<?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">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1102412</article-id><article-id pub-id-type="publisher-id">OALibJ-69112</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Reciprocity Principle in Gravitational Interactions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Angel</surname><given-names>Fierros Palacios</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>Instituto de Investigaciones Eléctricas, Divisi&amp;amp;#243;n de Energ&amp;amp;#237;as Alternas, Cuernavaca, México</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>afierros@iie.org.mx</email></corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>03</month><year>2016</year></pub-date><volume>03</volume><issue>03</issue><fpage>1</fpage><lpage>4</lpage><history><date date-type="received"><day>4</day>	<month>March</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>20</month>	<year>March</year>	</date><date date-type="accepted"><day>24</day>	<month>March</month>	<year>2016</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 it is proposed that the ratio between the apparent radius of any two celestial bodies separated by a very big distance, as seemed each other at a distance, is numerically equal to the ratio of the respective real values of their radius. That relationship is what is called in the paper the Reciprocity Principle. In other words, the apparent size of heavenly bodies, as seemed at a distance, plays a special role in the gravitational interactions. This is so because of some kind of effect over the size due to the very big distances in space. When a couple of celestial bodies interact each other, both of them can be considered as sources of the gravity attraction. In that situation, each body acts upon the other in such a way that it can be considered that there are some degree of reciprocal interaction. In this paper, a formal definition of that reciprocal effect is given. 
  
 
</p></abstract><kwd-group><kwd>Escape Velocity</kwd><kwd> Apparent Size</kwd><kwd> Reciprocity Principle</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let us consider two heavenly bodies having masses m<sub>1</sub> and m<sub>2</sub>, and radius r<sub>1</sub> and r<sub>2</sub>, respectively, separated by a certain distance, and in gravitational attraction acting along the line joining them. In that situation, the values of their escape velocities due to its apparent size are dependent on their masses, and critically on their apparent radius [<xref ref-type="bibr" rid="scirp.69112-ref1">1</xref>] . When those celestial bodies interact each other, both of them must be considered as sources of gravity force. Then, along that dynamical process, as it was said before, there exist some degree of reciprocity [<xref ref-type="bibr" rid="scirp.69112-ref1">1</xref>] . By definition of escape velocity it has that [<xref ref-type="bibr" rid="scirp.69112-ref2">2</xref>]</p><disp-formula id="scirp.69112-formula1015"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x6.png"  xlink:type="simple"/></disp-formula><p>where G is the Gravitational Constant, M the mass of the source of the gravity force, and R its radius [<xref ref-type="bibr" rid="scirp.69112-ref1">1</xref>] .</p></sec><sec id="s2"><title>2. The Reciprocity Principle</title><p>When the heavenly bodies before mentioned, are in gravitational interaction, it is easy to see that from Equation (1) the following relationship can be obtained</p><disp-formula id="scirp.69112-formula1016"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x7.png"  xlink:type="simple"/></disp-formula><p>where the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x8.png" xlink:type="simple"/></inline-formula> are the apparent radius of the bodies.</p><p>Let’s consider one of the bodies as the source of the gravity attraction; and be that body the one marked with the index 2. Its mass is m<sub>2</sub>, and its apparent radius is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x9.png" xlink:type="simple"/></inline-formula>. So that, the equation (1) takes the following form [<xref ref-type="bibr" rid="scirp.69112-ref1">1</xref>] .</p><disp-formula id="scirp.69112-formula1017"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x10.png"  xlink:type="simple"/></disp-formula><p>In order to obtain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x11.png" xlink:type="simple"/></inline-formula>, and also <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x12.png" xlink:type="simple"/></inline-formula> it can be use the following procedure. It is well known from Optics that the ratio of the image size q, to the object size p is the Magnification A, that is to say</p><disp-formula id="scirp.69112-formula1018"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x13.png"  xlink:type="simple"/></disp-formula><p>To obtain the apparent size of that body, it can be used some optical astronomical instrument that has a magnification A; in order to get the apparent image, and also the apparent size, given by the following formula</p><disp-formula id="scirp.69112-formula1019"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x14.png"  xlink:type="simple"/></disp-formula><p>Given that A is a number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x15.png" xlink:type="simple"/></inline-formula>is equal to p/2. To calculate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x16.png" xlink:type="simple"/></inline-formula> is enough to introduce into Equation (2) the result obtained. However, in that equation it has the unknown quantity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x17.png" xlink:type="simple"/></inline-formula>. In order to known its value, it is pro- posed that:</p><p>The ratio between the apparent radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x18.png" xlink:type="simple"/></inline-formula> keep the same proportion among them as the ratio of the respectives real values of their radius; that is to say</p><disp-formula id="scirp.69112-formula1020"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x19.png"  xlink:type="simple"/></disp-formula><p>where r<sub>1</sub> and r<sub>2</sub> are the values of the real radius. The proposition before given is the Reciprocity Principle.