<?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">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2023.142011</article-id><article-id pub-id-type="publisher-id">JMP-122726</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>
 
 
  A Fine-Structure Constant Can Be Explained Using the Electrochemical Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tomofumi</surname><given-names>Miyashita</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>Miyashita Clinic, Osaka, Japan</addr-line></aff><pub-date pub-type="epub"><day>18</day><month>01</month><year>2023</year></pub-date><volume>14</volume><issue>02</issue><fpage>160</fpage><lpage>170</lpage><history><date date-type="received"><day>21,</day>	<month>December</month>	<year>2022</year></date><date date-type="rev-recd"><day>28,</day>	<month>January</month>	<year>2023</year>	</date><date date-type="accepted"><day>31,</day>	<month>January</month>	<year>2023</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>
 
 
  We proposed an empirical equation for a fine-structure constant: 
  <inline-formula><inline-graphic xlink:href="dit_3958e503-0050-4f84-91b8-6297158ecb33.png" xlink:type="simple"/></inline-formula>. Then, 
  <inline-formula><inline-graphic xlink:href="dit_756c639d-7cbc-4803-9740-602134cbf846.png" xlink:type="simple"/></inline-formula>. where 
  <em>m</em>
  <sub><em>p</em></sub> and 
  <em>m</em>
  <sub><em>e</em></sub> are the rest mass of a proton and the rest mass of an electron, respectively. In this report, using the electrochemical method, we proposed an equivalent circuit. Then, we proposed a refined version of our own old empirical equations about the electromagnetic force and gravity. Regarding the factors of 9/2 and π, we used 3.132011447 and 4.488519503, respectively. The calculated values of 
  <em>T</em>
  <sub><em>c</em></sub> and 
  <em>G</em> are 2.726312 K and 6.673778 &#215; 10
  <sup>-11</sup> (m
  <sup>3</sup>
  &amp;sdot;kg
  <sup>-1</sup>
  &amp;sdot;s
  <sup>-2</sup>).
 
</p></abstract><kwd-group><kwd>Fine-Structure Constant</kwd><kwd> Electrochemical Method</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The symbol list is shown in Section 2. We discovered Equation 1 [<xref ref-type="bibr" rid="scirp.122726-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.122726-ref2">2</xref>] and [<xref ref-type="bibr" rid="scirp.122726-ref3">3</xref>], which appeared very simple. Equations (1)-(3) were mathematically connected [<xref ref-type="bibr" rid="scirp.122726-ref3">3</xref>]. However, we could not establish the background theory. Furthermore, there appeared to be dimension mismatch problems.</p><p>G m p 2 h c = 4.5 2 &#215; k T c 1   kg &#215; c 2 (1)</p><p>G m p 2 ( e 2 4 π ε 0 ) = 4.5 2 π &#215; m e e &#215; h c &#215; ( 1   C J ⋅ m &#215; 1 1   kg ) (2)</p><p>m e c 2 e &#215; ( e 2 4 π ε 0 ) = π k T c &#215; ( 1   J ⋅ m C ) (3)</p><p>These equations have small errors of approximately 10<sup>−3</sup> and 10<sup>−4</sup> [<xref ref-type="bibr" rid="scirp.122726-ref3">3</xref>]. We attempted to reduce the errors in the previous reports by changing the factors of 4.5, π and T<sub>c</sub> [<xref ref-type="bibr" rid="scirp.122726-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.122726-ref5">5</xref>]. Regarding the factors of 9/2 and π, we used 4.48870 and 3.13189, respectively. Then, the errors became smaller than 10<sup>−5</sup>.</p><p>Then, 4.48870 and 3.13189 Ω are connected as follows.</p><p>m p m e = 1 4.4887 &#215; 3.13189   Ω q m e (4)</p><p>Next, we discovered the empirical equation for a fine-structure constant [<xref ref-type="bibr" rid="scirp.122726-ref6">6</xref>].