<?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">MSCE</journal-id><journal-title-group><journal-title>Journal of Materials Science and Chemical Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-6045</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msce.2015.36007</article-id><article-id pub-id-type="publisher-id">MSCE-57078</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>
 
 
  Determination of Molecular Mass of Strong Acids by Differential Temperature Model (DTM) Using H&lt;sub&gt;3&lt;/sub&gt;PO&lt;sub&gt;4&lt;/sub&gt; and HBF&lt;sub&gt;4&lt;/sub&gt; for Classical Demonstration
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>I.</surname><given-names>A. Akpan</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Thermodynamics and Electrochemical Laboratory, Department of Chemistry, University of Uyo, Uyo, Nigeria</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>iaakpanchem2007@yahoo.com</email></corresp></author-notes><pub-date pub-type="epub"><day>11</day><month>06</month><year>2015</year></pub-date><volume>03</volume><issue>06</issue><fpage>41</fpage><lpage>47</lpage><history><date date-type="received"><day>February</day>	<month>2015</month>	</date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   A new chemical hypothesis based on the differential temperature model (DTM) for estimation of molecular masses of some strong acids (H<sub>2</sub>SO<sub>4</sub>, HNO<sub>3</sub> and HCl) in solutions have previously been propounded and tested theoretically and analytically by the author. The results were published in the Bulletin of Pure and Applied Sciences–Chemistry in 2012. The changes in temperature following various dilutions of the acids were found to be proportional to their molecular properties. The new chemical hypothesis and model is hereby tested on H<sub>3</sub>PO<sub>4</sub> and HBF<sub>4</sub> and their exact molecular masses have been evaluated analytically and theoretically. The validity of the hypothesis and the model is hereby presented for chemical proof and adoption to theory by chemists. 
 
</p></abstract><kwd-group><kwd>Differential Temperature</kwd><kwd> Molecular Mass</kwd><kwd> Strong Acids</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Strong acids are strong electrolytes with high ionization potential in solution.</p><disp-formula id="scirp.57078-formula332"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57078x3.png"  xlink:type="simple"/></disp-formula><p>The reaction in the above chemical equation is an endothermic process. A lattice energy is absorbed by the reacting system and thus, is responsible for the ionisation of the acidic species in solution. Proton theory of acids developed by Bronsted and Bjerrum in Denmark and Lowry in England in 1923 defines acids as proton-trans- ferring species [<xref ref-type="bibr" rid="scirp.57078-ref1">1</xref>]. The proton discharged during ionisation process has a great tendency to be solvated being an empty orbital. It then implies that, a proton does not exist in a free state in solution but in the solvated form. Water molecule as a solvent, interacts with proton, forming a solvated ion known as an oxonium ion. Solvation reaction is an exothermic process, accompanied by evolution of hydration or solvation energy in the form of heat.</p><disp-formula id="scirp.57078-formula333"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57078x4.png"  xlink:type="simple"/></disp-formula><p>The extent of ionisation or dissociation of acids depends upon the intrinsic acidic strength and upon the degree of affinity of the solvent for proton (protophilicity). Hence all acids which ionise completely in solution at finite dilution are called strong acids.</p></sec><sec id="s2"><title>2. Methods of Determination of Molecular Mass</title><p>Hitherto, several methods abound for the determination molecular mass. Physical methods include measurements via colligative properties in ideal solution [<xref ref-type="bibr" rid="scirp.57078-ref2">2</xref>], diffusion rates, etc. Analytical methods make use of titrimetry which depends on the stoichiometric relationship between the amount of the standard solution and that of the analyte (solute). The volume-mass relationship of the analyte is then used in the determination of molecular mass [<xref ref-type="bibr" rid="scirp.57078-ref3">3</xref>].</p><p>Instrumental methods make use of electronic instrument such as mass spectrometry, X-ray diffraction analysis, viscometer etc. [<xref ref-type="bibr" rid="scirp.57078-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.57078-ref5">5</xref>].</p><p>Apart from the high financial costs associated with procurement of most apparatus used for the determination of molecular properties in physical chemistry laboratories spectrophotometric equipment such as mass spectrophotometer and X-ray diffraction machines often break down and remain obsolete due to electric current fluctuations which characterise our economy.</p><p>The author’s interest is to study the thermochemical potentials in solutions of chemical substances and to develop hypothesis in order to devise alternative methods of determining their molecular properties without recourse to sophisticated instruments.</p><p>Attention is first focused on strong acids and bases because of their wide applications in chemical studies. Earlier research efforts in our electrochemical laboratory had led to the discovery of thermal constants of strong acids at various dilutions.</p><p>From the thermal constant discovered we had proposed an hypothesis and developed a valid mathematical model for the calculation of molecular mass of strong acids and tests their validity in HCl, HNO<sub>3</sub> and H<sub>2</sub>SO<sub>4</sub> [<xref ref-type="bibr" rid="scirp.57078-ref6">6</xref>].