<?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">JASMI</journal-id><journal-title-group><journal-title>Journal of Analytical Sciences, Methods and Instrumentation</journal-title></journal-title-group><issn pub-type="epub">2164-2745</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jasmi.2014.44014</article-id><article-id pub-id-type="publisher-id">JASMI-52018</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Medicine&amp;Healthcare</subject><subject> Chemistry&amp;Materials Science</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Generalized Electron Balance for Dynamic Redox Systems in Mixed-Solvent Media
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>nna</surname><given-names>Maria Michałowska-Kaczmarczyk</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tadeusz</surname><given-names>Michałowski</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Oncology, The University Hospital in Cracow, Cracow, Poland</addr-line></aff><aff id="aff2"><addr-line>Faculty of Engineering and Chemical Technology, Cracow University of Technology, Cracow, Poland</addr-line></aff><pub-date pub-type="epub"><day>02</day><month>12</month><year>2014</year></pub-date><volume>04</volume><issue>04</issue><fpage>102</fpage><lpage>109</lpage><history><date date-type="received"><day>16</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>25</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>5</day>	<month>November</month>	<year>2014</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>
 
 
  A complex example of electrolytic redox system involving 47 species, 3 electron-active elements and five (3 am-phiprotic + 2 aprotic) co-solvents, is presented. Mixed solvates of the species thus formed are admitted in the system considered. It is proved that the Generalized Electron Balance (GEB) in its simplest form obtained according to the Approach II to GEB is identical with the one obtained for aqueous media and binary-solvent system, and is equivalent to the Approach I to GEB.
 
</p></abstract><kwd-group><kwd>Electrolytic Redox Systems</kwd><kwd> Generalized Electron Balance</kwd><kwd> Mixed-Solvent Media</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Motto: “Everything should be made as simple as possible, but not simpler” [<xref ref-type="bibr" rid="scirp.52018-ref1">1</xref>] .</p><p>In the previous issues [<xref ref-type="bibr" rid="scirp.52018-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.52018-ref8">8</xref>] and in earlier papers cited therein, the concept of Generalized Electron Balance (GEB), completing the set of compatible equations necessary for quantitative/mathematical solution of electrolytic redox systems, was introduced as two alternative options, named as Approach I and Approach II to GEB. In both Approaches it is assumed/admitted, that all the species <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x5.png" xlink:type="simple"/></inline-formula> exist in an electrolytic system in their natural form, i.e., as solvates. In particular, there are hydrates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x6.png" xlink:type="simple"/></inline-formula> in aqueous (W = H<sub>2</sub>O) media, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x7.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x8.png" xlink:type="simple"/></inline-formula>or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x9.png" xlink:type="simple"/></inline-formula> in binary-solvent media (W, A), (W, B) or (A, B) [<xref ref-type="bibr" rid="scirp.52018-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.52018-ref11">11</xref>] , respectively. The values of n<sub>Wi</sub>, n<sub>Ai</sub> and n<sub>Bi</sub>, considered as mean numbers of W, A and B attached to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x10.png" xlink:type="simple"/></inline-formula>, are unknown, in principle, and vary with the co-solvent(s) composition, and solute(s) concentration.</p><p>In this paper, we refer also to more complex media with the mixture of co-solvents: W, A, B, E and F. We assume that the co-solvents are mutually miscible and at least one of the co-solvents has amphiprotic properties</p><p>[<xref ref-type="bibr" rid="scirp.52018-ref5">5</xref>] . Eeach of the co-solvents has potential/real solvating properties, i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x12.png" xlink:type="simple"/></inline-formula>in the solvated species<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x13.