<?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.2016.23031</article-id><article-id pub-id-type="publisher-id">JHEPGC-67955</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>
 
 
  5D World-Universe Model. Gravitation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vladimir</surname><given-names>S. Netchitailo</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>Biolase Inc., Irvine, CA, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>v.netchitailo@sbcglobal.net</email></corresp></author-notes><pub-date pub-type="epub"><day>20</day><month>06</month><year>2016</year></pub-date><volume>02</volume><issue>03</issue><fpage>328</fpage><lpage>343</lpage><history><date date-type="received"><day>29</day>	<month>March</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>1</month>	<year>July</year>	</date><date date-type="accepted"><day>5</day>	<month>July</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>
 
 
  5D World-Universe Model is based on the decisive role of the Medium of the World composed of massive particles: protons, electrons, photons, neutrinos, and dark matter particles. In this manuscript we discuss different aspects of the gravitation: measured values of the Newtonian parameter of Gravitation and different Gravitational effects (gravitational lensing, cosmological redshift, gravitational deflection of light and gravitational refraction, proposed in the present paper). We show inter-connectivity of all cosmological parameters and provide a mathematical framework that allows direct calculation of them based on the value of the gravitational parameter. We analyze the difference between Electromagnetism and Gravitoelectromagnetism and make a conclusion about the mandatory existence of the Medium of the World. This paper aligns the World-Universe Model with the Le Sage’s theory of gravitation and makes a deduction on Gravity, Space and Time be emergent phenomena.
 
</p></abstract><kwd-group><kwd>5D World-Universe Model</kwd><kwd> Newtonian Parameter of Gravitation</kwd><kwd> Le Sage’s Gravity</kwd><kwd> Cosmic Neutrino Background</kwd><kwd> Gravitoelectromagnetism</kwd><kwd> Medium of the World</kwd><kwd> Cosmological Parameters</kwd><kwd> Emergent Phenomena</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We can’t solve problems by using the same kind of thinking we used when we created them.</p><p>Albert Einstein</p><p>Today, a growing feeling of stagnation is shared by a large number of researchers. In his “The Twilight of the Scientific Age” (2013), Martin Lopez Corredoira outlines the most significant issues he believes, Physics todays’ experiences, as a discipline: increasingly expensive experiments that yield less and less, lack of outstanding results, lack of openness to new ideas exhibited by scientific journals and community as a whole.</p><p>In some respects, the situation today is similar to that at the end of 19<sup>th</sup> century, when the common consensus held that the body of Physics was nearly complete. Discoveries of special and general relativity, quantum mechanics and elementary particles shook that belief and led to a new renaissance in Physics that lasted for a century. The genius of Einstein, Planck, Bohr, Dirac, Heisenberg, and Schr&#246;dinger allowed them to propose fundamentally new theories with very little experimental data to back them up.</p><p>During the 20<sup>th</sup> century, their theories were validated and elaborated with newly acquired experimental results. The pendulum may, however, have swung too far: today, all results must be made fit into the existing framework. The frameworks get adjusted when necessary, particularly inconvenient results may even get discarded at times. The time may be ripe to propose new fundamental models that will be both simpler than the current state of the art, as well as open up new areas of research.</p><p>In 1937, Paul Dirac proposed a new basis for cosmology: the hypothesis of a variable gravitational “constant”; and later added the notion of continuous creation of matter in the World. In 1983, Paul Wesson developed 5D Space-Time-Mass theory that associated the fifth dimension with rest mass of particles. The gravitational constant serves as the dimension-transposing parameter.</p><p>5D World-Universe Model (WUM) follows these ideas, albeit introducing a different mechanism of matter creation. WUM rests on the theoretical basis developed by Prof. Wesson, with the following modifications [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] : the fifth dimension is associated with the total energy of the Medium of the World, and the gravitomagnetic parameter of the Medium serves as the dimension-transposing parameter.</p><p>A number of ideas presented in this paper are not new, and I don’t claim credit for them. In fact, several ideas belonging to classical physicists such as P. A. M. Dirac, P. S. Wesson, A. D. Sakharov, O. Heaviside, Le Sage, and J. McCullagh, are revisited in a new light.</p><p>The 5D WUM is proposed as an alternative to the prevailing Bing Bang Model of standard physical cosmology. The main differences are the existence of the Medium of the World and the source of the World’s energy.</p><p>WUM analyzes the role of the Intergalactic plasma consisting of protons, electrons, and photons as part of the Medium of the World [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] , discusses Multicomponent Dark Matter and its decisive role in the Medium and Macroobjects of the World [<xref ref-type="bibr" rid="scirp.67955-ref2">2</xref>] , and considers mass-varying neutrinos as part of the Medium of the World [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] .</p><p>This paper discusses the Gravitation of the World. In Section 2 we make analysis of the measured values of the Newtonian parameter of Gravitation. In Section 3 we show inter-connectivity of all cosmological parameters and provide a mathematical framework that allows their direct calculation based on the value of the Gravitational parameter. In Section 4 we present different gravitational effects: gravitational lensing, cosmological redshift, gravitational deflection of light and gravitational refraction, proposed in the present paper. The Gravitoelectromagnetism is discussed in Section 5. Le Sage’s gravity mechanism is analyzed in Section 6. In Section 7 we deduce on Gravity, Space and Time to be emergent phenomena.</p></sec><sec id="s2"><title>2. Observations of Newtonian Parameter of Gravitation</title><p>The accuracy of the measured value of Gravitational parameter G has increased only modestly since the original Cavendish experiment. Published values of G have varied rather broadly, and some recent measurements of high precision are, in fact, mutually exclusive.</p><p><xref ref-type="table" rid="table1">Table 1</xref>, borrowed from CODATA Recommended Values of the Fundamental Physical Constants, 2010, summarizes the results of measurements of the Newtonian parameter of gravitation relevant to the 2010 adjustment [<xref ref-type="bibr" rid="scirp.67955-ref4">4</xref>] :</p><p>Observe that the values of G vary significantly depending on method. The disagreement in the values of G obtained by the various teams far exceeds the standard uncertainties provided with the values.</p><p>Detailed analysis of the results of measurements of the Newtonian parameter of gravitation in <xref ref-type="table" rid="table1">Table 1</xref> shows that there are three groups of measurements. Inside each such group, the measurements are not mutually exclusive; however measurements outside of a group contradict the entire group.</p><p>・ The first such group consists of six measurements with the average value of</p><disp-formula id="scirp.67955-formula1036"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x6.png"  xlink:type="simple"/></disp-formula><p>and relative standard uncertainty 28.5 ppm;</p><p>・ The second one consists of four measurements with the average value of</p><disp-formula id="scirp.67955-formula1037"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x7.png"  xlink:type="simple"/></disp-formula><p>and relative standard uncertainty 24 ppm;</p><p>The third one consists of one measurement with the value of</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Measurements of Newtonian parameter of gravitation</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Source</th><th align="center" valign="middle" >Identification<sup>a</sup></th><th align="center" valign="middle" >Method</th><th align="center" valign="middle" >10<sup>11</sup> G</th><th align="center" valign="middle" >Rel. stand.