<?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.2014.53010</article-id><article-id pub-id-type="publisher-id">JBPC-46663</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 Stage Dissociation Step (pK&lt;sub&gt;2&lt;/sub&gt;) of Buffer Monosodium 1,4-Piperazinediethanesulfonate 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>John</surname><given-names>J. Dinga</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>Matthew</surname><given-names>R. Medcalf</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>Eric</surname><given-names>B. Hines</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>Ryan</surname><given-names>R. Parmar</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>Jamie</surname><given-names>A. Veliz</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>Clark</surname><given-names>B. Summers</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, 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>10</day><month>06</month><year>2014</year></pub-date><volume>05</volume><issue>03</issue><fpage>91</fpage><lpage>98</lpage><history><date date-type="received"><day>28</day>	<month>April</month>	<year>2014</year></date><date date-type="rev-recd"><day>28</day>	<month>May</month>	<year>2014</year>	</date><date date-type="accepted"><day>4</day>	<month>June</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>
 
  
    Values of the second thermodynamic dissociation constant pK
   <sub>2</sub> of the protonated form of monosodium 1,4-piperazinediethanesulfonate (PIPES) have been determined at twelve different temperatures in the temperature range from (278.15 to 328.15) K including the body temperature 310.15 K by measurement of the electromotive-force for cells without liquid junction of the type: Pt (s), H
   <sub>2</sub> (g), 101.325 kPa|Na-PIPES (m1) + Na
   <sub> 2</sub>-PIPES (m
   <sub>2</sub>) + NaCl (m
   <sub>3</sub>)|AgCl (s), Ag (s), where m
   <sub>1</sub>, m
   <sub>2</sub> and m
   <sub>3</sub> indicate the molalities of the corresponding species at 1 atm = 101.325 kPa in SI units. The pK2 values for the dissociation of Na-PIPES are represented by the equation: pK
   <sub>2</sub> = -1303.76/T + 48.369 - 6.46889 lnT with an uncertainty of &#177; 0.001. The values of pK
   <sub>2</sub> for Na-PIPES were found to be 7.1399 &#177; 0.0004 at 298.15 K and 7.0512 &#177; 0.0004 at 310.15 K, respectively, and indicate that this buffer would be useful as pH standard in the range of physiological application. Standard thermodynamic quantities 
   <img src="Edit_1270981e-7602-4e5d-ba5b-fe9831ea10bb.bmp" alt="" height="17" width="233" /> for the acidic dissociation process of Na-PIPES have been derived from the temperature coefficients of the pK
   <sub>2</sub>. These values are compared with those of structurally related N-substituted PIPERAZINE and TAURINE at 298.15 K. 
  
 
</html></p></abstract><kwd-group><kwd>Dissociation Constant</kwd><kwd> Zwitterion</kwd><kwd> Ionic Strength</kwd><kwd> pK&lt;sub&gt;2&lt;/sub&gt;</kwd><kwd> Buffer Compound</kwd><kwd> e.m.f</kwd><kwd> Thermodynamic Quantities</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The control of pH in the physiologically important pH range is difficult because of the limitation in the number of weak acid-base systems whose pH values fall within the pH range of 6 - 8. Second-stage dissociation process and the acid-base behavior of the simplest zwitterionic amino acids, 2-aminoethanesulfonic acid (TAURINE) [<xref ref-type="bibr" rid="scirp.46663-ref1">1</xref>] and (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] , have been studied. The pK<sub>2</sub> values of these two buffers at 298.15 K are 9.061 and 9.731, respectively. Careful thermodynamic investigation of the dissociation of other amino acids, (MES) [<xref ref-type="bibr" rid="scirp.46663-ref3">3</xref>] , (MOPS) [<xref ref-type="bibr" rid="scirp.46663-ref4">4</xref>] , (BES) [<xref ref-type="bibr" rid="scirp.46663-ref5">5</xref>] , (TES) [<xref ref-type="bibr" rid="scirp.46663-ref6">6</xref>] , and (CHES) [<xref ref-type="bibr" rid="scirp.46663-ref7">7</xref>] , has contributed significantly to an understanding of this important subject. Biological buffers are of great importance for research in biomedicine, pharmaceutical chemistry, clinical chemistry, and oceanography. Good et al. [<xref ref-type="bibr" rid="scirp.46663-ref8">8</xref>] recommended several biological buffer substances which are useful in the physiological pH region of 6 - 8. One of the buffer compounds selected was monosodium 1,4-pi- perazine diethanesulfonate (PIPES) whose deprotonation constant is about 10<sup>−8</sup> at 298.15 K. The compound PIPES is, therefore, a better buffer for pH control in the buffer region of greatest physiological interest than its parent compound, (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] .