<?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">JBPC</journal-id><journal-title-group><journal-title>Journal of Biophysical Chemistry</journal-title></journal-title-group><issn pub-type="epub">2153-036X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jbpc.2014.54016</article-id><article-id pub-id-type="publisher-id">JBPC-51670</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>
 
 
  Thermodynamics of the Second Dissociation Constants (pK&lt;sub&gt;2&lt;/sub&gt;) of Piperazine-N,N′-bis-2-hydroxypropanesulfonic Acid (POPSO Sesquisodium Salt) and Associated Thermodynamic Functions from (278.15 to 328.15) K
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>abindra</surname><given-names>N. Roy</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>Lakshmi</surname><given-names>N. Roy</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>Katherine</surname><given-names>E. Hundley</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>Taylor</surname><given-names>R. Wehmeyer</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>Lucas</surname><given-names>S. Tebbe</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Hoffman Department of Chemistry, Drury University, Springfield, MO, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>rroy@drury.edu(ANR)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>14</day><month>11</month><year>2014</year></pub-date><volume>05</volume><issue>04</issue><fpage>143</fpage><lpage>151</lpage><history><date date-type="received"><day>17</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>16</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>17</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><html>
 <head></head>
 
  The second acidic dissociation constants of protonated piperazine-N,N′-bis-2-hydroxypropane-sulfonic acid (POPSO sesquisodium salt) have been determined at 12 different temperatures from (278.15 to 328.15) K including 310.15 K. Electromotive-force measurement technique was used employing hydrogen-silver chloride cells without liquid junction. The results of pK
  <sub>2</sub> are given by the equation: pK
  <sub>2</sub> = -1041.77/T + 51.0459 - 6.97646lnT. The uncertainty of the fit is &#177;0.0008. At 289.15 K, pK
  <sub>2</sub> = 7.8029; whereas, at 310.15 K (body temperature), pK
  <sub>2</sub> = 7.6862. Thus, the buffer solutions of POPSO and its sodium salt are useful for pH control in the physiological pH region of (7.0 to 8.5). The changes of Gibbs free energy (
  <img src="Edit_a5edfd53-4f92-426c-9ecf-507d5045dc76.bmp" alt="" height="12" width="11" />G&#176;), enthalpy (
  <img src="Edit_e26296bf-9632-4afd-8f66-da1a57badfae.bmp" alt="" height="11" width="11" />H&#176;), entropy (
  <img src="Edit_8cefb2d7-15d9-42ac-a0b1-de6ce5e04451.bmp" alt="" height="11" width="11" />S&#176;) and heat capacity 
  <img src="Edit_0078f002-3a7b-4c51-9836-eda1fc8c57ca.bmp" alt="" height="11" width="11" />Cp&#176; were computed from the temperature derivative of the pK
  <sub>2</sub> for the dissociation of the zwitterionic acid POPSO
  <sup>&#177;-3</sup> = POPSO
  <sup>-4</sup> + H
  <sup>+</sup> in the standard state. At 298.15 K, these results are compared with those of similar components, which are the derivatives of the parent compounds TAURINE, PIPERAZINE and MORPHOLINE.
 
</html></p></abstract><kwd-group><kwd>pH</kwd><kwd> Buffer Compound</kwd><kwd> Liquid Junction</kwd><kwd> Thermodynamic Functions</kwd><kwd> Activity Coefficients</kwd><kwd> Electromotive-Force</kwd><kwd> pK&lt;sub&gt;2&lt;/sub&gt;</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Piperazine-N,N′-bis-2-hydroxypropanesulfonic acid (POPSO sesquisodium salt) is a water soluble solid of considerable interest as a physiological buffer [<xref ref-type="bibr" rid="scirp.51670-ref1">1</xref>] for the control of pH between (7.0 and 8.5). Very recently, we have reported the values of the second dissociation constant (pK<sub>2</sub>) of 2,2-bis(hydroxymethyl)-2,2′,2″-nitrilotri- ethanol (BIS-TRIS) [<xref ref-type="bibr" rid="scirp.51670-ref2">2</xref>] , N-(2-acetamino)-iminodiacetic acid monosodium (ADA) [<xref ref-type="bibr" rid="scirp.51670-ref3">3</xref>] and monosodium 1,4-pi- perazinediethanesulfonate [<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>] from (278.15 to 328.15) K. Hetzer et al. [<xref ref-type="bibr" rid="scirp.51670-ref5">5</xref>] have determined pK<sub>2</sub> values of PIPERAZINE, the parent compound of (POPSO), from (273.15 to 323.15) K. Thiel et al. [<xref ref-type="bibr" rid="scirp.51670-ref6">6</xref>] did not provide any pK<sub>2</sub> value for (POPSO) but they did study the effect of pH on the variation of enzyme activity and growth of bacterial strain with some zwitterionic buffers including Good Buffer (POPSO) [<xref ref-type="bibr" rid="scirp.51670-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.51670-ref7">7</xref>] . Goldberg et al. [<xref ref-type="bibr" rid="scirp.51670-ref8">8</xref>] , in their comprehensive review article, reported that no accurate thermodynamic data of pK<sub>2</sub> and related thermodynamic quantities for POPSO sesquisodium salt are available in literature. They also recommended (POPSO) buffer for use in the physiological pH range of 7.0 - 8.5.</p><p>We have now studied to report the values of the second thermodynamic dissociation constants of (POPSO) and the associated thermodynamic functions from (278.15 to 328.15) K. The dissociation process of POPSO sesquisodium salt is represented by</p><disp-formula id="scirp.51670-formula104"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7100223x6.png"  xlink:type="simple"/></disp-formula><p>where K<sub>2</sub> is the thermodynamic equilibrium constant. The structure of POPSO sesquisodium salt is given below:</p><disp-formula id="scirp.51670-formula105"><graphic  xlink:href="http://html.scirp.org/file/3-7100223x7.png"  xlink:type="simple"/></disp-formula><p>The pK<sub>2 </sub>value of (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.51670-ref5">5</xref>] is 9.731 and for (PIPES) it is 7.140 [<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>] . From the preliminary titration of POPSO sesquisodium salt with NaOH [<xref ref-type="bibr" rid="scirp.51670-ref1">1</xref>] , the approximate pK<sub>2</sub> value of (POPSO) at 298.15 K is 7.785; whereas, our value from a comprehensive study is 7.803.