</th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >m<sup>3</sup>∙kg<sup>−</sup><sup>1</sup>∙s<sup>−2</sup></td><td align="center" valign="middle"  colspan="2"  >uncert u<sub>r</sub></td></tr><tr><td align="center" valign="middle" >Luther and Towler (1982)</td><td align="center" valign="middle" >NIST-82</td><td align="center" valign="middle" >Fiber torsion balance,</td><td align="center" valign="middle" >6.672 48(43)</td><td align="center" valign="middle"  colspan="2"  >6.4 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >dynamic mode</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Karagioz and Izmailov (1996)</td><td align="center" valign="middle" >TR&amp;D-96</td><td align="center" valign="middle" >Fiber torsion balance,</td><td align="center" valign="middle" >6.672 9(5)</td><td align="center" valign="middle"  colspan="2"  >7.5 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >dynamic mode</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Bagley and Luther (1997)</td><td align="center" valign="middle" >LANL-97</td><td align="center" valign="middle" >Fiber torsion balance,</td><td align="center" valign="middle" >6.673 98(70)</td><td align="center" valign="middle"  colspan="2"  >1.0 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >dynamic mode</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Gundlach and Merkowitz (2000, 2002)</td><td align="center" valign="middle" >UWash-00</td><td align="center" valign="middle" >Fiber torsion balance,</td><td align="center" valign="middle" >6.674 255(92)</td><td align="center" valign="middle"  colspan="2"  >1.4 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >dynamic compensation</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Quinn et al. (2001)</td><td align="center" valign="middle" >BIPM-01</td><td align="center" valign="middle" >Strip torsion balance,</td><td align="center" valign="middle" >6.675 59(27)</td><td align="center" valign="middle"  colspan="2"  >4.0 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >compensation mode, static deflection</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Kleinevo&#223; (2002); Kleinvo&#223; et al. (2002)</td><td align="center" valign="middle" >UWup-02</td><td align="center" valign="middle" >Suspended body,</td><td align="center" valign="middle" >6.674 22(98)</td><td align="center" valign="middle"  colspan="2"  >1.5 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >displacement</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Armstrong and Fitzgerald (2003)</td><td align="center" valign="middle" >MSL-03</td><td align="center" valign="middle" >Strip torsion balance,</td><td align="center" valign="middle" >6.673 87(27)</td><td align="center" valign="middle"  colspan="2"  >4.0 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >compensation mode</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Hu et al. (2005)</td><td align="center" valign="middle" >HUST-05</td><td align="center" valign="middle" >Fiber torsion balance,</td><td align="center" valign="middle" >6.672 28(87)</td><td align="center" valign="middle"  colspan="2"  >1.3 &#215; 10<sup>−4</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >dynamic mode</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Schlamminger et al. (2006)</td><td align="center" valign="middle" >UZur-06</td><td align="center" valign="middle" >Stationary body,</td><td align="center" valign="middle" >6.674 25(12)</td><td align="center" valign="middle"  colspan="2"  >1.9 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >weight change</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Luo et al. (2009); Tu et al. (2010)</td><td align="center" valign="middle" >HUST-09</td><td align="center" valign="middle" >Fiber torsion balance,</td><td align="center" valign="middle" >6.673 49(18)</td><td align="center" valign="middle"  colspan="2"  >2.7 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >dynamic mode</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr><tr><td align="center" valign="middle" >Parks and Faller (2010)</td><td align="center" valign="middle" >JILA-10</td><td align="center" valign="middle" >Suspended body,</td><td align="center" valign="middle" >6.672 34(14)</td><td align="center" valign="middle"  colspan="2"  >2.1 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >displacement</td><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  ></td></tr></tbody></table></table-wrap><p><sup>a</sup>NIST: National Institute of Standards and Technology, Gaithersburg, MD, USA; TR &amp; D: Tribotech Research and Development Company, Moscow, Russian Federation; LANL: Los Alamos National Laboratory, Los Alamos, New Mexico, USA; UWash: University of Washington, Seattle, Washington, USA; BIPM: International Bureau of Weights and Measures, S`evres, France; UWup: University of Wuppertal, Wuppertal, Germany; MSL: Measurement Standards Laboratory, Lower Hutt, New Zeland; HUST: Huazhong University of Science and Technology, Wuhan, PRC; UZur: University of Zurich, Zurich, Switzerland; JILA: JILA, University of Colorado and National Institute of Standards and Technology, Boulder, Colorado, USA.</p><disp-formula id="scirp.67955-formula1038"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x8.png"  xlink:type="simple"/></disp-formula><p>and relative standard uncertainty 40 ppm.</p><p>Clearly, the relative uncertainty of any such group is better than the uncertainty of the entire result set. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x9.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x10.png" xlink:type="simple"/></inline-formula> have relative standard uncertainties that are smaller than the average value of G. Out of the three distinct groups of G measurements, how shall we identify the correct one?</p><p>In accordance with WUM, the Gravitational parameter G and Fermi coupling parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x11.png" xlink:type="simple"/></inline-formula> can be expressed as follows [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] :</p><disp-formula id="scirp.67955-formula1039"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x12.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1040"><label>(2.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x13.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x14.png" xlink:type="simple"/></inline-formula> is Dirac constant, c is the electrodynamic constant, α is fine-structure constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x15.png" xlink:type="simple"/></inline-formula>is the mass of a proton, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x16.png" xlink:type="simple"/></inline-formula>is the mass of an electron, and basic energy unit <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x17.png" xlink:type="simple"/></inline-formula> equals to</p><disp-formula id="scirp.67955-formula1041"><label>(2.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x18.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x19.png" xlink:type="simple"/></inline-formula> is Planck constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x20.png" xlink:type="simple"/></inline-formula>is the classical radius of an electron, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x21.png" xlink:type="simple"/></inline-formula>.</p><p>For the three groups of G measurements, parameter Q will take on the following values, respectively (see 2.4):</p><disp-formula id="scirp.67955-formula1042"><label>(2.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x22.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1043"><label>(2.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x23.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1044"><label>(2.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x24.png"  xlink:type="simple"/></disp-formula><p>The calculated value of the parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x25.png" xlink:type="simple"/></inline-formula> (see 2.5) based on the average value of the Fermi coupling parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x26.png" xlink:type="simple"/></inline-formula> is:</p><disp-formula id="scirp.67955-formula1045"><label>(2.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x27.png"  xlink:type="simple"/></disp-formula><p>The value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x28.png" xlink:type="simple"/></inline-formula> is much more precise than the values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x29.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x30.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x31.png" xlink:type="simple"/></inline-formula>. With this value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x32.png" xlink:type="simple"/></inline-formula> we can make the choice of the first group of G measurements and significantly increase the precision of all Q-dependent parameters (see Section 3).</p><p>The calculated value of the parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x33.png" xlink:type="simple"/></inline-formula> based on the average value of the gravitational parameter</p><disp-formula id="scirp.67955-formula1046"><label>(CODATA, 2014)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x34.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1047"><label>(2.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x35.png"  xlink:type="simple"/></disp-formula><p>is very close to the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x36.png" xlink:type="simple"/></inline-formula> and correspond to the value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x37.png" xlink:type="simple"/></inline-formula>. The calculated value of G based on the average value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x38.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1048"><label>(2.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x39.png"  xlink:type="simple"/></disp-formula><p>The CODATA, 2014 value of G is slightly smaller (&lt;0.007%) than this calculated value.