molecular structures of the studied compounds were constructed by starting with the readily available MOL structures for the amino acids (ChemSpider: www.chemspider.com, PubChem: https://pubchem.ncbi.nlm.nih.gov/). The most stable conformers were obtained by means of the Avogadro 1.2.0 program [<xref ref-type="bibr" rid="scirp.75774-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref19">19</xref>] through a random sampling with Molecular Mechanics techniques and a consideration of all the torsional angles through the general AMBER force field [<xref ref-type="bibr" rid="scirp.75774-ref20">20</xref>] .</p><p>The energies of the neutral, positive and negative peptides were obtained within the framework of QM:MM calculations performed through the ONIOM method [<xref ref-type="bibr" rid="scirp.75774-ref21">21</xref>] in the presence of water as a solvent, by doing IEF-PCM computations according to the SMD solvation model [<xref ref-type="bibr" rid="scirp.75774-ref22">22</xref>] . For the QM region, the MN12SX density functional [<xref ref-type="bibr" rid="scirp.75774-ref23">23</xref>] in connection with the Def2TZVP basis set was chosen [<xref ref-type="bibr" rid="scirp.75774-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref25">25</xref>] . The MN12SX density functional is a range-separated hybrid nonse- parable meta-NGA [<xref ref-type="bibr" rid="scirp.75774-ref23">23</xref>] . The Amber force field [<xref ref-type="bibr" rid="scirp.75774-ref26">26</xref>] was considered for the MM part. All the ONIOM calculations were performed as implemented in the Gaussian 09 [<xref ref-type="bibr" rid="scirp.75774-ref27">27</xref>] series of programs.</p></sec><sec id="s4"><title>4. Results and Discussion</title><p>The following peptides proposed by Venkatraman et al [<xref ref-type="bibr" rid="scirp.75774-ref1">1</xref>] were studied as mentioned before:</p><p>KD4: Ac-EYUALKAUADUAAUR-NH2</p><p>KD2: Ac-EYUALUAKADUAAUR-NH2</p><p>KH4: Ac-EYUALKAUAHUAAUR-NH2</p><p>RKD4: Ac-EYRULKAUADUAAUA-NH2</p><p>K14: Ac-EYUALKAUAUAAUR-NH2</p><p>From the cluster analysis, some members were selected for further analysis: 3 for KD4, 4 for KD2, 3 for KH4, 3 for RKD4 and 1 for K14.</p><p>The ionization potentials <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula> and electron affinities <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x24.png" xlink:type="simple"/></inline-formula> (in eV), and global electronegativity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x25.png" xlink:type="simple"/></inline-formula>, total chemical hardness<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x26.png" xlink:type="simple"/></inline-formula>, global electrophilicity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x27.png" xlink:type="simple"/></inline-formula>, electrodonating power, (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x28.png" xlink:type="simple"/></inline-formula>), electroaccepting power (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x29.png" xlink:type="simple"/></inline-formula>), and net electrophilicity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x30.png" xlink:type="simple"/></inline-formula> of the optimized conformers of the KD4, KD2, KH4, RKD4 and K14 model peptides calculated with the ONIOM method (MN12SX/ Def2TZVP:Amber) using water as solvent simulated with the SMD parame- trization of the IEF-PCM model are presented in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Within Conceptual DFT, the Fukui function is defined in terms of the derivative of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x31.png" xlink:type="simple"/></inline-formula> with respect to N [<xref ref-type="bibr" rid="scirp.75774-ref5">5</xref>] : <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x32.png" xlink:type="simple"/></inline-formula>The function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x33.png" xlink:type="simple"/></inline-formula> reflects the ability of a molecular site to accept or donate electrons. High values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x34.png" xlink:type="simple"/></inline-formula> are related to a high reactivity at point r [<xref ref-type="bibr" rid="scirp.75774-ref5">5</xref>] .</p><p>By applying a finite difference approximation to the previous expression, two definitions of Fukui functions depending on total electronic densities are obtained: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x38.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x39.png" xlink:type="simple"/></inline-formula>, are the electronic densities at point r for the system with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x40.