</p><p>In order to get very accurate and reproducible pH values required for biomedical research and the calibration of the pH meter assembly with glass electrode, highly reliable pK<sub>2 </sub>values are prerequisites. The main purpose of this paper is to establish (POPSO) as a pH buffer standard for physiological use. We have undertaken to determine the pK<sub>2</sub> values of (POPSO) at 12 different temperatures in the range (278.15 to 328.15) K employing the following galvanic cell for the electromotive-force measurements (e.m.f):</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x8.png" xlink:type="simple"/></inline-formula>[A]</p><p>where, for the cell A, there is no liquid junction; m<sub>1</sub>, m<sub>2</sub>, m<sub>3</sub> indicate the molalities of the respective species; and two electrodes (hydrogen gas electrode and the silver-silver chloride) are used.</p></sec><sec id="s2"><title>2. Experimental</title><p>Materials―POPSO sesquisodium salt was obtained from Sigma-Aldrich (St. Louis, Missouri) and was used as received. Its assay was ≥98%. The molecular formula is C<sub>20</sub>H<sub>41</sub>N<sub>4</sub>Na<sub>3</sub>O<sub>16</sub>S<sub>4</sub> and the molecular mass is 790.79 g/mol. It is highly soluble in water. The buffer solutions were prepared from weighted amounts of CO<sub>2</sub>-free redistilled water, dried samples of NaCl, POPSO sesquisodium salt, and CO<sub>2</sub>-free standard solution of NaOH. Usually, all buffer solutions were prepared a day before the e.m.f measurements were made. Vacuum corrections were made to all masses. The ionic strength (I) range for all experimental buffer solutions was from I = 0.0354 to 0.101 mol・kg<sup>−1</sup>. The uncertainty in the concentration (molality) is estimated to be within &#177;0.03%.</p></sec><sec id="s3"><title>3. Methods and Results</title><p>The method of making e.m.f measurements over the temperature range was essentially the same as that used in the study of (PIPES) [<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>] . At 298.15 K, the standard deviation between the initial and the middle e.m.f reading was &#177;0.04 mV. The preparation of the thermal electrolytic type Ag-AgCl electrode, the hydrogen electrode, the design of cells [<xref ref-type="bibr" rid="scirp.51670-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>] , and other experimental details have been described in previous publications [<xref ref-type="bibr" rid="scirp.51670-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.51670-ref11">11</xref>] . The e.m.f values have been corrected, as usual, to the partial pressure of one atmosphere of dry hydrogen. These cell voltage values are listed in <xref ref-type="table" rid="table1">Table 1</xref>.</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Electromotive-force (e.m.f) of cell A (in volts): Pt(s); H<sub>2</sub>(g), 1 atm|Na<sub>3</sub>POPSO (m<sub>1</sub>) + Na<sub>4</sub>POPSOate (m<sub>2</sub>) + NaCl (m<sub>3</sub>)|AgCl(s), Ag(s)</title></caption><table-wrap id="1_1"><table><tbody><thead><tr><th align="center" valign="middle" ><sup>a</sup>m<sub>1</sub></th><th align="center" valign="middle" ><sup>a</sup>m<sub>2</sub></th><th align="center" valign="middle" ><sup>a</sup>m<sub>3</sub></th><th align="center" valign="middle" >278.15 K</th><th align="center" valign="middle" >283.15 K</th><th align="center" valign="middle" >288.15 K</th><th align="center" valign="middle" >293.15 K</th><th align="center" valign="middle" >298.15 K</th><th align="center" valign="middle" >303.15 K</th></tr></thead><tr><td align="center" valign="middle" >0.001400</td><td align="center" valign="middle" >0.002500</td><td align="center" valign="middle" >0.002000</td><td align="center" valign="middle" >0.85947</td><td align="center" valign="middle" >0.86490</td><td align="center" valign="middle" >0.87023</td><td align="center" valign="middle" >0.87519</td><td align="center" valign="middle" >0.88000</td><td align="center" valign="middle" >0.88400</td></tr><tr><td align="center" valign="middle" >0.001667</td><td align="center" valign="middle" >0.003006</td><td align="center" valign="middle" >0.002500</td><td align="center" valign="middle" >0.85502</td><td align="center" valign="middle" >0.86048</td><td align="center" valign="middle" >0.86581</td><td align="center" valign="middle" >0.87070</td><td align="center" valign="middle" >0.87549</td><td align="center" valign="middle" >0.87921</td></tr><tr><td align="center" valign="middle" >0.001730</td><td align="center" valign="middle" >0.004000</td><td align="center" valign="middle" >0.003904</td><td align="center" valign="middle" >0.85097</td><td align="center" valign="middle" >0.85636</td><td align="center" valign="middle" >0.86167</td><td align="center" valign="middle" >0.86655</td><td align="center" valign="middle" >0.87135</td><td align="center" valign="middle" >0.87492</td></tr><tr><td align="center" valign="middle" >0.001833</td><td align="center" valign="middle" >0.004900</td><td align="center" valign="middle" >0.004901</td><td align="center" valign="middle" >0.84931</td><td align="center" valign="middle" >0.85470</td><td align="center" valign="middle" >0.86004</td><td align="center" valign="middle" >0.86495</td><td align="center" valign="middle" >0.86977</td><td align="center" valign="middle" >0.87316</td></tr><tr><td align="center" valign="middle" >0.002017</td><td align="center" valign="middle" >0.005500</td><td align="center" valign="middle" >0.006002</td><td align="center" valign="middle" >0.84510</td><td