<?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.2019.53043</article-id><article-id pub-id-type="publisher-id">JHEPGC-93668</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>
 
 
  On Intrinsic Rotation of Bodies
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ogaba</surname><given-names>Philip Obande</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>Retired, Department of Chemistry, Ahmadu Bello University, Zaria, Nigeria</addr-line></aff><pub-date pub-type="epub"><day>08</day><month>05</month><year>2019</year></pub-date><volume>05</volume><issue>03</issue><fpage>868</fpage><lpage>883</lpage><history><date date-type="received"><day>5,</day>	<month>May</month>	<year>2019</year></date><date date-type="rev-recd"><day>12,</day>	<month>July</month>	<year>2019</year>	</date><date date-type="accepted"><day>15,</day>	<month>July</month>	<year>2019</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>
 
 
  Spontaneous rotation of matter is investigated. The results provide further evidence in support of earlier indications of a wave-only reality in which the quantum energy packet exists in the form of a conjugate wave—particle doublet. It reveals that matter, be it wave or particle, is a harmonic oscillator defined with full spectrum of the usual mechanical properties of simple harmonic motion SHM. Notably, the quantum energy packet’s stress field correlates with radius to generate intrinsic torque, it motivates spontaneous rotation at all levels of the cosmic mass scale from the electron to the universe; its atomic and natural units are 
  <inline-formula><inline-graphic xlink:href="dit_b1201a5c-1112-433d-882c-82e6235ded4d.png" xlink:type="simple"/></inline-formula>and 
  <inline-formula><inline-graphic xlink:href="dit_6b00e027-6319-4da9-9008-1685d9c4e7eb.png" xlink:type="simple"/></inline-formula> respectively for matter’s wave (bosonic) and particulate (fermionic) forms. The proton’s observational internal pressure 
  <inline-formula><inline-graphic xlink:href="dit_5350f110-bfcd-4d87-b236-9571c02f99a2.png" xlink:type="simple"/></inline-formula>Pa reported recently by Burkert 
  et al. deviates markedly from the theoretical value ~10
  <sup>22</sup> Pa, the difference attributes to challenges with existing energy measurement procedures. Velocities of electron waveform in random thermal motion evaluated with the new approach agree remarkably well with values obtained with kinetic-molecular theory KT; much more importantly, the analysis reveals existence, at standard conditions, of electron waveform’s hyper-luminal root-mean-square velocity, 
  <inline-formula><inline-graphic xlink:href="dit_7b7ae99c-cde3-467d-8192-94f22204c474.png" xlink:type="simple"/></inline-formula>, if verified, this finding might inform on-going neutrino research. The evidence suggests that effects formalized in the theories of thermodynamics and kinetics trace to mobile torque fields.
 
</p></abstract><kwd-group><kwd>Atomic Internal Pressure</kwd><kwd> Atomic Mechanical Property</kwd><kwd> Atomic Torque Unit</kwd><kwd> Hyper-Luminal Speed</kwd><kwd> Metric Space Expansion</kwd><kwd> Spontaneous Rotation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>As observed recently, Ellis &amp; Silk [<xref ref-type="bibr" rid="scirp.93668-ref1">1</xref>], physics is, indeed, “Faced with difficulties in applying fundamental theories to the observed universe…”. Of immediate relevance is the search for tenable account of scale-free observational rotation of: the photon, Beth [<xref ref-type="bibr" rid="scirp.93668-ref2">2</xref>], Leach et al. [<xref ref-type="bibr" rid="scirp.93668-ref3">3</xref>]; the atom, Jaffe [<xref ref-type="bibr" rid="scirp.93668-ref4">4</xref>], Peterson [<xref ref-type="bibr" rid="scirp.93668-ref5">5</xref>]; the galaxy, Raghuprasad [<xref ref-type="bibr" rid="scirp.93668-ref6">6</xref>], Tsati et al. [<xref ref-type="bibr" rid="scirp.93668-ref7">7</xref>] and the active galactic nucleus (black hole), McClintock et al. [<xref ref-type="bibr" rid="scirp.93668-ref8">8</xref>], Imanishi et al. [<xref ref-type="bibr" rid="scirp.93668-ref9">9</xref>]; they all rotate but the causality remains unknown, Williams and van der Mark [<xref ref-type="bibr" rid="scirp.93668-ref10">10</xref>]. The prevailing notion is undecided. At the atomic level, we have brilliant cases that attempt to convince that choreographed dance steps of constituent “embryonic” quarks and gluons inside the atomic sac give rise to proton spin with the gluon field dominating the stage, Shea [<xref ref-type="bibr" rid="scirp.93668-ref11">11</xref>]. To our best knowledge, no attempt exists to extend the idea to sub- and supra-proton species with explanation for how well the notion sits with the atomic point-mass concept. At the cosmic level the authorities attribute rotation to imbalance (“asymmetry”) of forces acting on a body in gravity-motivated collapse, Spagna [<xref ref-type="bibr" rid="scirp.93668-ref12">12</xref>], Palacios [<xref ref-type="bibr" rid="scirp.93668-ref13">13</xref>], Benesch [<xref ref-type="bibr" rid="scirp.93668-ref14">14</xref>], Crawford [<xref ref-type="bibr" rid="scirp.93668-ref15">15</xref>]. Many, particularly among the student population, find this explanation less than satisfactory as evident from lively exchanges at the Physics Forum [<xref ref-type="bibr" rid="scirp.93668-ref16">16</xref>] which center on the popular but erroneous notion that “The spin of elementary particles [isn’t] ‘normal’ Newtonian force vector but rather a property of the particle itself…”.</p><p>The privilege of an observational theory of the atom now enables us to see that Dirac [<xref ref-type="bibr" rid="scirp.93668-ref17">17</xref>] was in error in his concepts of the “singularity” and the atomic “point-mass”. As proposed earlier by Born [<xref ref-type="bibr" rid="scirp.93668-ref18">18</xref>], the atom is indeed “extended” and imbued with elaborate structures and mechanical properties, Golubev [<xref ref-type="bibr" rid="scirp.93668-ref19">19</xref>], Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>]. Sadly, Dirac [<xref ref-type="bibr" rid="scirp.93668-ref17">17</xref>] also established the supremacy of elegance with the historic position that the aim “is not so much to get a model of an electron as to get a simple scheme of equations which can be used to calculate all the results that can be obtained from experiment”; the position sustains a storm that rages on, Hossenfelder [<xref ref-type="bibr" rid="scirp.93668-ref21">21</xref>], Wilczek [<xref ref-type="bibr" rid="scirp.93668-ref22">22</xref>]. Theory rules out the “singularity” and rejects the atomic “point mass” conjecture, we side with others, Rugh &amp; Zinkernagel [<xref ref-type="bibr" rid="scirp.93668-ref23">23</xref>] who attribute the current crisis to these two foundational errors. The positions are contrary to nature, therefore, cannot describe same; they leave no room for contemplation of structured co-ordinate space and intrinsic mechanical properties of the quantum energy packet. Perpetual motion of any kind cannot exist without a perpetuating agent and the latter is inconceivable for a point mass and structureless space.