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x41.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x42.png" xlink:type="simple"/></inline-formula> electrons, respectively. The first one, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x43.png" xlink:type="simple"/></inline-formula>, has been associated to reactivity for a nucleophilic attack so that it measures the intra- molecular reactivity at the site r towards a nucleophilic reagent. The second one, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x44.png" xlink:type="simple"/></inline-formula>, has been associated to reactivity for an electrophilic attack so that this function measures the intramolecular reactivity at the site r toward an electrophilic reagent [<xref ref-type="bibr" rid="scirp.75774-ref14">14</xref>] .</p><p>Morell et al. [<xref ref-type="bibr" rid="scirp.75774-ref28">28</xref>] - [<xref ref-type="bibr" rid="scirp.75774-ref34">34</xref>] have proposed a local reactivity descriptor (LRD) which is called the dual descriptor (DD) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x45.png" xlink:type="simple"/></inline-formula>The dual descriptor can be condensed over the atomic sites: when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x46.png" xlink:type="simple"/></inline-formula> the process is driven by a</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The ionization potentials I and electron affinities A (in eV), and global elec- tronegativity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x47.png" xlink:type="simple"/></inline-formula>, otal chemical hardness<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x48.png" xlink:type="simple"/></inline-formula>, global electrophilicity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x49.png" xlink:type="simple"/></inline-formula>, electrodonating power, (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x50.png" xlink:type="simple"/></inline-formula>), electroaccepting power (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x51.png" xlink:type="simple"/></inline-formula>), and net electrophilicity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x52.png" xlink:type="simple"/></inline-formula> of the optimized conformers of the KD4, KD2, KH4, RKD4 and K14 model peptides calculated with the ONIOM method (MN12SX/Def2TZVP:Amber) using water as solvent simulated with the SMD parametrization of the IEF-PCM model</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Peptide</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x53.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x54.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x55.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x56.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x57.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >(<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x58.png" xlink:type="simple"/></inline-formula>)</th><th align="center" valign="middle" >(<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x59.png" xlink:type="simple"/></inline-formula>)</th><th align="center" valign="middle" ><sup><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x60.png" xlink:type="simple"/></inline-formula> </sup></th></tr></thead><tr><td align="center" valign="middle" >KD4-1</td><td align="center" valign="middle" >6.241</td><td align="center" valign="middle" >0.336</td><td align="center" valign="middle" >3.289</td><td align="center" valign="middle" >5.905</td><td align="center" valign="middle" >0.916</td><td align="center" valign="middle" >3.845</td><td align="center" valign="middle" >0.556</td><td align="center" valign="middle" >4.402</td></tr><tr><td align="center" valign="middle" >KD4-2</td><td align="center" valign="middle" >6.323</td><td align="center" valign="middle" >0.399</td><td align="center" valign="middle" >3.361</td><td align="center" valign="middle" >5.924</td><td align="center" valign="middle" >0.954</td><td align="center" valign="middle" >3.958</td><td align="center" valign="middle" >0.597</td><td align="center" valign="middle" >4.555</td></tr><tr><td align="center" valign="middle" >KD4-3</td><td align="center" valign="middle" >6.451</td><td align="center" valign="middle" >0.350</td><td align="center" valign="middle" >3.400</td><td align="center" valign="middle" >6.101</td><td align="center" valign="middle" >0.947</td><td align="center" valign="middle" >3.976</td><td align="center" valign="middle" >0.576</td><td align="center" valign="middle" >4.552</td></tr><tr><td align="center" valign="middle" >KD2-1</td><td align="center" valign="middle" >6.418</td><td