align="center" valign="middle" >0.85043</td><td align="center" valign="middle" >0.85574</td><td align="center" valign="middle" >0.86061</td><td align="center" valign="middle" >0.86537</td><td align="center" valign="middle" >0.86859</td></tr><tr><td align="center" valign="middle" >0.002167</td><td align="center" valign="middle" >0.005500</td><td align="center" valign="middle" >0.005996</td><td align="center" valign="middle" >0.84341</td><td align="center" valign="middle" >0.84871</td><td align="center" valign="middle" >0.85398</td><td align="center" valign="middle" >0.85884</td><td align="center" valign="middle" >0.86357</td><td align="center" valign="middle" >0.86675</td></tr><tr><td align="center" valign="middle" >0.002333</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.84359</td><td align="center" valign="middle" >0.84891</td><td align="center" valign="middle" >0.85423</td><td align="center" valign="middle" >0.85912</td><td align="center" valign="middle" >0.86386</td><td align="center" valign="middle" >0.86698</td></tr><tr><td align="center" valign="middle" >0.002667</td><td align="center" valign="middle" >0.006900</td><td align="center" valign="middle" >0.005803</td><td align="center" valign="middle" >0.84437</td><td align="center" valign="middle" >0.84973</td><td align="center" valign="middle" >0.85512</td><td align="center" valign="middle" >0.86009</td><td align="center" valign="middle" >0.86485</td><td align="center" valign="middle" >0.86786</td></tr><tr><td align="center" valign="middle" >0.003017</td><td align="center" valign="middle" >0.007500</td><td align="center" valign="middle" >0.005998</td><td align="center" valign="middle" >0.84247</td><td align="center" valign="middle" >0.84781</td><td align="center" valign="middle" >0.85320</td><td align="center" valign="middle" >0.85819</td><td align="center" valign="middle" >0.86292</td><td align="center" valign="middle" >0.86580</td></tr><tr><td align="center" valign="middle" >0.003333</td><td align="center" valign="middle" >0.006500</td><td align="center" valign="middle" >0.006498</td><td align="center" valign="middle" >0.83486</td><td align="center" valign="middle" >0.84005</td><td align="center" valign="middle" >0.84527</td><td align="center" valign="middle" >0.85007</td><td align="center" valign="middle" >0.85467</td><td align="center" valign="middle" >0.85750</td></tr><tr><td align="center" valign="middle" >0.005000</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.006996</td><td align="center" valign="middle" >0.82139</td><td align="center" valign="middle" >0.82634</td><td align="center" valign="middle" >0.83135</td><td align="center" valign="middle" >0.83594</td><td align="center" valign="middle" >0.84029</td><td align="center" valign="middle" >0.84282</td></tr><tr><td align="center" valign="middle" >0.001667</td><td align="center" valign="middle" >0.005000</td><td align="center" valign="middle" >0.005002</td><td align="center" valign="middle" >0.85159</td><td align="center" valign="middle" >0.85702</td><td align="center" valign="middle" >0.86240</td><td align="center" valign="middle" >0.86735</td><td align="center" valign="middle" >0.87221</td><td align="center" valign="middle" >0.87570</td></tr><tr><td align="center" valign="middle" >0.002020</td><td align="center" valign="middle" >0.005556</td><td align="center" valign="middle" >0.006057</td><td align="center" valign="middle" >0.84500</td><td align="center" valign="middle" >0.85033</td><td align="center" valign="middle" >0.85564</td><td align="center" valign="middle" >0.86052</td><td align="center" valign="middle" >0.86528</td><td align="center" valign="middle" >0.86850</td></tr><tr><td align="center" valign="middle" >0.002333</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.006503</td><td align="center" valign="middle" >0.84174</td><td align="center" valign="middle" >0.84702</td><td align="center" valign="middle" >0.85231</td><td align="center" valign="middle" >0.85717</td><td align="center" valign="middle" >0.86187</td><td align="center" valign="middle" >0.86496</td></tr><tr><td align="center" valign="middle" >0.002500</td><td align="center" valign="middle" >0.006500</td><td align="center" valign="middle" >0.006895</td><td align="center" valign="middle" >0.84043</td><td align="center" valign="middle" >0.84571</td><td align="center" valign="middle" >0.85100</td><td align="center" valign="middle" >0.85588</td><td align="center" valign="middle" >0.86057</td><td align="center" valign="middle" >0.86355</td></tr><tr><td align="center" valign="middle" >0.002750</td><td align="center" valign="middle" >0.006800</td><td align="center" valign="middle" >0.006999</td><td align="center" valign="middle" >0.83885</td><td align="center" valign="middle" >0.84411</td><td align="center" valign="middle" >0.84940</td><td align="center" valign="middle" >0.85427</td><td align="center" valign="middle" >0.85894</td><td align="center" valign="middle" >0.86184</td></tr><tr><td align="center" valign="middle" >0.002834</td><td align="center" valign="middle" >0.006999</td><td align="center" valign="middle" >0.007498</td><td align="center" valign="middle" >0.83710</td><td align="center" valign="middle" >0.84233</td><td align="center" valign="middle" >0.84761</td><td align="center" valign="middle" >0.85247</td><td align="center" valign="middle" >0.85711</td><td align="center" valign="middle" >0.85994</td></tr><tr><td align="center" valign="middle" >0.002884</td><td align="center" valign="middle" >0.007199</td><td align="center" valign="middle" >0.007705</td><td align="center" valign="middle" >0.83654</td><td align="center" valign="middle" >0.84178</td><td align="center" valign="middle" >0.84706</td><td align="center" valign="middle" >0.85192</td><td align="center" valign="middle" >0.85655</td><td align="center" valign="middle" >0.85935</td></tr><tr><td align="center" valign="middle" >0.003000</td><td align="center" valign="middle" >0.007500</td><td align="center" valign="middle" >0.008003</td><td