<?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">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2016.79078</article-id><article-id pub-id-type="publisher-id">JMP-66431</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>
 
 
  Gravitational Space-Time Curve Generation via Accelerated Charged Particles
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>dward</surname><given-names>A. Walker</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>Mathematics Department, Florida Memorial University, Miami Gardens, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>dwrdwalker@yahoo.com</email></corresp></author-notes><pub-date pub-type="epub"><day>13</day><month>05</month><year>2016</year></pub-date><volume>07</volume><issue>09</issue><fpage>863</fpage><lpage>874</lpage><history><date date-type="received"><day>8</day>	<month>April</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>10</month>	<year>May</year>	</date><date date-type="accepted"><day>13</day>	<month>May</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>
 
 
  A force with an acceleration that is equal to multiples greater than the speed of light per unit time is exerted on a cloud of charged particles. The particles are resultantly accelerated to within an infinitesimal fraction of the speed of light. As the force or acceleration increases, the particles’ velocity asymptotically approaches but never achieves the speed of light obeying relativity. The asymptotic increase in the particles’ velocity toward the speed of light as acceleration increasingly surpasses the speed of light per unit time does not compensate for the momentum value produced on the particles at sub-light velocities. Hence, the particles’ inertial mass value must increase as acceleration increases. This increase in the particles’ inertial mass as the particles are accelerated produce a gravitational field which is believed to occur in the oscillation of quarks achieving velocities close to the speed of light. The increased inertial mass of the density of accelerated charged particles becomes the source mass (or Big “M”) in Newton’s equation for gravitational force. This implies that a space-time curve is generated by the accelerated particles. Thus, it is shown that the acceleration number (or multiple of the speed of light greater than 1 per unit of time) and the number of charged particles in the cloud density are surjectively mapped to points on a differential manifold or space-time curved surface. Two aspects of Einstein’s field equations are used to describe the correspondence between the gravitational field produced by the accelerated particles and the resultant space-time curve. The two aspects are the Schwarzchild metric and the stress energy tensor. Lastly, the possibility of producing a sufficient acceleration or electromagnetic force on the charged particles to produce a gravitational field is shown through the Lorentz force equation. Moreover, it is shown that a sufficient voltage can be generated to produce an acceleration/force on the particles that is multiples greater than the speed of light per unit time thereby generating gravity. 
 