</p><p>In order to calculate pH values with the accuracy needed for a pH buffer standard, it is essential to determine very accurate values of the thermodynamic dissociation constant pK<sub>2</sub> for the second-stage dissociation equilibria of PIPES. Roy et al. [<xref ref-type="bibr" rid="scirp.46663-ref9">9</xref>] determined pK<sub>2</sub> values and related thermodynamic quantities of PIPES at 12 temperatures using the galvanic cell without liquid junction:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x5.png" xlink:type="simple"/></inline-formula>[A]</p><p>In this cell, Ag, AgBr electrode and KBr solid were used. Because of the importance of the chloride ion Cl<sup>−</sup> in clinical samples such as blood, plasma and cerebrospinal fluids, we have undertaken to study PIPES at 12 temperatures from (278.15 to 328.15) K employing the cell:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x6.png" xlink:type="simple"/></inline-formula>[B]</p><p>in which NaCl salt and Ag, AgCl were used. Thus, there is a great difference between cell A and cell B in terms of the use of the salt and the electrode. No thermodynamic data on pK<sub>2</sub> of PIPES is available in the literature using Ag-AgCl electrode. This is the original research work. The monosodium salt of the (PIPES) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x7.png" xlink:type="simple"/></inline-formula> is designated as P<sup>&#177;−</sup>, and the deprotonation process is represented by</p><disp-formula id="scirp.46663-formula230"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7100214x8.png"  xlink:type="simple"/></disp-formula><p>where K<sub>2</sub> is the thermodynamic equilibrium constant. The structure of the monosodium 1,4-piperazinedietha- nesulfonate (PIPES) is shown below.</p><disp-formula id="scirp.46663-formula231"><graphic  xlink:href="http://html.scirp.org/file/1-7100214x9.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2"><title>2. Experimental</title><p>The commercial sample of monosodium 1,4-piperazinediethanesulfonate (PIPES) was obtained from Research Organics (Cleveland, Ohio). The technique to determine the assay of PIPES has been previously reported [<xref ref-type="bibr" rid="scirp.46663-ref9">9</xref>] . It assayed 99.98% when titrated with a standard solution of NaOH. From the preliminary measurements, the difference in e.m.f (cell voltage) between a purified and unpurified sample was well within the experimental error &#177;0.05 mV. Thus, the commercial sample was used as received. It was always dried and stored in a desiccator. The preparation of all 16 experimental buffer solutions of Na-PIPES were made by mixing accurate amounts of the commercial sample of PIPES, CO<sub>2</sub>-free NaOH, Fisher ACS certified grade NaCl, and CO<sub>2</sub>-free double distilled water. The molality range of the buffer solutions varied from 0.002 to 0.04 mol∙kg<sup>−1</sup>, and the ionic strength range was from I = 0.006 to 0.12 mol∙kg<sup>−1</sup>. Vacuum corrections were applied to all masses with accuracy better than &#177;0.02 mass percent. The precise e.m.f measurement technique was originally used by Harned and Ehlers [<xref ref-type="bibr" rid="scirp.46663-ref10">10</xref>] . The e.m.f method used in the present study was modified by Gary et al. [<xref ref-type="bibr" rid="scirp.46663-ref11">11</xref>] and was successfully used by Sankar and Bates [<xref ref-type="bibr" rid="scirp.46663-ref12">12</xref>] as well as Roy et al. [<xref ref-type="bibr" rid="scirp.46663-ref13">13</xref>] . The following galvanic cell without liquid junction of the type was used:</p><disp-formula id="scirp.46663-formula232"><label>(A)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7100214x10.png"  xlink:type="simple"/></disp-formula><p>In all previous publications from this laboratory, the preparation of the platinum black hydrogen electrode and the silver-silver chloride electrode (thermal electrolytic type [<xref ref-type="bibr" rid="scirp.46663-ref14">14</xref>] ), the cell design of all glass cells, purification of the hydrogen gas, and other experimental details have been described in detail elsewhere [<xref ref-type="bibr" rid="scirp.46663-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.46663-ref16">16</xref>] . The bias potential of the (silver + silver chloride) electrodes was within &#177;0.05 mV. The e.m.f measurements were made at intervals of 5 K from (278.15 to 328.15) K for all 16 buffer solutions at 12 temperatures in the molality range 0.002 to 0.04 mol∙kg<sup>−1</sup>. The e.m.f at 298.15 K was recorded two times (sometimes three times), namely at the beginning, in the middle, and at the end of the run. These e.m.f values, on average, agreed to within &#177;0.04 mV, demonstrating excellent stability and high reproducibility of the silver-silver chloride in the presence of nitrogen base. The constant temperature of the water bath was regulated to &#177;0.005 K within a digital thermometer (Guildline model 9540). All e.m.f measurements were made by employing Hewlett-Packard 2000 multimeter.