<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2017.52034</article-id><article-id pub-id-type="publisher-id">JAMP-74192</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Solutions of the Exponential Equation &lt;i&gt;y&lt;/i&gt;&lt;sup&gt;&lt;i&gt;x/y&lt;/i&gt;&lt;/sup&gt; = &lt;i&gt;x&lt;/i&gt; or ln&lt;i&gt;x&lt;/i&gt;/&lt;i&gt;x&lt;/i&gt; = ln&lt;i&gt;y&lt;/i&gt;/&lt;i&gt;y&lt;/i&gt; and Fine Structure Constant
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sabaratnasingam</surname><given-names>Gnanarajan</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>CSIRO Manufacturing, Lindfield, Australia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>15</day><month>02</month><year>2017</year></pub-date><volume>05</volume><issue>02</issue><fpage>386</fpage><lpage>391</lpage><history><date date-type="received"><day>29,</day>	<month>November</month>	<year>2016</year></date><date date-type="rev-recd"><day>14,</day>	<month>February</month>	<year>2017</year>	</date><date date-type="accepted"><day>17,</day>	<month>February</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  In this paper, we study the equation of the form of 
  <img src="Edit_d7133fbc-584e-4cbe-8ea7-a7f32e6cc21b.bmp" alt="" /> which can also be written as 
  <img src="Edit_4d962a78-f87a-46d7-8412-effc52fb18a7.bmp" alt="" /> . Apart from the trivial solution 
  <em>x</em> = 
  <em>y</em>, a non-trivial solution can be expressed in terms of Lambert 
  <em>W</em> function as 
  <img src="Edit_5c8ec8d6-a9a7-4351-938e-c794ad0ed17b.bmp" alt="" /> . For 
  <em>y</em> &gt; e, the solutions of 
  <em>x</em> are in-between 1 and e. For integer 
  <em>y</em> values between 4 and 12, the solutions of 
  <em>x</em> written in base 
  <em>y</em> are in-between 1.333 and 1.389. The non-trivial solutions of the equations 
  <img src="Edit_6630fc90-4687-4985-9989-d915c1ab47be.bmp" alt="" /> and 
  <img src="Edit_d94e64aa-9691-4ce3-b89a-efa2e958cfe5.bmp" alt="" /> written in base 
  <em>y</em> are exactly one and two orders higher respectively than the solutions of the equation 
  <img src="Edit_851ed03d-e07f-4538-9348-0da3ed1f9518.bmp" alt="" /> . If 
  <em>y</em> = 10, the rounded nontrivial solutions for the three equations are 1.3713, 13.713 and 137.13, 
  <em>i.e</em>
  <em>.</em> 10
  <sup>0.13713</sup> = 1.3713. Further, ln(1.3713)/1.3713 = 0.2302 and 
  <em>W</em>(-0.2302) = -2.302. The value 137.13 is very close to the fine structure constant value of 137.04 within 0.1%.
 
</html></p></abstract><kwd-group><kwd>Exponential Equation</kwd><kwd> Lambert W Function</kwd><kwd> Fine Structure Constant</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Lambert W function is a transcendental function [<xref ref-type="bibr" rid="scirp.74192-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.74192-ref2">2</xref>] which has applications in many areas of science which include QCD renormalisation, Planck’s spectral distribution law, water movement in soil and population growth [<xref ref-type="bibr" rid="scirp.74192-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.74192-ref8">8</xref>] .</p><p>Considering the equation</p><p>y x y = x (1)</p><p>The Equation (1) can be written as</p><p>log y x = x y (2)</p><p>Converting the Equation (2) in terms of natural log gives</p><p>ln x x = ln y y (3)</p><p>Equations ((1)-(3)) have a trivial solution x = y , but they also have a non- trivial solution.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows the plot of the function ln x x . The plot indicates that, for any value of the function ln x x in the range of 1 to infinity, it has two different solutions of x . i.e. for any value of y between 1 and infinity, a non-trivial solution of x can be found. The plot also indicates that, at y = e , there is only one solution x = e and ln x x = 1 / e = 0.3679 (rounded). For any value of y between e and infinity, a solution for x can be found in-between 1 and e.</p><p>The solution of Equations ((1)-(3)) can be written in terms of Lambert W function [<xref ref-type="bibr" rid="scirp.74192-ref9">9</xref>] ,</p><p>y = W [ − ln ( x ) x ] [ − ln ( x ) x ] (4)</p><p>If x = e , y = W [ − 1 e ] [ − 1 e ] and according to Dence [<xref ref-type="bibr" rid="scirp.74192-ref2">2</xref>] , W [ − 1 e ] = − 1 , hence y = e , which is the result obtained graphically and numerically.</p><p>Some variations of Equation (1) are:</p><p>y x / y 2 = x / y (5)</p><p>y x / y 3 = x / y 2 (6)</p><p>Equation (5) can be written as</p><p>ln x ln y = x y 2 + 1 (7)</p><p>Equation (6) can be written as</p><p>ln x ln y = x y 3 + 2 (8)</p><p>Equation (5) and Equation (6) have trivial solutions of x = y 2 and x = y 3 respectively.