</p><p>The present work is yet a further application of the mathematical model for the determination of molecular masses of H<sub>3</sub>PO<sub>4</sub> and HBF<sub>4</sub>.</p><sec id="s2_1"><title>2.1. The Propounded Hypothesis and Its Mathematical Implication</title><p>“At constant temperature and pressure, the differential temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x5.png" xlink:type="simple"/></inline-formula> of the dilution of equal volumes of strong acids in a fixed volume of water is directly proportional to the product of the sum of the relative masses of the ionised species and the square of the basicity of the acid”.</p><disp-formula id="scirp.57078-formula334"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57078x6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x7.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x8.png" xlink:type="simple"/></inline-formula> are the relative masses of the cation and anion species respectively and b, the basicity of the acid.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x9.png" xlink:type="simple"/></inline-formula>is the change in temperature between the maximum temperature attained after dilution and the initial temperature of the solvent (water) before dilution.</p><p>If a constant is introduced into the proportion in 1 above, we obtain</p><disp-formula id="scirp.57078-formula335"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57078x10.png"  xlink:type="simple"/></disp-formula><p>k is the thermal constant of strong acids at equivalent dilution at constant pressure and temperature</p><p>From Equation (2)</p><disp-formula id="scirp.57078-formula336"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57078x11.png"  xlink:type="simple"/></disp-formula><p>Method of evaluation of k for HBF<sub>4</sub> and H<sub>3</sub>PO<sub>4</sub> can apply to other strong acids.</p></sec><sec id="s2_2"><title>2.2. Experimental</title><p>The solvent de-ionsied water and the solutes H<sub>3</sub>PO<sub>4</sub> and HBF<sub>4</sub> were purchased from BDH Limited. Both solutes were used as purchased without further purification. The reaction was carried out in a well-insulated vessel, known as the colorimeter as described elsewhere [<xref ref-type="bibr" rid="scirp.57078-ref7">7</xref>]. Being perfectly insulated, it could effectively measure the heat energy transferred during the reaction.</p><p>Dewar flask was used as calorimeter as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, because it has a large heat capacity. The inner surface of the vessel was silvered and a space between the inner and outer wall was evacuated in order to minimise exchange of heat energy with the surrounding. A cork stopper was fitted at the top of the mouth and it contained a thermometer. The heat was measured in calories and converted to Joules. The gram-calorie is the amount of heat required to raise the temperature of 1 g of water through 1˚C. The amount of heat evolved in the process was measured as, mass of the system multiplied by rise in temperature, multiplied by specific heat of the system. Thermal constants and other thermochemical properties were evaluated and recorded.</p></sec></sec><sec id="s3"><title>3. Result and Discussion</title><sec id="s3_1"><title>3.1. Results</title><p>The results of the experiments are presented in Tables 1-4. Relevant plots are presented in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec><sec id="s3_2"><title>3.2. Discussion</title><sec id="s3_2_1"><title>3.2.1. Thermal Mechanism of Fluoroboric Acid (HBF<sub>4</sub>)</title><p>The thermochemical process resulting from the ionisation of Fluoroboric Acid following the absorption of lattice energy attracts solvation of the proton with the evolution of heat energy according to the mechanism.</p><disp-formula id="scirp.57078-formula337"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57078x12.png"  xlink:type="simple"/></disp-formula><p>The thermal constant following the ionisation process is calculated as follows</p><p>Mass of solvated cation = <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x13.png" xlink:type="simple"/></inline-formula> = 19, Mass of anion = <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x14.png" xlink:type="simple"/></inline-formula> = 87</p><p>(<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x15.png" xlink:type="simple"/></inline-formula>+<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x16.png" xlink:type="simple"/></inline-formula>) = (19 + 87) = 106</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Dewar flask for thermochemical measurements</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57078x17.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Variation of basic constant kb<sup>2</sup>(mole) versus thermohydrobasic constant ∆T ? 18 kb<sup>3</sup> (g) for the determination of the molecular mass of Fluoroboric Acid (HBF<sub>4</sub>)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57078x18.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Thermal constants k determined for Fluoroboric acid (HBF<sub>4</sub> at various concentrations at constant temperature and pressure (25˚C and 1 atm)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Percentage Dilution (v/v%)</th><th align="center" valign="middle" >T<sub>1</sub> ˚C</th><th align="center" valign="middle" >T<sub>2</sub> ˚C</th><th align="center" valign="middle" >T ˚C</th><th align="center" valign="middle" >b</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x19.png" xlink:type="simple"/></inline-formula> (degree∙mol∙g<sup>−1</sup>)</th></tr></thead><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >26.0</td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.009452</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >27.0</td><td align="center" valign="middle" >2.0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.018904</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >3.0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.028355</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >3.0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.028355</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >29.0</td><td align="center" valign="middle" >4.0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.037807</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >30.0</td><td align="center" valign="middle" >5.0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.047170</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Values of basic constants (kb<sup>2</sup>) hydrobasic constants (18kb<sup>2</sup>) and thermohydrobasic constant ( T ? 