</p><p>No one seems to question the basis of Newton’s translational second law, not so with the rotational second law, physicists are interested in how perpetual rotation is contrived. Of course, a body cannot be in perpetual rotational motion unless impacted upon by a perpetuating torque, see, for instance, Rees [<xref ref-type="bibr" rid="scirp.93668-ref24">24</xref>] but, no one seems to know just how nature manufactures torque in an isolated body. The result of a recent attempt to trace the physical origin of torque and of the rotational second law was not quite satisfactory, Cross [<xref ref-type="bibr" rid="scirp.93668-ref25">25</xref>], neither was a subsequent attempt to improve upon the first, Gorbatyy and Tarsov [<xref ref-type="bibr" rid="scirp.93668-ref26">26</xref>]. In any case, use of a force carrier in the form of a rod connecting the mass to a pivot automatically rules out any semblance of Cross’ model to an isolated body such as the atom or the galaxy. The problem centers on a simple question: How does nature, using no force carrier, create matter’s rotation at each rung of the hierarchical structures that define the cosmic mass scale? We have accumulated overwhelming evidences in support of the “extended” atom, see, e.g., Obande ( [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.93668-ref27">27</xref>] ); based on the atom’s internal structure and dynamics, we attempt here a quantitative account of Newton’s second law of translational, rotational or any other mode of motion.</p>Wave, Particle or Wave-Particle?<p>The outcome of a debate on the nature of reality: Is it field or particle? SCIAM [<xref ref-type="bibr" rid="scirp.93668-ref28">28</xref>], expertly summarized by Kuhlman [<xref ref-type="bibr" rid="scirp.93668-ref29">29</xref>], came up with the unavoidable conclusion that reality is wave-only. It tallies with consistent theoretical and experimental results reported by investigators widely separated in time and in space, Descartes [<xref ref-type="bibr" rid="scirp.93668-ref30">30</xref>], Madelung [<xref ref-type="bibr" rid="scirp.93668-ref31">31</xref>], Born [<xref ref-type="bibr" rid="scirp.93668-ref18">18</xref>], Macken [<xref ref-type="bibr" rid="scirp.93668-ref32">32</xref>], Hobson [<xref ref-type="bibr" rid="scirp.93668-ref33">33</xref>], Obande [<xref ref-type="bibr" rid="scirp.93668-ref34">34</xref>], Consiglio [<xref ref-type="bibr" rid="scirp.93668-ref35">35</xref>], Kirakosyan [<xref ref-type="bibr" rid="scirp.93668-ref36">36</xref>]; it now seems capable of generating renewed research interest, Wilczek [<xref ref-type="bibr" rid="scirp.93668-ref37">37</xref>], Colbert and Renner [<xref ref-type="bibr" rid="scirp.93668-ref38">38</xref>]. As observed recently, “whether it appears as radiation or as mass, energy is a radiative phenomenon”, Laidlaw [<xref ref-type="bibr" rid="scirp.93668-ref39">39</xref>]. Musser [<xref ref-type="bibr" rid="scirp.93668-ref40">40</xref>] suggests that “Physicists will need to find some new foundational structure …”, we beg to differ, there has, for over four centuries, always been one—the wave-only imponderable material vacuum field defined with articulated structures and mechanical properties. One of the most informative descriptions of this “foundational structure” is available at Physics Forum posted by a well-informed source with the pseudonym “Good Elf” [<xref ref-type="bibr" rid="scirp.93668-ref41">41</xref>] sadly, it constrains independent interaction. Consistent results of our investigations point to a reality that is essentially field defined, on the one hand, with the following fundamental quantum vacuum (boson field) characteristics: oscillation frequency ϑ w = 1.0 s − 1 , angular speed c o = 2.99792458 &#215; 10 8 rad ⋅ s − 1 , not m&#183;s<sup>−1</sup> and energy E w = h ϑ w = 6.62607 &#215; 10 − 34 J and, on the other hand, with the following fundamental quantum matter (fermion field) characteristics: ϑ p = 2.034 s − 1 , c o = 3.71535229 &#215; 10 − 14 rad ⋅ s − 1 and E p = h ϑ p = 1.34774 &#215; 10 − 33 J . It delivers a classical field theory (CFT) absolutely free of existing crises of the probabilistic theory but, it’s quantitative approach is easily dismissible for being rather simplistic and desperately devoid of even a pretence at elegance. The approach, however, more than compensates for these “shortcomings” in providing a most formidable theoretical analytical tool, see, for instance, Obande ( [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.93668-ref42">42</xref>] [<xref ref-type="bibr" rid="scirp.93668-ref43">43</xref>] ); here, we employ its analytical power to probe intrinsic rotation of matter.</p></sec><sec id="s2"><title>2. Procedure</title><p>The quantum packet’s field parameters are generated from classical (Newtonian) expressions for radius r, density ρ, angular speed ω, centripetal force F, tensile modulus є, longitudinal stress σ and strain τ using the element’s ϑ and m values. Field-specific correlation of values of these parameters yields the desired property, the details have been reported, Obande ( [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.93668-ref44">44</xref>] [<xref ref-type="bibr" rid="scirp.93668-ref45">45</xref>] ).</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>The results are presented in two figures and five tables. <xref ref-type="fig" rid="fig1">Figure 1</xref> is a plot of values of the atom’s bosonic r<sub>w</sub> and fermionic r<sub>p</sub> radii versus mass number Z<sub>n</sub> while <xref ref-type="fig" rid="fig2">Figure 2</xref> is a plot of r<sub>w</sub> versus r<sub>p</sub>. <xref ref-type="table" rid="table1">Table 1</xref> is a compilation of some of nature’s torque fields; <xref ref-type="table" rid="table2">Table 2</xref> lists some tensile properties of the atomic harmonic oscillator; <xref ref-type="table" rid="table3">Table 3</xref> presents evidence for periodic variation in values of the ratio r<sub>w</sub>/r<sub>p</sub>; <xref ref-type="table" rid="table4">Table 4</xref> is a list of some observational effects of the atom’s intrinsic strain and <xref ref-type="table" rid="table5">Table 5</xref> presents internal stress (pressure) σ<sub>p</sub> values for a sample of elements in the visible universe U p o and in its invisible analogue U ′ p .</p><p>The torque field identifies by its unit following dimensional analysis of the coefficient of correlation of two interacting parameters, it must include the generic term Newton-meter N m. For example, field stress couples with radius to give, σ p r p 4 = Γ n u = 3.867 &#215; 10 − 47 kg ⋅ m 3 ⋅ s − 2 , Equation (4), the waveform equivalent is σ w r w 4 = Γ a u = 3.162 &#215; 10 − 25 kg ⋅ m 3 ⋅ s − 2 , these coefficients are the primitive causality of rotation, they are the natural unit Γ<sub>nu</sub> and the atomic unit Γ<sub>au</sub> of torque. Notice the similarity between the difference 8 &#215; 10<sup>21</sup> and the “molar” constant N<sub>A</sub> = 6.022 &#215; 10<sup>23</sup> units. We examine the data in <xref ref-type="table" rid="table1">Table 1</xref>.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Nature’s causal torque fields and rotation-motivated effects (ref. Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>] )</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Equation</th><th align="center" valign="middle" >Correlation coefficient</th><th align="center" valign="middle" >Correlation coefficient</th><th align="center" valign="middle" >Fundamental</th><th align="center" valign="middle" >Observational</th></tr></thead><tr><td align="center" valign="middle" >No.</td><td align="center" valign="middle" >Graphical</td><td align="center" valign="middle" >Computed</td><td align="center" valign="middle" >Constant</td><td align="center" valign="middle" >Effect</td></tr><tr><td align="center" valign="middle" >1)</td><td align="center" valign="middle" >ρ p / τ p 4 = 2.089 &#215; 10 − 19</td><td align="center" valign="middle" >2.074 &#215; 10<sup>−19</sup> N m</td><td align="center" valign="middle" >1.602 &#215; 10<sup>−19</sup> C</td><td align="center" valign="middle" >Charge quant.