</p></sec><sec id="s2"><title>2. Non-Trivial Solutions</title><p>If y = 10 then Equation (1) becomes 10 ( x / 10 ) = x and x = 1.3713 (rounded) is the nontrivial solution, i.e. 10<sup>0.13713</sup> = 1.3713 and</p><p>ln x x = ln y y = 0.2302</p><p>If y = 10 then Equation (5) and Equation (6) become 10 ( x / 100 ) = x / 10 and 10 ( x / 1000 ) = x / 100 respectively and their solutions are 13.713 (rounded) and 137.13 (rounded) respectively. These solutions are exactly one and two orders larger than the solution of Equation (1).</p><p>Also if x = 1.3713 and y = 10 , Equation (4) gives</p><p>W [ − ln ( 1.3713 ) 1.3713 ] = 10 [ − ln ( 1.3713 ) 1.3713 ]</p><p>Hence W ( − 0.2302 ) = − 2.302</p><p>For the range of integer y values of 4 to 12, the non-trivial solutions for x of Equations ((1), (5) and (6)) were obtained using iterative method. The solutions of x are written in base 10 and in base y (<xref ref-type="table" rid="table1">Table 1</xref>). Plots of y vs x with x in base 10 and in base y are shown in Figures 2-4 respectively.</p></sec><sec id="s3"><title>3. Conclusions</title><p>The non-trivial solutions of Equations ((1), (5) and (6)) written in base y, differ exactly by one order. For y values in the range of 4 to 12, the solutions of Equation (6) written in base y are in the range of 133.33 to 138.99.</p><p>When y = 10 , the rounded nontrivial solutions for Equation (1), Equation (5) and Equation (6) are 1.3713, 13.713 and 137.13, i.e. 10<sup>0.13713</sup> = 1.3713, ln ( 1.3713 ) / 1.3713 = 0.2302 and W ( − 0.2302 ) = − 2.302 , i.e. for the argument values of 1.3713 and −0.2302, the function values are exactly one order higher. To our knowledge, these results were not reported before.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Rounded non-trivial solutions for x of Equations ((1), (5) and (6)) for y values from 4 to 12 are written in base 10 and base y</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >y</th><th align="center" valign="middle"  colspan="2"  >Solutions of Equation (1)</th><th align="center" valign="middle"  colspan="2"  >Solutions of Equation (5)</th><th align="center" valign="middle"  colspan="2"  >Solutions of Equation (6)</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >In base 10</td><td align="center" valign="middle" >In base y</td><td align="center" valign="middle" >In base 10</td><td align="center" valign="middle" >In base y</td><td align="center" valign="middle" >In base 10</td><td align="center" valign="middle" >In base y</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >1.3122</td><td align="center" valign="middle" >1.389</td><td align="center" valign="middle" >15.75</td><td align="center" valign="middle" >13.89</td><td align="center" valign="middle" >189.0</td><td align="center" valign="middle" >138.9</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >1.3389</td><td align="center" valign="middle" >1.380</td><td align="center" valign="middle" >14.73</td><td align="center" valign="middle" >13.80</td><td align="center" valign="middle" >162.0</td><td align="center" valign="middle" >138.0</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >1.3713</td><td align="center" valign="middle" >1.371</td><td align="center" valign="middle" >13.71</td><td align="center" valign="middle" >13.71</td><td align="center" valign="middle" >137.1</td><td align="center" valign="middle" >137.1</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >1.4114</td><td align="center" valign="middle" >1.363</td><td align="center" valign="middle" >12.70</td><td align="center" valign="middle" >13.63</td><td align="center" valign="middle" >114.3</td><td align="center" valign="middle" >136.3</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >1.4625</td><td align="center" valign="middle" >1.355</td><td align="center" valign="middle" >11.70</td><td align="center" valign="middle" >13.55</td><td align="center" valign="middle" >93.6</td><td align="center" valign="middle" >135.5</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1.5301</td><td align="center" valign="middle" >1.350</td><td align="center" valign="middle" >10.71</td><td align="center" valign="middle" >13.50</td><td align="center" valign="middle" >75.0</td><td align="center" valign="middle" >135.0</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1.6242</td><td align="center" valign="middle" >1.343</td><td align="center" valign="middle" >9.75</td><td align="center" valign="middle" >13.42</td><td align="center" valign="middle" >58.5</td><td align="center" valign="middle" >134.3</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1.7649</td><td align="center" valign="middle" >1.340</td><td align="center" valign="middle" >8.82</td><td align="center" valign="middle" >13.40</td><td align="center" valign="middle" >44.1</td><td align="center" valign="middle" >1340</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >1.333..