18kb<sup>3</sup>) for Fluoroboric acid at various concentrations at constant temperature and pressure</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Percentage dilution (v/v%)</th><th align="center" valign="middle" >kb<sup>2</sup> (mole)</th><th align="center" valign="middle" >18 kb<sup>2</sup> (g)</th><th align="center" valign="middle" >T ? 18 kb<sup>3</sup> (g)</th></tr></thead><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.009452</td><td align="center" valign="middle" >0.170</td><td align="center" valign="middle" >0.830</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.018904</td><td align="center" valign="middle" >0.340</td><td align="center" valign="middle" >1.660</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >0.028355</td><td align="center" valign="middle" >0.510</td><td align="center" valign="middle" >2.490</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >0.028355</td><td align="center" valign="middle" >0.510</td><td align="center" valign="middle" >2.490</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.037807</td><td align="center" valign="middle" >0.681</td><td align="center" valign="middle" >3.319</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >0.047170</td><td align="center" valign="middle" >0.849</td><td align="center" valign="middle" >4.151</td></tr></tbody></table></table-wrap><p>For HBF<sub>4</sub>, k = <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x20.png" xlink:type="simple"/></inline-formula> (7)</p><p>where b represents the basicity of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x21.png" xlink:type="simple"/></inline-formula> = 1.</p><p>From thermal constant, the value of basic constant kb<sup>2</sup> and thermohydrobasic constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x22.png" xlink:type="simple"/></inline-formula> − 18kb<sup>3</sup> can be evaluated in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Variation of basic constant kb<sup>2</sup> (mole) versus thermohydrobasic constant ∆T ? 18kb<sup>3</sup> (g) for the determination of the molecular mass of Phosphoric Acid (H<sub>3</sub>PO<sub>4</sub>)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/57078x23.png"/></fig><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Thermal constants for phosphoric acid (H<sub>3</sub>PO<sub>4</sub>) at various dilution at constant temperature and pressure (28˚C and 1atm)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Percentage Dilution (v/v%)</th><th align="center" valign="middle" >T<sub>1</sub> ˚C</th><th align="center" valign="middle" >T<sub>2</sub> ˚C</th><th align="center" valign="middle" >T ˚C</th><th align="center" valign="middle" >b</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x24.png" xlink:type="simple"/></inline-formula> (degree∙mol∙g<sup>−1</sup>)</th></tr></thead><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >32.0</td><td align="center" valign="middle" >4.0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.002924</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >36.0</td><td align="center" valign="middle" >8.0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.005848</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >40.0</td><td align="center" valign="middle" >12.0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.008772</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >45.0</td><td align="center" valign="middle" >17.0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.012427</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >46.0</td><td align="center" valign="middle" >18.0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.013158</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >28.0</td><td align="center" valign="middle" >47.0</td><td align="center" valign="middle" >19.0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.013889</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Values of basic constants (kb<sup>2</sup>), hydrobasic constants (18kb<sup>2</sup>) and thermohydrobasic constant ( T ? 18kb<sup>3</sup>) for phosphoric acid, at various dilution at constant temperature and pressure (28˚C and 1atm)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Percentage dilution (v/v%)</th><th align="center" valign="middle" >kb<sup>2</sup>(mole)</th><th align="center" valign="middle" >18kb<sup>2</sup> (g)</th><th align="center" valign="middle" >T ? 