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x14.png" xlink:type="simple"/></inline-formula> denotes N<sub>i</sub> entities of these species in the related</p><p>system. In further part of the paper, we assume W = H<sub>2</sub>O, A = CH<sub>3</sub>OH, B = C<sub>2</sub>H<sub>5</sub>OH, E = (CH<sub>3</sub>)<sub>2</sub>SO, F = CH<sub>3</sub>CN;</p><p>W, A, B have amphiprotic properties, and E, F―have not. In particular, N<sub>15</sub> ions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x15.png" xlink:type="simple"/></inline-formula> contain: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x16.png" xlink:type="simple"/></inline-formula>atoms of H, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x17.png" xlink:type="simple"/></inline-formula>atoms of O, N<sub>15</sub></p><p>atoms of I, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x18.png" xlink:type="simple"/></inline-formula>atoms of C, N<sub>15</sub>n<sub>15E</sub> atoms of S, and N<sub>15</sub>n<sub>15F</sub> atoms of N. It is as-</p><p>sumed that the solvents do not form―with solvates―the species <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x19.png" xlink:type="simple"/></inline-formula> other than those formed in (known from) aqueous media. In other words, W, A, B, E, F enter (potentially) the solvating sphere of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x20.png" xlink:type="simple"/></inline-formula>. On this basis, the elemental balances f(E(i)) for particular elements E(i) are formulated. For ordering purposes, we denote: E(1) = H, E(2) = O, E(3) = I, E(4) = C, E(5) = S, E(6) = N. We apply also the balances f(C(Y)) for the cores C(Y), Y = A, B, E, F. The “core” is a cluster of elements of the same composition, structure and charge, that does not undergo a change in the system in question; e.g., CH<sub>3</sub>OH, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x21.png" xlink:type="simple"/></inline-formula>and CH<sub>3</sub>O<sup>?</sup> contain the cluster CH<sub>3</sub>O<sup>?</sup>, considered as the core. We denote C(A) = CH<sub>3</sub>O<sup>?</sup>, C(B) = C<sub>2</sub>H<sub>5</sub>O<sup>?</sup>, C(E) = (CH<sub>3</sub>)<sub>2</sub>SO = E, C(F) = CH<sub>5</sub>CN = F. The species: H<sub>2</sub>CO<sub>3</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x22.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x23.png" xlink:type="simple"/></inline-formula> have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x24.png" xlink:type="simple"/></inline-formula> as the common core. However, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x25.png" xlink:type="simple"/></inline-formula>(anion of HClO<sub>2</sub>) and ClO<sub>2</sub> (chlorine dioxide) have different cores.</p><p>All the balances in this paper will be presented explicitly, to check the validity of the reasoning and accept it without reservations.</p></sec><sec id="s2"><title>2. Formulation of Balances</title><p>Let us consider a system obtained after addition of V mL of titrant (T) containing I<sub>2</sub> (C) + KI (C<sub>1</sub>) + CO<sub>2</sub> (C<sub>2</sub>) in A + B + E + F into V<sub>0</sub> mL of titrand (D) containing KBrO<sub>3</sub> (C<sub>0</sub>) + HCl (C<sub>01</sub>) + CO<sub>2</sub> (C<sub>02</sub>) in W + A + E; all concentrations are expressed in mol/L. The volume V<sub>0</sub> mL of D is composed of N<sub>01</sub> molecules of KBrO<sub>3</sub>, N<sub>02</sub> molecules of HCl, N<sub>03</sub> molecules of CO<sub>2</sub>, N<sub>04</sub> molecules of W, N<sub>05</sub> molecules of A, and N<sub>06</sub> molecules of E; V mL of T is composed of N<sub>07</sub> molecules of I<sub>2</sub>, N<sub>08</sub> molecules of KI, N<sub>09</sub> molecules of CO<sub>2</sub> and N<sub>011</sub> molecules of A, N<sub>012</sub> molecules of B, N<sub>013</sub> molecules of E, and N<sub>014</sub> molecules of F.</p><p>We assume that the solutes composing D and T were introduced in single solvents or mixtures of solvents. In ca. V<sub>0</sub> + V mL of a D + T mixture thus obtained, we have the following species (all changes in oxidation degrees are admitted).</p><disp-formula id="scirp.52018-formula404"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x26.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula405"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x27.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula406"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x28.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula407"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x29.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula408"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x30.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula409"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x31.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula410"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x32.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula411"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x33.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula412"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x34.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula413"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x35.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula414"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x36.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula415"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x37.