<?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.2023.144024</article-id><article-id pub-id-type="publisher-id">JMP-123707</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>
 
 
  Explanation of the Necessity of the Empirical Equations That Relate the Gravitational Constant and the Temperature of the CMB
 
</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>14</day><month>03</month><year>2023</year></pub-date><volume>14</volume><issue>04</issue><fpage>432</fpage><lpage>444</lpage><history><date date-type="received"><day>6,</day>	<month>February</month>	<year>2023</year></date><date date-type="rev-recd"><day>13,</day>	<month>March</month>	<year>2023</year>	</date><date date-type="accepted"><day>16,</day>	<month>March</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>
 
 
  In previous papers, we proposed an empirical equation for the fine-structure constant. Using this equation, we proposed a refined version of our own former empirical equations about the electromagnetic force and gravity in terms of the temperature of the cosmic microwave background. The calculated values of the temperature of the cosmic microwave background (
  <em>T</em>
  <sub><em>c</em></sub>) and the gravitational constant (
  <em>G</em>) were 2.726312 K and 6.673778 &#215; 10
  <sup>-11</sup> m
  <sup>3</sup>
  &amp;#8901;kg
  <sup>-1</sup>
  &amp;#8901; s
  <sup>-2</sup>, respectively. Then, for the values of the factors 9/2 and 
  π in our equations, we used 4.488519503 and 3.132011447, respectively. However, we could not provide a theoretical explanation for the necessity of these empirical equations. In this paper, using the redefinition method for the UNIT, we show the necessity for our empirical equations.
 
</p></abstract><kwd-group><kwd>Gravitational Constant</kwd><kwd> Temperature of the Cosmic Microwave Background</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The symbol list is shown in Section 2. Previously, we discovered Equations (1)-(3) [<xref ref-type="bibr" rid="scirp.123707-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.123707-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.123707-ref3">3</xref>] in terms of the temperature of the cosmic microwave background (CMB), which are mathematically connected [<xref ref-type="bibr" rid="scirp.123707-ref3">3</xref>] .</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; ( C J ⋅ m &#215; 1 kg = 1 V ⋅ m &#215; 1 kg ) (2)</p><p>m e c 2 e &#215; ( e 2 4 π ε 0 ) = π &#215; k T c &#215; ( J ⋅ m C = V ⋅ m ) (3)</p><p>We attempted to reduce the errors in the previous papers by changing the values of 4.5, π and the temperature of the cosmic microwave background (T<sub>c</sub>) [<xref ref-type="bibr" rid="scirp.123707-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.123707-ref5">5</xref>] . Next, we discovered an empirical equation for the fine-structure constant [<xref ref-type="bibr" rid="scirp.123707-ref6">6</xref>] .