—false</td></tr><tr><td align="center" valign="middle" >2)</td><td align="center" valign="middle" >F p / ϑ p 2 = 5.248 &#215; 10 − 19</td><td align="center" valign="middle" >3.548 &#215; 10<sup>−19</sup> N m</td><td align="center" valign="middle" >1.602 &#215; 10<sup>−19</sup> C</td><td align="center" valign="middle" >Charge quant.—false</td></tr><tr><td align="center" valign="middle" >3)</td><td align="center" valign="middle" >ρ w / ϑ w 4 = 5.248 &#215; 10 − 19</td><td align="center" valign="middle" >1.069 &#215; 10<sup>−19</sup> N m (m/s)<sup>−3</sup> rad/s<sup>−1</sup></td><td align="center" valign="middle" >1.602 &#215; 10<sup>−19</sup> C</td><td align="center" valign="middle" >Charge quant.—false</td></tr><tr><td align="center" valign="middle" >4)</td><td align="center" valign="middle" >σ p r p 4 = 3.890 &#215; 10 − 47</td><td align="center" valign="middle" >3.867 &#215; 10<sup>−47</sup> kg m<sup>3</sup> s<sup>−2</sup></td><td align="center" valign="middle" >Unknown (new)</td><td align="center" valign="middle" >Rotation of matter</td></tr><tr><td align="center" valign="middle" >5)</td><td align="center" valign="middle" >r w ρ w 0.25 = 2.291 &#215; 10 − 11</td><td align="center" valign="middle" >2.266 &#215; 10<sup>−11</sup> (N m)<sup>0.25</sup></td><td align="center" valign="middle" >6.674 &#215; 10<sup>−11</sup> m<sup>3</sup>&#183;kg<sup>−1</sup>s<sup>−2</sup></td><td align="center" valign="middle" >Grav. Constant</td></tr><tr><td align="center" valign="middle" >6)</td><td align="center" valign="middle" >ρ w / ϵ w 1.33 = 2.754 &#215; 10 − 11</td><td align="center" valign="middle" >2.610 &#215; 10<sup>−11</sup> (mr<sup>2</sup>ω)<sup>−0.3</sup> (m/s)<sup>−2.3</sup></td><td align="center" valign="middle" >6.674 &#215; 10<sup>−11</sup>m<sup>3</sup>&#183;kg<sup>−1</sup>s<sup>−2</sup></td><td align="center" valign="middle" >Grav. Constant</td></tr><tr><td align="center" valign="middle" >7)</td><td align="center" valign="middle" >r p ρ p 0.25 = 6.792 &#215; 10 − 6</td><td align="center" valign="middle" >5.712 &#215; 10<sup>−6</sup> (N m)<sup>0.25</sup></td><td align="center" valign="middle" >~1.0 &#215; 10<sup>−6</sup> m&#183;s<sup>−2</sup> (gal.)</td><td align="center" valign="middle" >Grav. Accl. Const.</td></tr><tr><td align="center" valign="middle" >8)</td><td align="center" valign="middle" >ϵ w / σ w 0.75 = 2 . 35 0 &#215; 1 0 − 6</td><td align="center" valign="middle" >2.348 &#215; 10<sup>−6</sup> (N m)<sup>0.25</sup> (m/s)<sup>0.5</sup></td><td align="center" valign="middle" >~1.0 &#215; 10<sup>−6</sup> m&#183;s<sup>−2</sup> (gal.)</td><td align="center" valign="middle" >Grav. Accl. Const.</td></tr><tr><td align="center" valign="middle" >9)</td><td align="center" valign="middle" >m p / ρ p 0.25 = 1.318 &#215; 10 − 15</td><td align="center" valign="middle" >1.352 &#215; 10<sup>−15</sup> (N m)<sup>0.75</sup></td><td align="center" valign="middle" >2.068 &#215; 10<sup>−15</sup> Wb</td><td align="center" valign="middle" >Mag. flux density</td></tr><tr><td align="center" valign="middle" >10)</td><td align="center" valign="middle" >F w / τ w 2 = 9.772 &#215; 10 − 24</td><td align="center" valign="middle" >9.676 &#215; 10<sup>−24</sup> N m (rad/s)<sup>2</sup></td><td align="center" valign="middle" >9.285 &#215; 10<sup>−24</sup> J&#183;T<sup>−1</sup></td><td align="center" valign="middle" >Electron. mag. momt.</td></tr><tr><td align="center" valign="middle" >11)</td><td align="center" valign="middle" >r w / σ w 0.25 = 7.482 &#215; 10 − 7</td><td align="center" valign="middle" >7.474 &#215; 10<sup>−7</sup> (N m)<sup>0.25</sup> (m/s)<sup>0.25</sup></td><td align="center" valign="middle" >12.566 &#215; 10<sup>−7</sup> N&#183;A<sup>−2</sup></td><td align="center" valign="middle" >Mag. perm. const.</td></tr><tr><td align="center" valign="middle" >12)</td><td align="center" valign="middle" >F w / σ w 0.5 = 1.778 &#215; 10 − 12</td><td align="center" valign="middle" >1.755 &#215; 10<sup>−12</sup> (N m)<sup>0.5</sup> m/s<sup>−1</sup></td><td align="center" valign="middle" >8.854 &#215; 10<sup>−12</sup> F&#183;m<sup>−1</sup></td><td align="center" valign="middle" >Electric. perm. const.</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Rotational properties of the isolated atom</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Property</th><th align="center" valign="middle" >E</th><th align="center" valign="middle" >H</th><th align="center" valign="middle" >Fe</th><th align="center" valign="middle" >Br</th><th align="center" valign="middle" >Ba</th><th align="center" valign="middle" >U</th></tr></thead><tr><td align="center" valign="middle" >ϑ<sub>w</sub>/s<sup>−1</sup></td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >2048.00</td><td align="center" valign="middle" >2.10 &#215; 10<sup>6</sup></td><td align="center" valign="middle" >3.93 &#215; 10<sup>6</sup></td><td align="center" valign="middle" >1.34 &#215; 10<sup>8</sup></td><td align="center" valign="middle" >4.83 &#215; 10<sup>9</sup></td></tr><tr><td align="center" valign="middle" >ϑ<sub>p</sub>/s<sup>−1</sup></td><td align="center" valign="middle" >2.00</td><td align="center" valign="middle" >3072.00</td><td align="center" valign="middle" >1.15 &#215; 10<sup>5</sup></td><td align="center" valign="middle" >1.64 &#215; 10<sup>5</sup></td><td align="center" valign="middle" >2.81 &#215; 10<sup>5</sup></td><td align="center" valign="middle" >4.87 &#215; 10<sup>5</sup></td></tr><tr><td align="center" valign="middle" >ω<sub>w</sub>/rad s<sup>−1</sup></td><td align="center" valign="middle" >6.28</td><td align="center" valign="middle" >1.29 &#215; 10<sup>4</sup></td><td align="center" valign="middle" >1.32 &#215; 10<sup>7</sup></td><td align="center" valign="middle" >2.47 &#215; 10<sup>7</sup></td><td align="center" valign="middle" >8.43 &#215; 10<sup>8</sup></td><td align="center" valign="middle" >4.05 &#215; 10<sup>10</sup></td></tr><tr><td align="center" valign="middle" >ω<sub>p</sub>/rad s<sup>−1</sup></td><td align="center" valign="middle" >12.78</td><td align="center" valign="middle" >2.62 &#215; 10<sup>4</sup></td><td align="center" valign="middle" >7.31 &#215; 10<sup>5</sup></td><td align="center" valign="middle" >1.05 &#215; 10<sup>6</sup></td><td align="center" valign="middle" >1.80 &#215; 10<sup>6</sup></td><td align="center" valign="middle" >3.12 &#215; 10<sup>6</sup></td></tr><tr><td align="center" valign="middle" >r<sub>w</sub>/m</td><td align="center" valign="middle" >1.5 &#215; 10<sup>8</sup></td><td align="center" valign="middle" >7.32 &#215; 10<sup>4</sup></td><td align="center" valign="middle" >71.48</td><td align="center" valign="middle" >38.10</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >3.10 &#215; 10<sup>−2</sup></td></tr><tr><td align="center" valign="middle" >r<sub>p</sub>/m</td><td align="center" valign="middle" >9.1 &#215; 10<sup>−15</sup></td><td align="center" valign="middle" >4.46 &#215; 10<sup>−18</sup></td><td align="center" valign="middle" >1.60 &#215; 10<sup>−19</sup></td><td align="center" valign="middle" >1.12 &#215; 10<sup>−19</sup></td><td align="center" valign="middle" >6.49 &#215; 10<sup>−20</sup></td><td align="center" valign="middle" >3.75 10<sup>−20</sup></td></tr><tr><td align="center" valign="middle" >m<sub>w</sub>/kg atom<sup>−1</sup></td><td align="center" valign="middle" >7.37 &#215; 10<sup>−51</sup></td><td align="center" valign="middle" >1.51 &#215; 10<sup>−47</sup></td><td align="center" valign="middle" >1.54 &#215; 10<sup>−41</sup></td><td align="center" valign="middle" >2.90 &#215; 10<sup>−41</sup></td><td align="center" valign="middle" >9.88 &#215; 10<sup>−40</sup></td><td align="center" valign="middle" >3.56 &#215; 10<sup>−38</sup></td></tr><tr><td align="center" valign="middle" >m<sub>p</sub>/kg u<sup>−1</sup></td><td align="center" valign="middle" >4.88 &#215; 10<sup>−7</sup></td><td align="center" valign="middle" >1.00 &#215; 10<sup>−3</sup></td><td align="center" valign="middle" >56.00</td><td align="center" valign="middle" >80.00</td><td align="center" valign="middle" >137.34</td><td align="center" valign="middle" >238.00</td></tr><tr><td align="center" valign="middle" >ρ<sub>w</sub>/kgm<sup>−3</sup></td><td align="center" valign="middle" >5.23 &#215; 10<sup>−76</sup></td><td align="center" valign="middle" >9.19 &#215; 10<sup>−63</sup></td><td align="center" valign="middle" >1.01 &#215; 10<sup>−50</sup></td><td align="center" valign="middle" >1.25 &#215; 10<sup>−49</sup></td><td align="center" valign="middle" >1.70 &#215; 10<sup>−43</sup></td><td align="center" valign="middle" >2.85 &#215; 10<sup>−37</sup></td></tr><tr><td align="center" valign="middle" >ρ<sub>p</sub>/kgm<sup>−3</sup></td><td align="center" valign="middle" >3.06 &#215; 10<sup>35</sup></td><td align="center" valign="middle" >5.39 &#215; 10<sup>48</sup></td><td align="center" valign="middle" >3.27 &#215; 10<sup>54</sup></td><td align="center" valign="middle" >1.37 &#215; 10<sup>55</sup></td><td align="center" valign="middle" >1.20 &#215; 10<sup>56</sup></td><td align="center" valign="middle" >1.08 &#215; 10<sup>57</sup></td></tr><tr><td align="center" valign="middle" >F<sub>w</sub>/N</td><td align="center" valign="middle" >4.36 &#215; 10<sup>−41</sup></td><td align="center" valign="middle" >1.83 &#215; 10<sup>−34</sup></td><td align="center" valign="middle" >1.92 &#215; 10<sup>−28</sup></td><td align="center" valign="middle" >6.75 &#215; 10<sup>−28</sup></td><td align="center" valign="middle" >7.86 &#215; 10<sup>−25</sup></td><td align="center" valign="middle" >1.02 &#215; 10<sup>−21</sup></td></tr><tr><td align="center" valign="middle" >F<sub>p</sub>/N</td><td align="center" valign="middle" >1.46 &#215; 10<sup>−18</sup></td><td align="center" valign="middle" >6.11 &#215; 10<sup>−12</sup></td><td align="center" valign="middle" >4.77 &#215; 10<sup>−9</sup></td><td align="center" valign="middle" >9.75 &#215; 10<sup>−9</sup></td><td align="center" valign="middle" >2.88 &#215; 10<sup>−8</sup></td><td align="center" valign="middle" >8.66 10<sup>−8</sup></td></tr><tr><td align="center" valign="middle" >ϵ<sub>w</sub>/Pa</td><td align="center" valign="middle" >2.91 &#215; 10<sup>−49</sup></td><td align="center" valign="middle" >2.50 &#215; 10<sup>−35</sup></td><td align="center" valign="middle" >2.68 &#215; 10<sup>−30</sup></td><td align="center" valign="middle" >1.76 &#215; 10<sup>−29</sup></td><td align="center" valign="middle" >7.04 &#215; 10<sup>−25</sup></td><td align="center" valign="middle" >3.28 &#215; 10<sup>−20</sup></td></tr><tr><td align="center" valign="middle" >ϵ<sub>p</sub>/Pa</td><td align="center" valign="middle" >1.60 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >1.37 &#215; 10<sup>6</sup></td><td align="center" valign="middle" >2.98 &#215; 10<sup>10</sup></td><td align="center" valign="middle" >8.74 &#215; 10<sup>10</sup></td><td align="center" valign="middle" >4.44 &#215; 10<sup>11</sup></td><td align="center" valign="middle" >2.31 &#215; 10<sup>12</sup></td></tr><tr><td align="center" valign="middle" >σ<sub>w</sub>/Pa</td><td align="center" valign="middle" >6.18 &#215; 10<sup>−58</sup></td><td align="center" valign="middle" >1.09 &#215; 10<sup>−44</sup></td><td align="center" valign="middle" >1.20 &#215; 10<sup>−32</sup></td><td align="center" valign="middle" >1.48 &#215; 10<sup>−31</sup></td><td align="center" valign="middle" >2.00 &#215; 10<sup>−25</sup></td><td align="center" valign="middle" >3.37 &#215; 10<sup>−19</sup></td></tr><tr><td align="center" valign="middle" >σ<sub>p</sub>/Pa</td><td align="center" valign="middle" >5.56 &#215; 10<sup>9</sup></td><td align="center" valign="middle" >9.79 &#215; 10<sup>22</sup></td><td align="center" valign="middle" >5.95 &#215; 10<sup>28</sup></td><td align="center" valign="middle" >2.49 &#215; 10<sup>29</sup></td><td align="center" valign="middle" >2.18 &#215; 10<sup>30</sup></td><td align="center" valign="middle" >1.96 &#215; 10<sup>31</sup></td></tr><tr><td align="center" valign="middle" >τ<sub>w</sub>/%</td><td align="center" valign="middle" >2.12 &#215; 10<sup>−11</sup></td><td align="center" valign="middle" >4.35 &#215; 10<sup>−8</sup></td><td align="center" valign="middle" >4.45 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >8.35 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >2.85 &#215; 10<sup>−3</sup></td><td align="center" valign="middle" >0.10</td></tr><tr><td align="center" valign="middle" >τ<sub>p</sub>/%</td><td align="center" valign="middle" >3.49 &#215; 10<sup>11</sup></td><td align="center" valign="middle" >7.14 &#215; 10<sup>14</sup></td><td align="center" valign="middle" >1.99 &#215; 10<sup>16</sup></td><td align="center" valign="middle" >2.85 &#215; 10<sup>16</sup></td><td align="center" valign="middle" >4.90 &#215; 10<sup>16</sup></td><td align="center" valign="middle" >8.50 &#215; 10<sup>16</sup></td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Variation of atomic wave/particle radii ratio of the chemical element</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Element</th><th align="center" valign="middle" >e-He</th><th align="center" valign="middle" >Li-B</th><th align="center" valign="middle" >O-Na</th><th align="center" valign="middle" >Mg-K</th><th align="center" valign="middle" >Ti-Zr</th><th align="center" valign="middle" >Nb-Pr</th><th align="center" valign="middle" >Nd-Fr</th><th align="center" valign="middle" >Ra-Am</th></tr></thead><tr><td align="center" valign="middle" >log(r<sub>w</sub>/r<sub>p</sub>)</td><td align="center" valign="middle" >22.2</td><td align="center" valign="middle" >22.5 - 22.2</td><td align="center" valign="middle" >22.0</td><td align="center" valign="middle" >21.8 - 21.4</td><td align="center" valign="middle" >20.9 - 20.0</td><td align="center" valign="middle" >19.9 - 19.0</td><td align="center" valign="middle" >18.9 - 18.5</td><td align="center" valign="middle" >18.2 - 17.8</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Some observational effects of intrinsic atomic strain</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" >Boson Field</th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >Correl.</td><td align="center" valign="middle" >ϑ<sub>w</sub>/τ<sub>w</sub></td><td align="center" valign="middle" >m<sub>w</sub>/τ<sub>w</sub></td><td align="center" valign="middle" >r<sub>w</sub>τ<sub>w</sub></td><td align="center" valign="middle" >ρ w / τ w 4</td><td align="center" valign="middle" >ω<sub>w</sub>/τ<sub>w</sub></td><td align="center" valign="middle" >F w / τ w 2</td><td align="center" valign="middle" >ϵ w / τ w 3</td><td align="center" valign="middle" >σ w / τ w 4</td></tr><tr><td align="center" valign="middle" >Coeff.