<?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">JHEPGC</journal-id><journal-title-group><journal-title>Journal of High Energy Physics, Gravitation and Cosmology</journal-title></journal-title-group><issn pub-type="epub">2380-4327</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jhepgc.2017.32020</article-id><article-id pub-id-type="publisher-id">JHEPGC-74770</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>
 
 
  Precise Ideal Value of the Universal Gravitational Constant G
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abed</surname><given-names>El Karim S. Abou Layla</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>Independent Researcher, Gaza City, Palestine</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>a.k.aboulayla@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>08</day><month>02</month><year>2017</year></pub-date><volume>03</volume><issue>02</issue><fpage>248</fpage><lpage>253</lpage><history><date date-type="received"><day>January</day>	<month>2,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>March</month>	<year>14,</year>	</date><date date-type="accepted"><day>March</day>	<month>17,</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>
 
 
  In this paper, we are going to rely on the first law in physics through which we can obtain a precise ideal value of the universal gravitational constant, a thing which has not happened so far. The significance of this law lies in the fact that, besides determining a precise ideal value of the gravitational constant, it connects three different physical disciplines together, which are mechanics, electromagnetism and thermodynamics. It is what distinguishes this from other law. Through this law, we have created the theoretical value of the gravitational constant 
  G<sub>i</sub> and we found it equivalent to 6.674010551359 &#215; 10
  <sup>-11</sup> m
  <sup>3</sup>
  &amp;#183kg
  <sup>-1</sup>
  &amp;#183s
  <sup>-2</sup>. In the discussion, the table of measurements of the gravitational constant was divided into three groups, and the average value of the first group 
  G
  <sub>1</sub> which is the best precision, equals the following sum 6.67401&#215;10
  <sup>-11</sup> m
  <sup>3</sup>
  &amp;#183kg
  <sup>-1</sup>
  &amp;#183s
  <sup>-2</sup>, and it’s the same equal value to the ideal value 
  G<sub>i</sub> that results from the law, as shown through our research that any other experimental values 
  must not exceed the relative standard uncertainty which has a certain amount that is equivalent to a value of 5.325&#215;10
  <sup>-5</sup>
   and that’s a square value of the fine-structure constant.
 
</p></abstract><kwd-group><kwd>Gravitational Constant</kwd><kwd> Newtonian Parameter of Gravitation</kwd><kwd> Khromatic Theory</kwd><kwd> CODATA</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Although 3 centuries have elapsed since Newton set forth his gravitational law, physiology has been unable so far to create an exact theoretical value for the universal gravitational constant with no available values of the gravitational constant values except those values concluded by scientific experiments, especially conducted for obtaining the most accurate values of this constant.</p><p>We are going, in this research, to surmount this problem by way of setting forth a universal gravitational constant sole theory value, to be calculated through an index of a law known in the Khromatic theory as “The Law of Gravitational Constant” [<xref ref-type="bibr" rid="scirp.74770-ref1">1</xref>] , although another problem yet lies here, which is that all results of experiments relating to determining the value of gravitational constants are confined to two values: a greater value and a lower value.</p><p>To overcome this problem, we put forth a supposition that a certain marginal velocity can be a basis for calculating a gravitational greater value acceptable as an ideal value within a certain error rate. And to ascertain the validity of the hypothesis we compared, through discussion, the values we obtained with those on the gravitation <xref ref-type="table" rid="table2">Table 2</xref> of 2014 CODATA, as the comparison showed that in both cases the values were significantly close together, a thing that enabled us to solve the discrepancy between the theoretical and experimental values, consequently modifying <xref ref-type="table" rid="table2">Table 2</xref>, thereby we will have left behind an era of incessant attempts to find out the most accurate value of the gravitational constant.</p></sec><sec id="s2"><title>2. Finding the Accurate and Approximate Value of the Gravitation Constant</title><sec id="s2_1"><title>2.1. The Precise Ideal Value of G</title><p>The law of gravitational constant looks like this:</p><disp-formula id="scirp.74770-formula249"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x2.png"  xlink:type="simple"/></disp-formula><p>as,</p><disp-formula id="scirp.74770-formula250"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x3.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74770-formula251"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x4.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74770-formula252"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x5.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74770-formula253"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x6.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74770-formula254"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x7.png"  xlink:type="simple"/></disp-formula><p>We are not going in our discussion, to deal with the method of the inference of this law, because of that it will be through another search that will be published completely, but we will content ourselves by reviewing the law and finds the precise ideal value of gravity through it.