</p><p>The gravitational parameter G in our Model is changing in time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x40.png" xlink:type="simple"/></inline-formula> with the following rate:</p><disp-formula id="scirp.67955-formula1049"><label>(2.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x41.png"  xlink:type="simple"/></disp-formula><p>During the 216 years elapsed from the first measurement of the value of G by Henry Cavendish, value of G has decreased by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x42.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.67955-formula1050"><label>(2.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x43.png"  xlink:type="simple"/></disp-formula><p>The above <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x44.png" xlink:type="simple"/></inline-formula> is far smaller than the precision that we have attained when measuring G , and thus measuring <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x45.png" xlink:type="simple"/></inline-formula> directly seems to be impossible using contemporary techniques.</p><p>In his papers Jean-Philippe Uzan reviewed the main experimental and observational constraints that have been obtained for variations of the gravitational parameter in different areas [<xref ref-type="bibr" rid="scirp.67955-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.67955-ref6">6</xref>] :</p><p>・ Solar systems constraints,</p><p>・ Pulsar timing,</p><p>・ Stellar constraints,</p><p>・ Cosmological constraints,</p><p>and found that</p><disp-formula id="scirp.67955-formula1051"><label>(2.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x46.png"  xlink:type="simple"/></disp-formula><p>The experimentally obtained constraints on G variation rates are significantly larger than theoretically calculated 2.13. Note that all obtained constraints are the results of the calculations based on different theoretical models. One example from review [<xref ref-type="bibr" rid="scirp.67955-ref6">6</xref>] :</p><p>“The Lunar Laser Ranging (LLR) experiment has measured the relative position of the Moon with respect to the Earth with accuracy of the order of 1 cm over 3 decades. An early analysis of this data assuming a Brans-Dicke theory of gravitation gave that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x47.png" xlink:type="simple"/></inline-formula>. It was improved by using 20 years of observation to get<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x48.png" xlink:type="simple"/></inline-formula>, the main uncertainty arising from Lunar tidal acceleration. With 24 years of data, one reached <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x49.png" xlink:type="simple"/></inline-formula> and finally, the latest analysis of the Lunar laser ranging experiment increased the constraint to</p><disp-formula id="scirp.67955-formula1052"><graphic  xlink:href="http://html.scirp.org/file/8-2180112x50.png"  xlink:type="simple"/></disp-formula><p>Another example from Uzan’s review [<xref ref-type="bibr" rid="scirp.67955-ref5">5</xref>] :</p><p>“Teller (1948) first emphasized that Dirac hypothesis may be in conflict with paleontological evidence. His argument is based on the estimation of the temperature at the center of the Sun <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x51.png" xlink:type="simple"/></inline-formula> using the virial theorem. The luminosity of the Sun is then proportional to the radiation energy gradient times the mean free path of a photon times the surface of the Sun, that is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x52.png" xlink:type="simple"/></inline-formula>, hence concluding that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x53.png" xlink:type="simple"/></inline-formula>. Computing the radius of the Earth orbit in Newtonian mechanics, assuming the conservation of angular momentum (so that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x54.png" xlink:type="simple"/></inline-formula> is constant) and stating that the Earth mean temperature is proportional to the fourth root of the energy received, he concluded that</p><disp-formula id="scirp.67955-formula1053"><graphic  xlink:href="http://html.scirp.org/file/8-2180112x55.png"  xlink:type="simple"/></disp-formula><p>If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x56.png" xlink:type="simple"/></inline-formula> is constant and G was 10% larger 300 million years ago, the Earth surface temperature should have been 20% higher, that is close to the boiling temperature. This was in contradiction with the existence of trilobites in the Cambrian”.</p><p>Moreover, Teller didn’t take the “Faint Young Sun” paradox into account: the young Sun’s output was only about 70% of what it is today [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] . So, all conclusions on the (almost) constancy of the Newtonian parameter of gravitation are model-dependent.</p></sec><sec id="s3"><title>3. Cosmological Parameters</title><p>The advantage of WUM is that two fundamental parameters in various rational exponents define all macro and micro features of the World: Fine-structure constant α, and dimensionless quantity Q. While α is constant, Q increases with time, and is in fact a measure of the size and the age of the World, as well as all other time-varying parameters of the World [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] . Q can be calculated based on the value of the gravitational parameter G:</p><disp-formula id="scirp.67955-formula1054"><label>(3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x57.png"  xlink:type="simple"/></disp-formula><p>Then all time-varying cosmological parameters can be calculated based on the value of G :</p><p>・ Hubble’s parameter H</p><disp-formula id="scirp.67955-formula1055"><label>(3.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x58.png"  xlink:type="simple"/></disp-formula><p>・ Age of the World <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x59.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1056"><label>(3.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x60.png"  xlink:type="simple"/></disp-formula><p>・ Size of the World R</p><disp-formula id="scirp.67955-formula1057"><label>(3.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x61.png"  xlink:type="simple"/></disp-formula><p>・ Critical energy density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x62.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1058"><label>(3.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x63.png"  xlink:type="simple"/></disp-formula><p>・ Temperature of the microwave background radiation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x64.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1059"><label>(3.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x65.png"  xlink:type="simple"/></disp-formula><p>・ Temperature of the far-infrared background radiation peak <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x66.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1060"><label>(3.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x67.png"  xlink:type="simple"/></disp-formula><p>・ Planck mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x68.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1061"><label>(3.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x69.png"  xlink:type="simple"/></disp-formula><p>・ Electronic neutrino mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x70.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1062"><label>(3.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x71.png"  xlink:type="simple"/></disp-formula><p>・ Muonic neutrino mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x72.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1063"><label>(3.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x73.png"  xlink:type="simple"/></disp-formula><p>・ Tauonic neutrino mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x74.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1064"><label>(3.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x75.png"  xlink:type="simple"/></disp-formula><p>・ Axion mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x76.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1065"><label>(3.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x77.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x78.png" xlink:type="simple"/></inline-formula> is the Boltzmann constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x79.png" xlink:type="simple"/></inline-formula>is a basic unit of energy density:</p><disp-formula id="scirp.67955-formula1066"><label>(3.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x80.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x81.png" xlink:type="simple"/></inline-formula> is a basic unit of mass:</p><disp-formula id="scirp.67955-formula1067"><label>(3.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x82.png"  xlink:type="simple"/></disp-formula><p>As shown in [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] , the calculated values of these parameters are in a good agreement with the latest results of their measurements. For example, calculating the value of Hubble’s parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x83.png" xlink:type="simple"/></inline-formula> based on G we find</p><disp-formula id="scirp.67955-formula1068"><label>(3.