</p><p>137.0359991 = 136.0113077 + 1 3 &#215; 13.5 + 1 (5)</p><p>13.5 &#215; 136.0113077 = 1836.152654 = m p m e (6)</p><p>To explain 136.0113077, we proposed the following values.</p><p>3.131777037 ( Ω ) = R k ( 3 &#215; 136.0113077 ) 1.5 (7)</p><p>4.488855463 = 136.0113077 &#215; 4 27 (8)</p><p>However, Equations (7) and (8) cannot be compatible with Equations (5) and (6). Main purpose of this report is to improve the compatibility between these equations.</p><p>The remainder of the paper is organized as follows. In Section 2, we show the symbol list. In Section 3, we reconsider the deviation from the factors of 9/2 and π. In Section 4, using the electrochemical method, we propose the equivalent circuit for the fine structure constant. In Section 5, we refine our three equations. In Section 6, general discussions are presented, which are mainly about the UNIT.</p></sec><sec id="s2"><title>2. Symbol List (These Values Were Obtained from Wikipedia)</title><p>G gravitational constant: 6.6743 &#215; 10<sup>−11</sup> (m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup>)</p><p>(we used the compensated value 6.673778 &#215; 10<sup>−11</sup> in this report)</p><p>T<sub>c</sub> temperature of the cosmic microwave background: 2.72548 (K)</p><p>(we used the compensated value 2.726312 K in this report)</p><p>k Boltzmann constant: 1.380649 &#215; 10<sup>−23</sup> (J K<sup>−1</sup>)</p><p>c speed of light: 299,792,458 (m/s)</p><p>h Planck constant: 6.62607015 &#215; 10<sup>−34</sup> (Js)</p><p>ε<sub>0</sub> electric constant: 8.8541878128 &#215; 10<sup>−12</sup> (N∙m<sup>2</sup>∙C<sup>−2</sup>)</p><p>μ<sub>0</sub> magnetic constant: 1.25663706212 &#215; 10<sup>−6</sup> (N∙A<sup>−2</sup>)</p><p>e electric charge of one electron: −1.602176634 &#215; 10<sup>−19</sup> (C)</p><p>q<sub>m</sub> magnetic charge of one magnetic monopole: 4.13566770 &#215; 10<sup>−15</sup> (Wb)</p><p>(this value is only a theoretical value, q<sub>m</sub> = h/e)</p><p>m<sub>p</sub> rest mass of a proton: 1.6726219059 &#215; 10<sup>−27</sup> (kg)</p><p>(we used the compensated value 1.672621923 &#215; 10<sup>−27</sup> kg in this report)</p><p>m<sub>e </sub>rest mass of an electron: 9.1093837 &#215; 10<sup>−31</sup> (kg)</p><p>Rk von Klitzing constant: 25812.80745 (Ω)</p><p>Z<sub>0</sub> wave impedance in free space: 376.730313668 (Ω)</p><p>α fine-structure constant: 1/137.035999081</p></sec><sec id="s3"><title>3. Reconsideration for the Deviation from 4.5 and π</title><p>In this section, we reconsider the deviation from 4.5 and π. We notice that 4.48870 and 3.1319 can be rewritten as follows.</p><p>4.48870 = q m c ( m p m e + 1 + 1 3.854377987 ) m p c 2 (9)</p><p>For example, Equation (9) can be made sure as follows.</p><p>4.48870 = 4.13567 &#215; 10 − 15 &#215; 299792458 ( 1836.15 + 1 + 1 3.854377987 ) &#215; 1.50328 &#215; 10 − 10 (10)</p><p>3.13189   Ω = ( m p m e + 1 + 1 3.854377987 ) m e c 2 e c (11)</p><p>Next, the deviation from 4.5 and π can be explained as follows.</p><p>4.5 π &#215; 3.13189 4.48870 = 0.999421207 ≐ 1 (12)</p><p>Regarding the values for 3.131777037 and 4.88855463,</p><p>4.488855463 = q m c ( m p m e + 1 + 1 5.106991198 ) m p c 2 (13)</p><p>3.1317770   Ω = ( m p m e + 1 + 1 5.106991198 ) &#215; m e c 2 e c (14)</p><p>Next, the deviation from 4.5 and π can be explained as follows.</p><p>4.5 π &#215; 3.1317770 4.488855463 = 0.999350548 ≐ 1 (15)</p><p>Therefore, using X, the deviation should be rewritten as follows.