</td><td align="center" valign="middle" >4.7 &#215; 10<sup>8</sup></td><td align="center" valign="middle" >3.55 &#215; 10<sup>42</sup></td><td align="center" valign="middle" >0.3184</td><td align="center" valign="middle" >2.57 &#215; 10<sup>−41</sup></td><td align="center" valign="middle" >2.96 &#215; 10<sup>9</sup></td><td align="center" valign="middle" >9.77 &#215; 10<sup>−24</sup></td><td align="center" valign="middle" >3.09 &#215; 10<sup>−23</sup></td><td align="center" valign="middle" >3.09 &#215; 10<sup>−23</sup></td></tr><tr><td align="center" valign="middle" >Effect</td><td align="center" valign="middle" >Radiation</td><td align="center" valign="middle" >polarizability</td><td align="center" valign="middle" >1/π</td><td align="center" valign="middle" >Polarizability</td><td align="center" valign="middle" >Magnetic</td><td align="center" valign="middle" >μ<sub>e</sub></td><td align="center" valign="middle" >μ<sub>au</sub></td><td align="center" valign="middle" >μ<sub>au</sub></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Fermion Field</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Correl.</td><td align="center" valign="middle" >ϑ<sub>p</sub>/τ<sub>p</sub></td><td align="center" valign="middle" >m<sub>p</sub>/τ<sub>p</sub></td><td align="center" valign="middle" >r<sub>p</sub>τ<sub>p</sub></td><td align="center" valign="middle" >ρ p / τ p 4</td><td align="center" valign="middle" >ω<sub>p</sub>/τ<sub>p</sub></td><td align="center" valign="middle" >F p / τ p 2</td><td align="center" valign="middle" >ϵ p / τ p 3</td><td align="center" valign="middle" >σ p / τ p 4</td></tr><tr><td align="center" valign="middle" >Coeff.</td><td align="center" valign="middle" >5.89 &#215; 10<sup>−14</sup></td><td align="center" valign="middle" >2.82 &#215; 10<sup>−20</sup></td><td align="center" valign="middle" >0.3184</td><td align="center" valign="middle" >2.09 &#215; 10<sup>−20</sup></td><td align="center" valign="middle" >7.31 &#215; 10<sup>−14</sup></td><td align="center" valign="middle" >1.2 &#215; 10<sup>−45</sup></td><td align="center" valign="middle" >3.8 &#215; 10<sup>−45</sup></td><td align="center" valign="middle" >3.8 &#215; 10<sup>−45</sup></td></tr><tr><td align="center" valign="middle" >Effect</td><td align="center" valign="middle" >Radiation</td><td align="center" valign="middle" >Charge</td><td align="center" valign="middle" >1/π</td><td align="center" valign="middle" >Charge</td><td align="center" valign="middle" >Radiation</td><td align="center" valign="middle" >Torque</td><td align="center" valign="middle" >Torque</td><td align="center" valign="middle" >Torque</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> The particulate atom’s internal pressure (σ/Pa) in U p o and U ′ p </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Element</th><th align="center" valign="middle" >e</th><th align="center" valign="middle" >H</th><th align="center" valign="middle" >Fe</th><th align="center" valign="middle" >Br</th><th align="center" valign="middle" >Ba</th><th align="center" valign="middle" >U</th></tr></thead><tr><td align="center" valign="middle" >( U p o ) σ/Pa</td><td align="center" valign="middle" >5.56 &#215; 10<sup>9</sup></td><td align="center" valign="middle" >9.79 &#215; 10<sup>22</sup></td><td align="center" valign="middle" >5.95 &#215; 10<sup>28</sup></td><td align="center" valign="middle" >2.49 &#215; 10<sup>29</sup></td><td align="center" valign="middle" >2.17 &#215; 10<sup>30</sup></td><td align="center" valign="middle" >1.97 &#215; 10<sup>31</sup></td></tr><tr><td align="center" valign="middle" >( U ′ p ) σ/Pa</td><td align="center" valign="middle" >3.48 &#215; 10<sup>8</sup></td><td align="center" valign="middle" >6.12 &#215; 10<sup>21</sup></td><td align="center" valign="middle" >5.37 &#215; 10<sup>33</sup></td><td align="center" valign="middle" >7.01 &#215; 10<sup>34</sup></td><td align="center" valign="middle" >1.12 &#215; 10<sup>43</sup></td><td align="center" valign="middle" >1.89 &#215; 10<sup>47</sup></td></tr></tbody></table></table-wrap><p><xref ref-type="table" rid="table1">Table 1</xref> reveals as follows:</p><p>&#183; Torque Γ is generated within the isolated quantum envelope by self-interaction of the field dynamics, the causality includes several SHM parameters of the harmonic oscillator; notably, the fermionic stress-radius correlation σ p r p 4 = Γ p = 3.867 &#215; 10 − 47   kg ⋅ m 3 ⋅ s − 2 identifies with the primitive causality of particulate matter’s scale-free intrinsic rotation, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>].</p><p>&#183; The parameter seems to differentiate radially in a convergent series within the quantum envelope, for the vacuum field it would account for effects associated with “spooky action-at-a-distance” observed in, say, Newtonian gravitation, it might also be responsible for atmospheric electric potential gradient, Macken ( [<xref ref-type="bibr" rid="scirp.93668-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.93668-ref46">46</xref>] ), Emiliani [<xref ref-type="bibr" rid="scirp.93668-ref47">47</xref>].</p><p>&#183; Two classes of torque are distinguishable, a “simple” torque field defines with the familiar unit N m as in <xref ref-type="table" rid="table1">Table 1</xref> Equations (1), (2), (5), (7) and (9), the unit modifies with exponents that vary from 0.25 to 1.0. A “complex” torque field is one in which the simple torque is itself in perpetual tangential and/or radial motion as in Equations (3), (6), (8), (10) to (12); notably, complex torques are uniquely bosonic features, with the exception of (3) they motivate perpetual translational (actually, tangential) motion of bodies through free space and orbital motion within the atom. Observe the tangential velocities (m&#183;s<sup>−1</sup>), v o 0.5 , Equation (8); v o 0.25 , Equation (11) and v<sub>o</sub>, Equation (12) where v o = π c o = 9.418 &#215; 10 8   m ⋅ s − 1 , Obande [<xref ref-type="bibr" rid="scirp.93668-ref48">48</xref>], the units present the vacuum field with tremendous electrical (permittivity) potential.</p><p>&#183; The interactions described in (1) and (2) have been presented in reasonable detail, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>], theory refutes the assignment of atomic unit of charge to the constant 1.6022 &#215; 10<sup>−19</sup>; it is a torque field, more in tune with angular momentum vector, i.e., electric potential than the scalar, electrostatic charge quantum, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>].</p><p>&#183; Attention is drawn to Equation (3). In terms of sheer design perfection, it reveals, arguably, the most intensive compressive force field in all of nature; it is a hydrostatic bosonic gravitational force field that compresses with a “bulk” speed of (2.99792458 &#215; π)<sup>−2.3</sup> (m&#183;s<sup>−1</sup>)<sup>−2.3</sup> bolstered with a matching angular shear stress. We have argued elsewhere, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>], that on atomic scale, it motivates natural radioactivity and on cosmic scale, it motivates stellar explosion or supernova.</p><sec id="s3_1"><title>3.1. Rotational Properties of the Isolated Atom</title><p>It refers to the non-bonded atom subjected to none other than its own field, an ideal theoretical entity absolutely impossible to isolate or shield from the vacuum field. Thus, the properties listed in <xref ref-type="table" rid="table2">Table 2</xref> refer to theoretical values, yet, some, e.g., theoretical electron radius r e ( p ) = 9.1 &#215; 10 − 15 m , come quite close to the classical value = 2.82 &#215; 10<sup>−15</sup> m; we highlight some physical characteristics of the quantum harmonic oscillator:</p><p>&#183; Oscillation frequency ϑ and angular speed ω: Values of ϑ and ω vary by nine and ten orders of magnitude respectively from start to the end of the chemical periodicity, notably, both quantities increase with mass number in sequential geometric series in which the segment coincides with the chemical period.