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x84.png"  xlink:type="simple"/></disp-formula><p>which is in good agreement with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x85.png" xlink:type="simple"/></inline-formula> obtained using WMAP data [<xref ref-type="bibr" rid="scirp.67955-ref7">7</xref>] .</p><p>We can calculate the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x86.png" xlink:type="simple"/></inline-formula> (see 3.6) and get <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x87.png" xlink:type="simple"/></inline-formula> which is in excellent agreement with experimentally measured value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x88.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.67955-ref8">8</xref>] .</p><p>In frames of WUM, some cosmological parameters are constants and can be calculated based on the value of the fine-structure constant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x89.png" xlink:type="simple"/></inline-formula>. WUM postulates that masses of Dark Matter Particles (DMP) are proportional to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x90.png" xlink:type="simple"/></inline-formula> multiplied by different exponents of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x91.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.67955-ref2">2</xref>] :</p><p>Cold DMP (neutralinos and WIMPs):</p><disp-formula id="scirp.67955-formula1069"><label>(3.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x92.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1070"><label>(3.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x93.png"  xlink:type="simple"/></disp-formula><p>DIRACs:</p><disp-formula id="scirp.67955-formula1071"><label>(3.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x94.png"  xlink:type="simple"/></disp-formula><p>ELOPs:</p><disp-formula id="scirp.67955-formula1072"><label>(3.19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x95.png"  xlink:type="simple"/></disp-formula><p>Warm DMP (sterile neutrinos):</p><disp-formula id="scirp.67955-formula1073"><label>(3.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x96.png"  xlink:type="simple"/></disp-formula><p>These values fall into the mass ranges estimated in literature [<xref ref-type="bibr" rid="scirp.67955-ref2">2</xref>] . The roles of those particles in macroobject cores built up from fermionic dark matter, in gamma-ray spectra of the diffuse gamma-ray background and the emission of various macroobjects in the World are discussed in [<xref ref-type="bibr" rid="scirp.67955-ref2">2</xref>] .</p><p>One of the principal ideas of WUM holds that relative energy densities of the World’s particles in terms of the critical energy density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x97.png" xlink:type="simple"/></inline-formula> are constants in all times; depend only on the fundamental parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x98.png" xlink:type="simple"/></inline-formula> and proportional to proton energy density in the World’s Medium [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] :</p><disp-formula id="scirp.67955-formula1074"><label>(3.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x99.png"  xlink:type="simple"/></disp-formula><p>The relative energy densities of the components of the World are:</p><p>Protons <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x100.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1075"><label>(3.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x101.png"  xlink:type="simple"/></disp-formula><p>Electrons <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x102.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1076"><label>(3.23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x103.png"  xlink:type="simple"/></disp-formula><p>Microwave background radiation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x104.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1077"><label>(3.24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x105.png"  xlink:type="simple"/></disp-formula><p>Dark Matter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x106.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1078"><label>(3.25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x107.png"  xlink:type="simple"/></disp-formula><p>Cosmic Neutrino Background <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x108.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1079"><label>(3.26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x109.png"  xlink:type="simple"/></disp-formula><p>Dineutrinos <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x110.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1080"><label>(3.27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x111.png"  xlink:type="simple"/></disp-formula><p>Far-infrared background radiation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x112.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1081"><label>(3.28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x113.png"  xlink:type="simple"/></disp-formula><p>The sum of all components densities of the World <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x114.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.67955-formula1082"><label>(3.29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x115.png"  xlink:type="simple"/></disp-formula><p>in all times. The implication is that the World is flat.</p><p>From (3.29) we can calculate the value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x116.png" xlink:type="simple"/></inline-formula>, using electron-to-proton mass ratio <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x117.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67955-formula1083"><label>(3.30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x118.png"  xlink:type="simple"/></disp-formula><p>which is in excellent agreement with the commonly adopted value of 137.035999074(44). It means that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x119.png" xlink:type="simple"/></inline-formula> is</p><p>not an independent constant, but is instead derived from α [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] .</p><p>With the exception of neutrinos, the calculated values of the energy densities of the components of the World are in good agreement with their latest measurements [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] . When it comes to neutrinos, WUM postulates a much higher energy density than is commonly accepted in literature. As we proceed to show in the next section, there is no need for Dark Energy in WUM.</p></sec><sec id="s4"><title>4. Gravitational Effects</title><p>The very first gravitational effect was calculated by J. G. von Soldner in 1801. In his paper “The deflection of a light ray from its rectilinear motion, by the attraction of a celestial body at which it nearly passes by” he found for the angle of deflection by Sun <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x120.png" xlink:type="simple"/></inline-formula> the value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x121.png" xlink:type="simple"/></inline-formula> which is very close to the value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x122.png" xlink:type="simple"/></inline-formula> calculated by Einstein in 1908 [<xref ref-type="bibr" rid="scirp.67955-ref9">9</xref>] . And only in 1915 Einstein presented the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x123.png" xlink:type="simple"/></inline-formula> calculation based on General Theory of Relativity.</p><p>In our opinion, there is another possibility to explain an increased value of the deflection angle by Sun. According to WUM, all macroobjects of the World have cores made up of fermionic DMP. In case of extrasolar systems, the cores of stars are made up of interacting neutralinos or WIMPs surrounded with white dwarf shells.</p><p>Surrounding the cores, there is a transitional region in which the density decreases rapidly to the point of the zero level of the fractal structure [<xref ref-type="bibr" rid="scirp.67955-ref10">10</xref>] characterized by radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x124.png" xlink:type="simple"/></inline-formula> and energy density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x125.png" xlink:type="simple"/></inline-formula> that satisfy the following equation for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x126.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.67955-formula1084"><label>(4.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x127.png"  xlink:type="simple"/></disp-formula><p>The transition region between solar core and the beginning of the Heliosphere, in which the density considerably decreases, may cause an additional deflection of a light ray due to the gravitational refraction.</p><p>A gravitational lens refers to a distribution of matter (such as a cluster of galaxies) between a distant source and an observer that is capable of bending the light from the source, as it travels towards the observer. Fritz Zwicky posited in 1937 that the effect could allow galaxy clusters to act as gravitational lenses. It was not until 1979 that this effect was confirmed by observation of the so-called “Twin QSO” SBS 0957 + 561.