align="center" valign="middle" >0.382</td><td align="center" valign="middle" >3.400</td><td align="center" valign="middle" >6.036</td><td align="center" valign="middle" >0.958</td><td align="center" valign="middle" >3.992</td><td align="center" valign="middle" >0.592</td><td align="center" valign="middle" >4.585</td></tr><tr><td align="center" valign="middle" >KD2-2</td><td align="center" valign="middle" >6.297</td><td align="center" valign="middle" >0.216</td><td align="center" valign="middle" >3.257</td><td align="center" valign="middle" >6.081</td><td align="center" valign="middle" >0.872</td><td align="center" valign="middle" >3.753</td><td align="center" valign="middle" >0.496</td><td align="center" valign="middle" >4.249</td></tr><tr><td align="center" valign="middle" >KD2-3</td><td align="center" valign="middle" >6.297</td><td align="center" valign="middle" >0.216</td><td align="center" valign="middle" >3.257</td><td align="center" valign="middle" >6.081</td><td align="center" valign="middle" >0.872</td><td align="center" valign="middle" >3.753</td><td align="center" valign="middle" >0.496</td><td align="center" valign="middle" >4.249</td></tr><tr><td align="center" valign="middle" >KD2-4</td><td align="center" valign="middle" >6.306</td><td align="center" valign="middle" >0.172</td><td align="center" valign="middle" >3.239</td><td align="center" valign="middle" >6.133</td><td align="center" valign="middle" >0.855</td><td align="center" valign="middle" >3.714</td><td align="center" valign="middle" >0.474</td><td align="center" valign="middle" >4.188</td></tr><tr><td align="center" valign="middle" >KH4-1</td><td align="center" valign="middle" >6.447</td><td align="center" valign="middle" >0.340</td><td align="center" valign="middle" >3.394</td><td align="center" valign="middle" >6.106</td><td align="center" valign="middle" >0.943</td><td align="center" valign="middle" >3.964</td><td align="center" valign="middle" >0.571</td><td align="center" valign="middle" >4.535</td></tr><tr><td align="center" valign="middle" >KH4-2</td><td align="center" valign="middle" >6.329</td><td align="center" valign="middle" >0.382</td><td align="center" valign="middle" >3.355</td><td align="center" valign="middle" >5.946</td><td align="center" valign="middle" >0.947</td><td align="center" valign="middle" >3.943</td><td align="center" valign="middle" >0.587</td><td align="center" valign="middle" >4.530</td></tr><tr><td align="center" valign="middle" >KH4-3</td><td align="center" valign="middle" >6.371</td><td align="center" valign="middle" >0.275</td><td align="center" valign="middle" >3.323</td><td align="center" valign="middle" >6.096</td><td align="center" valign="middle" >0.906</td><td align="center" valign="middle" >3.854</td><td align="center" valign="middle" >0.531</td><td align="center" valign="middle" >4.385</td></tr><tr><td align="center" valign="middle" >RKD4-1</td><td align="center" valign="middle" >6.228</td><td align="center" valign="middle" >0.578</td><td align="center" valign="middle" >3.403</td><td align="center" valign="middle" >5.649</td><td align="center" valign="middle" >1.025</td><td align="center" valign="middle" >4.104</td><td align="center" valign="middle" >0.701</td><td align="center" valign="middle" >4.806</td></tr><tr><td align="center" valign="middle" >RKD4-2</td><td align="center" valign="middle" >6.407</td><td align="center" valign="middle" >0.308</td><td align="center" valign="middle" >3.357</td><td align="center" valign="middle" >6.099</td><td align="center" valign="middle" >0.924</td><td align="center" valign="middle" >3.908</td><td align="center" valign="middle" >0.551</td><td align="center" valign="middle" >4.459</td></tr><tr><td align="center" valign="middle" >RKD4-3</td><td align="center" valign="middle" >6.358</td><td align="center" valign="middle" >0.350</td><td align="center" valign="middle" >3.354</td><td align="center" valign="middle" >6.008</td><td align="center" valign="middle" >0.936</td><td align="center" valign="middle" >3.925</td><td align="center" valign="middle" >0.571</td><td align="center" valign="middle" >4.496</td></tr><tr><td align="center" valign="middle" >K14-1</td><td align="center" valign="middle" >6.377</td><td align="center" valign="middle" >0.234</td><td align="center" valign="middle" >3.306</td><td align="center" valign="middle" >6.143</td><td align="center" valign="middle" >0.889</td><td align="center" valign="middle" >3.816</td><td align="center" valign="middle" >0.510</td><td align="center" valign="middle" >4.326</td></tr></tbody></table></table-wrap><p>nucleophilic attack on atom k and then that atom acts as an electrophilic 100 species; conversely, when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x61.png" xlink:type="simple"/></inline-formula> the process is driven by an electrophilic attack over atom k and therefore atom k acts as a nucleophilic species. </p><p>In 2014, Domingo proposed the Parr functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x62.