</p><p>3.1317770 = ( m p m e + 1 + 1 X ) &#215; m e c 2 e c (16)</p><p>4.488855463 = q m c ( m p m e + 1 + 1 X ) m p c 2 (17)</p><p>The value of 4.5 is from the degree of freedom as 9/2. Therefore, 4.488855 should be dimensionless.</p><p>( m p m e + 1 + 1 X ) = q m c 4.488855463 &#215; m p c 2 = Wb ⋅ m / s J = Wb ⋅ m J ⋅ s = m C (18)</p><p>The correct value of X and the UNIT will be discussed in detail in a later section.</p></sec><sec id="s4"><title>4. Equivalent Circuit of the Fine Structure Constant with the Electrochemical Method</title><sec id="s4_1"><title>4.1. Explanation Using the Transference Number</title><p>For convenience, Equations (5) and (6) are rewritten as follows:</p><p>137.0359991 = 136.0113077 + 1 + 1 3 &#215; 13.5 (19)</p><p>13.5 &#215; 136.0113077 = 1836.152654 = m p m e (20)</p><p>We strongly believe that the fine structure constant should be explained by the transference number [<xref ref-type="bibr" rid="scirp.122726-ref7">7</xref>]. According to Rickert [<xref ref-type="bibr" rid="scirp.122726-ref8">8</xref>],</p><p>J 1 = L 11 g r a d η 1 T + L 12 g r a d η 2 T (21)</p><p>J 2 = L 21 g r a d η 1 T + L 22 g r a d η 2 T (22)</p><p>whereJ<sub>1</sub> and J<sub>2</sub> are the current densities of two different carriers; η<sub>1</sub>and η<sub>2</sub>are the electrochemical potentials of the two different carriers; L<sub>11</sub>, L<sub>12</sub>, L<sub>21</sub>, and L<sub>22</sub> are Onsagar coefficients.</p><p>In the area of solid-state ionics, Rickert proposed the following equation.</p><p>L 12 = L 21 = 0 (23)</p><p>Then, the transference number (t<sub>1</sub> and t<sub>2</sub>) can be explained as follows.</p><p>t 1 = R 2 R 1 + R 2 (24)</p><p>t 2 = R 1 R 1 + R 2 (25)</p><p>where R<sub>1</sub> and R<sub>2</sub> are different resistance values. Next, we consider the following equation.</p><p>( V 1 V 2 ) = Z 1 &#215; ( 1 − 1 81 − 1 81 136.0113077 ) ( I 1 I 2 ) (26)</p><p>where V<sub>1</sub> and V<sub>2</sub> are the voltage losses due to different carriers; I<sub>1</sub> and I<sub>2</sub> are the currents due to different carriers; Z<sub>1</sub> is the resistance, which will be explained later. In Equation (26), using an inverse of the matrix, Onsager coefficients can be obtained. Because the derivation is too complex to show here, we have:</p><p>V 1 = Z 1 &#215; I 1 − Z 1 81 &#215; I 2 (27)</p><p>V 2 = − Z 1 81 &#215; I 1 + Z 1 &#215; 136.0113077 &#215; I 2 (28)</p><p>Next, we consider the following situation, which implies the open circuit condition.</p><p>I 1 = − I 2 (29)</p><p>Therefore, the theoretical voltage (V<sub>th</sub>) is,</p><p>V t h = V 1 − V 2 = Z 1 &#215; ( 136.0113077 + 1 + 1 3 &#215; 13.5 ) &#215; I 1 (30)</p><p>In Equation (30), −V<sub>2</sub> is the voltage loss due to the opposite drift (not diffusion) current (I<sub>2</sub>). Thus, in Equation (30), we obtained the value of a fine-structure constant. For convenience, Equation (5) is rewritten as follows.</p><p>137.0359991 = 136.0113077 + 1 + 1 3 &#215; 13.5 (31)</p><p>Next, we define the interaction voltage (V<sub>3</sub>) as follows.