18kb<sup>3</sup> (g)</th></tr></thead><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.02632</td><td align="center" valign="middle" >0.47376</td><td align="center" valign="middle" >2.5789</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.05263</td><td align="center" valign="middle" >0.94734</td><td align="center" valign="middle" >5.1579</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >0.07895</td><td align="center" valign="middle" >1.42110</td><td align="center" valign="middle" >7.7368</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >0.11180</td><td align="center" valign="middle" >0.20124</td><td align="center" valign="middle" >10.9605</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.11840</td><td align="center" valign="middle" >0.21315</td><td align="center" valign="middle" >11.2505</td></tr><tr><td align="center" valign="middle" >60</td><td align="center" valign="middle" >0.12500</td><td align="center" valign="middle" >2.25000</td><td align="center" valign="middle" >12.2499</td></tr></tbody></table></table-wrap></sec><sec id="s3_2_2"><title>3.2.2. Thermal Mechanism of Phosphoric Acid H<sub>3</sub>PO<sub>4 </sub></title><p>The ionisation of H<sub>3</sub>PO<sub>4</sub> catalysed by adsorption of lattice energy is followed by solvation which is an exothermic process, according to the mechanism.</p><disp-formula id="scirp.57078-formula338"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/57078x25.png"  xlink:type="simple"/></disp-formula><p>The thermal constant following the ionisation process is evaluated as follows:</p><p>Mass of solvated cation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x26.png" xlink:type="simple"/></inline-formula> = 57, Mass of anion = <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x27.png" xlink:type="simple"/></inline-formula> = 95</p><p>(<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x28.png" xlink:type="simple"/></inline-formula>+<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x29.png" xlink:type="simple"/></inline-formula>) = (57+95) =152</p><p>For H<sub>3</sub>PO<sub>4</sub>, k = <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x30.png" xlink:type="simple"/></inline-formula> (9)</p><p>where b = 3 because the acid is tribasic.</p><p>Other related constants are evaluated from thermal constant as previously explained [<xref ref-type="bibr" rid="scirp.57078-ref8">8</xref>].<sup> </sup></p></sec><sec id="s3_2_3"><title>3.2.3. Determination of Molecular Mass by Differential Temperature Model (DTM)</title><p>The Differential Temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x31.png" xlink:type="simple"/></inline-formula> for both HBF<sub>4</sub> and H<sub>3</sub>PO<sub>4</sub> are recorded in <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table3">Table 3</xref> respectively. Calculated values of kb<sup>2</sup> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x32.png" xlink:type="simple"/></inline-formula> - 18kb<sup>3</sup> for both acids are recorded in <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table4">Table 4</xref> accordingly.</p><p>The plot of kb<sup>2</sup> (mole) versus <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/57078x33.png" xlink:type="simple"/></inline-formula> - 18kb<sup>3</sup>(g) for HBF<sub>4</sub> produces a straight line from the origin with slope = 0.0114. The slope obtained gives the reciprocal of the molecular mass of the acid. Consequently, by taking the reciprocal of the slope, the molecular mass HBF<sub>4</sub> is obtained as 87.83. The value obtained takes cognizance of experimental error.</p><p>Similar plot for H<sub>3</sub>PO<sub>4</sub> reveals a straight line from the origin with slope = 0.0102 which is the reciprocal of the molecular mass, such that the experimental molecular mass of 98.003 is obtained for H<sub>3</sub>PO<sub>4</sub></p></sec></sec></sec><sec id="s4"><title>4. Conclusion</title><p>The actual molecular masses of HBF<sub>4</sub> and H<sub>3</sub>PO<sub>4</sub> are 87.81 g∙mol<sup>−1</sup> and 97.99 g∙mol<sup>−1</sup> respectively. The result shows that both the propounded hypothesis and the Differential Temperature Model are valid for the determination of the molecular masses of strong acids.</p></sec><sec id="s5"><title>5. Recommendation</title><p>The correspondent author, Dr. I. A. Akpan has propounded a new chemical hypothesis for chemical challenge. He has discovered a thermochemical model for the determination of the relative molecular masses of strong acids. The discovery has added to the list of physical methods available for the determination of molecular properties of substances. Additional chapter has been opened for numerous chemical calculations of molecular properties of strong acids in solution such as thermal constant, basic constant, hydrobasic constant and thermohydrobasic constants. The author expects that the relevant society of chemistry will subject this hypothesis and discovery to test to approve the hypothesis for chemical theory such that a new law credited to the author may come to nobel.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The author is grateful to his 1998 final year project students and 2013 third year students for their assistance in taking measurements. Financial assistance received from my wife is specially acknowledged. Useful discussions and advice received from my mentors, Prof. A. I. Onuchukwu (Professor of Physical and Industrial Chemistry), Prof. A. C. I. Anusiem (Professor of Physical Chemistry) and Prof. A. A. Ayuk (Professor of Theoretical and Quantum Chemistry) are also acknowledged.</p></sec><sec id="s7"><title>Cite this paper</title><p>I. A. Akpan, (2015) Determination of Molecular Mass of Strong Acids by Differential Temperature Model (DTM) Using H<sub>3</sub>PO<sub>4</sub> and HBF<sub>4</sub> for Classical Demonstration. Journal of Materials Science and Chemical Engineering,03,41-47. doi: 10.4236/msce.2015.36007</p></sec></body><back><ref-list><title>References</title><ref id="scirp.57078-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ebbing, D.D. and Gammon, S.D. (1999) General Chemistry. 6th Edition, Houghton Miffin Company; Boston, New York, 105, 320, 485.</mixed-citation></ref><ref id="scirp.57078-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Sharma, K.K. and Sharma, L.K. (1999) A Textbook of Physical Chemistry. 4th Rev. 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