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.75774-ref35">35</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref36">36</xref>] which are given by the following equations:  <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x63.png" xlink:type="simple"/></inline-formula> (for electrophilic attacks) and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x64.png" xlink:type="simple"/></inline-formula> (for nucleophilic attacks) which are related to the atomic spin density (ASD) at the r atom of the radical cation or anion of a given molecule, respectively. The ASD over each atom of the radical cation and radical anion of the molecule gives the local nucleophilic <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x65.png" xlink:type="simple"/></inline-formula> and electrophilic <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x66.png" xlink:type="simple"/></inline-formula> Parr functions of the neutral molecule [<xref ref-type="bibr" rid="scirp.75774-ref37">37</xref>] .</p><p>The condensed Fukui functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x67.png" xlink:type="simple"/></inline-formula>, condensed dual descriptors <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x68.png" xlink:type="simple"/></inline-formula> and electrophilic Parr functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x69.png" xlink:type="simple"/></inline-formula> over the N atoms of the amino groups of the Lys residues of the optimized conformers of the KD4, KD2, KH4, RKD4 and K14 model peptides calculated with the ONIOM method (MN12SX/Def2TZVP: Amber) using water as solvent simulated with the SMD parametrization of the IEF-PCM model are presented in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>The first thing that can be observed from <xref ref-type="table" rid="table2">Table 2</xref> is that the results for the descriptors through calculations based on the Mulliken Population Analysis (MPA) or Hirshfeld Population Analysis (HPA) are roughly the same and that there are not qualitatively differences between them.</p><p>However, it can be observed from <xref ref-type="table" rid="table1">Table 1</xref> that the chemical reactivity will be</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The condensed Fukui functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x70.png" xlink:type="simple"/></inline-formula>, condensed dual descriptors <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x71.png" xlink:type="simple"/></inline-formula> and electrophilic Parr functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x72.png" xlink:type="simple"/></inline-formula> over the N atoms of the amino groups of the Lys residues of the optimized conformers of the KD4, KD2, KH4, RKD4 and K14 model peptides calculated with the ONIOM method (MN12SX/Def2TZVP:Amber) using water as solvent simulated with the SMD parametrization of the IEF-PCM model. MPA: Mulliken Population Analysis, HPA: Hirshfeld Population Analysis</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Peptide</th><th align="center" valign="middle"  colspan="3"  >MPA</th><th align="center" valign="middle"  colspan="3"  >HPA</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x73.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x74.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x75.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x76.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x77.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x78.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >KD4-1</td><td align="center" valign="middle" >0.417</td><td align="center" valign="middle" >−0.424</td><td align="center" valign="middle" >0.537</td><td align="center" valign="middle" >0.411</td><td align="center" valign="middle" >−0.537</td><td align="center" valign="middle" >0.514</td></tr><tr><td align="center" valign="middle" >KD4-2</td><td align="center" valign="middle" >0.728</td><td align="center" valign="middle" >−0.732</td><td align="center" valign="middle" >0.834</td><td align="center" valign="middle" >0.656</td><td align="center" valign="middle" >−0.834</td><td align="center" valign="middle" >0.803</td></tr><tr><td align="center" valign="middle" >KD4-3</td><td align="center" valign="middle" >0.766</td><td