align="center" valign="middle" >0.83555</td><td align="center" valign="middle" >0.84077</td><td align="center" valign="middle" >0.84605</td><td align="center" valign="middle" >0.85092</td><td align="center" valign="middle" >0.85554</td><td align="center" valign="middle" >0.85827</td></tr><tr><td align="center" valign="middle" >m<sub>1</sub></td><td align="center" valign="middle" >m<sub>2</sub></td><td align="center" valign="middle" >m<sub>3</sub></td><td align="center" valign="middle" >308.15 K</td><td align="center" valign="middle" >310.15 K</td><td align="center" valign="middle" >313.15 K</td><td align="center" valign="middle" >318.15 K</td><td align="center" valign="middle" >323.15 K</td><td align="center" valign="middle" >328.15 K</td></tr><tr><td align="center" valign="middle" >0.001400</td><td align="center" valign="middle" >0.002500</td><td align="center" valign="middle" >0.002000</td><td align="center" valign="middle" >0.88829</td><td align="center" valign="middle" >0.88983</td><td align="center" valign="middle" >0.89217</td><td align="center" valign="middle" >0.89582</td><td align="center" valign="middle" >0.89938</td><td align="center" valign="middle" >0.90257</td></tr><tr><td align="center" valign="middle" >0.001667</td><td align="center" valign="middle" >0.003006</td><td align="center" valign="middle" >0.002500</td><td align="center" valign="middle" >0.88356</td><td align="center" valign="middle" >0.88508</td><td align="center" valign="middle" >0.88739</td><td align="center" valign="middle" >0.89100</td><td align="center" valign="middle" >0.89448</td><td align="center" valign="middle" >0.89754</td></tr><tr><td align="center" valign="middle" >0.001730</td><td align="center" valign="middle" >0.004000</td><td align="center" valign="middle" >0.003904</td><td align="center" valign="middle" >0.87916</td><td align="center" valign="middle" >0.88066</td><td align="center" valign="middle" >0.88294</td><td align="center" valign="middle" >0.88648</td><td align="center" valign="middle" >0.89000</td><td align="center" valign="middle" >0.89287</td></tr><tr><td align="center" valign="middle" >0.001833</td><td align="center" valign="middle" >0.004900</td><td align="center" valign="middle" >0.004901</td><td align="center" valign="middle" >0.87742</td><td align="center" valign="middle" >0.87890</td><td align="center" valign="middle" >0.88117</td><td align="center" valign="middle" >0.88469</td><td align="center" valign="middle" >0.88817</td><td align="center" valign="middle" >0.89103</td></tr><tr><td align="center" valign="middle" >0.002017</td><td align="center" valign="middle" >0.005500</td><td align="center" valign="middle" >0.006002</td><td align="center" valign="middle" >0.87281</td><td align="center" valign="middle" >0.87426</td><td align="center" valign="middle" >0.87649</td><td align="center" valign="middle" >0.87994</td><td align="center" valign="middle" >0.88337</td><td align="center" valign="middle" >0.88612</td></tr></tbody></table></table-wrap><table-wrap id="1_2"><table><tbody><thead><tr><th align="center" valign="middle" >0.002167</th><th align="center" valign="middle" >0.005500</th><th align="center" valign="middle" >0.005996</th><th align="center" valign="middle" >0.87094</th><th align="center" valign="middle" >0.87238</th><th align="center" valign="middle" >0.87459</th><th align="center" valign="middle" >0.87801</th><th align="center" valign="middle" >0.88141</th><th align="center" valign="middle" >0.88413</th></tr></thead><tr><td align="center" valign="middle" >0.002333</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.87120</td><td align="center" valign="middle" >0.87264</td><td align="center" valign="middle" >0.87485</td><td align="center" valign="middle" >0.87828</td><td align="center" valign="middle" >0.88171</td><td align="center" valign="middle" >0.88441</td></tr><tr><td align="center" valign="middle" >0.002667</td><td align="center" valign="middle" >0.006900</td><td align="center" valign="middle" >0.005803</td><td align="center" valign="middle" >0.87214</td><td align="center" valign="middle" >0.87358</td><td align="center" valign="middle" >0.87581</td><td align="center" valign="middle" >0.87926</td><td align="center" valign="middle" >0.88273</td><td align="center" valign="middle" >0.88540</td></tr><tr><td align="center" valign="middle" >0.003017</td><td align="center" valign="middle" >0.007500</td><td align="center" valign="middle" >0.005998</td><td align="center" valign="middle" >0.87008</td><td align="center" valign="middle" >0.87149</td><td align="center" valign="middle" >0.87371</td><td align="center" valign="middle" >0.87712</td><td align="center" valign="middle" >0.88059</td><td align="center" valign="middle" >0.88319</td></tr><tr><td align="center" valign="middle" >0.003333</td><td align="center" valign="middle" >0.006500</td><td align="center" valign="middle" >0.006498</td><td align="center" valign="middle" >0.86161</td><td align="center" valign="middle" >0.86298</td><td align="center" valign="middle" >0.86510</td><td align="center" valign="middle" >0.86838</td><td align="center" valign="middle" >0.87169</td><td align="center" valign="middle" >0.87419</td></tr><tr><td align="center" valign="middle" >0.005000</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.006996</td><td align="center" valign="middle" >0.84671</td><td align="center" valign="middle" >0.84797</td><td align="center" valign="middle" >0.84996</td><td align="center" valign="middle" >0.85299</td><td align="center" valign="middle" >0.85607</td><td align="center" valign="middle" >0.85831</td></tr><tr><td align="center" valign="middle" >0.001667</td><td align="center" valign="middle" >0.005000</td><td align="center" valign="middle" >0.005002</td><td align="center" valign="middle" >0.87995</td><td align="center" valign="middle" >0.88145</td><td align="center" valign="middle" >0.88374</td><td align="center" valign="middle" >0.88730</td><td