<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2013.44094</article-id><article-id pub-id-type="publisher-id">AM-30714</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>
 
 
  The Distances in the Stable Systems Due to the Virial Theorem
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>asan</surname><given-names>Arslan</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>Physics Department, Bing?l University, Bing?l, Turkey </addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hasanarslan46@yahoo.com</email></corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>04</month><year>2013</year></pub-date><volume>04</volume><issue>04</issue><fpage>688</fpage><lpage>689</lpage><history><date date-type="received"><day>January</day>	<month>30,</month>	<year>2013</year></date><date date-type="rev-recd"><day>March</day>	<month>4,</month>	<year>2013</year>	</date><date date-type="accepted"><day>March</day>	<month>11,</month>	<year>2013</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>
 
 
   The virial theorem is written by using the canonical equations of motion in classical mechanics. A moving particle with an initial speed in an n-particle system is considered. The distance of the moving particle from the origin of the system to the final position is derived as a function of the kinetic energy of the particle. It is thought that the considered particle would not collide with other particles in the system. The relation between the final and initial distance of the particle from the origin of the system is given by a single equation. 
 
</p></abstract><kwd-group><kwd>Virial Theorem; Distance; Stable System</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The calculations on the virial theorem are done to obtain an equation explaining the relations between the kinetic energy and potential energy of a particle and an equation describing the maximum distance travelled by this particle in a stable system. In Section 2, these equations are obtained due to the calculations. The previous works are searched. It was realized that the Equations (13) and (16) are first presented in this study. The calculations done in this study will be useful in astronomy. In Section 3, the results of this study are discussed.</p></sec><sec id="s2"><title>2. Calculations</title><p>The virial theorem gives the general equation between kinetic energy and potential energy of a stable system of n particles bound by potential forces. R. J. E. Claussius formulated the virial theorem in 1870 after twenty years long study [<xref ref-type="bibr" rid="scirp.30714-ref1">1</xref>]. The word “virial” comes from the Latin word vis which means “force” or “energy”. The reader who likes to learn more about the virial theorem is recommended to see the book [<xref ref-type="bibr" rid="scirp.30714-ref2">2</xref>]. The article [<xref ref-type="bibr" rid="scirp.30714-ref3">3</xref>] includes an extensive research on the virial theorem. The article [<xref ref-type="bibr" rid="scirp.30714-ref4">4</xref>] includes a search about finite deformations in the boundary conditions.</p><p>For system of masses at points <img src="13-7401376\2ae9594a-b359-48b1-ac83-3598008d95cb.jpg" /> the equations of motion are;</p><disp-formula id="scirp.30714-formula32746"><label>(1)</label><graphic position="anchor" xlink:href="13-7401376\3a2374fd-7ac8-4764-9fa0-e272619cf281.jpg"  xlink:type="simple"/></disp-formula><p>A quantity G is defined in [<xref ref-type="bibr" rid="scirp.30714-ref5">5</xref>] as:</p><disp-formula id="scirp.30714-formula32747"><label>(2)</label><graphic position="anchor" xlink:href="13-7401376\57f1ce27-28a4-4f90-9b4e-755a669779d1.jpg"  xlink:type="simple"/></disp-formula><p>The time derivative of this quantity is</p><disp-formula id="scirp.30714-formula32748"><label>(3)</label><graphic position="anchor" xlink:href="13-7401376\41cdd596-db32-4be2-8599-17752063a7ef.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.30714-formula32749"><label>(4)</label><graphic position="anchor" xlink:href="13-7401376\a379ae04-b74c-41f4-ab37-e7ee426bb25f.jpg"  xlink:type="simple"/></disp-formula><p>In Equations (3) and (4) T is the kinetic energy, m is the mass of the particle, p is the momentum related to the particle, F is the force acting on the particle, and r is the distance vector of the particle. We are going to obtain the virial theorem from the Equations (3) and (4) as below.</p><p>For a bounded quantity G, in a time interval of<img src="13-7401376\4a5d184b-3aaf-4262-b696-2dc9d51a483a.jpg" />, one can write:</p><disp-formula id="scirp.30714-formula32750"><label>(5)</label><graphic position="anchor" xlink:href="13-7401376\7b55af5c-aecb-4ad8-a18c-f375bfa93091.