</p><p>137.0359991 = 136.0113077 + 1 3 &#215; 13.5 + 1 (4)</p><p>13.5 &#215; 136.0113077 = 1836.152654 = m p m e (5)</p><p>We thought that Equations (4) and (5) should be related to the transference number [<xref ref-type="bibr" rid="scirp.123707-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.123707-ref8">8</xref>] . Then, we proposed an equivalent circuit and the following values as the deviation for the values of 9/2 and π [<xref ref-type="bibr" rid="scirp.123707-ref8">8</xref>] .</p><p>3.13201   Ω = ( m p m e + 4 3 ) m e c 2 e c (6)</p><p>4.48852 = q m c ( m p m e + 4 3 ) m p c 2 (7)</p><p>Then, ( m p m e + 4 3 ) have the unit of ( m C ) . We can freely define the UNITs for</p><p>1 C, 1 Wb and 1 kg. Therefore, we must show the necessity for Equations (6) and (7) that these values are related to 4.5 and π. Using the redefinition method for the UNIT, we can show the necessity for our empirical equations in this report.</p><p>The remainder of the paper is organized as follows. In Section 2, we show the symbol list. In Section 3, we discuss the purpose of this report. In Section 4, we explain the redefinition method for the UNIT. In Section 5, using the redefinition method, we can refine Equations (1)-(3). Furthermore, we propose a fourth empirical equation that relates the gravitational constant and the temperature of the cosmic microwave background. In Section 6, our conclusions are described.</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: 299792458 (m/s).</p><p>h: Planck constant: 6.62607015 &#215; 10<sup>−34</sup> (J∙s).</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. Purpose</title><p>In this section, we show the purpose of this report. For convenience, Equations (5) and (6) are rewritten as follows. The units have been corrected.</p><p>3.132011447 ( V ⋅ m ) = ( m p m e + 4 3 ) m e c 2 e c ( m 2 s &#215; J A ⋅ m = J ⋅ m C = V ⋅ m ) (8)</p><p>4.488519503 ( 1 A ⋅ m ) = q m c ( m p m e + 4 3 ) m p c 2 ( s m 2 &#215; V ⋅ m J = V J &#215; s m = s C ⋅ m = 1 A ⋅ m ) (9)</p><p>Then, ( m p m e + 4 3 ) have the unit of ( m 2 s ) . 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 (10)</p><p>Then, we can freely define the UNITs for 1 C, 1 Wb and 1 kg. It does not seem necessary that these values are related to 4.5 and π. Unfortunately, we could not establish the background theory. Using the redefinition method for the UNIT, we can show the necessity why these values should be related to 4.5 and π.</p></sec><sec id="s4"><title>4. Methods</title><sec id="s4_1"><title>4.1. Redefinitions for the Electric Charge of One Electron and the Magnetic Charge of One Magnetic Monopole</title><p>We redefine the electric charge of one electron as follows.</p><p>e new = e &#215; 4.48852 4.5 = 1.59809 E − 19 ( C ) (11)</p><p>We redefine the magnetic charge of one magnetic monopole as follows.</p><p>q m _ new = q m &#215; π 3.13201 = 4.14832 E − 15 ( Wb ) (12)</p><p>Then, we can redefine the Planck constant and von Klitzing constant as follows.</p><p>h new = e new &#215; q m _ new = h &#215; 4.48852 4.5 &#215; π 3.13201 = 6.62938 E − 34 (13)</p><p>R k _ new = q m _ new e _ new = R k &#215; 4.5 4.48852 &#215; π 3.13201 = 25958.0 ( Ω ) (14)</p><p>Then, we can redefine the wave impedance in free space, electric constant and magnetic constant.