align="center" valign="middle" >0.89082</td><td align="center" valign="middle" >0.89372</td></tr><tr><td align="center" valign="middle" >0.002020</td><td align="center" valign="middle" >0.005556</td><td align="center" valign="middle" >0.006057</td><td align="center" valign="middle" >0.87272</td><td align="center" valign="middle" >0.87417</td><td align="center" valign="middle" >0.87639</td><td align="center" valign="middle" >0.87984</td><td align="center" valign="middle" >0.88327</td><td align="center" valign="middle" >0.88603</td></tr><tr><td align="center" valign="middle" >0.002333</td><td align="center" valign="middle" >0.006000</td><td align="center" valign="middle" >0.006503</td><td align="center" valign="middle" >0.86914</td><td align="center" valign="middle" >0.87056</td><td align="center" valign="middle" >0.87276</td><td align="center" valign="middle" >0.87615</td><td align="center" valign="middle" >0.87955</td><td align="center" valign="middle" >0.88221</td></tr><tr><td align="center" valign="middle" >0.002500</td><td align="center" valign="middle" >0.006500</td><td align="center" valign="middle" >0.006895</td><td align="center" valign="middle" >0.86775</td><td align="center" valign="middle" >0.86916</td><td align="center" valign="middle" >0.87134</td><td align="center" valign="middle" >0.87472</td><td align="center" valign="middle" >0.87811</td><td align="center" valign="middle" >0.88073</td></tr><tr><td align="center" valign="middle" >0.002750</td><td align="center" valign="middle" >0.006800</td><td align="center" valign="middle" >0.006999</td><td align="center" valign="middle" >0.86602</td><td align="center" valign="middle" >0.86742</td><td align="center" valign="middle" >0.86959</td><td align="center" valign="middle" >0.87293</td><td align="center" valign="middle" >0.87631</td><td align="center" valign="middle" >0.87888</td></tr><tr><td align="center" valign="middle" >0.002834</td><td align="center" valign="middle" >0.006999</td><td align="center" valign="middle" >0.007498</td><td align="center" valign="middle" >0.86410</td><td align="center" valign="middle" >0.86548</td><td align="center" valign="middle" >0.86763</td><td align="center" valign="middle" >0.87095</td><td align="center" valign="middle" >0.87430</td><td align="center" valign="middle" >0.87683</td></tr><tr><td align="center" valign="middle" >0.002884</td><td align="center" valign="middle" >0.007199</td><td align="center" valign="middle" >0.007705</td><td align="center" valign="middle" >0.86351</td><td align="center" valign="middle" >0.86487</td><td align="center" valign="middle" >0.86700</td><td align="center" valign="middle" >0.87033</td><td align="center" valign="middle" >0.87368</td><td align="center" valign="middle" >0.87617</td></tr><tr><td align="center" valign="middle" >0.003000</td><td align="center" valign="middle" >0.007500</td><td align="center" valign="middle" >0.008003</td><td align="center" valign="middle" >0.86243</td><td align="center" valign="middle" >0.86380</td><td align="center" valign="middle" >0.86594</td><td align="center" valign="middle" >0.86923</td><td align="center" valign="middle" >0.87258</td><td align="center" valign="middle" >0.87505</td></tr></tbody></table></table-wrap></table-wrap-group><p>The general equation for calculating the thermodynamic acidic dissociation constant, pK<sub>2</sub>, is obtained by combining the e.m.f equations (the Nernst equation for the cell) with the dissociation step (mass-law expression) of Equation (1) and with the extended form of the Debye-H&#252;ckel equation for the molal activity coefficients (γ) of all ions present in the buffer solution. The resulting equation is given below:</p><disp-formula id="scirp.51670-formula106"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7100223x9.png"  xlink:type="simple"/></disp-formula><p>whereas the last term of Equation (2) is equal to</p><disp-formula id="scirp.51670-formula107"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7100223x10.png"  xlink:type="simple"/></disp-formula><p>In this equation, E is the corrected e.m.f from <xref ref-type="table" rid="table1">Table 1</xref>, E&#176; is the standard electrode potential of the cell, I is the ionic strength of the buffer solution, A and B are the Debye-H&#252;ckel constants [<xref ref-type="bibr" rid="scirp.51670-ref12">12</xref>] and Ba<sup>&#176;</sup> is 1.38 kg<sup>1/2</sup>&#215;mol<sup>−1/2</sup> [<xref ref-type="bibr" rid="scirp.51670-ref12">12</xref>] for all experimental temperatures corresponding to an “ion-size parameter” a<sup>&#176;</sup> of 4.2 A<sup>&#176;</sup>.</p><p>In Equation (2), the “apparent” thermodynamic dissociation constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x11.png" xlink:type="simple"/></inline-formula>, becomes equal to the true pK<sub>2</sub> (intercept) at an ionic strength (I) of zero from the linear plot of the following equation:</p><disp-formula id="scirp.51670-formula108"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7100223x12.png"  xlink:type="simple"/></disp-formula><p>in which:</p><disp-formula id="scirp.51670-formula109"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7100223x13.png"  xlink:type="simple"/></disp-formula><p>and &#223; is the slope parameter. The terms m<sub>1</sub>, m<sub>2</sub>, m<sub>3</sub> correspond to the molalities of species indicated in cell A and Equation (2). The values of pK<sub>2</sub>, together with standard deviation of the intercept and also the values &#223; with the standard deviation of the least squares fit, are listed in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>In order to calculate the associated thermodynamic quantities for the dissociation process, the values of pK<sub>2 </sub>for 12 experimental temperatures (278.15 to 328.15) K were fitted to the following Ives-Moseley equation [<xref ref-type="bibr" rid="scirp.51670-ref13">13</xref>] :</p><disp-formula id="scirp.51670-formula110"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7100223x14.png"  xlink:type="simple"/></disp-formula><p>The resulting equation is:</p><disp-formula id="scirp.51670-formula111"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7100223x15.png"  xlink:type="simple"/></disp-formula><p>and the standard deviation of the fit is 0.0008.