</p><p>Taking the values of the constants above from an abbreviated list of the 2014 CODATA recommended values of the fundamental constants of physics and chemistry, we get</p><disp-formula id="scirp.74770-formula255"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x8.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74770-formula256"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x9.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74770-formula257"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x10.png"  xlink:type="simple"/></disp-formula><p>So, using substitution in the value of constants we get the precise value of the gravitation constant equaling:</p><disp-formula id="scirp.74770-formula258"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x11.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74770-formula259"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x12.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. The Expected Value of the Gravitation Constant</title><p>Perhaps the ideal precise value of the gravitation constant is suitable for the static large blocks or those having negligible velocity-induced increment.</p><p>As for small masses moving at high speeds, it is more suitable to deal with relativity when calculated, however, we can handle expected values of the gravitational constant for experiments in which the body's velocity is so limited that the block's increment may be overlooked.</p><p>And to find such values, we can suppose that the block’s laboratory speed limit should not exceed the orbital speed of electron in an atom of hydrogen and consequently the maximum expected gravitational value should not exceed a maximum value of the gravitational constant that is calculable using the equation.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x13.png" xlink:type="simple"/></inline-formula>as,</p><disp-formula id="scirp.74770-formula260"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x14.png"  xlink:type="simple"/></disp-formula><p>And on calculation of this value we get the following:</p><disp-formula id="scirp.74770-formula261"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x15.png"  xlink:type="simple"/></disp-formula><p>Hence we can deduce the ideal standard uncertainty vale <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x16.png" xlink:type="simple"/></inline-formula> from the equation:</p><disp-formula id="scirp.74770-formula262"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x17.png"  xlink:type="simple"/></disp-formula><p>And the ideal value of the relative standard uncertainty is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x18.png" xlink:type="simple"/></inline-formula> of the equation:</p><disp-formula id="scirp.74770-formula263"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x19.png"  xlink:type="simple"/></disp-formula><p>which is a somewhat an acceptable value.</p></sec></sec><sec id="s3"><title>3. Relationship between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x20.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x21.png" xlink:type="simple"/></inline-formula></title><p>Since</p><disp-formula id="scirp.74770-formula264"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x22.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x23.png" xlink:type="simple"/></inline-formula>,</p><p>Thus</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x24.png" xlink:type="simple"/></inline-formula>,</p><p>and</p><disp-formula id="scirp.74770-formula265"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x25.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Discussion</title><p>In this discussion we are going to compare the ideal values we had got by theoretical means and the documented experimental values in CODATA gravitational tables, and we will show that the values are close in both cases.</p><sec id="s4_1"><title>4.1. Comparison of the Ideal and Results of Measurements of Gravitational Constant</title><p><xref ref-type="table" rid="table1">Table 1</xref>, borrowed from CODATA Recommended Values of the Fundamental Physical Constants, 2010, summarizes the results of measurements of the Newtonian parameter of gravitation relevant to the 2010 adjustment [<xref ref-type="bibr" rid="scirp.74770-ref2">2</xref>] .</p><p>In this table there are three groups of measurements [<xref ref-type="bibr" rid="scirp.74770-ref3">3</xref>] .</p><p>・ The first such group consists of six measurements with the average value of</p><disp-formula id="scirp.74770-formula266"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x26.png"  xlink:type="simple"/></disp-formula><p>Standard uncertainty <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x27.png" xlink:type="simple"/></inline-formula> and relative standard uncertainty 28.5 ppm;</p><p>・ The second one consists of four measurements with the average value of</p><disp-formula id="scirp.74770-formula267"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x28.png"  xlink:type="simple"/></disp-formula><p>Standard uncertainty <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x29.png" xlink:type="simple"/></inline-formula> and relative standard uncertainty 24 ppm;</p><p>・ The third one consists of one measurement with the value of</p><disp-formula id="scirp.74770-formula268"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x30.png"  xlink:type="simple"/></disp-formula><p>Standard uncertainty <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x31.png" xlink:type="simple"/></inline-formula> and relative standard uncertainty 40 ppm.