</p><p>V 3 = Z 1 81 &#215; I 1 (32)</p><p>The transference number for the small voltage loss (V<sub>1</sub>) is</p><p>t 1 = V 3 − V 2 V 1 − V 2 = Z 1 &#215; ( 136.0113 + 1 3 &#215; 13.5 ) &#215; I 1 Z 1 &#215; ( 136.0113 + 1 + 1 3 &#215; 13.5 ) &#215; I 1 = 136.0359991 137.0359991 (33)</p><p>Therefore, the interaction coefficient is</p><p>1 − t 1 = 1 − 136.0359991 137.0359991 = 1 137.0359991 = 1 α (34)</p><p>The transference number for the large voltage loss (V<sub>2</sub>) is</p><p>t 2 = V 1 − V 3 V 1 − V 2 = Z 1 &#215; I 1 Z 1 &#215; ( 136.0113 + 1 + 1 3 &#215; 13.5 ) &#215; I 1 = 1 137.0359991 (35)</p><p>Equation 35 means the strong interaction. From Equations 33 and 35, V<sub>3</sub> should be transferred from the carriers with a large voltage loss (V<sub>2</sub>) to those with the small voltage loss (V<sub>1</sub>). From Equations (33) and (35),</p><p>t 1 + t 2 = 136.0359991 137.0359991 + 1 137.0359991 = 1 (36)</p></sec><sec id="s4_2"><title>4.2. Determination of the Important Resistance</title><p>The total resistance is Z<sub>0</sub>, so the large resistance (Z<sub>2</sub>) should be</p><p>Z 2 = Z 0 &#215; 137.035999081 = 2 R k (37)</p><p>The small resistance is</p><p>Z 1 = Z 0 &#215; 137.035999081 136.0113077 = 2 R k 136.0113077 = 379.5685505   Ω (38)</p><p>We discover Z<sub>1</sub> as follows:</p><p>Z 1 = 3 3 &#215; q m e &#215; m e m p = 27 &#215; 25812.807459 1836.152654 = 379.5685505   Ω (39)</p><p>Therefore, our argument is not a coincidence. From Equation (32), the interaction resistance (Z<sub>3</sub>) should be</p><p>Z 3 = Z 1 81 = 1 3 &#215; q m e &#215; m e m p = 4.686031487   Ω (40)</p><p>Consequently, Equation (26) can be rewritten as follows,</p><p>( V 1 V 2 ) = ( Z 1 − Z 3 − Z 3 Z 2 ) ( I 1 I 2 ) (26b)</p></sec><sec id="s4_3"><title>4.3. Suitable Charge and Equivalent Circuit</title><p>We are discussing the equivalent circuit at the quantum level. Clearly, one charge is an electron. However, it is difficult to search for the other charge. The suitable charge is</p><p>q m Z 1 = 1.08957070 &#215; 10 − 17 ( C ) = 68.00565 &#215; e (41)</p><p>Because q<sub>m</sub> has never been observed, the charge + q m Z 1 should be the set of an antiparticle − q m Z 1 , which may be related to quarks. Then, we propose the equivalent circuit in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The total charge is</p><p>2 q m Z 1 = 136.0113 &#215; e (42)</p><p>When the charge + q m Z 1 cannot be realized at the low energy level, it cannot be observed as the mass.</p><p>The direction of + q m Z 1 is opposite to the electrical field, which may prevent the increase of the electrical field.</p></sec></sec><sec id="s5"><title>5. Our Refined Three Empirical Equations</title><sec id="s5_1"><title>5.1. The Most Suitable Value for X</title><p>For convenience, Equations (5) and (6) are rewritten as follows:</p><p>137.0359991 = 136.0113077 + 1 + 1 3 &#215; 13.5 (43)</p><p>13.5 &#215; 136.0113077 = 1836.152654 = m p m e (44)</p><p>For convenience, Equations (16) and (17) are rewritten as follows:</p><p>3.1317770   Ω = ( m p m e + 1 + 1 X ) &#215; m e c 2 e c (45)</p><p>4.488855463 = q m c ( m p m e + 1 + 1 X ) m p c 2 (46)</p><p>Then, we notice that X should be 3. Therefore,</p><p>3.132011447   Ω = ( m p m e + 1 + 1 3 ) m e c 2 e c = ( m p m e + 4 3 ) m e c 2 e c = 1837.48599 &#215; m e c 2 e c (47)</p><p>4.488519503 = q m c ( m p m e + 1 + 1 3 ) m p c 2 = q m c ( m p m e + 4 3 ) m p c 2 = q m c 1837.48599 &#215; m p c 2 (48)</p><p>Here, 4/3m<sub>e</sub>c<sup>2</sup> is well known and has been discussed by Feynman. Next, the deviation from 4.5 and π can be explained as follows.</p><p>4.5 π &#215; 3.132011447 4.488519503 = 0.999500154 ≐ 1 (49)</p></sec><sec id="s5_2"><title>5.2. Determination of the Important Resistance</title><p>1 m p m e + 1 + 1 3 = 1 1837.485988 appears to be a transference number. The total resistance (Z<sub>5</sub>), small resistance (Z<sub>6</sub>), large resistance (Z<sub>7</sub>) and interaction resistance (Z<sub>8</sub>) can be defined.