align="center" valign="middle" >−0.771</td><td align="center" valign="middle" >0.860</td><td align="center" valign="middle" >0.678</td><td align="center" valign="middle" >−0.860</td><td align="center" valign="middle" >0.832</td></tr><tr><td align="center" valign="middle" >KD2-1</td><td align="center" valign="middle" >0.753</td><td align="center" valign="middle" >−0.759</td><td align="center" valign="middle" >0.842</td><td align="center" valign="middle" >0.665</td><td align="center" valign="middle" >−0.842</td><td align="center" valign="middle" >0.812</td></tr><tr><td align="center" valign="middle" >KD2-2</td><td align="center" valign="middle" >0.689</td><td align="center" valign="middle" >−0.690</td><td align="center" valign="middle" >0.810</td><td align="center" valign="middle" >0.615</td><td align="center" valign="middle" >−0.810</td><td align="center" valign="middle" >0.774</td></tr><tr><td align="center" valign="middle" >KD2-3</td><td align="center" valign="middle" >0.689</td><td align="center" valign="middle" >−0.690</td><td align="center" valign="middle" >0.810</td><td align="center" valign="middle" >0.615</td><td align="center" valign="middle" >−0.810</td><td align="center" valign="middle" >0.774</td></tr><tr><td align="center" valign="middle" >KD2-4</td><td align="center" valign="middle" >0.554</td><td align="center" valign="middle" >−0.564</td><td align="center" valign="middle" >0.618</td><td align="center" valign="middle" >0.508</td><td align="center" valign="middle" >−0.618</td><td align="center" valign="middle" >0.603</td></tr><tr><td align="center" valign="middle" >KH4-1</td><td align="center" valign="middle" >0.765</td><td align="center" valign="middle" >−0.770</td><td align="center" valign="middle" >0.858</td><td align="center" valign="middle" >0.677</td><td align="center" valign="middle" >−0.858</td><td align="center" valign="middle" >0.830</td></tr><tr><td align="center" valign="middle" >KH4-2</td><td align="center" valign="middle" >0.737</td><td align="center" valign="middle" >−0.740</td><td align="center" valign="middle" >0.844</td><td align="center" valign="middle" >0.662</td><td align="center" valign="middle" >−0.844</td><td align="center" valign="middle" >0.813</td></tr><tr><td align="center" valign="middle" >KH4-3</td><td align="center" valign="middle" >0.320</td><td align="center" valign="middle" >−0.324</td><td align="center" valign="middle" >0.404</td><td align="center" valign="middle" >0.322</td><td align="center" valign="middle" >−0.404</td><td align="center" valign="middle" >0.385</td></tr><tr><td align="center" valign="middle" >RKD4-1</td><td align="center" valign="middle" >0.582</td><td align="center" valign="middle" >−0.596</td><td align="center" valign="middle" >0.707</td><td align="center" valign="middle" >0.524</td><td align="center" valign="middle" >−0.707</td><td align="center" valign="middle" >0.683</td></tr><tr><td align="center" valign="middle" >RKD4-2</td><td align="center" valign="middle" >0.751</td><td align="center" valign="middle" >−0.753</td><td align="center" valign="middle" >0.859</td><td align="center" valign="middle" >0.669</td><td align="center" valign="middle" >−0.859</td><td align="center" valign="middle" >0.826</td></tr><tr><td align="center" valign="middle" >RKD4-3</td><td align="center" valign="middle" >0.724</td><td align="center" valign="middle" >−0.729</td><td align="center" valign="middle" >0.835</td><td align="center" valign="middle" >0.636</td><td align="center" valign="middle" >−0.835</td><td align="center" valign="middle" >0.794</td></tr><tr><td align="center" valign="middle" >R14-1</td><td align="center" valign="middle" >0.319</td><td align="center" valign="middle" >−0.326</td><td align="center" valign="middle" >0.400</td><td align="center" valign="middle" >0.318</td><td align="center" valign="middle" >−0.400</td><td align="center" valign="middle" >0.383</td></tr></tbody></table></table-wrap><p>different for the different conformational structures of the model peptides. The amino groups of the Lys residues in the model helical peptides make these systems to behave as electrodonating molecules in the glycation reaction. Thus, KD4-3 and KD4-2 will be more reactive than KD4-1. The same trend is observed for the chemical hardness<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x79.png" xlink:type="simple"/></inline-formula>, the global electrophilicity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x80.png" xlink:type="simple"/></inline-formula> and the net electrophilicity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x81.png" xlink:type="simple"/></inline-formula>. If we