</p></sec><sec id="s3"><title>3. The Sun-Earth System</title><p>As an illustrative example, let’s consider the case of the gravitational interaction between the Sun and our planet. Therefore, Equation (2) becomes</p><disp-formula id="scirp.69112-formula1021"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x20.png"  xlink:type="simple"/></disp-formula><p>Then, it has that</p><disp-formula id="scirp.69112-formula1022"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x21.png"  xlink:type="simple"/></disp-formula><p>according to relationship (6).</p><p>Taking into account the values that appears in the Appendix, it is obtained that</p><disp-formula id="scirp.69112-formula1023"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x22.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.69112-formula1024"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x23.png"  xlink:type="simple"/></disp-formula><p>in such a way that in Equation (8) it has that</p><disp-formula id="scirp.69112-formula1025"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x24.png"  xlink:type="simple"/></disp-formula><p>Substituting this result into Equation (8) the following value for the Earth’s escape velocity due to its apparent size is obtained; that is to say</p><disp-formula id="scirp.69112-formula1026"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x25.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x26.png" xlink:type="simple"/></inline-formula> = 13c, and c is the speed of light in vacuum [<xref ref-type="bibr" rid="scirp.69112-ref1">1</xref>] . Then</p><disp-formula id="scirp.69112-formula1027"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x27.png"  xlink:type="simple"/></disp-formula><p>That result means that, due to the smallness of the Earth in comparison to the Sun, its escape velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x28.png" xlink:type="simple"/></inline-formula> is orders of magnitude smaller than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x29.png" xlink:type="simple"/></inline-formula>. Hence, when both of those velocities meets in some point of the space, they pull each other, because they are the carriers of the respective gravity force.</p><p>Finally, from Equation (10) it is easy to obtain that</p><disp-formula id="scirp.69112-formula1028"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x30.png"  xlink:type="simple"/></disp-formula><p>Thus,</p><disp-formula id="scirp.69112-formula1029"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x31.png"  xlink:type="simple"/></disp-formula><p>But, this is the same numerical value given in (10).</p></sec><sec id="s4"><title>4. The Point of Meet</title><p>It is clear that in the meantime the escape velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x32.png" xlink:type="simple"/></inline-formula> travels 68,371 km, the escape velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x33.png" xlink:type="simple"/></inline-formula> travels a distance equal to 3.9 &#180; 10<sup>6</sup> km. Let us suppose that along the whole distance, those velocities maintain its values. Then, let the time transit that takes to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x34.png" xlink:type="simple"/></inline-formula> to travel the given distance, be the unit of measure; that is to say</p><disp-formula id="scirp.69112-formula1030"><graphic  xlink:href="http://html.scirp.org/file/69112x35.png"  xlink:type="simple"/></disp-formula><p>In that time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x36.png" xlink:type="simple"/></inline-formula> travels the distance</p><disp-formula id="scirp.69112-formula1031"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x37.png"  xlink:type="simple"/></disp-formula><p>in the meantime <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x38.png" xlink:type="simple"/></inline-formula> travels the distance</p><disp-formula id="scirp.69112-formula1032"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69112x39.png"  xlink:type="simple"/></disp-formula><p>Those results indicate that the point of meet occurs near the Earth</p></sec><sec id="s5"><title>5. Conclusions</title><p>It is proposed that in Gravitational Interactions, the Reciprocity Principle is valid for any couple of heavenly bodies that interact each other. Also, it is a useful concept, and a powerful tool to calculate the escape velocities and radius due to the apparent size of each body. In other words, its validity can be extended to the whole Universe. On the other hand, it is possible to prove that the ratios <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x40.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x41.png" xlink:type="simple"/></inline-formula> for two celestial bodies 1 and 2, respectively, are numerically equal. The same is valid for the ratios <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x42.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x43.png" xlink:type="simple"/></inline-formula>; in such a way that from this point of view; it is always true that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x44.png" xlink:type="simple"/></inline-formula>; and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x45.png" xlink:type="simple"/></inline-formula></p><p>where the prime refers the escape velocity of these bodies due to their apparent size.</p><p>In the case of the Sun-Earth System, it has that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x46.png" xlink:type="simple"/></inline-formula>; and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x47.png" xlink:type="simple"/></inline-formula></p><p>and also,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x48.png" xlink:type="simple"/></inline-formula>; and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69112x49.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s6"><title>Cite this paper</title><p>Angel Fierros Palacios, (2016) The Reciprocity Principle in Gravitational Interactions. Open Access Library Journal,03,1-4. doi: 10.4236/oalib.1102412</p></sec><sec id="s7"><title>Appendix</title><disp-formula id="scirp.69112-formula1033"><graphic  xlink:href="http://html.scirp.org/file/69112x50.png"  xlink:type="simple"/></disp-formula></sec></body><back><ref-list><title>References</title><ref id="scirp.69112-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Fierros Palacios, A. (2015) Gravitation. Scientific Research Publishing, Wuhan. In printing press.</mixed-citation></ref><ref id="scirp.69112-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Resnick, R. and Holliday, D. (1966) Physics. John Wiley and Sons Inc., Hoboken.</mixed-citation></ref></ref-list></back></article>