</td><td align="center" valign="middle" >8.00</td><td align="center" valign="middle" >13.33..</td><td align="center" valign="middle" >32.0</td><td align="center" valign="middle" >133.3</td></tr></tbody></table></table-wrap><p>The trivial solutions of Equations ((1), (5) and (6)) can be written as 10, 100 and 1000 in base y for any y value.</p><p>The non-trivial solution for x of Equation (6), 137.128857 is within 0.1% of the reciprocal value of the atomic fine structure constant α − 1 , 137.0359991.</p></sec><sec id="s4"><title>4. Possible Connection to Fine Structure Constant</title><p>Allen suggested that m e / M p ~ 10 α 2 [<xref ref-type="bibr" rid="scirp.74192-ref10">10</xref>] however for the current values of m e / M p and α , the relationship is m e / M p = 10.227 α 2 . Edward Teller suggested ln T 0 3 / 2 = α − 1 , where T o is the age of the universe [<xref ref-type="bibr" rid="scirp.74192-ref11">11</xref>] . There could be a connection between Equations ((1) to (8)) and α − 1 .</p></sec><sec id="s5"><title>Cite this paper</title><p>Gnanarajan, S. (2017) Solutions of the Exponential Equation or and Fine Structure Constant. Journal of Applied Mathematics and Physics, 5, 386-391. https://doi.org/10.4236/jamp.2017.52034</p></sec></body><back><ref-list><title>References</title><ref id="scirp.74192-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Dence, T.P. (2013) A Brief Look into the Lambert W Function. Applied Mathematics, 4, 887. https://doi.org/10.4236/am.2013.46122</mixed-citation></ref><ref id="scirp.74192-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Kalman, D. (2001) A Generalized Logarithm for Exponential-Linear Equations. College Mathematics Journal, 32, 2-14. https://doi.org/10.2307/2687213</mixed-citation></ref><ref id="scirp.74192-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Corless, R.M., Gonnet, G.H., Hare, D.E., Jeffrey, D.J. and Knuth, D.E. (1996) On the Lambert W Function. Advances in Computational Mathematics, 5, 329-359. https://doi.org/10.1007/BF02124750</mixed-citation></ref><ref id="scirp.74192-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Barry, D.A., et al. (2000) Analytical Approximations for Real Values of the Lambert W-Function. Mathematics and Computers in Simulation, 53, 95-103. https://doi.org/10.1016/S0378-4754(00)00172-5</mixed-citation></ref><ref id="scirp.74192-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Valluri, S.R., Jeffrey, D.J. and Corless, R.M. (2000) Some Applications of the Lambert W Function to Physics. Canadian Journal of Physics, 78, 823-831.</mixed-citation></ref><ref id="scirp.74192-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Barry, D.A., et al. (1993) A Class of Exact Solutions for Richards’ Equation. Journal of Hydrology, 142, 29-46. https://doi.org/10.1016/0022-1694(93)90003-R</mixed-citation></ref><ref id="scirp.74192-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Jain, A. and Kapoor, A. (2004) Exact Analytical Solutions of the Parameters of Real Solar Cells Using Lambert W-Function. Solar Energy Materials and Solar Cells, 81, 269-277. https://doi.org/10.1016/j.solmat.2003.11.018</mixed-citation></ref><ref id="scirp.74192-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Scott, T.C., Mann, R. and Martinez II, R.E. (2006) General Relativity and Quantum Mechanics: Towards a Generalization of the Lambert W Function. A Generalization of the Lambert W Function. Applicable Algebra in Engineering, Communication and Computing, 17, 41-47. https://doi.org/10.1007/s00200-006-0196-1</mixed-citation></ref><ref id="scirp.74192-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Weisstein, E.W. (2016) Lambert W-Function. From MathWorld—A Wolfram Web Resource. http://mathworld.wolfram.com/LambertW-Function.html</mixed-citation></ref><ref id="scirp.74192-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Allen, H.S. (1915) Numerical Relations between Electronic and Atomic Constants. Proceedings of the Physical Society (London), 27, 425-431. https://doi.org/10.1088/1478-7814/27/1/331</mixed-citation></ref><ref id="scirp.74192-ref11"><label>11</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Kragh</surname><given-names> H. </given-names></name>,<etal>et al</etal>. (<year>2003</year>)<article-title>Magic Number: A Partial History of the Fine-Structure Constant</article-title><source> Archive for History of Exact Sciences</source><volume> 57</volume>,<fpage> 395</fpage>-<lpage>431</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref></ref-list></back></article>