</p></sec><sec id="s3"><title>3. Methods and Results</title><p>The equation for the calculation of the “apparent” thermodynamic dissociation constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x11.png" xlink:type="simple"/></inline-formula> for the second dissociation step of PIPES is expressed:</p><disp-formula id="scirp.46663-formula233"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7100214x12.png"  xlink:type="simple"/></disp-formula><p>where P<sup>&#177;−</sup> is the zwitterionic species for Na-PIPES; m<sub>1</sub>, m<sub>2</sub>, and m<sub>3</sub> are stoichiometric molalities of the corresponding species; P<sup>−2</sup> stands for Na<sub>2</sub>-PIPES; pK<sub>2</sub> the thermodynamic dissociation constant; γ the activity coefficient of the respective species; E the e.m.f corrected to a hydrogen partial pressure of 101.325 kPa; F is the Faraday constant (96487 C・mol<sup>−1</sup>); RT ln10/F = k = 0.059156 at 298.15 K; and E˚ is the standard electrode potential of the (silver + silver chloride) electrode. The cell voltage (E) values are listed in <xref ref-type="table" rid="table1">Table 1</xref>. The values of (E˚) [<xref ref-type="bibr" rid="scirp.46663-ref17">17</xref>] were obtained in the authors’ laboratory by using 0.01 mol・kg<sup>−1</sup> HCl solution with a value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x13.png" xlink:type="simple"/></inline-formula> = 0.904 at 298.15 K. The activity coefficient of Equation (2) is unknown. In such situations, the simple form of Equation</p><p>(2) involves assumptions that a) the activity coefficient term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x14.png" xlink:type="simple"/></inline-formula> will, because of charge</p><p>type, be small and is expected to become linear function of the ionic strength I, and b) the nearly neutral pH of the buffer solutions which make hydrolysis correction of the ratio m<sub>1</sub>/m<sub>2</sub> unnecessary. The ionic strength of the solution of cell B is indicated by:</p><disp-formula id="scirp.46663-formula234"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7100214x15.png"  xlink:type="simple"/></disp-formula><p>and the simplified version of Equation (2) becomes:</p><disp-formula id="scirp.46663-formula235"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7100214x16.png"  xlink:type="simple"/></disp-formula><p>As expected, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x17.png" xlink:type="simple"/></inline-formula>varies linearly with I at each temperature and is represented by the following equation:</p><disp-formula id="scirp.46663-formula236"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7100214x18.png"  xlink:type="simple"/></disp-formula><p>where the intercept at I = 0 yields the value of pK<sub>2</sub> and β is the slope parameter. These values of pK<sub>2</sub> together with the standard deviation are listed in <xref ref-type="table" rid="table2">Table 2</xref>. The experimental values of pK<sub>2</sub> are fitted as a function of the thermodynamic temperature T from (278.15 to 323.15) K by the method of least squares to an equation of the form suggested by Ives and Mosely [<xref ref-type="bibr" rid="scirp.46663-ref18">18</xref>] . The final equation takes the form</p><disp-formula id="scirp.46663-formula237"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7100214x19.png"  xlink:type="simple"/></disp-formula><p>The standard deviation of regression for Equation (6) is 0.0014. The values of the standard changes of Gibbs energy (∆G˚), enthalpy (∆H˚), entropy (∆S˚) and the heat capacity (∆C<sub>p</sub>˚) for the dissociation process indicated by Equation (1) have been derived from the constants of Equation (6) by using simple thermodynamic relationships. The values of these thermodynamic functions, along with the estimates of the standard deviations calculated by the method of Please [<xref ref-type="bibr" rid="scirp.46663-ref19">19</xref>] are summarized in <xref ref-type="table" rid="table3">Table 3</xref>. It is of interest to compare the values of the pK<sub>2</sub> and thermodynamic functions of Na-PIPES with some structurally related N-substituted zwitterionic compounds of (TAURINE) [<xref ref-type="bibr" rid="scirp.46663-ref1">1</xref>] and (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] . At 298.15 K, these values are compiled in <xref ref-type="table" rid="table4">Table 4</xref>.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Cell potential of cell B (in volts)</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="9"  >Pt (s); H<sub>2</sub> (g), 101.325 kPa|Na-PIPES (m<sub>1</sub>), Na<sub>2</sub>-PIPES (m<sub>2</sub>), NaCl (m<sub>3</sub>)|AgCl (s), Ag (s)</th></tr></thead><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" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  >T/K</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >mol∙kg<sup>−1</sup></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >278.15 K</td><td align="center" valign="middle" >283.15 K</td><td align="center" valign="middle" >288.15 K</td><td align="center" valign="middle" >293.15 K</td><td align="center" valign="middle" >298.15 K</td><td align="center" valign="middle" >303.15 K</td></tr><tr><td align="center" valign="middle" >0.001999</td><td align="center" valign="middle" >0.000667</td><td align="center" valign="middle" >0.001993</td><td align="center" valign="middle" >0.75837</td><td align="center" valign="middle" >0.76320</td><td align="center" valign="middle" >0.76770</td><td align="center" valign="middle" >0.77218</td><td align="center" valign="middle" >0.77633</td><td align="center" valign="middle" >0.78021</td></tr><tr><td align="center" valign="middle" >0.003336</td><td align="center" valign="middle" >0.001113</td><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.71954</td><td align="center" valign="middle" >0.72369</td><td align="center" valign="middle" >0.72752</td><td align="center" valign="middle" >0.73130</td><td