</p><p>Z 5 = 2 &#215; q m e &#215; 1 m p m e + 4 3 = 28.095787   Ω (50)</p><p>Z 6 = 2 &#215; q m e &#215; m e m p = 2 R k 1836.152654 = 28.11618892   Ω (51)</p><p>Z 7 = 2 &#215; q m e = 2 R k (52)</p><p>Z 8 = 13.5 81 &#215; Z 6 = 13.5 81 &#215; 2 &#215; q m e &#215; m e m p = 1 3 &#215; q m e &#215; m e m p = 4 .686031487   Ω = Z 3 (53)</p><p>Consequently, Z<sub>8</sub> is equal to Z<sub>3</sub>.</p></sec><sec id="s5_3"><title>5.3. Our Refined Three Empirical Equations</title><p>We use 2.726312143 K instead of 2.72548 K. We use 6.6737778665 &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup> instead of 6.6743 &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup>. Equation (1) is refined as follows:</p><p>G m p 2 h c = 4.488519503 2 k T c 1   kg &#215; c 2 (54)</p><p>G m p 2 h c = 6.6737778665 &#215; 10 − 11 &#215; ( 1.6726219 &#215; 10 − 27 ) 2 6 .626070 &#215; 10 − 34 &#215; 2.9979246 &#215; 10 8 = 9.39919318 &#215; 10 − 40 (55)</p><p>4.488519503 2 k T c 1   kg &#215; c 2 = 4.488519503 2 &#215; 1.3806490 &#215; 10 − 23 &#215; 2.726312143 ( 2.9979246 &#215; 10 8 ) 2 = 9.39919318 &#215; 10 − 40 (56)</p><p>Equation (55) is equal to Equation (56). Therefore, the compensation method is perfect. Next, Equation (2) is refined as follows:</p><p>G m p 2 ( e 2 4 π ε 0 ) = 4.488519503 2 &#215; 3.132011447   Ω &#215; m e e &#215; h c &#215; ( 1   C ⋅ Ω J ⋅ m &#215; 1 1   kg ) (57)</p><p>G m p 2 e 2 4 π ε 0 = 6.6737778665 &#215; 10 − 11 &#215; ( 1.672621923 &#215; 10 − 27 ) 2 ( 1.60217663 &#215; 10 − 19 ) 2 4 π &#215; 8.8541878 &#215; 10 − 12 = 8.0929175 &#215; 10 − 37 (58)</p><p>4.488519503 2 &#215; 3.132011447 &#215; m e e &#215; h c = 4.488519503 &#215; 9.10938 &#215; 10 − 31 &#215; 1.986446 &#215; 10 − 25 2 &#215; 3.132011447 &#215; 1.602177 &#215; 10 − 19 = 8.0929175 &#215; 10 − 37 (59)</p><p>Equation (58) is equal to Equation (59). Therefore, the compensation method is perfect. Next, Equation (3) is refined as follows:</p><p>m e c 2 e &#215; ( e 2 4 π ε 0 ) = 3.132011447   Ω &#215; k T c &#215; ( 1   J ⋅ m C ⋅ Ω ) (60)</p><p>m e c 2 e &#215; ( e 2 4 π ε 0 ) = 9.10938 &#215; 10 − 31 &#215; ( 2.9979246 &#215; 10 8 ) 2 &#215; ( 1.60217663 &#215; 10 − 19 ) 2 1.60217663 &#215; 10 − 19 &#215; 4 π &#215; 8.8541878 &#215; 10 − 12 = 1.1789142 &#215; 10 − 22 (61)</p><p>3.132011447 &#215; k T c = 3.132011447 &#215; 1.3806490 &#215; 10 − 23 &#215; 2.726312143 = 1.1789142 &#215; 10 − 22 (62)</p><p>Equation (61) is equal to Equation (62). Therefore, the compensation method is perfect.</p></sec></sec><sec id="s6"><title>6. Discussion</title><sec id="s6_1"><title>6.1. Dimension Mismatch Problem</title><p>For convenience, Equation (54) is rewritten as follows:</p><p>G m p 2 h c = 4.488519503 2 k T c 1   kg &#215; c 2 (63)</p><p>The value of 4.488519503 is the deviation from the degree of freedom 9/2, which is dimensionless.</p><p>Therefore, there are no dimension mismatch problems. For convenience, Equation (56) is rewritten as follows:</p><p>m e c 2 e &#215; ( e 2 4 π ε 0 ) = 3.132011447 Ω &#215; k T c &#215; ( J ⋅ m C ⋅ Ω = A m ) (64)</p><p>In Equation (64), there remains the unexplained UNIT as “Am”.