</p><p>&#183; Atomic Radius r: Fundamentally, isotropic spatial dimension quantifies in mass/density quotient, r = 0.62038 ( m / ρ ) 0.333 ; for a harmonic oscillator the value also retrieves with r = λ/2, or centripetal force/elastic modulus quotient, r = F/є. In contrast with the bonded atom, radius of the isolated atom decreases exponentially with mass number and also in segments that coincide with the chemical periods, see <xref ref-type="fig" rid="fig1">Figure 1</xref>; its value at the beginning and end of the periodicity differs by ten and five orders of magnitude for the atomic wave and particulate forms respectively. A plot of values of r<sub>w</sub> vs. r<sub>p</sub> in <xref ref-type="fig" rid="fig2">Figure 2</xref> reproduces a familiar bimodal gradient commonly encountered in classical analysis of physical properties of the atom, Obande ( [<xref ref-type="bibr" rid="scirp.93668-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.93668-ref43">43</xref>] ). From e to H, comprising 23 inaccessible elements, we have a perfect linear correlation for which log ( r w / r p ) = L = 22.2 ; from He onwards, the value decreases logarithmically in measured periodic sequences to give L<sub>He</sub> = 22.2 and L<sub>Am</sub> = 17.8, see <xref ref-type="table" rid="table3">Table 3</xref>. In some cases the value is held constant over an interval, e.g., e to He, O to Na and Ni to Se, in others only one decimal place separates any two neighboring elements such as in the range Nd to Fr. These details necessitate with hope to probe causality of physical (gaseous, liquid or solid) states of the elements at standard conditions but available information proved inadequate hence we make only the following generalizations: 1) with a few exceptions, most elements registering with r w = 1.622 &#215; 10 22 r p , are either invisible or gaseous; 2) the elements H to He (five in number, Obande [<xref ref-type="bibr" rid="scirp.93668-ref42">42</xref>] constitute a visible-invisible condensed matter transition, they share common spacetime characteristics with both visible and invisible phases of reality, Obande [<xref ref-type="bibr" rid="scirp.93668-ref43">43</xref>]; 3) with the exception of a few gases and liquids, most elements with log ( r w / r p ) = 21.8 to 18.5 are solids, however, the element becomes spontaneously radioactive at log ( r w / r p ) ≤ 18.5 ; 4) electron wave or particulate form has the largest atomic radius of all elements hence, in the vacuum field and in bonded systems, the electron field encloses all other elements’ fields, this position can be checked against existing x-ray diffraction rings of compounds containing H atoms, e.g., benzene, where the H ring would be found to enclose C rings, Levine ( [<xref ref-type="bibr" rid="scirp.93668-ref49">49</xref>], p. 877); visible reality actually resides inside the electron waveform!, r e ( w ) = 1.499 &#215; 10 8 m .</p><p>&#183; Rest mass: It defines in the expression amu/ev = k = τ/(ω/r)<sup>1/2</sup> where k = 1.037528 &#215; 10<sup>−5</sup> and 9.31494 &#215; 10<sup>5</sup> (rad s<sup>−1</sup> m<sup>−1</sup>)<sup>−</sup><sup>1/2</sup> are amu/MeV of the bosonic and fermionic quantum fields respectively, observe that the value 9.31494 &#215; 10<sup>5</sup> corresponds to empirical amu = 931.4 MeV, observe also that the unit reveals the parametric definition of the eV. Interestingly, reduction of the element’s strain to hydrogen’s value also retrieves relative atomic mass, i.e., τ<sub>E</sub>/τ<sub>H</sub> = m<sub>r</sub>u<sup>−1</sup>, Obande [<xref ref-type="bibr" rid="scirp.93668-ref42">42</xref>].</p><p>&#183; Density ρ: Elemental bosonic density varies from electron’s ρ e ( w ) = 5.23 &#215; 10 − 76 kg ⋅ m − 3 to uranium’s ρ U ( w ) = 2.85 &#215; 10 − 37 kg ⋅ m − 3 , while corresponding fermionic densities are ρ e ( p ) = 3.06 &#215; 10 35 to ρ U ( p ) = 1.08 &#215; 10 57 kg ⋅ m − 3 . It reveals an invisible condensed matter field over 10<sup>100</sup> denser than the vacuum field thus, visible reality floats in a pool of very dense invisible (“dark”) particulate matter. Notably, bosonic densities of the chemical elements sum up to give vacuum material density ρ v a c = 2.6089 &#215; 10 − 39 g ⋅ cm − 3 and the cosmological lambda Λ = 4.87 &#215; 10 − 66 cm − 2 , Obande [<xref ref-type="bibr" rid="scirp.93668-ref50">50</xref>].</p><p>&#183; Centripetal force F: As shown in <xref ref-type="table" rid="table1">Table 1</xref>, it motivates quite a number of effects: electrical, Equations (10), (12); magnetic, Equation (11); mechanical, Equation (2) and spatial dimension in both the boson and fermion fields. We attribute the bosonic field correlation coefficient F w / m w 2 = 7.9433 &#215; 10 59 m ⋅ s 2 ⋅ kg − 1 to the strong nuclear force SNF, it holds matter together on all scales from the atom to cosmos, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>].</p><p>&#183; Elastic (tensile) modulus є: Vacuum material modulus varies across the chemical periodicity from e’s ϵ w / Pa = 2.91 &#215; 10 − 49 to U = 3.28 &#215; 10 − 20 , corresponding values for the fermionic field are ϵ p = 1.60 &#215; 10 − 4 to 2.21 &#215; 10<sup>12</sup> Pa for e to U respectively. Since the values refer to the isolated atom, the results reveal a highly elastic electromagnetic e-m vacuum spacetime fabric.</p><p>&#183; Strain τ: Intrinsic strain rate on the elemental bosonic quantum varies across the chemical periodicity from 2.12 &#215; 10<sup>−11</sup>% to 0.10% for electron to uranium, corresponding values for condensed matter are 3.49 &#215; 10<sup>11</sup>% to 8.6 &#215; 10<sup>16</sup>%. The values follow from the quantitative expression τ = 2 ϑ / π c = ω / π 2 c where ϑ, ω and c are oscillation frequency, angular speed and the transverse field respectively, for the vacuum c o = 2.99792458 &#215; 10 8 “m&#183;s<sup>−1</sup>” and for condensed matter c o = 3.71535229 &#215; 10 − 14 “m&#183;s<sup>−1</sup>”. Strain correlates with a number of other physical properties to manifest electro-magnetism, mechanical properties and spatial dimensions, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>], a small sample is presented in <xref ref-type="table" rid="table4">Table 4</xref>.</p></sec><sec id="s3_2"><title>3.2. Observational Effects of Intrinsic Rotation</title><p>Recall that complex torques (Equations (3), (8), (10), (11) and (12), <xref ref-type="table" rid="table1">Table 1</xref> are simple torques in perpetual motion in free space or in matter; some, e.g., (3), combine tangential and angular motions, others, e.g., (8), (11) and (12) execute sub- and super-luminal velocities, i.e., v o 0.25 , v o 0.5 and v<sub>o</sub>, where v o = π c o , yet others, e.g., (10) attribute to only angular speed. A detailed presentation of the subject would lengthen this report far beyond the intended scope; we highlight only some key observational effects.