align="center" valign="middle" >0.73477</td><td align="center" valign="middle" >0.73793</td></tr><tr><td align="center" valign="middle" >0.009996</td><td align="center" valign="middle" >0.003337</td><td align="center" valign="middle" >0.004991</td><td align="center" valign="middle" >0.73623</td><td align="center" valign="middle" >0.74067</td><td align="center" valign="middle" >0.74482</td><td align="center" valign="middle" >0.74890</td><td align="center" valign="middle" >0.75267</td><td align="center" valign="middle" >0.75612</td></tr><tr><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.003333</td><td align="center" valign="middle" >0.009997</td><td align="center" valign="middle" >0.71951</td><td align="center" valign="middle" >0.72365</td><td align="center" valign="middle" >0.72750</td><td align="center" valign="middle" >0.73128</td><td align="center" valign="middle" >0.73474</td><td align="center" valign="middle" >0.73790</td></tr><tr><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.003333</td><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.71940</td><td align="center" valign="middle" >0.72354</td><td align="center" valign="middle" >0.72740</td><td align="center" valign="middle" >0.73119</td><td align="center" valign="middle" >0.73465</td><td align="center" valign="middle" >0.73780</td></tr><tr><td align="center" valign="middle" >0.006658</td><td align="center" valign="middle" >0.002210</td><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.70276</td><td align="center" valign="middle" >0.70659</td><td align="center" valign="middle" >0.71015</td><td align="center" valign="middle" >0.71364</td><td align="center" valign="middle" >0.71678</td><td align="center" valign="middle" >0.71964</td></tr><tr><td align="center" valign="middle" >0.008330</td><td align="center" valign="middle" >0.002777</td><td align="center" valign="middle" >0.025000</td><td align="center" valign="middle" >0.69734</td><td align="center" valign="middle" >0.70109</td><td align="center" valign="middle" >0.70456</td><td align="center" valign="middle" >0.70795</td><td align="center" valign="middle" >0.71101</td><td align="center" valign="middle" >0.71377</td></tr><tr><td align="center" valign="middle" >0.015000</td><td align="center" valign="middle" >0.005000</td><td align="center" valign="middle" >0.015000</td><td align="center" valign="middle" >0.70956</td><td align="center" valign="middle" >0.71353</td><td align="center" valign="middle" >0.71722</td><td align="center" valign="middle" >0.72085</td><td align="center" valign="middle" >0.72413</td><td align="center" valign="middle" >0.72711</td></tr><tr><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.006663</td><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.70264</td><td align="center" valign="middle" >0.70648</td><td align="center" valign="middle" >0.71006</td><td align="center" valign="middle" >0.71356</td><td align="center" valign="middle" >0.71670</td><td align="center" valign="middle" >0.71956</td></tr><tr><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.006667</td><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.70264</td><td align="center" valign="middle" >0.70649</td><td align="center" valign="middle" >0.71008</td><td align="center" valign="middle" >0.71358</td><td align="center" valign="middle" >0.71673</td><td align="center" valign="middle" >0.71957</td></tr><tr><td align="center" valign="middle" >0.021990</td><td align="center" valign="middle" >0.008665</td><td align="center" valign="middle" >0.021990</td><td align="center" valign="middle" >0.70415</td><td align="center" valign="middle" >0.70803</td><td align="center" valign="middle" >0.71167</td><td align="center" valign="middle" >0.71520</td><td align="center" valign="middle" >0.71838</td><td align="center" valign="middle" >0.72125</td></tr><tr><td align="center" valign="middle" >0.025000</td><td align="center" valign="middle" >0.008333</td><td align="center" valign="middle" >0.025010</td><td align="center" valign="middle" >0.69714</td><td align="center" valign="middle" >0.70090</td><td align="center" valign="middle" >0.70441</td><td align="center" valign="middle" >0.70782</td><td align="center" valign="middle" >0.71087</td><td align="center" valign="middle" >0.71361</td></tr><tr><td align="center" valign="middle" >0.029999</td><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.029990</td><td align="center" valign="middle" >0.69269</td><td align="center" valign="middle" >0.69636</td><td align="center" valign="middle" >0.69979</td><td align="center" valign="middle" >0.70312</td><td align="center" valign="middle" >0.70610</td><td align="center" valign="middle" >0.70876</td></tr><tr><td align="center" valign="middle" >0.033300</td><td align="center" valign="middle" >0.011100</td><td align="center" valign="middle" >0.033300</td><td align="center" valign="middle" >0.68995</td><td align="center" valign="middle" >0.69359</td><td align="center" valign="middle" >0.69701</td><td align="center" valign="middle" >0.70031</td><td align="center" valign="middle" >0.70323</td><td align="center" valign="middle" >0.70584</td></tr><tr><td align="center" valign="middle" >0.039960</td><td align="center" valign="middle" >0.013320</td><td align="center" valign="middle" >0.039960</td><td