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula416"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x38.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula417"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x39.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula418"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x40.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula419"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula420"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x42.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula421"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x43.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula422"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x44.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.52018-formula423"><graphic  xlink:href="http://html.scirp.org/file/2-1000157x47.png"  xlink:type="simple"/></disp-formula><p>where I<sub>2(s)</sub>―solid iodine, I<sub>2</sub>―soluble iodine. In the above list of species, H<sub>2</sub>O (N<sub>1</sub>), CH<sub>3</sub>OH (N<sub>44</sub>), C<sub>2</sub>H<sub>5</sub>OH (N<sub>47</sub>), (CH<sub>3</sub>)<sub>2</sub>SO (N<sub>51</sub>) and CH<sub>3</sub>CN (N<sub>52</sub>) are free molecules of the corresponding solvents, i.e., not involved in the solvates. We prove that the numbers: N<sub>1</sub>, N<sub>44</sub>, N<sub>47</sub>, N<sub>51</sub> and N<sub>52</sub> of the free molecules and the numbers: n<sub>iW</sub>, n<sub>iA</sub>, n<sub>iB</sub>, n<sub>iE</sub>, n<sub>iF</sub> of these molecules in the solvates do not enter the simplest form of the resulting GEB.</p><p>The elemental balances: f(H) for H, and f(O) for O are as follows:</p><p>・ f(H)</p><disp-formula id="scirp.52018-formula424"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x48.png"  xlink:type="simple"/></disp-formula><p>・ f(O)</p><disp-formula id="scirp.52018-formula425"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x49.png"  xlink:type="simple"/></disp-formula><p>From (1) and (2) we obtain</p><p>・ 2・f(O) ? f(H)</p><disp-formula id="scirp.52018-formula426"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x50.png"  xlink:type="simple"/></disp-formula><p>As we see, Equation (3) does not involve the terms N<sub>1</sub>, N<sub>04</sub>, and {n<sub>iW</sub>} related to water. To cancel the terms involved with A, B, E and F, we add Equation (3) to the core balances (4) - (7): 2・f(CH<sub>3</sub>O) (4), 4・f(C<sub>2</sub>H<sub>5</sub>O) (5), 4・f((CH<sub>3</sub>)<sub>2</sub>SO) (6), 3・f(CH<sub>3</sub>CN) (7) and charge balance (8). Further simplification gives addition of the balance for K (9), and of the core balance 4・f(CO<sub>3</sub>) (10):</p><p>・ 2・f(CH<sub>3</sub>O)</p><disp-formula id="scirp.52018-formula427"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x51.png"  xlink:type="simple"/></disp-formula><p>・ 4・f(C<sub>2</sub>H<sub>5</sub>O)</p><disp-formula id="scirp.52018-formula428"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x52.png"  xlink:type="simple"/></disp-formula><p>・ 4・f((CH<sub>3</sub>)<sub>2</sub>SO)</p><disp-formula id="scirp.52018-formula429"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x53.png"  xlink:type="simple"/></disp-formula><p>・ 3・f(CH<sub>3</sub>CN)</p><disp-formula id="scirp.52018-formula430"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x54.png"  xlink:type="simple"/></disp-formula><p>・ Charge balance</p><disp-formula id="scirp.52018-formula431"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x55.png"  xlink:type="simple"/></disp-formula><p>・ f(K)</p><disp-formula id="scirp.52018-formula432"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x56.png"  xlink:type="simple"/></disp-formula><p>・ 4・f(CO<sub>3</sub>)</p><disp-formula id="scirp.52018-formula433"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x57.png"  xlink:type="simple"/></disp-formula><p>As the result of this addition, considered as a kind of linear combination [<xref ref-type="bibr" rid="scirp.52018-ref4">4</xref>] , we obtain the simplest form of GEB, expressed in terms of numbers of entities:</p><disp-formula id="scirp.52018-formula434"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x58.png"  xlink:type="simple"/></disp-formula><p>Applying the relations:</p><disp-formula id="scirp.52018-formula435"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x59.png"  xlink:type="simple"/></disp-formula><p>(where N<sub>A</sub>―Avogadro’s constant), from Equations (11), (12) we have</p><disp-formula id="scirp.52018-formula436"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x60.png"  xlink:type="simple"/></disp-formula><p>Elemental balances for electro-active elements (“players”) are as follows:</p><p>f(Br)</p><disp-formula id="scirp.52018-formula437"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x61.png"  xlink:type="simple"/></disp-formula><p>f(Cl)</p><disp-formula