</p><p>By application of the customary thermodynamic relations to the constants of Equation (7), the values of the standard changes of Gibbs energy (∆G&#176;), enthalpy (∆H&#176;), entropy (∆S&#176;) and heat capacity (∆Cp&#176;) for the dissociation of one mole of POPSO<sup>&#177;−3</sup> in the standard state were derived. The uncertainties of these quantities were computed by the method of Please [<xref ref-type="bibr" rid="scirp.51670-ref14">14</xref>] . These values of the thermodynamic quantities with the standard deviations of regression are entered in <xref ref-type="table" rid="table3">Table 3</xref>. The estimated standard errors of these thermodynamic quantities are as follows: ∆G&#176;, 5 J・mol<sup>−1</sup>; ∆H&#176;, 34 J・mol<sup>−1</sup>; ∆S&#176;, 0.11 J・K<sup>−1</sup>・mol<sup>−1</sup>; and ∆Cp&#176;, 4 J・K<sup>−1</sup>・mol<sup>−1</sup>.</p></sec><sec id="s4"><title>4. Discussion</title><p>There does not appear to be any accurate thermodynamic data in the literature for the dissociation of (POPSO). Only very preliminary data from a simple titration method [<xref ref-type="bibr" rid="scirp.51670-ref1">1</xref>] is available, with no mention of the ionic strength. At 298.15 K the value was reported to be 7.785 (calculated from the temperature derivative). From the precise and rigorous experimental measurements, our values of pK<sub>2</sub> at 298.15 K from <xref ref-type="table" rid="table2">Table 2</xref> are 7.8029 &#177; 0.0008. Thus, there is a significant difference between these two measurements. Also Azab et al. [<xref ref-type="bibr" rid="scirp.51670-ref15">15</xref>] reported the pK<sub>2</sub> value of (POPSO) from the simple titration of (POPSO) buffer solution against KOH. Their value is 7.60 &#177; 0.02. This significant difference is explained. The titration method involves ion-selective electrode with a calomel reference causing a greater uncertainty in e.m.f value due to the liquid junction potential. Our method involves precise measurement using hydrogen and Ag-AgCl electrodes without liquid junction.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Second dissociation constant of Na<sub>3</sub>POPSO from (278.15 to 328.15) K</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >T/K</th><th align="center" valign="middle" >pK<sub>2</sub></th><th align="center" valign="middle" >σ (pK<sub>2</sub>)<sup>a</sup></th><th align="center" valign="middle" >&#223;</th><th align="center" valign="middle" >σ (&#223;)<sup>b</sup></th></tr></thead><tr><td align="center" valign="middle" >278.15</td><td align="center" valign="middle" >8.0363</td><td align="center" valign="middle" >0.0009</td><td align="center" valign="middle" >2.888</td><td align="center" valign="middle" >0.011</td></tr><tr><td align="center" valign="middle" >283.15</td><td align="center" valign="middle" >7.9785</td><td align="center" valign="middle" >0.0009</td><td align="center" valign="middle" >2.859</td><td align="center" valign="middle" >0.010</td></tr><tr><td align="center" valign="middle" >288.15</td><td align="center" valign="middle" >7.9192</td><td align="center" valign="middle" >0.0009</td><td align="center" valign="middle" >2.784</td><td align="center" valign="middle" >0.010</td></tr><tr><td align="center" valign="middle" >293.15</td><td align="center" valign="middle" >7.8614</td><td align="center" valign="middle" >0.0009</td><td align="center" valign="middle" >2.689</td><td align="center" valign="middle" >0.010</td></tr><tr><td align="center" valign="middle" >298.15</td><td align="center" valign="middle" >7.8029</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >2.691</td><td align="center" valign="middle" >0.010</td></tr><tr><td align="center" valign="middle" >303.15</td><td align="center" valign="middle" >7.7445</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >2.918</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >308.15</td><td align="center" valign="middle" >7.6862</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >2.878</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >310.15</td><td align="center" valign="middle" >7.6628</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >2.893</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >313.15</td><td align="center" valign="middle" >7.6277</td><td align="center" valign="middle" >0.0009</td><td align="center" valign="middle" >2.898</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >318.15</td><td align="center" valign="middle" >7.5693</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >2.913</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >323.15</td><td align="center" valign="middle" >7.5113</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >2.891</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >328.15</td><td align="center" valign="middle" >7.4535</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >2.983</td><td align="center" valign="middle" >0.009</td></tr></tbody></table></table-wrap><p><sup>a</sup>Standard deviation of pK<sub>2</sub>; <sup>b</sup>Slope parameter.