align="center" valign="middle" >0.68553</td><td align="center" valign="middle" >0.68907</td><td align="center" valign="middle" >0.69244</td><td align="center" valign="middle" >0.69566</td><td align="center" valign="middle" >0.69849</td><td align="center" valign="middle" >0.70101</td></tr><tr><td align="center" valign="middle" >0.040000</td><td align="center" valign="middle" >0.013330</td><td align="center" valign="middle" >0.040000</td><td align="center" valign="middle" >0.68548</td><td align="center" valign="middle" >0.68904</td><td align="center" valign="middle" >0.69241</td><td align="center" valign="middle" >0.69561</td><td align="center" valign="middle" >0.69844</td><td align="center" valign="middle" >0.70097</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" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >T/K</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >mol∙kg<sup>−1</sup></td><td align="center" valign="middle" ></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" >0.001999</td><td align="center" valign="middle" >0.000667</td><td align="center" valign="middle" >0.001993</td><td align="center" valign="middle" >0.78381</td><td align="center" valign="middle" >0.78502</td><td align="center" valign="middle" >0.78721</td><td align="center" valign="middle" >0.79032</td><td align="center" valign="middle" >0.79318</td><td align="center" valign="middle" >0.79582</td></tr><tr><td align="center" valign="middle" >0.003336</td><td align="center" valign="middle" >0.001113</td><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.74081</td><td align="center" valign="middle" >0.74174</td><td align="center" valign="middle" >0.74350</td><td align="center" valign="middle" >0.74589</td><td align="center" valign="middle" >0.74804</td><td align="center" valign="middle" >0.74995</td></tr><tr><td align="center" valign="middle" >0.009996</td><td align="center" valign="middle" >0.003337</td><td align="center" valign="middle" >0.004991</td><td align="center" valign="middle" >0.75929</td><td align="center" valign="middle" >0.76034</td><td align="center" valign="middle" >0.76229</td><td align="center" valign="middle" >0.76498</td><td align="center" valign="middle" >0.76745</td><td align="center" valign="middle" >0.76968</td></tr><tr><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.003333</td><td align="center" valign="middle" >0.009997</td><td align="center" valign="middle" >0.74078</td><td align="center" valign="middle" >0.74170</td><td align="center" valign="middle" >0.74347</td><td align="center" valign="middle" >0.74587</td><td align="center" valign="middle" >0.74803</td><td align="center" valign="middle" >0.74994</td></tr><tr><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.003333</td><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.74066</td><td align="center" valign="middle" >0.74158</td><td align="center" valign="middle" >0.74333</td><td align="center" valign="middle" >0.74572</td><td align="center" valign="middle" >0.74787</td><td align="center" valign="middle" >0.74978</td></tr><tr><td align="center" valign="middle" >0.006658</td><td align="center" valign="middle" >0.002210</td><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.72220</td><td align="center" valign="middle" >0.72300</td><td align="center" valign="middle" >0.72459</td><td align="center" valign="middle" >0.72668</td><td align="center" valign="middle" >0.72854</td><td align="center" valign="middle" >0.73016</td></tr><tr><td align="center" valign="middle" >0.008330</td><td align="center" valign="middle" >0.002777</td><td align="center" valign="middle" >0.025000</td><td align="center" valign="middle" >0.71622</td><td align="center" valign="middle" >0.71697</td><td align="center" valign="middle" >0.71851</td><td align="center" valign="middle" >0.72050</td><td align="center" valign="middle" >0.72226</td><td align="center" valign="middle" >0.72377</td></tr><tr><td align="center" valign="middle" >0.015000</td><td align="center" valign="middle" >0.005000</td><td align="center" valign="middle" >0.015000</td><td align="center" valign="middle" >0.72977</td><td align="center" valign="middle" >0.73060</td><td align="center" valign="middle" >0.73226</td><td align="center" valign="middle" >0.73445</td><td align="center" valign="middle" >0.73643</td><td align="center" valign="middle" >0.73815</td></tr><tr><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.006663</td><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.72209</td><td align="center" valign="middle" >0.72286</td><td align="center" valign="middle" >0.72446</td><td align="center" valign="middle" >0.72653</td><td align="center" valign="middle" >0.72839</td><td align="center" valign="middle" >0.73000</td></tr><tr><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.006667</td><td align="center" valign="middle" >0.020000</td><td align="center" valign="middle" >0.72210</td><td align="center" valign="middle" >0.72287</td><td align="center" valign="middle" >0.72447</td><td align="center" valign="middle" >0.72655</td><td align="center" valign="middle" >0.72840</td><td align="center" valign="middle" >0.73000</td></tr><tr><td align="center" valign="middle" >0.021990</td><td align="center" valign="middle" >0.008665</td><td align="center" valign="middle" >0.021990</td><td