</p><p>Z 0 _ new = α &#215; 2 h new e new 2 = 2 α &#215; R k new = Z 0 &#215; 4.5 4.48852 &#215; π 3.13201 = 378.849 ( Ω ) (15)</p><p>μ 0 _ new = Z 0 _ new c = μ 0 &#215; 4.5 4.48852 &#215; π 3.13201 = 1.26371 E − 06 ( N ⋅ A − 2 ) (16)</p><p>ε 0 _ new = 1 Z 0 _ new &#215; c = ε 0 &#215; 4.48852 4.5 &#215; 3.13201 π = 8.80466 E − 12 ( F ⋅ m − 1 ) (17)</p><p>Next, we must ensure that there are no contradictions.</p><p>c _ new = 1 ε 0 _ new μ 0 _ new = 1 ε 0 μ 0 = c = 299792458 ( m ⋅ s − 1 ) (18)</p><p>Z 0 _ new = μ 0 _ new ε 0 _ new = μ 0 ε 0 &#215; 4.5 4.48852 &#215; π 3.13201 = Z 0 &#215; 4.5 4.48852 &#215; π 3.13201 = 378.849 ( Ω ) (19)</p><p>The value in the speed of light should not be changed because the UNITs for 1 m and 1 s are unchanged. In Equation (19), the value of the impedance in free space is the same as the value in Equation (15).</p></sec><sec id="s4_2"><title>4.2. The Macroscopic Explanation of Our Redefinition Method</title><p>By our redefinition method for the units of the particles, 1 C and 1 Wb as MKSA units are not fixed. We redefine the electric charge of one electron. Then, the number of electrons in 1 C is changed.</p><p>N 1 = 1   C e = 1 1.60218 E − 19 = 6.24151 E + 18 (20)</p><p>N 2 = 1   C e new = 1   C 4.48852 4.5 &#215; e = 4.5 4.48852 &#215; 6.24151 E + 18 (21)</p><p>Then, the number of magnetic monopoles in 1 Wb is changed.</p><p>N 3 = 1   Wb q m = 1 4.13567 E − 15 = 2.41799 E + 14 (22)</p><p>N 4 = 1   Wb q m _ new = 1   Wb π 3.13201 &#215; 1 q m = 3.13201 π &#215; 2.41799 E + 14 (23)</p><p>The number of electrons in 1 C is related to the Faraday constant and the Avogadro’s number. Therefore, we redefined the Faraday constant and the Avogadro’s number, which will be explained in the later section.</p><p>1   C new 1   C = 4.5 4.48852 (24)</p><p>1   Wb new 1   Wb = 3.13201 π (25)</p><p>However, the relationship between Equations (26) and (27) should hold.</p><p>1   J ⋅ s new = 1   C new &#215; 1   Wb new (26)</p><p>1   Ω new = 1   Wb new 1   C new (27)</p><p>We used A∙m<sub>_new</sub> and C<sub>new</sub> in the later sections. Then, these units are from the microscopic redefinition. From the macroscopic redefinition, A∙m<sub>_new</sub> and C<sub>new</sub> should be different values.</p></sec><sec id="s4_3"><title>4.3. Redefinitions of the Mass of One Electron and One Proton</title><p>The Compton wavelength (λ) is as follows.</p><p>λ = h m c (28)</p><p>This value should (λ) be unchanged since the UNIT for 1 m is unchanged. However, in Equation (13), the Planck constant is changed. Therefore, the UNIT for the mass of one electron and one proton should be redefined.</p><p>m e _ new = 4.48852 4.5 &#215; π 3.13201 &#215; m e = 9.11394 E − 31 ( kg ) (29)</p><p>m p _ new = 4.48852 4.5 &#215; π 3.13201 &#215; m p = 1.67346 E − 27 ( kg ) (30)</p><p>Next, we must ensure that the following equation is satisfied.</p><p>m p _ new m e _ new = 1.67346 E − 27 9.11394 E − 31 = 1836.152654 = m p m e (31)</p></sec><sec id="s4_4"><title>4.4. Redefinitions of Equations (8) and (9)</title><p>Equations (8) and (9) can be redefined as follows.