</p><p>Therefore, we conclude that the ideal value of the gravitational constant equals the sum</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Summary of the results of measurements of the Newtonian constant of gravitation relevant to the 2010 adjustment</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Source</th><th align="center" valign="middle" >Identification<sup>a</sup></th><th align="center" valign="middle" >Method</th><th align="center" valign="middle" >10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup></th><th align="center" valign="middle" >Rel.stand. uncert. ur</th></tr></thead><tr><td align="center" valign="middle" >Luther and Towler (1982)</td><td align="center" valign="middle" >NIST-82</td><td align="center" valign="middle" >Fiber torsion balance, dynamic mode</td><td align="center" valign="middle" >6.67248 (43)</td><td align="center" valign="middle" >6.4 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Karagioz and Izmailov (1996)</td><td align="center" valign="middle" >TR&amp;D-96</td><td align="center" valign="middle" >Fiber torsion balance, dynamic mode</td><td align="center" valign="middle" >6.6729 (5)</td><td align="center" valign="middle" >7.5 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Bagley and Luther (1997)</td><td align="center" valign="middle" >LANL-97</td><td align="center" valign="middle" >Fiber torsion balance, dynamic mode</td><td align="center" valign="middle" >6.67398 (70)</td><td align="center" valign="middle" >1.0 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" >Gundlach and Merkowitz (2000, 2002)</td><td align="center" valign="middle" >UWash-00</td><td align="center" valign="middle" >Fiber torsion balance, Dynamic compensation</td><td align="center" valign="middle" >6.674255 (92)</td><td align="center" valign="middle" >1.4 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Quinn et al. (2001)</td><td align="center" valign="middle" >BIPM-01</td><td align="center" valign="middle" >Strip torsion balance, Compensation mode, static deflection</td><td align="center" valign="middle" >6.67559 (27)</td><td align="center" valign="middle" >4.0 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Kleinevo&#223; (2002) and Kleinvo&#223; et al. (2002)</td><td align="center" valign="middle" >UWup-02</td><td align="center" valign="middle" >Suspended body, displacement</td><td align="center" valign="middle" >6.67422 (98)</td><td align="center" valign="middle" >1.5 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" >Armstrong and Fitzgerald (2003)</td><td align="center" valign="middle" >MSL-03</td><td align="center" valign="middle" >Strip torsion balance, compensation mode</td><td align="center" valign="middle" >6.67387 (27)</td><td align="center" valign="middle" >4.0 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Hu, Guo, and Luo (2005)</td><td align="center" valign="middle" >HUST-05</td><td align="center" valign="middle" >Fiber torsion balance, dynamic mode</td><td align="center" valign="middle" >6.67222 (87)</td><td align="center" valign="middle" >1.3 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" >Schlamminger et al. (2006)</td><td align="center" valign="middle" >UZur-06</td><td align="center" valign="middle" >Stationary body, weight change</td><td align="center" valign="middle" >6.67425 (12)</td><td align="center" valign="middle" >1.9 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Luo et al. (2009) and Tu et al. (2010)</td><td align="center" valign="middle" >HUST-09</td><td align="center" valign="middle" >Fiber torsion balance, dynamic mode</td><td align="center" valign="middle" >6.67349 (18)</td><td align="center" valign="middle" >2.7 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Parks and Faller (2010)</td><td align="center" valign="middle" >JILA-10</td><td align="center" valign="middle" >Suspended body, displacement</td><td align="center" valign="middle" >6.67234 (14)</td><td align="center" valign="middle" >2.1 &#215; 10<sup>−5</sup></td></tr></tbody></table></table-wrap><disp-formula id="scirp.74770-formula269"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x32.png"  xlink:type="simple"/></disp-formula><p>which is extremely close to the average value G<sub>1</sub>, that equals the following sum</p><disp-formula id="scirp.74770-formula270"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x33.png"  xlink:type="simple"/></disp-formula><p>So we can choice the first group of G measurements as the best precision group of all others.</p></sec><sec id="s4_2"><title>4.2. Comparison of the Ideal and 2014 CODATA-Recommended Value of the Gravitational Constant [<xref ref-type="bibr" rid="scirp.74770-ref4">4</xref>]</title><p>We learn from <xref ref-type="table" rid="table2">Table 2</xref> the recommended values of 2014 CODATA [<xref ref-type="bibr" rid="scirp.74770-ref4">4</xref>] as follows:</p><p>That is, based upon the above table, the experimental value of the gravitational constant should range from a maximum value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x34.png" xlink:type="simple"/></inline-formula> equaling <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x35.png" xlink:type="simple"/></inline-formula> to a maximum value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x36.png" xlink:type="simple"/></inline-formula> equaling <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x37.