align="center" valign="middle" >0.72380</td><td align="center" valign="middle" >0.72457</td><td align="center" valign="middle" >0.72619</td><td align="center" valign="middle" >0.72829</td><td align="center" valign="middle" >0.73017</td><td align="center" valign="middle" >0.73179</td></tr><tr><td align="center" valign="middle" >0.025000</td><td align="center" valign="middle" >0.008333</td><td align="center" valign="middle" >0.025010</td><td align="center" valign="middle" >0.71602</td><td align="center" valign="middle" >0.71674</td><td align="center" valign="middle" >0.71828</td><td align="center" valign="middle" >0.72025</td><td align="center" valign="middle" >0.72202</td><td align="center" valign="middle" >0.72352</td></tr><tr><td align="center" valign="middle" >0.029999</td><td align="center" valign="middle" >0.010000</td><td align="center" valign="middle" >0.029990</td><td align="center" valign="middle" >0.71108</td><td align="center" valign="middle" >0.71175</td><td align="center" valign="middle" >0.71326</td><td align="center" valign="middle" >0.71515</td><td align="center" valign="middle" >0.71682</td><td align="center" valign="middle" >0.71823</td></tr><tr><td align="center" valign="middle" >0.033300</td><td align="center" valign="middle" >0.011100</td><td align="center" valign="middle" >0.033300</td><td align="center" valign="middle" >0.70809</td><td align="center" valign="middle" >0.70873</td><td align="center" valign="middle" >0.71021</td><td align="center" valign="middle" >0.71204</td><td align="center" valign="middle" >0.71366</td><td align="center" valign="middle" >0.71500</td></tr><tr><td align="center" valign="middle" >0.039960</td><td align="center" valign="middle" >0.013320</td><td align="center" valign="middle" >0.039960</td><td align="center" valign="middle" >0.70318</td><td align="center" valign="middle" >0.70376</td><td align="center" valign="middle" >0.70520</td><td align="center" valign="middle" >0.70695</td><td align="center" valign="middle" >0.70849</td><td align="center" valign="middle" >0.70977</td></tr><tr><td align="center" valign="middle" >0.040000</td><td align="center" valign="middle" >0.013330</td><td align="center" valign="middle" >0.040000</td><td align="center" valign="middle" >0.70314</td><td align="center" valign="middle" >0.70374</td><td align="center" valign="middle" >0.70518</td><td align="center" valign="middle" >0.70692</td><td align="center" valign="middle" >0.70846</td><td align="center" valign="middle" >0.70975</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Second dissociation constant of Na-PIPES</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >From (278.15 to 328.15) K</th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >T/K</td><td align="center" valign="middle" >pK<sub>2</sub></td><td align="center" valign="middle" >σ (pK<sub>2</sub>)<sup>a</sup></td><td align="center" valign="middle" >β</td><td align="center" valign="middle" >σ (β)<sup>b</sup></td></tr><tr><td align="center" valign="middle" >278.15</td><td align="center" valign="middle" >7.2752</td><td align="center" valign="middle" >0.0005</td><td align="center" valign="middle" >0.154</td><td align="center" valign="middle" >0.009</td></tr><tr><td align="center" valign="middle" >283.15</td><td align="center" valign="middle" >7.2413</td><td align="center" valign="middle" >0.0005</td><td align="center" valign="middle" >0.149</td><td align="center" valign="middle" >0.008</td></tr><tr><td align="center" valign="middle" >288.15</td><td align="center" valign="middle" >7.2055</td><td align="center" valign="middle" >0.0004</td><td align="center" valign="middle" >0.124</td><td align="center" valign="middle" >0.007</td></tr><tr><td align="center" valign="middle" >293.15</td><td align="center" valign="middle" >7.1734</td><td align="center" valign="middle" >0.0004</td><td align="center" valign="middle" >0.117</td><td align="center" valign="middle" >0.007</td></tr><tr><td align="center" valign="middle" >298.15</td><td align="center" valign="middle" >7.1399</td><td align="center" valign="middle" >0.0004</td><td align="center" valign="middle" >0.120</td><td align="center" valign="middle" >0.007</td></tr><tr><td align="center" valign="middle" >303.15</td><td align="center" valign="middle" >7.1048</td><td align="center" valign="middle" >0.0004</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" >0.007</td></tr><tr><td align="center" valign="middle" >308.15</td><td align="center" valign="middle" >7.0680</td><td align="center" valign="middle" >0.0004</td><td align="center" valign="middle" >0.143</td><td align="center" valign="middle" >0.007</td></tr><tr><td align="center" valign="middle" >310.15</td><td align="center" valign="middle" >7.0512</td><td align="center" valign="middle" >0.0004</td><td align="center" valign="middle" >0.158</td><td align="center" valign="middle" >0.007</td></tr><tr><td align="center" valign="middle" >313.15</td><td align="center" valign="middle" >7.0320</td><td align="center" valign="middle" >0.0005</td><td align="center" valign="middle" >0.151</td><td align="center" valign="middle" >0.008</td></tr><tr><td align="center" valign="middle" >318.15</td><td align="center" valign="middle" >6.9950</td><td align="center" valign="middle" >0.0004</td><td align="center" valign="middle" >0.158</td><td