</p><p>According to WUM, sterile neutrinos make up cores of galaxy clusters. The cores are surrounded by shells made up of DM and baryonic matter. Every macroobject consists of all particles under consideration that are present in the same proportion as they exist in the World’s Medium [<xref ref-type="bibr" rid="scirp.67955-ref2">2</xref>] .</p><p>In our opinion, the structure of galaxy clusters described above should be taken into account whenever gravitational lenses are calculated.</p><p>Gravitational redshift is the process by which electromagnetic radiation originating from a source that is in a gravitational field is reduced in frequency, or redshifted, when observed in a region of a weaker gravitational field. This effect is now considered to have been definitively verified by the experiments of Pound, Rebka and Snider between 1959 and 1965.</p><p>The gravitational redshift depends on the mass of the gravitating body. WUM holds that 1/3 of the total mass is in the central macroobject (for example, a star in extrasolar system) and 2/3 of the total mass is in the fractal structure around it [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] . This mass ratio should be taken into account when calculating gravitational redshift.</p><p>The gravitational redshift is a part of the total cosmological redshift. Let us analyze the movement of photons as they travel from distant galaxies to Earth in the time-varying Medium. As we have shown in [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] , energy of photons remains constant in the ideal frictionless Medium. In the actual rotationally elastic Medium [<xref ref-type="bibr" rid="scirp.67955-ref11">11</xref>] with a friction coefficient for photons</p><disp-formula id="scirp.67955-formula1085"><label>(4.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x128.png"  xlink:type="simple"/></disp-formula><p>the equation for the photons momentum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x129.png" xlink:type="simple"/></inline-formula> is:</p><disp-formula id="scirp.67955-formula1086"><label>(4.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x130.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x131.png" xlink:type="simple"/></inline-formula> is a parameter. Solving equation 4.3 we obtain</p><disp-formula id="scirp.67955-formula1087"><label>(4.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x132.png"  xlink:type="simple"/></disp-formula><p>Consider a photon with initial momentum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x133.png" xlink:type="simple"/></inline-formula> emitted at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x134.png" xlink:type="simple"/></inline-formula>. The photon is continuously losing momentum as it moves through the Medium until time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x135.png" xlink:type="simple"/></inline-formula> when it is observed. The observer will measure<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x136.png" xlink:type="simple"/></inline-formula>, compare it with well-known wavelength<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x137.png" xlink:type="simple"/></inline-formula>, and calculate a redshift:</p><disp-formula id="scirp.67955-formula1088"><label>(4.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x138.png"  xlink:type="simple"/></disp-formula><p>By definition,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x139.png" xlink:type="simple"/></inline-formula>. When <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x140.png" xlink:type="simple"/></inline-formula> we obtain:</p><disp-formula id="scirp.67955-formula1089"><label>(4.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x141.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1090"><label>(4.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x142.png"  xlink:type="simple"/></disp-formula><p>Recall that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x143.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x144.png" xlink:type="simple"/></inline-formula> are cosmological times (ages of the World at the moments of emitting and observing), both measured from the Beginning of the World. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x145.png" xlink:type="simple"/></inline-formula>equals to the present age of the World<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x146.png" xlink:type="simple"/></inline-formula>. If the photon travelled for time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x147.png" xlink:type="simple"/></inline-formula>, then</p><disp-formula id="scirp.67955-formula1091"><label>(4.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x148.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1092"><label>(4.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x149.png"  xlink:type="simple"/></disp-formula><p>The cosmological redshift is then described by a nonlinear equation on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x150.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.67955-formula1093"><label>(4.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x151.png"  xlink:type="simple"/></disp-formula><p>As an example, a photon travelling for 7.11 Byr (half of the World’s age<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x152.png" xlink:type="simple"/></inline-formula>) will have a redshift of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x153.png" xlink:type="simple"/></inline-formula>. Photon travelling for 12.64 Byr will have a redshift of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x154.png" xlink:type="simple"/></inline-formula>. The difference is due to the dependence of the Medium friction on time: it was 9 times greater at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x155.png" xlink:type="simple"/></inline-formula> than it is now at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x156.png" xlink:type="simple"/></inline-formula>.</p><p>In accordance with Hubble’s law, the distance d to galaxies for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x157.png" xlink:type="simple"/></inline-formula> is found to be proportional to z:</p><disp-formula id="scirp.67955-formula1094"><label>(4.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x158.png"  xlink:type="simple"/></disp-formula><p>The relationship of distance d to the redshift z for large values of z is not presently conclusive, active research is conducted in the area. In our Model, the distance to galaxies equals to:</p><disp-formula id="scirp.67955-formula1095"><label>(4.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x159.png"  xlink:type="simple"/></disp-formula><p>which reduces to 4.11 for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x160.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x161.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x162.png" xlink:type="simple"/></inline-formula>.</p><p>Experimental observations measuring light from distant galaxies and supernovae seem to imply that the World is expanding at an accelerated pace, as is evident from the observed redshift. Since 1990s, Dark Energy became the widely accepted hypothesis that explains this phenomenon.</p><p>The time varying friction of the Medium offered above provides an alternative interpretation of these observations. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x163.png" xlink:type="simple"/></inline-formula>, the distance to supernovae is smaller than expected and hence supernovae are brighter. There is then no reason to introduce dark energy in order to explain the nonlinear relationship of distance to the redshift.</p><p>In WUM the theoretical need for additional energy density distinct from the baryon matter and dark matter densities to form our observationally flat World is satisfied with the considerably larger fraction of the neutrino energy density in the total energy density of the World (see 3.26). Consequently, we are dealing with well- known particles instead of dark energy.</p><p>The idea of loss of energy of the photon in the intergalactic medium was first suggested in 1929 by Zwicky. But there are two problems: 1) all images of distant objects look blurred if the intergalactic space produces scattering; 2) the scattering effect and the consequent loss of energy is frequency dependent [<xref ref-type="bibr" rid="scirp.67955-ref12">12</xref>] .</p><p>Different mechanisms were proposed to avoid blurring and scattering. Laio A., et al. showed that the shift of photon frequency in low density plasma (which is the case in our Model [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] ) could come from quantum effects derived from standard quantum electrodynamics [<xref ref-type="bibr" rid="scirp.67955-ref13">13</xref>] . According to E. J. Lerner, quantum mechanics indicates that a photon gives up a tiny amount of energy as it collides with an electron, but its trajectory does not change [<xref ref-type="bibr" rid="scirp.67955-ref14">14</xref>] .