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.30714-formula32751"><label>(6)</label><graphic position="anchor" xlink:href="13-7401376\29dc1aae-13ed-450d-8119-cc01606599ec.jpg"  xlink:type="simple"/></disp-formula><p>if the momentum is periodic. Then we get the virial theorem as</p><disp-formula id="scirp.30714-formula32752"><label>(7)</label><graphic position="anchor" xlink:href="13-7401376\c2f70099-3b94-4248-8319-f8554b442c03.jpg"  xlink:type="simple"/></disp-formula><p>Writing T as</p><disp-formula id="scirp.30714-formula32753"><label>(8)</label><graphic position="anchor" xlink:href="13-7401376\2c2f1a70-3dac-4cfb-ac9d-7dee48244d94.jpg"  xlink:type="simple"/></disp-formula><p>and dropping the summation sign, the Equation (7) is written in the form:</p><disp-formula id="scirp.30714-formula32754"><label>(9)</label><graphic position="anchor" xlink:href="13-7401376\975cabb6-5aa9-4c44-a058-d38aa13ea798.jpg"  xlink:type="simple"/></disp-formula><p>In [<xref ref-type="bibr" rid="scirp.30714-ref6">6</xref>] the force is related to the Hamiltonian by</p><disp-formula id="scirp.30714-formula32755"><label>(10)</label><graphic position="anchor" xlink:href="13-7401376\c83fa365-4278-4189-8a29-3d08fe2ea6dd.jpg"  xlink:type="simple"/></disp-formula><p>The scalar product <img src="13-7401376\f2fe56ac-d66e-4ebe-a56b-ec5e7b47583b.jpg" /> has to result in a scalar quantity. Therefore, the vector r changes to the distance r in the following equations. By using this, the Equation (9) is written as</p><disp-formula id="scirp.30714-formula32756"><label>(11)</label><graphic position="anchor" xlink:href="13-7401376\35c18a53-f8f0-43d1-a1f1-5babefaca9bc.jpg"  xlink:type="simple"/></disp-formula><p>Here, the notation <img src="13-7401376\d309e874-6a24-4754-94df-3254795e4f8a.jpg" /> is used as the differential d. Integrating this equation we get</p><disp-formula id="scirp.30714-formula32757"><label>(12)</label><graphic position="anchor" xlink:href="13-7401376\af894b10-f674-4c26-a3d7-d423a69eb460.jpg"  xlink:type="simple"/></disp-formula><p>For a particle moving with constant speed and using H = E = T + V and q = r one can integrate from r<sub>0</sub> to r to find the relation between kinetic energy T and potential energy V in time averaged values as</p><disp-formula id="scirp.30714-formula32758"><label>(13)</label><graphic position="anchor" xlink:href="13-7401376\0dc46634-665d-4b07-96b5-09a111e6eece.jpg"  xlink:type="simple"/></disp-formula><p>For circular motion the equation is</p><disp-formula id="scirp.30714-formula32759"><label>(14)</label><graphic position="anchor" xlink:href="13-7401376\e8995e94-baae-4f0d-98ea-435e21d3b332.jpg"  xlink:type="simple"/></disp-formula><p>In this case, the Equation (12) gives the correct classical gravitational potential energy if we integrate it from <img src="13-7401376\0ae3faff-36fc-4652-8094-a6d572a8eb10.jpg" /> ;</p><disp-formula id="scirp.30714-formula32760"><label>(15)</label><graphic position="anchor" xlink:href="13-7401376\67de0a85-4937-4f23-b3e5-edc74e738e05.jpg"  xlink:type="simple"/></disp-formula><p>If we relate to this study, M is the mass of the set of particles in the system and m is the mass of the particle under consideration. The Equation (13) can be written as</p><disp-formula id="scirp.30714-formula32761"><label>(16)</label><graphic position="anchor" xlink:href="13-7401376\4fb349b4-89f4-421e-8038-18719711a03c.jpg"  xlink:type="simple"/></disp-formula><p>This is the equation for the kinetic energy T of a particle in a stable system at distance r from the origin of the system. E is the total energy of the particle, and <img src="13-7401376\19bf7c77-d8a6-4bd5-b71c-98862dd3cd5c.jpg" /> is the initial distance of the particle from the origin of the system.</p></sec><sec id="s3"><title>3. Conclusion</title><p>The Equation (16) derived in this study explains that the distance of a moving particle in a stable system has a maximum distance r if it remains in the system. The maximum distance must be the distance from the origin of the system to the outer surface of the system at most. When something moves away from the distance to the outer surface, it is out of the system. In other words, it can be said that; when this is reached, the stability of the system is destroyed or the travelled body is not a member of the system. The Equations (13) and (16) are first derived here comparing to the previous works.</p></sec><sec id="s4"><title>4. Acknowledgements</title><p>I would like to thank to Prof. Dr. Amirullah Mamedov for his valuable discussion.</p></sec><sec id="s5"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.30714-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">G. W. Collins II, “The Virial Theorem in Stellar Astrophics,” 2003. 
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