align="center" valign="middle" >0.008</td></tr><tr><td align="center" valign="middle" >323.15</td><td align="center" valign="middle" >6.9570</td><td align="center" valign="middle" >0.0005</td><td align="center" valign="middle" >0.159</td><td align="center" valign="middle" >0.008</td></tr><tr><td align="center" valign="middle" >328.15</td><td align="center" valign="middle" >6.9175</td><td align="center" valign="middle" >0.0006</td><td align="center" valign="middle" >0.164</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-PIPES 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˚</td><td align="center" valign="middle" >38.734 &#177; 2</td><td align="center" valign="middle" >39.763 &#177; 2</td><td align="center" valign="middle" >40.749 &#177; 3</td><td align="center" valign="middle" >41.694 &#177; 3</td><td align="center" valign="middle" >42.599 &#177; 3</td><td align="center" valign="middle" >43.465 &#177; 3</td></tr><tr><td align="center" valign="middle" >∆H˚</td><td align="center" valign="middle" >9.487 &#177; 51</td><td align="center" valign="middle" >10.726 &#177; 33</td><td align="center" valign="middle" >11.964 &#177; 18</td><td align="center" valign="middle" >13.203 &#177; 19</td><td align="center" valign="middle" >14.441 &#177; 36</td><td align="center" valign="middle" >15.679 &#177; 57</td></tr><tr><td align="center" valign="middle" >∆S˚</td><td align="center" valign="middle" >−105.1 &#177; 0.2</td><td align="center" valign="middle" >−100.8 &#177; 0.1</td><td align="center" valign="middle" >−96.5 &#177; 0.1</td><td align="center" valign="middle" >−92.5 &#177; 0.1</td><td align="center" valign="middle" >−88.5 &#177; 0.1</td><td align="center" valign="middle" >−84.7 &#177; 0.2</td></tr><tr><td align="center" valign="middle" >∆C<sub>p</sub>˚</td><td align="center" valign="middle" >124 &#177; 2</td><td align="center" valign="middle" >124 &#177; 2</td><td align="center" valign="middle" >124 &#177; 2</td><td align="center" valign="middle" >124 &#177; 2</td><td align="center" valign="middle" >124 &#177; 2</td><td align="center" valign="middle" >124 &#177; 2</td></tr></tbody></table></table-wrap><p>Units: ∆G˚. ∆H˚, J∙mol<sup>−1</sup>; ∆S˚, ∆C<sub>p</sub>˚, J∙K<sup>−1</sup>∙mol<sup>−1</sup>.</p></sec><sec id="s4"><title>4. Discussion</title><p>For each of the structurally related compounds in <xref ref-type="table" rid="table4">Table 4</xref>, two methylene groups separate positive and negative charge centers. The comparison of the thermodynamic properties of some substituted compounds and the parent compound (TAURINE) [<xref ref-type="bibr" rid="scirp.46663-ref1">1</xref>] and the derivative of TAURINE such as (MOPS) [<xref ref-type="bibr" rid="scirp.46663-ref4">4</xref>] , (BES) [<xref ref-type="bibr" rid="scirp.46663-ref5">5</xref>] , (TES) [<xref ref-type="bibr" rid="scirp.46663-ref6">6</xref>] , (CHES) [<xref ref-type="bibr" rid="scirp.46663-ref7">7</xref>] , (MOBS) [<xref ref-type="bibr" rid="scirp.46663-ref20">20</xref>] and (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] and its N-substituted PIPERAZINE such as (HEPBS) [<xref ref-type="bibr" rid="scirp.46663-ref20">20</xref>] , (HEPES) [<xref ref-type="bibr" rid="scirp.46663-ref21">21</xref>] , (TAPS) [<xref ref-type="bibr" rid="scirp.46663-ref22">22</xref>] and PIPES [this investigation] reveal useful information in terms of acidic strength, steric and inductive effects. The parent compound PIPERAZINE has a pK<sub>2</sub> of 9.731 at 298.15 K whereas that of PIPES in the present work is 7.140. The interpretation is that the substitutions of methylene-(CH<sub>2</sub>)<sub>2</sub> and hydroxymethyl- (HOCH<sub>2</sub>)<sub>2</sub> groups on the nitrogen atom of (TAURINE) [<xref ref-type="bibr" rid="scirp.46663-ref1">1</xref>] and (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] enhance the acidic strength for the dissociation of (BES) [<xref ref-type="bibr" rid="scirp.46663-ref5">5</xref>] and PIPES [this study], respectively.</p><p><xref ref-type="table" rid="table4">Table 4</xref> clearly shows a decrease in pK<sub>2</sub> value (increase in acidic strength) for both N-substituted PIPERAZINE and TAURINE compounds. The alterations in acidic strength for the dissociation process of PIPES are attributable to the inductive effects of the oxygen atom from both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x20.png" xlink:type="simple"/></inline-formula> groups as well as the steric effects of the -(CH<sub>2</sub>)<sub>4</sub> groups in PIPERAZINE from which the dissociation of H<sup>+</sup> occurs.</p><p>It is interesting to discuss the trend of the standard thermodynamic properties from <xref ref-type="table" rid="table4">Table 4</xref>. Usually, the decrease in pK<sub>2</sub> value is paralleled by the decrease in values of ∆H˚, which are observed for PIPERAZINE and PIPES. <xref ref-type="table" rid="table4">Table 4</xref> shows the value of ∆H˚ at 298.15 K for (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] is 53,390 J・mol<sup>−1</sup> whereas for PIPES ∆H˚ = 11,964 J・mol<sup>−1</sup>. The explanation is that in addition to lowering the pK<sub>2</sub>, the hydroxymethyl and hydroxyethyl substitutions lower the value of ∆H˚ for isoelectric dissociation process [<xref ref-type="bibr" rid="scirp.46663-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.46663-ref24">24</xref>] . This pattern is</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Thermodynamic quantities for the dissociation of a series of structurally related compounds of Taurine, Morpho- line and Piperazine in water at 298.15 K</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Structure x</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˚</th><th align="center" valign="middle" >∆S˚</th><th align="center" valign="middle" >∆C<sub>p</sub>˚</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/1-7100214x21.