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Thermodynamic quantities for the dissociation of Na<sub>3</sub>POPSO from (278.15 - 328.15) K</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >278.15 K</th><th align="center" valign="middle" >288.15 K</th><th align="center" valign="middle" >298.15 K</th><th align="center" valign="middle" >308.15 K</th><th align="center" valign="middle" >318.15 K</th><th align="center" valign="middle" >328.15 K</th></tr></thead><tr><td align="center" valign="middle" >∆G&#176;</td><td align="center" valign="middle" >42,792 &#177; 4</td><td align="center" valign="middle" >43,688 &#177; 5</td><td align="center" valign="middle" >44,538 &#177; 5</td><td align="center" valign="middle" >45,343 &#177; 5</td><td align="center" valign="middle" >46,104 &#177; 5</td><td align="center" valign="middle" >46,824 &#177; 5</td></tr><tr><td align="center" valign="middle" >∆H&#176;</td><td align="center" valign="middle" >17,206 &#177; 96</td><td align="center" valign="middle" >18,541 &#177; 62</td><td align="center" valign="middle" >19,877 &#177; 34</td><td align="center" valign="middle" >21,213 &#177; 36</td><td align="center" valign="middle" >22,548 &#177; 68</td><td align="center" valign="middle" >23,884 &#177; 107</td></tr><tr><td align="center" valign="middle" >∆S&#176;</td><td align="center" valign="middle" >−92.0 &#177; 0.3</td><td align="center" valign="middle" >−87.3 &#177; 0.2</td><td align="center" valign="middle" >−82.7 &#177; 0.1</td><td align="center" valign="middle" >−78.3 &#177; 0.1</td><td align="center" valign="middle" >−74.0 &#177; 0.2</td><td align="center" valign="middle" >−69.9 &#177; 0.3</td></tr><tr><td align="center" valign="middle" >∆Cp&#176;</td><td align="center" valign="middle" >134 &#177; 4</td><td align="center" valign="middle" >134 &#177; 4</td><td align="center" valign="middle" >134 &#177; 4</td><td align="center" valign="middle" >134 &#177; 4</td><td align="center" valign="middle" >134 &#177; 4</td><td align="center" valign="middle" >134 &#177; 4</td></tr></tbody></table></table-wrap><p>Units: ∆G&#176;, ∆H&#176;, J・mol<sup>−1</sup>; ∆S&#176;, ∆Cp&#176;, J・K<sup>−1</sup>・mol<sup>−1</sup>.</p><p>It is interesting to mention that at the human body temperature of 310.15 K, our pK<sub>2</sub> value is 7.6628. The pH of blood at this temperature is equal to 7.407. Thus, the (POPSO) buffer can be used as pH primary standard for physiological use. Moreover, the usefulness of (POPSO) and other Good Buffers [<xref ref-type="bibr" rid="scirp.51670-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.51670-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.51670-ref11">11</xref>] for pH control in the range of physiological interest, in the aggregation of peptides [<xref ref-type="bibr" rid="scirp.51670-ref16">16</xref>] and surface active behavior [<xref ref-type="bibr" rid="scirp.51670-ref17">17</xref>] , have been reported.</p><p>It is interesting to compare the values of the thermodynamic quantities of some structurally related zwitterio- nic buffer compounds with that of (POPSO). Such a comparison of the values at 298.15 K is summarized in <xref ref-type="table" rid="table4">Table 4</xref>. Examples of structurally similar compounds are; N-substituted amino sulfonic acids, (TABS) [<xref ref-type="bibr" rid="scirp.51670-ref9">9</xref>] , (MOBS)</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Comparison of the thermodynamic functions for the second acid dissociation constant of Na<sub>3</sub>POPSO with structurally related compounds in water at 298.15 K</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Structure</th><th align="center" valign="middle" >Common name</th><th align="center" valign="middle" >pK<sub>2</sub></th><th align="center" valign="middle" >∆H&#176;</th><th align="center" valign="middle" >∆S&#176;</th><th align="center" valign="middle" >∆Cp&#176;</th><th align="center" valign="middle" >Ref.</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x16.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >TAURINE</td><td align="center" valign="middle" >9.061</td><td align="center" valign="middle" >41,840</td><td align="center" valign="middle" >−33.1</td><td align="center" valign="middle" >−33</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref19">19</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x17.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >PIPERAZINE</td><td align="center" valign="middle" >9.731</td><td align="center" valign="middle" >53,390</td><td align="center" valign="middle" >−33.9</td><td align="center" valign="middle" >88</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref5">5</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x18.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >MORPHOLINE</td><td align="center" valign="middle" >8.492</td><td align="center" valign="middle" >39,030</td><td align="center" valign="middle" >−31.7</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref20">20</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x19.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >MES</td><td align="center" valign="middle" >6.270</td><td align="center" valign="middle" >14,602</td><td align="center" valign="middle" >−1.1</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref24">24</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x20.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >AMPSO</td><td align="center" valign="middle" >9.138</td><td align="center" valign="middle" >43,166</td><td align="center" valign="middle" >−31.2</td><td align="center" valign="middle" >−59</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.51670-ref18">18</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x21.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >DIPSO</td><td align="center" valign="middle" >7.576</td><td align="center" valign="middle" >30,192</td><td align="center" valign="middle" >−45.5</td><td align="center" valign="middle" >42</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref10">10</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x22.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >MOBS</td><td align="center" valign="middle" >7.702</td><td align="center" valign="middle" >24,442</td><td align="center" valign="middle" >−61.1</td><td align="center" valign="middle" >74</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref11">11</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x23.