</p><p>( m p m e + 4 3 ) &#215; m e _ new c 2 e new c = 3.13201 ( V ⋅ m ) &#215; 4.5 4.48852 &#215; 4.48852 4.5 &#215; π 3.13201 = π ( V ⋅ m ) (32)</p><p>q m _ new c ( m p m e + 4 3 ) m p _ new c 2 = 4.48852 ( 1 A ⋅ m ) &#215; π 3.13201 &#215; 4.5 4.48852 &#215; 3.13201 π = 4.5 ( 1 A ⋅ m ) (33)</p><p>Using Equations (32) and (33), Equations (34) and (35) can be obtained.</p><p>( m p m e + 4 3 ) &#215; m e _ new c 2 e new c &#215; q m _ new c ( m p m e + 4 3 ) m p _ new c 2 = m e _ new e new &#215; q m _ new m p _ new = 4.5 &#215; π ( V ⋅ m A ⋅ m = Ω ) (34)</p><p>q m _ new c ( m p m e + 4 3 ) m p _ new c 2 ( m p m e + 4 3 ) &#215; m e _ new c 2 e new c = h new c 2 ( m p m e + 4 3 ) 2 &#215; m e _ new c 2 &#215; m p _ new c 2 = 4.5 π ( 1 A ⋅ m &#215; V ⋅ m = s J &#215; m 2 ) (35)</p></sec></sec><sec id="s5"><title>5. Results</title><sec id="s5_1"><title>5.1. Explanation for the Necessity of Using the Values of 4.5 and π</title><p>When we define the Avogadro’s number (N<sub>A</sub>) and the Faraday constant (F) as follows,</p><p>N A = 1   g m p = 5.97565 E + 23 ≈ 6.02214076 E + 23 (A)</p><p>F = e &#215; N A = 9.57405 E + 04 ≈ 9.6485 E + 04 (B)</p><p>The redefined Avogadro’s number(N<sub>A</sub>) and the refined Faraday constant (F) are as follows,</p><p>N A _ new = 1   g m p _ new = 1   g m p &#215; 4.5 4.48852 &#215; 3.13201 π (C)</p><p>F new = e new &#215; N A _ new = 1   g m p &#215; 3.13201 π (D)</p><p>Next, we can define 1 J freely. Using arbitrary number (a), N<sub>5</sub> and N<sub>6</sub> can be calculated as follows.</p><p>N 5 = a &#215; 1   J ( m p m e + 4 3 ) m e _ new c 2 ( s m 2 ) = a &#215; 6.64398 E + 09 ( s m 2 ) (36)</p><p>N 6 = a &#215; 1   J e _ new c ( J A ⋅ m ) = a &#215; 2.08726 E + 10 ( J A ⋅ m ) (37)</p><p>N 6 N 5 = 2.08726 E + 10 6.64398 E + 09 ( J A ⋅ m &#215; m 2 s = J ⋅ m C = V ⋅ m ) = π ( V ⋅ m ) (38)</p><p>The ratio should be π V∙m and constant. Next,</p><p>N 7 = a &#215; 1   J ( m p m e + 4 3 ) m p _ new c 2 ( s m 2 ) = a &#215; 3.61843 E + 06 ( s m 2 ) (39)</p><p>N 8 = a &#215; 1   J q m _ new c ( J Wb ⋅ m / s = J ⋅ s Wb ⋅ m = C m ) = a &#215; 8.04095 E + 05 ( C m ) (40)</p><p>N 7 N 8 = 3.61843 E + 06 8.04095 E + 05 = 4.5 ( s m 2 &#215; m C = 1 A ⋅ m ) (41)</p><p>The ratio should be 4.5 and π are constant. Consequently, we can explain the necessity for the values of 4.5 and π in Equations (8) and (9).</p></sec><sec id="s5_2"><title>5.2. Explanation for the Necessity of Using the Values of 4.5 and π in Equations (1)-(3)</title><sec id="s5_2_1"><title>5.2.1. Our Main Three Equations</title><p>Equations (1)-(3) are our main three equations. Then, the unit (V∙m and 1/A∙m) should be replaced. Alternatively, the redefinition of V∙m and 1/A∙m is needed in the equations.