id="scirp.52018-formula438"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x62.png"  xlink:type="simple"/></disp-formula><p>f(I)</p><disp-formula id="scirp.52018-formula439"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x63.png"  xlink:type="simple"/></disp-formula><p>Multiplying (14) - (16) by atomic numbers: Z<sub>Br</sub> = 35, Z<sub>Cl</sub> = 17, Z<sub>I</sub> = 53, for Br, Cl and I, respectively, adding them and applying Equation (12), we have:</p><disp-formula id="scirp.52018-formula440"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x64.png"  xlink:type="simple"/></disp-formula><p>After subtracting (13) from (17), we get the equation for GEB, identical with one obtained according to Approach I to GEB</p><disp-formula id="scirp.52018-formula441"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x65.png"  xlink:type="simple"/></disp-formula><p>The balance (18) is equivalent to the balance (13).</p><p>A remark is needed in relation to the charge balance. Rewriting Equation (8) in terms of concentrations (see Equation (12)), we have</p><disp-formula id="scirp.52018-formula442"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1000157x66.png"  xlink:type="simple"/></disp-formula><p>As we see, Equation (19) involves the ionic species related to amphiprotic co-solvents. However, in accordance with the remarks presented in [<xref ref-type="bibr" rid="scirp.52018-ref5">5</xref>] , the solvates of pairs of ions: (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x67.png" xlink:type="simple"/></inline-formula>, CH<sub>3</sub>O<sup>?</sup>) and (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x68.png" xlink:type="simple"/></inline-formula>, C<sub>2</sub>H<sub>5</sub>O<sup>?</sup>) can be perceived as pairs of solvates of H<sup>+</sup> and OH<sup>−</sup> ions.</p></sec><sec id="s3"><title>3. Final Comments</title><p>The complex redox system in a mixture with five solvents is considered. The discussion can be extended on mixtures with S solvents, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x69.png" xlink:type="simple"/></inline-formula>, where at least one of the co-solvents has amphiprotic properties. In such</p><p>systems, the solvates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x70.png" xlink:type="simple"/></inline-formula> are considered/admitted, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x71.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x72.png" xlink:type="simple"/></inline-formula>; Equation (13) is the simplest/shortest form of GEB obtained for the redox system considered according to Approach II to GEB.</p><p>Equation (13) was obtained from linear combination of the related balance 2・f(O) ? f(H) (Equation (3)) with: charge balance (Equation (8)), elemental balances for other “fans” (C, K) (Equations (9), (10)), and core balances (Equations (4) - (7)) related to organic solvents in this system. This GEB does not involve the species composed only of “fans”: H, O, C, K. In particular, it does not contain the components explicitly related to the solvent species. The paper is an illustration of the compact formulation of redox systems according to GATES/ GEB Principles, presented in Ref. [<xref ref-type="bibr" rid="scirp.52018-ref5">5</xref>] .</p><p>One can notice that uncharged (neutral) species: I<sub>2</sub>, I<sub>2</sub><sub>(s</sub><sub>)</sub>, Cl<sub>2</sub>, Br<sub>2</sub>, ICl, IBr are not present in Equation (13). Note also that Cl<sup>−</sup>, Br<sup>−</sup>, I<sup>−</sup>, Cl<sub>2</sub>, Br<sub>2</sub>, I<sub>2</sub>, I<sub>2(s)</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x73.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x74.png" xlink:type="simple"/></inline-formula>, I<sub>2</sub>Cl<sup>−</sup>, ICl, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x75.png" xlink:type="simple"/></inline-formula>, IBr, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1000157x76.png" xlink:type="simple"/></inline-formula> are the species composed only of “players”. In other species, “players” are associated with “fans”, e.g. in HIO<sub>3</sub> (I―“player”; H, O― “fans”).</p><p>Note that―at the start―the Approach II does not distinguish between “fans” and “players”; the terms “fans” and “players” are used here only for the needs of the Approach I to GEB. In further parts of this text, the “players” (the electro-active elements) are distinguished later only to indicate the equivalency of the Approaches I and II.</p></sec><sec id="s4"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.52018-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">http://quoteinvestigator.com/2011/05/13/einstein-simple/</mixed-citation></ref><ref id="scirp.52018-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Michalowski, T., Toporek, M., Michalowska-Kaczmarczyk, A.M. and Asuero, A.G. (2013) New Trends in Studies on Electrolytic Redox Systems. 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