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >TABS</td><td align="center" valign="middle" >8.834</td><td align="center" valign="middle" >43,663</td><td align="center" valign="middle" >−23.6</td><td align="center" valign="middle" >39</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref9">9</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x24.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >PIPES</td><td align="center" valign="middle" >7.140</td><td align="center" valign="middle" >11,964</td><td align="center" valign="middle" >−96.5</td><td align="center" valign="middle" >124</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>]</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7100223x25.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >Na<sub>3</sub>POPSO</td><td align="center" valign="middle" >7.803</td><td align="center" valign="middle" >19,877</td><td align="center" valign="middle" >−82.7</td><td align="center" valign="middle" >134</td><td align="center" valign="middle" >This study</td></tr></tbody></table></table-wrap><p>Units: ∆H&#176;, J∙mol<sup>−1</sup>; ∆S&#176;, ∆Cp&#176;, J∙K<sup>−1</sup>∙mol<sup>−1</sup>.</p><p>[<xref ref-type="bibr" rid="scirp.51670-ref11">11</xref>] and (AMPSO) [<xref ref-type="bibr" rid="scirp.51670-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.51670-ref18">18</xref>] . These are the parent compounds (TAURINE) [<xref ref-type="bibr" rid="scirp.51670-ref19">19</xref>] , (MORPHOLINE) [<xref ref-type="bibr" rid="scirp.51670-ref20">20</xref>] , and (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.51670-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.51670-ref21">21</xref>] , respectively. The value of pK<sub>2</sub> of (PIPES) [<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>] at 298.15 K is 7.1399; whereas, that for a similar structure (POPSO) from the present study is 7.8029. It is evident that lengthening of the chain has, as expected, increased the basicity (decreased the acidity) of the NH<sup>+</sup> group from (PIPES) to (POPSO) (this study). The enthalpy of dissociation has increased from 11,965 J・mol<sup>−1</sup> to 19,877 J・mol<sup>−1</sup>. The increase in pK<sub>2</sub> is usually paralleled by the increase in ∆H&#176;. This trend is consistent with this study.</p><p>Also it indicates that there is a significant effect on the entropy of dissociation. From <xref ref-type="table" rid="table4">Table 4</xref>, the values of ∆S&#176; at 298.15 K for (PIPES) [<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>] , and (POPSO) [this investigation] are: −96.5 J・K<sup>−1</sup>・mol<sup>−1</sup> and −82.7 J・K<sup>−1</sup>・mol<sup>−1</sup> respectively. These values are generally in qualitative agreement. The slightly less negative value of (POPSO) is consistent with the explanation for the stabilization of the solvent structure (decreased order) in the proximity of the ions H<sup>+</sup>, Na<sup>+</sup>, POPSO<sup>−4</sup>. In addition, this small change (less negative) in ∆S&#176; (entropy of solvation of the NH<sup>+</sup> group) is due to the effect of the successive introduction of hydroxyl group and (MORPHOLINE) compound into the ethyl groups of monosodium POPSO.</p><p>In <xref ref-type="table" rid="table4">Table 4</xref>, the values of ∆Cp&#176; at 298.15 K for (PIPES) [<xref ref-type="bibr" rid="scirp.51670-ref4">4</xref>] and (POPSO) [this study] are 124 J・K<sup>−1</sup>・mol<sup>−1</sup> and 134 J・K<sup>−1</sup>・mol<sup>−1</sup> respectively. These results (slight increase in ∆Cp&#176; of POPSO) suggest that the substitution and the presence of an extra monosodium POPSO molecule in POPSO disodium salt apparently have two effects: 1) progressive increasing of hydrophobic characters (tending to increase ∆Cp&#176;), and 2) some changes in the solvation pattern, that is, progressively greater steric hindrance (tending to increase ∆Cp&#176; value by exclusion of solvent) [<xref ref-type="bibr" rid="scirp.51670-ref22">22</xref>] .</p><p>It is better to point out that the interactions of NaCl with N-substituted aminosulfonic acid (POPSO) [this study] and (MES) [<xref ref-type="bibr" rid="scirp.51670-ref23">23</xref>] or aminocarboxylacid (TRICINE) [<xref ref-type="bibr" rid="scirp.51670-ref24">24</xref>] , are very complex. Thus, detailed quantitative explanations for these interactions are somewhat difficult.</p></sec><sec id="s5"><title>5. Conclusion</title><p>For the 16 buffer solutions of <xref ref-type="table" rid="table1">Table 1</xref>, the largest difference between the final e.m.f reading at 298.15 K and that collected in the beginning was well within &#177;0.03 mV. The data is highly accurate and reproducible. The hydrogen and Ag-AgCl electrodes are reversible [<xref ref-type="bibr" rid="scirp.51670-ref25">25</xref>] without any complex formation with N-substituted amino acids. The results of pK<sub>2</sub> and related thermodynamic functions are very reliable. Unfortunately, no thermodynamic data of (POPSO) is available in the literature for the purpose of comparison. Since the value of pK<sub>2</sub> at 310.15 K (body temperature) of (POPSO) is 7.6628 &#177; 0.0008, the buffer solution of Na<sub>3</sub>POPSO and Na<sub>4</sub>POPSO would be a useful pH primary buffer standard for pH control in the region close to that of blood serum (pH = 7.407 at an ionic strength I = 0.16 mol・kg<sup>−1</sup>). Manuscript is under preparation, based on the new experimental data, for buffer solutions of Na<sub>3</sub>POPSO + Na<sub>4</sub>POPSO with and without the presence of NaCl in the physiological range of pH (7.0 to 8.5) at 12 different temperatures from (278.15 to 328.25) K.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors are grateful for the funding from the National Institutes of Health (NIH-AREA) under the grant 2R15GM66866-3. The content of this paper is the sole responsibility of the authors and does not necessarily represent the official views of the NIH of the National Institutes of the General Medical Science. R. N. 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