</p><p>G m p 2 h c = 4.48852 2 k T c 1   kg &#215; c 2 &#215; ( A ⋅ m ) (42)</p><p>G m p 2 ( e 2 4 π ε 0 ) = 4.48852 2 &#215; 3.13201 &#215; m e e &#215; h c &#215; ( A ⋅ m &#215; V ⋅ m &#215; 1 V ⋅ m &#215; 1 kg = A ⋅ m &#215; 1 kg ) (43)</p><p>m e c 2 e &#215; ( e 2 4 π ε 0 ) = 3.13201 &#215; k T c &#215; ( 1 V ⋅ m &#215; V ⋅ m = 1 ) (44)</p></sec><sec id="s5_2_2"><title>5.2.2. Our Fourth Equation</title><p>Our fourth equation can be derived as follows. From Equation (43),</p><p>G m p 2 ( e 2 4 π ε 0 ) 2 = 4.48852 2 &#215; 3.13201 &#215; m e e &#215; 2 π α &#215; ( A ⋅ m &#215; 1 kg ) (45)</p><p>From Equation (44),</p><p>e 2 4 π ε 0 = 3.13201 &#215; k T c &#215; e m e c 2 (46)</p><p>From Equations (45) and (46),</p><p>G m p 2 ( 3.13201 &#215; k T c &#215; e m e c 2 ) 2 = 4.48852 2 &#215; 3.13201 &#215; m e e &#215; 2 π α &#215; ( A ⋅ m &#215; 1 kg ) (47)</p><p>Therefore,</p><p>G m p 2 ( k T c ) 2 = 4.48852 &#215; 3.13201 &#215; e m e c 4 &#215; π α &#215; ( A ⋅ m &#215; 1 kg ) (48)</p><p>Here,</p><p>4.48852 &#215; 3.13201 ( Ω ) = q m e &#215; m e m p ( Ω ) (49)</p><p>In Equation (48), the unit of Ω is already considered. Therefore,</p><p>G m p 2 = q m m p c 4 &#215; π α &#215; ( k T c ) 2 &#215; ( A ⋅ m &#215; 1 kg ) (50)</p><p>Equation (50) is our fourth equation.</p></sec><sec id="s5_2_3"><title>5.2.3. Redefinition for Equation (42)</title><p>We define G free from 1 kg (G<sub>N</sub>) as follows.</p><p>G N = G &#215; 1   kg (51)</p><p>The UNIT for G<sub>N</sub> is m<sup>3</sup>∙s<sup>−2</sup>. By our redefinition method, the UNITs for 1 m and 1 s are unchanged. However, when G<sub>N</sub> is a function of C or Wb, G<sub>N</sub> should be changed.</p><p>G N _ n e w ≠ G N (52)</p><p>From Equations (42) and (51),</p><p>G N m p 2 h c = 4.4885 2 k T c c 2 &#215; ( A ⋅ m ) (53)</p><p>Therefore,</p><p>G N m p _ new 2 &#215; ( 4.5 4.48852 &#215; 3.13201 π ) 2 h new &#215; 4.5 4.48852 &#215; 3.13201 π c = 4.48852 2 k T c c 2 &#215; A ⋅ m (54)</p><p>Therefore,</p><p>G N m p _ new 2 h new c = 4.5 2 &#215; ( 4.48852 4.5 ) 2 &#215; π 3.13201 &#215; k T c c 2 &#215; ( A ⋅ m ) (55)</p><p>Next, using G<sub>N_</sub><sub>new</sub> and kT<sub>c_</sub><sub>new</sub>, we proposed the following equation, which is the same formula as Equation (1). Then, the unit of 4.5 is 1/A∙m in Equation (9).</p><p>G N _ new m p _ new 2 h new c = 4.5 2 &#215; k T c _ new c 2 &#215; ( A ⋅ m ) new (56)</p><p>Therefore,</p><p>G N _ new G N = ( 4.5 4.48852 ) 2 &#215; 3.13201 π &#215; k T c _ new k T &#215; ( A ⋅ m ) new A ⋅ m (57)</p></sec><sec id="s5_2_4"><title>5.2.4. Redefinition of Equation (43)</title><p>Using G<sub>N</sub>, Equation (43) is rewritten as follows.</p><p>G N m p 2 ( e 2 4 π ε 0 ) = 4.48852 2 &#215; 3.13201 &#215; m e e &#215; h c &#215; ( A ⋅ m ) (58)</p><p>Therefore,</p><p>G N m p _ new 2 = m e _ new e new h new c 4 π ε 0 _ new &#215; 4.48852 2 &#215; 3.13201 &#215; 4.5 4.48852   &#215; 4.48852 4.5 &#215; 3.13201 π &#215; ( A ⋅ m ) (59)</p><p>Using G<sub>N_</sub><sub>new</sub> and A∙m<sub>new</sub>, we propose the following equation, which is the same formula as Equation (2).</p><p>G N _ new m p _ new 2 ( e 2 4 π ε 0 ) new = 4.5 2 &#215; π &#215; m e _ new e _ new &#215; h _ new c &#215; ( A ⋅ m ) new (60)</p><p>Therefore,</p><p>G N _ new G N = 4.5 4.48852 &#215; ( A ⋅ m ) new A ⋅ m (61)</p></sec><sec id="s5_2_5"><title>5.2.5. Redefinition of Equation (44)</title><p>Equation (44) is rewritten as follows.