</p><sec id="s3_2_1"><title>3.2.1. Metric Expansion of Space and Matter</title><p>All natural spatial periodic quanta are ellipsoids, see, e.g., the “Static Sky”, New Castle [<xref ref-type="bibr" rid="scirp.93668-ref51">51</xref>] and the galaxies in Galaxy [<xref ref-type="bibr" rid="scirp.93668-ref52">52</xref>]. The morphology provides an important clue to the profile of metric space expansion, there are only two straight (axial) lines in an ellipsoid—the major and minor axes; in cosmic envelopes these two directions are totally forbidden on account of the (galactic) nucleus; in condensed matter the nucleus is encased in a shell of fermionic matter but, on account of gravity, remains impassable. In nature, therefore, projectiles circumvent the nucleus and trace only geodesics (parabolas), see Physics Forum.org [<xref ref-type="bibr" rid="scirp.93668-ref16">16</xref>]. The “Static Sky” provides an excellent perspective, condensed matter fields are constrained within the vertical cylindrical elliptic envelope, it constrains expansion to within the toriod. A superluminal tangential velocity that traces a larger ellipsoid creates the impression of radial acceleration of space, Castelvicchi [<xref ref-type="bibr" rid="scirp.93668-ref53">53</xref>], Nielson et al. [<xref ref-type="bibr" rid="scirp.93668-ref54">54</xref>], Brax [<xref ref-type="bibr" rid="scirp.93668-ref55">55</xref>], Billings [<xref ref-type="bibr" rid="scirp.93668-ref56">56</xref>], it is motivated by the bosonic field coupling ρ w / σ w = 8.5114 &#215; 10 − 19 , (m rad s<sup>−1</sup>)<sup>−2</sup>; theoretical analysis yields the expansion rate v o = 0.5 π c o = 4.709 &#215; 10 8 m ⋅ s − 1 , notably, it is measurable as the vacuum characteristic (“atmospheric electrostatic charge”) 8.5 &#215; 10<sup>−19</sup> “C”, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>].</p></sec><sec id="s3_2_2"><title>3.2.2. Motions in Free Space and in Condensed Matter</title><p>In free space the complex torque field motivates spontaneous translational motion, i.e., inertia, Lynden-Bell [<xref ref-type="bibr" rid="scirp.93668-ref57">57</xref>] of bodies including galaxies, stars, satellites, comets, et cetera; notably, these motions are not random events, each occurs within a well-defined trajectory fixed at formation of the body. Of particular interest in this class of motions is the seeming expansion of space broached above but belongs to a very rich subject that touches upon the details of birth, growth and death of matter. In condensed matter, bonding restricts the “primary” motion modes of Equations (3), (8), (10), (11) and (12) to within a limited radius resulting in a “secondary” mode that comprises mostly rotation and vibration about fixed axes. The secondary mode gives rise to vital observational effects: spin identifies, of course, with the primitive torque fields quantitatively expressed in Γ<sub>au</sub> and Γ<sub>nu</sub>, Equation (4); orbital motion or revolution identifies with angular motion, see Equation (10), and recession attributes to a coupling having only rectilinear dimension as in Equations (8), (11), (12). Of course, the rectilinear dimension refers to tangential motion which, as noted above, creates the illusion of radial expansion. In reality it refers to a process that gradually transforms a given elliptical envelope to a larger one until the envelope disintegrates and disappears spewing its content into vacuum space as asteroid, comet, other trans-stellar/galactic voyager which eventually also disintegrates and disappears into the void. The process is the universal scale-free death process of all matter, atomic, elemental, stellar, galactic, chemical, geological and biological bodies, Obande [<xref ref-type="bibr" rid="scirp.93668-ref27">27</xref>].</p><p>Observe that the mobile torque field informs: 1) Newton’s second law of motion where it accounts for sundry perpetual motion including: axial spin, orbital motion, and recession from the center e.g. moon from earth, BBC.com [<xref ref-type="bibr" rid="scirp.93668-ref58">58</xref>]; bulk expansion of cosmological bodies, e.g., earth, Diaz [<xref ref-type="bibr" rid="scirp.93668-ref59">59</xref>], sun, Appell [<xref ref-type="bibr" rid="scirp.93668-ref60">60</xref>] and expansion of the galaxy, Sciama, [<xref ref-type="bibr" rid="scirp.93668-ref61">61</xref>], Wall [<xref ref-type="bibr" rid="scirp.93668-ref62">62</xref>]. 2) Random Thermal (Brownian) Motion which, of course, is a condensed-phase internal motion limited by chemical bond to localized translational, rotational, vibrational, rocking and twisting modes. Interestingly, energies of these secondary modes quantize alongside the primary modes; as is well known, it enables applications in a variety of high-precision analytical devices, see, e.g., Levine (1988). 3) Kinetic Molecular Theory KT; Equations (8), (11) and (12) give the free-space tangential velocities (v/m&#183;s<sup>−1</sup>): π c o 0.5 = 3.069 &#215; 10 4 ; π c o 0.25 = 175.183 , and π c o = 9.418 &#215; 10 8 . It implicates moving torque fields in the familiar effects associated with random (thermal) motion whose observational root-mean-square velocity v r m s = ( 3 R T / M ) 0.5 . Substitution of electron molar and atomic mass values, m e 2 ( p ) / kg ⋅ u − 1 = 9.766 &#215; 10 − 7 and m e ( w ) / kg ⋅ atom − 1 = 7.373 &#215; 10 − 51 , yields v r m s / m ⋅ s − 1 = 8.724 &#215; 10 4 and 1.004 &#215; 10<sup>27</sup> respectively. The molar value 8.724 &#215; 10<sup>4</sup> m&#183;s<sup>−1</sup> tallies with π c o 0.5 and speaks well in favor of consistency of both KT and the present classical mechanics CM approach; however, bosonic electron’s v r m s = 1.004 &#215; 10 27 m ⋅ s − 1 presents an entirely new speed limit scenario. KT is well established, it serves here to cross-check the values obtained with the CM approach. The indication here of existence in nature of velocity on the order of 10<sup>27</sup> m&#183;s<sup>−1</sup> comes with tremendous implications specifically for on-going neutrino research but, the subject must await further investigation. The analysis clearly indicates that much of chemical kinetics and thermodynamics, particularly the concepts of enthalpy, entropy and thermodynamic temperature scale, easily trace to physics of the mobile torque field.</p></sec><sec id="s3_2_3"><title>3.2.3. Internal Pressure σ of the Quantum Envelope</title><p>Atomic stress (internal pressure) evaluates with σ = F / π r 2 = 8 π m ϑ 3 / c , Obande [<xref ref-type="bibr" rid="scirp.93668-ref48">48</xref>]. The value varies across the chemical periodicity from bosonic electron’s 6.18 &#215; 10<sup>−58</sup> to uranium’s 10<sup>−19</sup> Pa, corresponding values for particulate e to U are 5.56 &#215; 10<sup>9</sup> to 1.96 &#215; 10<sup>31</sup> Pa. In other words, the fermionic energy packet is some fifty orders of magnitude more internally pressurized than its bosonic conjugate. Burkert et al. [<xref ref-type="bibr" rid="scirp.93668-ref63">63</xref>] recently reported the value σ proton ~ 10 35 Pa ; theoretical analysis gives σ proton / Pa = 9.79 &#215; 10 22 and 6.12 &#215; 10<sup>21</sup> for the visible proton and its invisible (mass generation) analogue respectively. Correct situation of the empirical and theoretical values requires unambiguous identification of the experimental proton’s phase, Obande [<xref ref-type="bibr" rid="scirp.93668-ref43">43</xref>], i.e., its candidature among the three particle generations. We present in <xref ref-type="table" rid="table5">Table 5</xref> σ values of some elements in our visible U p o and in its invisible analogue U ′ p ; clearly, H<sup>+</sup> does not register with σ p ~ 10 35 in any ref. frame. The theoretical analysis therefore suggests a possibility that either the experimental set up over-estimates σ<sub>proton</sub> or, a rogue non-visible particulate element other than the proton is involved. We must, however, observe that in the course of this project we have uncovered significant divergences between theoretical and empirical atomic property values, e.g., a whopping twenty-order magnitude exists between electron empirical rest mass 9.1 &#215; 10<sup>−31</sup> and theoretical value 7.37 &#215; 10<sup>−51</sup> kg&#183;atom<sup>−1</sup>, Obande [<xref ref-type="bibr" rid="scirp.93668-ref42">42</xref>]. However, there is no doubt that Burkert et al. [<xref ref-type="bibr" rid="scirp.93668-ref63">63</xref>] ’s result makes an indispensable contribution to the position that the condensed matter energy packet is a highly pressurized vessel, see Zhou [<xref ref-type="bibr" rid="scirp.93668-ref64">64</xref>].