now turn to <xref ref-type="table" rid="table2">Table 2</xref>, it can be seen that the values of the condensed dual descriptor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x82.png" xlink:type="simple"/></inline-formula> and the electrophilic Parr functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x83.png" xlink:type="simple"/></inline-formula> over the N atoms of the amino groups of the Lys residues are larger for the KD4-3 and KD4-2 model peptides than for the KD4-1 system. Therefore, the global and local Conceptual DFT descriptors predict the same behavior and can discriminate between the different conformational structures. The same conclusions may be extracted from the values of the Conceptual DFT descriptors from <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref> for the other model helical peptides.</p><p>Indeed, the sites for glycation will be also the preferred sites for protonation. Thus, the pKa’s of the Lys residues will be also dependent on the conformational structures of the model peptides. Moreover, the trend in the pKa of the different conformers may be predicted in terms of the local hypersoftness (LHS), which is a local reactivity descriptor that has been defined so that it permits to measure local reactivitiesaccording to the molecular size [<xref ref-type="bibr" rid="scirp.75774-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref32">32</xref>] . The working equation is expressed as follows:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x84.png" xlink:type="simple"/></inline-formula>, where S stands for the global softness [<xref ref-type="bibr" rid="scirp.75774-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.75774-ref39">39</xref>] . As the local hypersoftness can be condensed over the atomic sites, the condensed local hypersoftness is simply computed as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x85.png" xlink:type="simple"/></inline-formula>. The procedure is explained as follows: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x86.png" xlink:type="simple"/></inline-formula>is expressed in atomic units, meanwhile S is measured in mili eV raised to the power of −1, however before performing the multiplication, the mili factor is turned back into 10<sup>−</sup><sup>3</sup> and then S is raised to the power of 2; the resulting value uses the unit mili eV raised to the power of −2, meaning m(eV<sup>−</sup><sup>2</sup>); the paren- thesis is put in order to make clear that the prefix mili is not raised to the power of -2. By considering the most reactive conformer of each model peptide, the following trend for the pKa’s of the Lys residues can be found: KD4 ≈ KD2 &gt; KH4 &gt; RKD4 &gt; K14. That is, although the exact value of the pKa cannot be predicted, a qualitative information about their relative ordering can be established by considering the global and local Conceptual DFT descriptors.</p></sec><sec id="s5"><title>5. Conclusion</title><p>The preferred glycation sites of several model helical peptides have been established by resorting to the calculation of some Conceptual DFT descriptors like the Fukui function indexes, the condensed dual descriptor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1710074x87.png" xlink:type="simple"/></inline-formula> and the electrophilic and nucleophilic Parr functions. The results were obtained within the framework of QM:MM calculations performed through the ONIOM method in the presence of water as a solvent. The pKa’s of the different Lys residues could be qualitatively predicted on the light of the obtained values for the Conceptual DFT descriptors. Therefore, the techniques presented in this work can be regarded as a practical computational tool for the prediction of the preferred glycation sites of peptides and proteins and for a qualitative description of the pKa’s associated to the ionizable side-chain groups.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This work has been partially supported by CIMAV, SC and Consejo Nacional de Ciencia y Tecnolog&#237;a (CONACYT, Mexico) through Grant 219566/2014 for Basic Science Research and Grant 265217/2016 for a Foreign Sabbatical Leave. Daniel Glossman-Mitnik conductedthis work while a Sabbatical Fellow at the University of the Balearic Islands from which support is gratefully acknowledged. This work was cofunded by the Ministerio de Econom&#237;a y Competitividad (MINECO) and the European Fund for Regional Development (FEDER) 175 (CTQ2014-55835-R).</p></sec><sec id="s7"><title>Cite this paper</title><p>Frau, J. and Gloss- man-Mitnik, D. 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