</p><p>There is another way to explain the absence of the blurring and scattering. Back in 1846 James McCullagh proposed a theory of rotationally elastic medium, i.e. the medium in which every particle resists absolute rotation [<xref ref-type="bibr" rid="scirp.67955-ref11">11</xref>] . This theory produces equations analogous to Maxwell’s electromagnetic equations. In our opinion, the Medium of the World is in fact such a rotationally elastic medium. We propose to review the interaction of photons with the Medium in light of this unique theory.</p></sec><sec id="s5"><title>5. Gravitoelectromagnetism</title><p>Gravitoelectromagnetism (GEM) refers to a set of formal analogies between the equations for electromagnetism and relativistic gravitation. GEM is an approximation to the Einstein field equations for general relativity in the weak field limit. The equations for GEM were first published in 1893, before general relativity, by O. Heaviside as a separate theory expanding Newton’s law [<xref ref-type="bibr" rid="scirp.67955-ref15">15</xref>] . WUM follows this theory.</p><p>Maxwell’s equations (ME) vary with the unit system used. Although the general shape remains the same, various definitions are changed, and different constants appear in different places. We’ll start our discussion with ME in SI units. We will not rewrite well-known equations, but only provide the relationships between physical quantities used in ME for electromagnetism and gravitoelectromagnetism in the <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref>:</p><p>In Maxwell’s equations, electrodynamic constant c is defined as the ratio of the absolute electromagnetic unit of charge to the absolute electrostatic unit of charge.</p><p>From <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref> it becomes clear that the dimensions of all physical quantities depend on the choice of the charge and mass dimensions (Coulomb &amp; kilogram in SI units). In other unit systems the dimensions are different. For instance, in Gaussian units (CGSE):</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Electromagnetism</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Charge</th><th align="center" valign="middle" >Impedance of Electromagnetic Field</th><th align="center" valign="middle" >Magnetic Flux</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x164.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x165.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x166.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Electric Current</td><td align="center" valign="middle" >Magnetic Constant</td><td align="center" valign="middle" >Electric Potential</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x167.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x168.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x169.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Magnetic Field Intensity</td><td align="center" valign="middle" >Electric Constant</td><td align="center" valign="middle" >Electric Field</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x170.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x171.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x172.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Electric Flux Density</td><td align="center" valign="middle" >Electrodynamic Constant</td><td align="center" valign="middle" >Magnetic Flux Density</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x173.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x174.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x175.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Gravitoelectromagnetism</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Mass</th><th align="center" valign="middle" >Impedance of Gravitational Field</th><th align="center" valign="middle" >Gravitomagnetic Flux</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x176.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x177.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x178.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Mass Current</td><td align="center" valign="middle" >Gravitomagnetic Parameter</td><td align="center" valign="middle" >Gravitoelectric potential</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x179.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x180.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x181.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Gravitomagnetic Field Intensity</td><td align="center" valign="middle" >Gravitoelectric Parameter</td><td align="center" valign="middle" >Gravitoelectric Field</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x182.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x183.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x184.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Gravitoelectric Flux Density</td><td align="center" valign="middle" >Gravitoelectrodynamic Constant</td><td align="center" valign="middle" >Gravitomagnetic Flux Density</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x185.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x186.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x187.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x188.png" xlink:type="simple"/></inline-formula></p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x189.png" xlink:type="simple"/></inline-formula></p><p>In CGSM:</p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x190.png" xlink:type="simple"/></inline-formula></p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x191.png" xlink:type="simple"/></inline-formula></p><p>We seem to possess a substantial degree of freedom when it comes to choosing the dimension of charge. For an arbitrary dimension-transposing parameter P we can</p><p>・ Multiply the charge and mass and all physical quantities on the left side of <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref> by an arbitrary parameter P,</p><p>・ Divide impedances by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x192.png" xlink:type="simple"/></inline-formula>,</p><p>・ Divide magnetic fluxes and all physical quantities on the right side of <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref> by P.</p><p>Following such a transformation, all physically measurable parameters such as energy density and energy flux density remain the same, and have the same mechanical dimensions.</p><p>By definition, 1 Coulomb equals to one tenth of the absolute electromagnetic unit of charge. It follows that in SI</p><p>we use electromagnetic unit of charge e in the electrostatic Coulomb law instead of the electrostatic unit<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x193.png" xlink:type="simple"/></inline-formula>. This</p><p>seems a bit odd.</p><p>Likewise, when describing Newtonian law of gravitation, we use m―the inertial mass, instead of gravitoelectrostatic charge<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x194.png" xlink:type="simple"/></inline-formula>―the gravitational mass. The gravitoelectromagnetic charge is then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x195.png" xlink:type="simple"/></inline-formula>. Similarly to the electromagnetic field, the gravitoelectrodynamic constant c is the ratio of the absolute gravitoelectromagnetic unit of charge to the absolute gravitoelectrostatic unit of charge.</p><p>All elementary particles in the World are fully characterized by their four-momentum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x196.png" xlink:type="simple"/></inline-formula> that satisfies</p><p>the following equation:</p><disp-formula id="scirp.67955-formula1096"><label>(5.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x197.png"  xlink:type="simple"/></disp-formula><p>where the invariant is, in fact, the gravitoelectrostatic charge mc squared, and E is the gravitoelectromagnetic charge.</p><p>The inertial mass and the gravitational mass are not the same physical quantity. Instead, they are proportional to each other, and their ratio equals to the gravitoelectrodynamic constant c. The classical theory offers no compelling reason why the gravitational mass mc has to equal the inertial mass m, commonly referred to as “rest mass”.</p><p>Analogous to electromagnetism, we can think of m as a gravitocapacitor. Then, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x198.png" xlink:type="simple"/></inline-formula>describes the accumulation of energy by gravitocapacitor with capacity m, rather than transformation of energy to mass.</p><p>But there is a principal physical difference between Electromagnetism (EM) and Gravitoelectromagnetism (GEM):</p><p>・ In EM, the magnetic constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x199.png" xlink:type="simple"/></inline-formula> and electric constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x200.png" xlink:type="simple"/></inline-formula> are the vacuum permeability and vacuum permittivity of free (empty) space correspondingly;</p><p>・ In GEM, the gravitomagnetic parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x201.png" xlink:type="simple"/></inline-formula> depends on the gravitational parameter G:</p><disp-formula id="scirp.67955-formula1097"><label>(5.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x202.png"  xlink:type="simple"/></disp-formula><p>which is not a constant in our model and cannot be introduced without the Medium of the World. In frames of WUM the gravitomagnetic parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x203.png" xlink:type="simple"/></inline-formula> can be calculated based on the value of the energy density of the Medium of the World<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x204.