</p><p>m e c 2 4 π ε 0 c = 3.132011447   Ω &#215; k T c &#215; A m e c (65)</p><p>Therefore,</p><p>Z 0 &#215; m e c 2 3.132011447   Ω &#215; 4 π = k T c &#215; A m e c (66)</p><p>In Equation (66), the UNITs of 1 J and 1 C can be separately defined. However,</p><p>1   J = 6.241509 &#215; 10 18   eV = 6.241509 &#215; 10 18 e c &#215; V c (67)</p><p>where V c is the unit of the electromagnetic four potential. Therefore, A m e c may be Faraday constant at the quantum level. The proof is difficult and will be published in a future report. From Equations (47) and (65), we have</p><p>k T c e 2 c 4 π ε 0 &#215; ( A m ) = 1 ( m p m e + 4 3 ) ( C m ) = 1 1837.485988 ( C m ) (68)</p><p>Next, the fine structure constant (α) is</p><p>e 2 4 π ε 0 = h c &#215; α 2 π (69)</p><p>From Equations (68) and (69),</p><p>k T c h c 2 = 1 ( m p m e + 4 3 ) &#215; α 2 π &#215; ( 1 A m ) = 1 1837.485988 &#215; α 2 π &#215; ( s m 2 ) = 6.3206454 E − 07 (70)</p><p>In Equations (68) and (70), from different coordinate systems, kT<sub>c</sub> should be changed because the unit C/m is not Lorentz invariant. Therefore, from Equation (63), G is not Lorentz invariant.</p></sec><sec id="s6_2"><title>6.2. Yukawa Potential</title><p>According to the advanced Wagner model, the diffusion time for mixed electronic and ionic currents should exponentially decrease with distance [<xref ref-type="bibr" rid="scirp.122726-ref9">9</xref>]. When the diffusion time for mixed electrons and quark flux should exponentially decrease with distance, the Yukawa potential can be explained.</p></sec><sec id="s6_3"><title>6.3. Consideration of the Degree of Freedom inside Electrons</title><p>We have never discussed the spin of electrons. In Equation (64), the number 3.132011447 Ω is the deviation from π. We believe that π is related to the spin of the electron. Angrick et al. have confirmed that the spin of electrons cannot be thermodynamically ignored [<xref ref-type="bibr" rid="scirp.122726-ref10">10</xref>]. Furthermore, Aquino et al. discovered a new method for vector analysis [<xref ref-type="bibr" rid="scirp.122726-ref11">11</xref>]. We hope that the degrees of freedom in electrons will be clarified in detail.</p></sec></sec><sec id="s7"><title>7. Conclusions</title><p>We proposed an empirical equation for a fine-structure constant:</p><p>137.0359991 = 136.0113077 + 1 + 1 3 &#215; 13.5 . We proposed several empirical equations to describe the relationship between an electromagnetic force and T<sub>c</sub>.</p><p>Three equations were explained by the factors of 9/2 and π. We attempted to improve the accuracies by changing the values of 9/2 and π. For this purpose, using the electrochemical method, we proposed the equivalent circuit. Then, we proposed the following two values,</p><p>3.132011447   Ω = ( m p m e + 1 + 1 3 ) m e c 2 e c , 4.488519503 = q m c ( m p m e + 1 + 1 3 ) m p c 2</p><p>The calculated values of T<sub>c</sub> and G are 2.726312 K and 6.673778 &#215; 10<sup>−11</sup> (m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup>). ( m p m e + 1 + 1 3 ) appears to be related to the transference number. However, there should be the UNIT (m/C) in ( m p m e + 1 + 1 3 ) . Therefore, the values of T<sub>c</sub> and G should not be Lorentz invariant.</p></sec><sec id="s8"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s9"><title>Cite this paper</title><p>Miyashita, T. (2023) A Fine-Structure Constant Can Be Explained Using the Electrochemical Method. Journal of Modern Physics, 14, 160-170. https://doi.org/10.4236/jmp.2023.142011</p></sec></body><back><ref-list><title>References</title><ref id="scirp.122726-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Miyashita, T. (2020) Journal of Modern Physics, 11, 1180-1192. https://doi.org/10.4236/jmp.2020.118074</mixed-citation></ref><ref id="scirp.122726-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Miyashita, T. 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