</p><p>m e c 2 e &#215; ( e 2 4 π ε 0 ) = 3.13201 &#215; k T c (62)</p><p>Therefore,</p><p>m e _ new c 2 e new &#215; e new 2 4 π ε 0 _ new &#215; 4.5 4.48852 &#215; 3.13201 π = π &#215; k T c (63)</p><p>Next, using kT<sub>c_</sub><sub>new</sub>, we propose the following Equation, which is the same formula as Equation (3).</p><p>m e _ new c 2 e new &#215; e new 2 4 π ε 0 _ new = π &#215; k T c _ new (64)</p><p>Therefore,</p><p>k T c _ new k T c = 4.48852 4.5 &#215; π 3.13201 (65)</p></sec><sec id="s5_2_6"><title>5.2.6. Redefinition of Equation (50)</title><p>Using G<sub>N</sub>, Equation (50) is rewritten as follows.</p><p>G N m p 2 = q m m p c 4 &#215; π α &#215; ( k T c ) 2 &#215; ( A ⋅ m ) (66)</p><p>Therefore,</p><p>G N = q m _ new m p _ new 3 &#215; π α &#215; ( k T c ) 2 c 4 &#215; ( 4.48852 4.5 ) 3 &#215; ( π 3.13201 ) 2 &#215; ( A ⋅ m ) (67)</p><p>Next, using G<sub>N_</sub><sub>new</sub>, kT<sub>c_</sub><sub>new</sub> and A∙m<sub>new</sub>, we propose the following equation.</p><p>G N _ new = q m _ new m p _ new 3 &#215; π α &#215; ( k T c _ new ) 2 c 4 &#215; ( A ⋅ m ) new (68)</p><p>Therefore,</p><p>G N _ n e w G N = ( 4.5 4.48852 ) 3 &#215; ( 3.13201 π ) &#215; ( k T c _ new k T c ) 2 &#215; ( A ⋅ m ) new A ⋅ m (69)</p></sec><sec id="s5_2_7"><title>5.2.7. Redefinition of kT<sub>c</sub> and Vm</title><p>Equations (57), (61), (65) and (69) are rewritten as follows.</p><p>G N _ new G N = ( 4.5 4.48852 ) 2 &#215; 3.13201 π &#215; k T c _ new k T &#215; ( A ⋅ m ) new A ⋅ m (70)</p><p>G N _ new G N = 4.5 4.48852 &#215; ( A ⋅ m ) new A ⋅ m (71)</p><p>k T c _ new k T c = 4.48852 4.5 &#215; π 3.13201 (72)</p><p>G N _ new G N = ( 4.5 4.48852 ) 3 &#215; ( 3.13201 π ) &#215; ( k T c _ new k T c ) 2 &#215; ( A ⋅ m ) new A ⋅ m (73)</p><p>In Equation (72), kT<sub>c</sub> is redefined and determined. Next,</p><p>( A ⋅ m ) new A ⋅ m = ( C &#215; m / s ) new C &#215; m / s = C new C = 4.48852 4.5 (74)</p><p>From Equations (71) and (74),</p><p>G N _ new G N = 1 (75)</p><p>Then, Equations (70) and (73) can be explained. In Equation (72), redefinition of kT<sub>c</sub>,is from redefinition of the mass of the particle as follows:</p><p>k T c _ new k T = 4.48852 4.5 &#215; π 3.13201 = m e _ new m e (76)</p><p>However, the unit Am remains in the three equations. We proposed the following unit. We will explain the unit (G<sub>N</sub><sub>/Am</sub>) in a future report, which maybe different from the standard approach for G and thermodynamics [<xref ref-type="bibr" rid="scirp.123707-ref9">9</xref>] .</p><p>G N / A m _ new G N / A m = ( G &#215; 1   kg A ⋅ m ) new G &#215; 1   kg A ⋅ m = ( G N A ⋅ m ) new G N A ⋅ m = 4.5 4.48852 (77)</p></sec><sec id="s5_2_8"><title>5.2.8. Making Sure for the Calculation</title><p>Equation (56) is rewritten as follows:</p><p>G N / A m _ new m p _ new 2 h new c = 4.5 2 &#215; k T c _ new c 2 = 9.4279464618 E − 40 (78)</p><p>Equation (60) is rewritten as follows:</p><p>G N / A m _ new m p _ new 2 ( e 2 4 π ε 0 ) new = 4.5 2 &#215; π &#215; m e _ new e _ new &#215; h _ new c = 8.1176747490 E − 37 (79)</p><p>Equation (64) is rewritten as follows:</p><p>m e _ new c 2 e new &#215; e new 2 4 π ε 0 _ new = π &#215; k T c _ new = 1.18311202 E − 22 (80)</p><p>Equation (68) is rewritten as follows:</p><p>G N / A m _ new = q m _ new m p _ new 3 &#215; π α &#215; ( k T c _ new ) 2 c 4 = 6.6908477020 E − 11 (81)</p><p>Consequently, our four equations can be redefined successfully.