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x38.png" xlink:type="simple"/></inline-formula> as the arithmetic mean of the two values that equals<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x39.png" xlink:type="simple"/></inline-formula>.</p><sec id="s4_2_1"><title>4.2.1. The Ideal Value of the Gravitational Constant Equals the Sum</title><disp-formula id="scirp.74770-formula271"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x40.png"  xlink:type="simple"/></disp-formula><p>which is extremely close to the gravitational experimental value, that equals the following sum</p><disp-formula id="scirp.74770-formula272"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x41.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_2_2"><title>4.2.2. Comparison of the Extent and Rate of Error</title><p>When comparing the ideal quantity of standard uncertainty, which equals</p><disp-formula id="scirp.74770-formula273"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x42.png"  xlink:type="simple"/></disp-formula><p>To its counterpart mentioned in <xref ref-type="table" rid="table2">Table 2</xref>, which has the value:</p><disp-formula id="scirp.74770-formula274"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x43.png"  xlink:type="simple"/></disp-formula><p>we find great similarity in values.</p></sec><sec id="s4_2_3"><title>4.2.3. Comparison of the Relative Error Rate</title><p>Likewise, when comparing the ideal value of the relative standard uncertainty, which equals:</p><disp-formula id="scirp.74770-formula275"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x44.png"  xlink:type="simple"/></disp-formula><p>To its counterpart contained in <xref ref-type="table" rid="table2">Table 2</xref> which has the value:</p><disp-formula id="scirp.74770-formula276"><graphic  xlink:href="http://html.scirp.org/file/5-2180180x45.png"  xlink:type="simple"/></disp-formula><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> 2014 CODATA- recommended values of gravitation G, ∆G, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x46.png" xlink:type="simple"/></inline-formula>, Concise form</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >Newtonian constant of gravitation G</th></tr></thead><tr><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >6.67408 &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup></td></tr><tr><td align="center" valign="middle" >Standard uncertainty ∆G</td><td align="center" valign="middle" >0.00031 &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup></td></tr><tr><td align="center" valign="middle" >Relative standard uncertainty u<sub>r</sub></td><td align="center" valign="middle" >4.7 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >Concise form</td><td align="center" valign="middle" >6.67408(31) &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup></td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Updated the values of gravitation G, ∆G, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x47.png" xlink:type="simple"/></inline-formula>, Concise form</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >ideal Newtonian constant of gravitation G<sub>i</sub></th></tr></thead><tr><td align="center" valign="middle" >Value</td><td align="center" valign="middle" >6.6740105 &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup></td></tr><tr><td align="center" valign="middle" >fine-structure constant α</td><td align="center" valign="middle" >7.2973525664 &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >Standard uncertainty ∆G</td><td align="center" valign="middle" >0.000 3554 &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup></td></tr><tr><td align="center" valign="middle" >Relative standard uncertainty <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-2180180x48.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >5.325 &#215; 10<sup>−5</sup> α<sup>2</sup></td></tr><tr><td align="center" valign="middle" >Concise form</td><td align="center" valign="middle" >6.6740105 (3554) &#215; 10<sup>−11</sup> m<sup>3</sup>∙kg<sup>−1</sup>∙s<sup>−2</sup></td></tr></tbody></table></table-wrap><p>we also find great similarity in values.</p><p>Therefore, we conclude that all ideal values we have obtained through the theoretical equations are extremely close to their experimental counterparts which we had got from <xref ref-type="table" rid="table2">Table 2</xref>, which shows the recommended values of 2014 CODATA, except that the ideal values are more accurate, having been theoretically concluded, and as such, the data of <xref ref-type="table" rid="table2">Table 2</xref> may be updated and substituted for the ideal values as illustrated below in <xref ref-type="table" rid="table3">Table 3</xref>.</p></sec></sec></sec><sec id="s5"><title>5. Conclusions</title><p>There is a precise ideal value of the universal gravitational constant which equals 6.674010551359 &#215; 10<sup>−11</sup>.</p><p>That may be calculated through a theoretically concluded equation of its own, and the cause of discrepancy of the gravitation value is attributable to the circumstances of the experiment as well as the sophistication of the nature and speed of particles used to measure the gravitational constant in such experiments.</p></sec><sec id="s6"><title>Cite this paper</title><p>Abou Layla, A.E.K.S. (2017) Precise Ideal Value of the Universal Gravitational Constant G. Journal of High Energy Physics, Gravitation and Cosmology, 3, 248-253. https://doi.org/10.4236/jhepgc.2017.32020</p></sec></body><back><ref-list><title>References</title><ref id="scirp.74770-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">AbouLayla, A.K. (2016) The Khromatic Theoary. 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