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.67955-formula1098"><label>(5.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x205.png"  xlink:type="simple"/></disp-formula><p>where a dimension-transposing parameter P equals to [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] :</p><disp-formula id="scirp.67955-formula1099"><label>(5.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x206.png"  xlink:type="simple"/></disp-formula><p>Nikola Tesla stated the existence of the Medium of the World: “All attempts to explain the workings of the universe without recognizing the existence of the ether and the indispensable function it plays in the phenomena are futile and destined to oblivion”.</p><p>James McCullagh has this to say about the Medium: “The constitution of the ether, if it ever would be discovered, will be found to be quite different from anything that we are in the habit of conceiving, though at the same time very simple and very beautiful. An elastic medium composed of points acting on each other in the way supposed by Poisson and others will not answer”.</p><p>Long time ago it was realized that there are no longitudinal waves in the Medium, and hence the Medium could not be an elastic matter of an ordinary type. In 1846 James McCullagh proposed a theory of a rotationally elastic medium, i.e. a medium in which every particle resists absolute rotation [<xref ref-type="bibr" rid="scirp.67955-ref11">11</xref>] .</p><p>The potential energy of deformation in such a medium depends only on the rotation of the volume elements and not on their compression or general distortion. This theory produces equations analogous to Maxwell’s electromagnetic equations.</p><p>The World-Universe Model is based on Maxwell’s equations, and McCullagh’s theory is a good fit for description of the Medium.</p><p>As the conclusion:</p><p>・ The gravitation does not exist without the Medium of the World;</p><p>・ The gravitation is connected to the main characteristic of the Medium-energy density.</p></sec><sec id="s6"><title>6. Le Sage’s Theory of Gravitation</title><p>Wikipedia summarizes this unique theory as follows:</p><p>“Le Sage’s theory of gravitation is a kinetic theory of gravity originally proposed by Nicolas Fatio de Duillier in 1690 and later by Georges-Louis Le Sage in 1748. The theory proposed a mechanical explanation for Newton’s gravitational force in terms of streams of tiny unseen particles (which Le Sage called ultra-mundane corpuscles) impacting all material objects from all directions. According to this model, any two material bodies partially shield each other from the impinging corpuscles, resulting in a net imbalance in the pressure exerted by the impact of corpuscles on the bodies, tending to drive the bodies together”.</p><p>Le Sage proposed quantitative estimates for some of the theory’s parameters:</p><p>・ He called the gravitational particles ultramundane corpuscles, because he supposed them to originate beyond our known universe. The distribution of the ultramundane flux is isotropic and the laws of its propagation are very similar to that of light.</p><p>・ He suggested that the ultramundane corpuscles might move at the speed of light.</p><p>・ To maintain mass proportionality, ordinary matter consists of cage-like structures, in which their diameter is only the 10<sup>7</sup>th part of their mutual distance, so the particles can travel through them nearly unhindered.</p><p>Lyman Spitzer in 1941 calculated that absorption of radiation between two dust particles lead to a net attractive force which varies proportional to 1/r<sup>2</sup> [<xref ref-type="bibr" rid="scirp.67955-ref16">16</xref>] .</p><p>The Le Sage mechanism also has been identified as a significant factor in the behavior of dusty plasma. A. M. Ignatov has shown that an attractive force arises between two dust grains suspended in isotropic collisionless plasma due to inelastic collisions between ions of the plasma and the grains of dust. This attractive force is inversely proportional to the square of the distance between dust grains, and can counterbalance the Coulomb repulsion between dust grains [<xref ref-type="bibr" rid="scirp.67955-ref17">17</xref>] .</p><p>Although it is not regarded as a viable theory within the mainstream scientific community, there are some attempts to re-habilitate the theory [<xref ref-type="bibr" rid="scirp.67955-ref18">18</xref>] - [<xref ref-type="bibr" rid="scirp.67955-ref25">25</xref>] . In this respect, we would like to stress the importance of the extended theories of gravity in the debate about gravitation, as it is clarified in [<xref ref-type="bibr" rid="scirp.67955-ref26">26</xref>] .</p><p>Every Le Sage-type model assumes the existence of a space-filling isotropic flux or radiation of enormous intensity and penetrating capability. The flux of neutrinos emanating from the Sun was discussed in literature. This flux possesses the penetrating properties envisaged by Le Sage, but it is not isotropic, and its intensity is even smaller than that of the Cosmic Microwave Background radiation.</p><p>In our model, the Cosmic Neutrino Background (CNB) is indeed a space-filling and fairly isotropic flux. It has a high intensity since its total neutrino energy density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x207.png" xlink:type="simple"/></inline-formula> is about 69% of the total energy density of the World <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x208.png" xlink:type="simple"/></inline-formula> (see 3.26). One may wonder―if there are so many neutrinos out there, how come the numerous neutrino detectors do not register them in significant quantities?</p><p>According to WUM, CNB consists of three different types of neutrinos: electronic<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x209.png" xlink:type="simple"/></inline-formula>, muonic<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x210.png" xlink:type="simple"/></inline-formula>, and tauonic<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x211.png" xlink:type="simple"/></inline-formula>, and their antiparticles with masses <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x212.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] :</p><disp-formula id="scirp.67955-formula1100"><label>(6.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x213.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1101"><label>(6.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x214.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1102"><label>(6.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x215.png"  xlink:type="simple"/></disp-formula><p>For Fermi momentum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x216.png" xlink:type="simple"/></inline-formula> we took the following value [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] :</p><disp-formula id="scirp.67955-formula1103"><label>(6.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x217.png"  xlink:type="simple"/></disp-formula><p>Then for Fermi energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x218.png" xlink:type="simple"/></inline-formula> we obtain:</p><disp-formula id="scirp.67955-formula1104"><label>(6.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x219.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1105"><label>(6.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x220.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.67955-formula1106"><label>(6.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x221.png"  xlink:type="simple"/></disp-formula><p>It follows that CNB consists of very low-energy neutrinos, whose energy is similar to that of the Cosmic Microwave Background radiation. Their interaction with matter is very weak. Since the neutrino-induced cross- sections depend on the neutrinos energy linearly, such background neutrinos will not be registered by standard neutrino detectors. In fact, we might never be able to directly observe the CNB.</p><p>The obtained results show that the proposed CNB mechanism of Gravitation is relevant for the Le Sage’s theory.</p><p>In our model, Dark Matter particles (DMP) are a space-filling and fairly isotropic flux as well. It possesses the penetrating properties envisaged by Le Sage for his ultramundane corpuscles, and has a high intensity since the total DMP energy density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x222.png" xlink:type="simple"/></inline-formula> is about 24% of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x223.png" xlink:type="simple"/></inline-formula> (see 3.25).</p><p>We should recall that 1/3 of the World energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x224.png" xlink:type="simple"/></inline-formula> is in all Macroobjects and 2/3 of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x225.png" xlink:type="simple"/></inline-formula> is in the Medium of the World which is a space-filling and fairly isotropic in our model [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>] and is responsible for the Le Sage’s mechanism of the gravitation.