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" >2</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x22.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" >This study</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x23.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >HEPBS</td><td align="center" valign="middle" >8.284</td><td align="center" valign="middle" >23.081</td><td align="center" valign="middle" >−84.4</td><td align="center" valign="middle" >77</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x24.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >HEPES</td><td align="center" valign="middle" >7.562</td><td align="center" valign="middle" >20.376</td><td align="center" valign="middle" >−76.6</td><td align="center" valign="middle" >46</td><td align="center" valign="middle" >21</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x25.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" >1</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x26.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >MOPS</td><td align="center" valign="middle" >7.183</td><td align="center" valign="middle" >21.008</td><td align="center" valign="middle" >−69.7</td><td align="center" valign="middle" >17</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x27.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >BES</td><td align="center" valign="middle" >7.187</td><td align="center" valign="middle" >24.184</td><td align="center" valign="middle" >−56.5</td><td align="center" valign="middle" >−4</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x28.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >TES</td><td align="center" valign="middle" >7.550</td><td align="center" valign="middle" >32.133</td><td align="center" valign="middle" >−36.8</td><td align="center" valign="middle" >−17</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7100214x29.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >CHES</td><td align="center" valign="middle" >9.394</td><td align="center" valign="middle" >39.551</td><td align="center" valign="middle" >−49.1</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >7</td></tr></tbody></table></table-wrap><p>Units: ∆H˚, J∙mol<sup>−</sup><sup>1</sup>; ∆S˚, ∆C<sub>p</sub>˚, J∙K<sup>−1</sup>∙mol<sup>−1</sup>.</p><p>also consistent for (TAURINE) [<xref ref-type="bibr" rid="scirp.46663-ref1">1</xref>] and its derivative (BES) [<xref ref-type="bibr" rid="scirp.46663-ref5">5</xref>] . The changes of entropy ∆S˚ from <xref ref-type="table" rid="table4">Table 4</xref> are −33.9 J・K<sup>−1</sup>・mol<sup>−1</sup> for (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] , whereas that for PIPES is −96.55 J・K<sup>−1</sup>・mol<sup>−1</sup>. The more negative values of ∆S˚ for PIPES compared to PIPERAZINE might indicate that for the dissociation process, the stabilization of the solvent structure causes an increased order (orientation) of polar water molecule in the proximity of the charged species (P<sup>&#177;−</sup>, H<sup>+</sup>, P<sup>−2</sup>, Na<sup>+</sup>). The values of ∆C<sub>p</sub>˚ for the dissociation of (PIPERAZINE) [<xref ref-type="bibr" rid="scirp.46663-ref2">2</xref>] is 88 J・K<sup>−1</sup>・mol<sup>−1</sup> and that found for PIPES is 124 J・K<sup>−1</sup>・mol<sup>−1</sup>. Since the value of ∆C<sub>p</sub>˚ for PIPES is more positive compared to PIPERAZINE, this represents a substantial change in the solvation patterns (water structure) for the dissociation process of PIPES. The charge type (electrostatic effects) appears to be the primary factor in determining the large positive P<sup>&#177;−</sup> values of ∆C<sub>p</sub>˚ [<xref ref-type="bibr" rid="scirp.46663-ref13">13</xref>] . The quantitative explanations for the interactions of Na<sup>+</sup>, Cl<sup>−</sup>, P<sup>&#177;−</sup>, H<sup>+</sup> and P<sup>−2</sup> with water are complex.</p></sec><sec id="s5"><title>5. Conclusion</title><p>The e.m.f data are stable and highly reproducible. The results of the second dissociation constant pK<sub>2</sub> and associated thermodynamic quantities are very accurate and reliable. The pK<sub>2</sub> value lies in the physiological region of pH 6 - 8. Thus buffer solutions of Na-PIPES and Na<sub>2</sub>-PIPES can be considered as a pH buffer standard for the physiological use. In a separate communication, pH values of buffer solutions without and with NaCl (isotonic saline media) from (278.15 - 328.15) K at an ionic strength I = 0.16 mol∙kg<sup>−1</sup> will be reported as what was done for the physiological buffer (TAPSO) [<xref ref-type="bibr" rid="scirp.46663-ref25">25</xref>] .</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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