</p></sec></sec></sec><sec id="s4"><title>4. Summary and Conclusions</title><p>&#183; Internal stress of a periodic quantum field correlates with the energy packet’s radius to generate the intrinsic torque Γ that motivates spontaneous rotation of matter, its atomic and natural units are electron’s bosonic Γ a u ( w ) = σ w r w 4 = 3.162 &#215; 10 − 25 kg ⋅ m 3 ⋅ s − 2 and fermionic Γ a u ( p ) = σ p r p 4 = 3.867 &#215; 10 − 47 kg ⋅ m 3 ⋅ s − 2 .</p><p>&#183; The evidence suggests that the field parameter differentiates radially in a convergent infinite series within the envelope to produce effects attributed to “spooky-action-at-a-distance” such as observed in Newtonian gravitation and in spatial electric potential gradient.</p><p>&#183; An earlier report was cited to inform that in addition to stress and radius, several other field parameters correlate to generate torque; for instance, the all-too-familiar fundamental constant 1.6022 &#215; 10<sup>−19</sup> attributes to the correlation coefficient of three different parametric couplings: ρ p / τ p 4 ; F p / ϑ p 2 and ρ w / ϑ w 4 where ρ, τ, and ϑ are flux density, strain and frequency and indices p and w denote fermionic and bosonic fields respectively.</p><p>&#183; As a result of intrinsic rotation, all bodies possess characteristic harmonic motion parameters including frequency, radius, mass, density, centripetal force, modulus, stress and strain. Since aggregate waveforms of the chemical elements constitute the vacuum field, Obande [<xref ref-type="bibr" rid="scirp.93668-ref44">44</xref>], the vacuum is actually an ideal elastic body defined with SHM properties of elemental waveforms; notably, the vacuum-value (amplitude) of a given property is not an average but sum total of values of elements of the chemical periodicity; e.g., vacuum density sums up to give the cosmological lambda, Obande [<xref ref-type="bibr" rid="scirp.93668-ref50">50</xref>].</p><p>&#183; The correlations describe conic sections, it accounts for ellipsoidal morphology of cosmic objects and rules out any notion of linear trajectory in nature, all seeming linear motions are tangential to larger geodesics; in other words, metric space cannot expand radially, it is an angular phenomenon.</p><p>&#183; As found in previous cases, theoretical results in this series call for caution in making deductions from particle physics experiments; we find, consistently, results which suggest that experimental energy regimes often diverge markedly from theoretical values. In the case in point, Burkert et al.’s recently reported proton internal pressure σ H + ~ 10 35 Pa differs significantly from the theoretical value of each of the proton’s three particle generations, specifically, σ H + / Pa = 9.79 &#215; 10 22 and 6.11 &#215; 10<sup>21</sup> in U p o , and U p ∗ / U ′ p respectively. Theoretical analysis reveals that σ value in the neighborhood of 10<sup>35</sup> registers only for invisible (“dark-matter”) trans-bromium elements, not earlier.</p><p>&#183; Restricted rotation in condensed matter creates all manner of modes of motion including, random thermal (Brownian), vibtrational, bending, rocking, twisting, et cetera. These modes are quantized in line with the causal harmonics, they manifest the spectrum of effects quantitatively associated with thermodynamics, kinetics and, in particular, kinetic-molecular theory. Most notably, the present CM approach leads to evaluation of the root-mean-square velocity v r m s = ( 3 R T / M ) 0.5 for which electron waveform’s m e ( w ) = 7.3725 &#215; 10 − 51 kg / atom , gives v r m s ( e w ) = 1.004 &#215; 10 27 m ⋅ s − 1 ; this result, suggesting existence of an imponderable hyper-luminal velocity, comes with important implications for on-going neutrino research, it is, however, set aside for further investigation.</p><p>The investigation has succeeded in explicitly accounting for the “mystery” of rotation such as proton spin, Moscowitz [<xref ref-type="bibr" rid="scirp.93668-ref65">65</xref>]; if taken with our earlier report on morphology of cosmological bodies, the present results point to a link between rotation and figure of celestial bodies St Katlin [<xref ref-type="bibr" rid="scirp.93668-ref66">66</xref>]. Notably, “gravitational accretion” is not in any way implicated in intrinsic rotation, Giuli [<xref ref-type="bibr" rid="scirp.93668-ref67">67</xref>]. It has become customary, in concluding a report of an investigation in this series, to call attention to the sheer power of the unassuming expression h ϑ = m c 2 ; it, of course, equates energies of the composite wave and particulate forms of the atom and in effect quantifies the atom’s essence and therein lies its analytical power. We do not think a simpler, yet more powerful, dual energy quantification is feasible, therefore, we submit the Planck-Einstein-de Broglie (PEB) mass equation the ultimate simplification of The Theory of Everything. In order to demonstrate its incredible simplicity and awesome analytical power, we have, quite deliberately, used the PEB to address areas considered intractable in the reigning physics paradigm, e.g., origin of the three-particle generations and identity of “dark” matter/energy, Obande [<xref ref-type="bibr" rid="scirp.93668-ref34">34</xref>]; elemental intrinsic atomic e-m resonance frequency, ϑ-value, Obande [<xref ref-type="bibr" rid="scirp.93668-ref44">44</xref>]; common causality of gravitation, electricity and magnetism, Obande [<xref ref-type="bibr" rid="scirp.93668-ref45">45</xref>]; atomic mass phenomenology, Obande [<xref ref-type="bibr" rid="scirp.93668-ref42">42</xref>]; cosmological constant phenomenology, Obande [<xref ref-type="bibr" rid="scirp.93668-ref50">50</xref>]; the photon’s identity, Obande [<xref ref-type="bibr" rid="scirp.93668-ref48">48</xref>]; phenomenology of the fundamental physical constants, Obande [<xref ref-type="bibr" rid="scirp.93668-ref20">20</xref>] and herein, origin of intrinsic rotation of matter. We have, in each case, submitted compelling positions that as yet await independent assessment. The goal is to assemble what would eventually become foundational materials of an all-embracing classical atomic theory with which an observational theory of nature is realizable. We think, even without going further, we have already assembled sufficient materials for development of an observational theory of nature.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Obande, O.P. (2019) On Intrinsic Rotation of Bodies. Journal of High Energy Physics, Gravitation and Cosmology, 5, 868-883. https://doi.org/10.4236/jhepgc.2019.53043</p></sec></body><back><ref-list><title>References</title><ref id="scirp.93668-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ellis, G. and Silk, J. 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