</p><p>According to WUM, all material objects of the World have gravitational charges. Two particles or microobjects will not exert gravity on one another when both of their masses are smaller than the Planck mass. Planck mass can then be viewed as the mass of the smallest macroobject capable of generating the gravitoelectromagnetic field, and serves as a natural borderline between classical and quantum physics [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] .</p><p>It is obvious that for the realization of Le Sage’s mechanism of gravitation at least one material object must be a macroobject. In our opinion, the smallest such macroobject has Planck mass. The validity of this statement follows from the work of Lyman Spitzer [<xref ref-type="bibr" rid="scirp.67955-ref16">16</xref>] and A. M. Ignatov [<xref ref-type="bibr" rid="scirp.67955-ref17">17</xref>] who identified Le Sage’s mechanism as a significant factor in the behavior ofdust particles and dusty plasma.</p><p>As the conclusion:</p><p>・ Gravity is not an interaction but a manifestation of the Medium of the World;</p><p>・ Le Sage’s theory is the very first theory which defines the Gravity as an emergent phenomenon.</p></sec><sec id="s7"><title>7. Emergent Gravity, Space and Time</title><p>By definition, an emergent phenomenon is a property that is a result of simple interactions that work cooperatively to create a more complex interaction. Physically, the simple interactions occur at a microscopic level, and the collective result can be observed at a macroscopic level. In Le Sage’s theory the gravity is just a result of microscopic interactions which appear to average out on a macroscopic scale and give us gravity as we recognize it.</p><p>C. Barcelo, S. Liberati, and M. Visser have this to say about emergent gravity:</p><p>“One of the more fascinating approaches to ‘quantum gravity’ is the suggestion, typically attributed to Sakharov [<xref ref-type="bibr" rid="scirp.67955-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.67955-ref28">28</xref>] that gravity itself may not be ‘fundamental physics’. Indeed it is now a relatively common opinion, maybe not mainstream but definitely a strong minority opinion, that gravity (and in particular the whole notion of spacetime and spacetime geometry) might be no more ‘fundamental’ than is fluid dynamics. The word ‘fundamental’ is here used in a rather technical sense―fluid mechanics is not fundamental because there is a known underlying microphysics that of molecular dynamics, of which fluid mechanics is only the low-energy low-momentum limit” [<xref ref-type="bibr" rid="scirp.67955-ref29">29</xref>] .</p><p>With Albert Einstein’s principle at heart―“When forced to summarize the theory of relativity in one sentence: time and space and gravitation have no separate existence from matter”―we introduced the Medium of the World consisting of protons, electrons, photons, neutrinos, and dark matter particles. In our model the Medium is not fundamental and has the macroscopic parameters like in fluid mechanics: impedance, gravitomagnetic parameter, etc.</p><p>In frames of WUM we can find the gravitomagnetic parameter of the Medium<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x226.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.67955-formula1107"><label>(7.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x227.png"  xlink:type="simple"/></disp-formula><p>and the impedance of the Medium<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x228.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.67955-formula1108"><label>(7.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x229.png"  xlink:type="simple"/></disp-formula><p>where R is the size of the World, H is Hubble’s parameter and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x230.png" xlink:type="simple"/></inline-formula> is the absolute cosmological time measured from the Beginning of the World like absolute temperature measured from absolute zero in kelvins.</p><p>It follows that measuring the value of Hubble’s parameter anywhere in the World and taking its inverse value allows us to calculate the absolute time of the World<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x231.png" xlink:type="simple"/></inline-formula>. The Hubble’s parameter is then the most important characteristic of the World, as it defines the Worlds’ age.</p><p>The second important characteristic of the World is the gravitomagnetic parameter. Taking its inverse value, we can find the absolute size of the World R. We emphasize that the above two parameters (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x232.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x233.png" xlink:type="simple"/></inline-formula>) are</p><p>principally different physical characteristics of the Medium that are connected through the gravitoelectrodynamic constant c.</p><p>In WUM, time and space are closely connected with the Mediums’ impedance and gravitomagnetic parameter. It follows that neither time nor space could be discussed in absence of the Medium. The gravitational parameter G can be introduced only for the World filled with matter. Matter, then, is primary to time and space and gravity, as Einstein has postulated.</p><p>It follows that the gravity, space and time itself can be introduced only for the World filled with matter consisting of elementary particles which take part in simple interactions at a microscopic level. The collective result of their interactions can be observed at a macroscopic level. It means that Gravity, Space and Time are the emergent phenomena.</p><p>When in history of the World can we introduce the Medium of the World―a macroscopic notion? According to WUM, at the beginning when the size of the World was equal to a and the extrapolated density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x234.png" xlink:type="simple"/></inline-formula> equaled to (see 3.5 at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x235.png" xlink:type="simple"/></inline-formula>)</p><disp-formula id="scirp.67955-formula1109"><label>(7.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x236.png"  xlink:type="simple"/></disp-formula><p>the extrapolated total amount of the surface energy of the World <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x237.png" xlink:type="simple"/></inline-formula> was equal to [<xref ref-type="bibr" rid="scirp.67955-ref1">1</xref>]</p><disp-formula id="scirp.67955-formula1110"><label>(7.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x238.png"  xlink:type="simple"/></disp-formula><p>which was sufficient to produce DIRACs and lighter particles only. The conditions for generating the very first ensemble of particles and the first objects actualized when the size of the World <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x239.png" xlink:type="simple"/></inline-formula> was about the Bohr radius multiplied by 2π (see 3.4)</p><disp-formula id="scirp.67955-formula1111"><label>(7.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x240.png"  xlink:type="simple"/></disp-formula><p>at the cosmological time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x241.png" xlink:type="simple"/></inline-formula> (see 3.3)</p><disp-formula id="scirp.67955-formula1112"><label>(7.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x242.png"  xlink:type="simple"/></disp-formula><p>The total energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x243.png" xlink:type="simple"/></inline-formula> was equal to</p><disp-formula id="scirp.67955-formula1113"><label>(7.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x244.png"  xlink:type="simple"/></disp-formula><p>and the Planck mass was equal to twice the mass of WIMPs (see 3.8)</p><disp-formula id="scirp.67955-formula1114"><label>(7.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2180112x245.png"  xlink:type="simple"/></disp-formula><p>At that time, neutralinos (the heaviest particles in our model with mass<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x246.png" xlink:type="simple"/></inline-formula>) could initiate a gravita-</p><p>tional collapse of all particles heavier than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x247.png" xlink:type="simple"/></inline-formula> (neutralinos, WIMPs, protons) [<xref ref-type="bibr" rid="scirp.67955-ref3">3</xref>] with the resulting microobjects―nuclei. All lighter particles would then be attracted to the nuclei, increasing their masses and initiating the macroobjects’ formation.</p><p>As the conclusion:</p><p>・ The macroscopic notion―the Medium of the World can be introduced at the cosmological time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x248.png" xlink:type="simple"/></inline-formula>.</p><p>・ The emergent Gravity, Space and Time can be introduced for cosmological times<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2180112x249.png" xlink:type="simple"/></inline-formula>.</p><p>While the Model needs significant further elaboration, it can already serve as a basis for a new physics proposed by Le Sage, J. McCullagh, O. Heaviside, P. Dirac, A. D. Sakharov, and P. Wesson.</p></sec><sec id="s8"><title>Acknowledgements</title><p>I am grateful to the anonymous referee for important remarks. 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