</p></sec><sec id="s5_2_9"><title>5.2.9. The Other Equations</title><p>From Equation (8),</p><p>3.132011447 ( V ⋅ m ) = ( m p m e + 4 3 ) m e c 2 e c ( m 2 s &#215; J A ⋅ m = J ⋅ m C = V ⋅ m ) (82)</p><p>From Equation (44),</p><p>m e c 2 &#215; e c 4 π ε 0 c = 3.132011447 ( V ⋅ m ) &#215; k T c (83)</p><p>In Equation (83), there are no dimension mismatch problems. From Equations (81) and (82),</p><p>m e c 2 &#215; e c 4 π ε 0 c = ( m p m e + 4 3 ) m e c 2 e c &#215; k T c (84)</p><p>Therefore,</p><p>k T c e 2 c 4 π ε 0 = 1 ( m p m e + 4 3 ) ( s m 2 ) = 1 1837.485988 ( s m 2 ) (85)</p><p>Therefore,</p><p>( k T c e 2 c 4 π ε 0 ) new 1 1837.485988 ( s m 2 ) = 1 ( m p m e + 4 3 ) ( s m 2 ) (86)</p><p>Consequently, Equation (85) can be successfully redefined. Therefore,</p><p>( k T c h c 2 ) new = 1 6.3206454 E − 07 = 1 ( m p m e + 4 3 ) &#215; α 2 π (87)</p><p>Furthermore, Equation (87) can also be redefined.</p></sec></sec></sec><sec id="s6"><title>6. Conclusions</title><p>In this report, using the redefinition method for the UNIT, we showed the necessity for our empirical equations. The redefinition method was explained in detail. Then, we proposed four empirical equations.</p><p>G N / A m _ new m p _ new 2 h new c = 4.5 2 ( 1 A ⋅ m ) &#215; k T c _ new c 2 = 9.4279464618 E − 40 (88)</p><p>where G<sub>N/Am</sub> = G &#215; 1 kg/A∙m</p><p>G N / A m _ new m p _ new 2 ( e 2 4 π ε 0 ) new = 4.5 2 &#215; π ( 1 A ⋅ m &#215; V ⋅ m ) &#215; m e _ new e _ new &#215; h _ new c = 8.1176747490 E − 37 (89)</p><p>m e _ new c 2 e new &#215; e new 2 4 π ε 0 _ new = π ( V ⋅ m ) &#215; k T c _ new = 1.18311202 E − 22 (90)</p><p>G N / A m _ new = q m _ new m p _ new 3 &#215; π ( V ⋅ m ) α &#215; ( k T c _ new ) 2 c 4 = 6.6908477020 E − 11 (91)</p><p>Furthermore, we derived four important equations.</p><p>m e _ new e n e w &#215; q m _ new m p _ new = 4.5 &#215; π ( V ⋅ m A ⋅ m = Ω ) (92)</p><p>h new c 2 ( m p m e + 4 3 ) 2 &#215; m e _ new c 2 &#215; m p _ new c 2 = 4.5 π ( 1 A ⋅ m &#215; V ⋅ m = s J &#215; m 2 ) (93)</p><p>k T c e 2 c 4 π ε 0 = 1 1837.485988 ( s 2 m ) = 1 ( m p m e + 4 3 ) ( s 2 m ) (94)</p><p>( k T c h c 2 ) new = 1 6.3206454 E − 07 = 1 ( m p m e + 4 3 ) &#215; α 2 π ( s 2 m ) (95)</p><p>About numerical connections considering the units, our redefinition is perfect, in which there are not any dimension mismatch problems. About the unit (G<sub>N</sub><sub>/Am</sub>), we will explain in the future report.</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Miyashita, T. (2023) Explanation of the Necessity of the Empirical Equations That Relate the Gravitational Constant and the Temperature of the CMB. Journal of Modern Physics, 14, 432-444. https://doi.org/10.4236/jmp.2023.144024</p></sec></body><back><ref-list><title>References</title><ref id="scirp.123707-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.123707-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Miyashita, T. 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