</p></abstract><kwd-group><kwd>Charged Particles</kwd><kwd> Accelerated Particles</kwd><kwd> Inertial Mass</kwd><kwd> Gravitational Force</kwd><kwd> Einstein’s Field Equations</kwd><kwd> Space-Time Manifold</kwd><kwd> Schwardchild Metric</kwd><kwd> Stress Energy Tensor</kwd><kwd> Surjective Mapping</kwd><kwd> Lorentz Force</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>It has been shown that a gravitational field can be generated by the oscillation of a quark in a paper written by author Eli Peter Manor published in 2016 in the Journal of Modern physics [<xref ref-type="bibr" rid="scirp.66431-ref1">1</xref>] . While oscillating, the quark would achieve velocities that near the speed of light; the inertial mass of the particle would increase resultantly generating a gravitational field [<xref ref-type="bibr" rid="scirp.66431-ref1">1</xref>] . The aim of this paper is to show that a gravitational field can also be produced as the inertial mass of a charged particle increases when accelerated to the verge of the speed of light via an electromagnetic field (as in a particle accelerators). Moreover, a description of the space-time curve associated with the gravitational field generated will be mathematically formulated.</p><p>In describing the assertion of this paper in more detail; a gravitational field is generated when a cloud of charged particles is accelerated to the precipice of the speed of light. The acceleration enacted on the particles exceed the speed of light per unit time, however massive particles cannot exceed the speed of light as is well known. Resultantly, as the acceleration increasingly exceeds the speed of light per unit time, the particles’ velocities approaches but never achieves a luminous velocity. Mathematically, the particles’ velocities asymptotically approaching the speed of light will not compensate for the amount of force or acceleration exerted on the particles; the inertial mass value of each particle must increase to compensate for the increasing acceleration or force. In this assertion, each charged particles’ velocity is approximated to a constant 99% of the speed of light (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x6.png" xlink:type="simple"/></inline-formula>), allowing the measurement of increased inertial particle mass. Consider Newtonian gravitational force as shown below [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula87"><graphic  xlink:href="http://html.scirp.org/file/1-7502714x7.png"  xlink:type="simple"/></disp-formula><p>All mass values correspond to a density value; even if the unit volume is infinitesimally small. The sum total of increasing individual inertial mass values of each particle in the density of accelerated particles is set equal to source mass M in the gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x8.png" xlink:type="simple"/></inline-formula> as the acceleration on the charged particles increase. Hence, as the force acting on the particles increase with an invariant approximate velocity of 99% the speed of light; the corresponding force of gravity increases proportionally. This implies that a curvature in space-time is also generated by the cloud of accelerated charged particles. Therefore, Einstein’s field equations are used to describe the curvature in space-time generated by the accelerated charged particles. It will be shown that there exist a surjective or “onto” map from the Cartesian product of the particles acceleration number (or the multiples of acceleration past the speed of light per unit time) and the number of particles in the cloud density to the codomain of points and displacements on a space-time manifold. Two descriptions using Einstein’s field equation are shown to correlate to the surjective mapping from the domain of the particle acceleration number and the number of particles to the codomain of points or displacements on the space-time curve produced by the accelerated cloud. The first description is the Schwarzchild metric description and the second is the stress-energy tensor description. Lastly, the electromagnetic force or Lorentz force equation is used to show that it is possible to obtain a sufficient voltage to accelerate a cloud of charged particles to a velocity that is an infinitesimal fraction below the speed of light to produce a gravitational field and/or space-time curve.</p></sec><sec id="s2"><title>2. Acceleration of Charged Particles and Newtonian Gravitation</title><p>In using electromagnetic force or Lorentz force to accelerate the cloud of charged particles, acceleration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x9.png" xlink:type="simple"/></inline-formula> is generated. Acceleration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x10.png" xlink:type="simple"/></inline-formula> is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x11.png" xlink:type="simple"/></inline-formula> multiples of the speed of light c per unit time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x12.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x13.png" xlink:type="simple"/></inline-formula> is any real number that is greater than or equal to one. Number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x14.png" xlink:type="simple"/></inline-formula> will be referred to as the acceleration number.</p><disp-formula id="scirp.66431-formula88"><label>(1.0)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x15.png"  xlink:type="simple"/></disp-formula><p>Acceleration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x16.png" xlink:type="simple"/></inline-formula> corresponds to the force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x17.png" xlink:type="simple"/></inline-formula> per area <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x18.png" xlink:type="simple"/></inline-formula> acting on the cloud of accelerated charged particles, which correspond to pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x19.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x20.png" xlink:type="simple"/></inline-formula>) [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] . Area <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x21.png" xlink:type="simple"/></inline-formula> is also the cross sectional area traversed by the charged particles. The force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x22.png" xlink:type="simple"/></inline-formula> can be expressed in terms of Newton’s second law such that [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] :</p><disp-formula id="scirp.66431-formula89"><label>(1.01)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x23.png"  xlink:type="simple"/></disp-formula><p>The momentum value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x24.png" xlink:type="simple"/></inline-formula> is conventionally obtained by integrating force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x25.png" xlink:type="simple"/></inline-formula> in respect to time t with limits of integration from zero to time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x26.png" xlink:type="simple"/></inline-formula> as shown below [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula90"><label>(1.02)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x27.png"  xlink:type="simple"/></disp-formula><p>Keep in mind that momentum value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula> corresponds to the relativistic energy value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula>; where the particles’ mass value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x30.png" xlink:type="simple"/></inline-formula> in energy E is treated as rest mass due to the fact that the charged particles are massive particles and not relativistic particles such as photons [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] . Acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x31.png" xlink:type="simple"/></inline-formula> varies proportionally to force<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x32.png" xlink:type="simple"/></inline-formula>. Thus momentum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x33.png" xlink:type="simple"/></inline-formula> corresponds to force<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x34.png" xlink:type="simple"/></inline-formula>, however it is well understood that the charged particles of inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x35.png" xlink:type="simple"/></inline-formula> cannot obtain super luminous velocities, therefore the particles’ approximate momentum will be denoted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x36.png" xlink:type="simple"/></inline-formula> as shown in Equation (1.03) below.</p><disp-formula id="scirp.66431-formula91"><label>(1.03)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x37.png"  xlink:type="simple"/></disp-formula><p>As acceleration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x38.png" xlink:type="simple"/></inline-formula> increases, the particles’ velocity asymptotically approach but never achieve the speed of light; to circumvent this infinite decimal expansion, the asymptotic increase is set equal to the constant approximate of velocity denoted<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x39.png" xlink:type="simple"/></inline-formula>. Velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x40.png" xlink:type="simple"/></inline-formula> is the particles’ approximate velocity “close to” but less than the speed of light as shown by Equation (1.04). Velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x41.png" xlink:type="simple"/></inline-formula> is approximated to 99 percent of the speed of light for the purposes of this formulation.</p><disp-formula id="scirp.66431-formula92"><label>(1.04)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x42.png"  xlink:type="simple"/></disp-formula><p>Mass value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x43.png" xlink:type="simple"/></inline-formula> corresponding to momentum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x44.png" xlink:type="simple"/></inline-formula> is referred to as variable inertial mass. Variable inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x45.png" xlink:type="simple"/></inline-formula> takes on values greater than or equal to inertial mass<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x46.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.66431-formula93"><label>(1.05)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x47.png"  xlink:type="simple"/></disp-formula><p>To avoid confusion, it must be noted that relativistic mass dilation is different from the variation of variable mass or inertial <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x48.png" xlink:type="simple"/></inline-formula> as the particle approaches the speed of light. This can be conveyed by setting variable inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x49.png" xlink:type="simple"/></inline-formula> equal to the product of the variable inertial mass and the Lorentz factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x50.png" xlink:type="simple"/></inline-formula> as shown below [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula94"><label>(1.06)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x51.png"  xlink:type="simple"/></disp-formula><p>This can alternatively be expressed such that [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] :</p><disp-formula id="scirp.66431-formula95"><label>(1.07)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x52.png"  xlink:type="simple"/></disp-formula><p>Equation (1.06) implies that the Lorentz factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x53.png" xlink:type="simple"/></inline-formula> is equal to 1 and implies that relative velocity v or the velocity of an observer is zero (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x54.png" xlink:type="simple"/></inline-formula>) for the purpose of this derivation.</p><disp-formula id="scirp.66431-formula96"><label>(1.08)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x55.png"  xlink:type="simple"/></disp-formula><p>Thus inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x56.png" xlink:type="simple"/></inline-formula> does not vary according to the Lorentz factor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x57.png" xlink:type="simple"/></inline-formula>. Conclusively, relativistic mass is dependent on the velocity and orientation of an observer while the inertial varies according to momentum. In continuing the formulation, momentum value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x58.png" xlink:type="simple"/></inline-formula> is set equal to momentum<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x59.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.66431-formula97"><label>(1.09)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x60.png"  xlink:type="simple"/></disp-formula><p>This equivalence can be expressed as:</p><disp-formula id="scirp.66431-formula98"><label>(1.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x61.png"  xlink:type="simple"/></disp-formula><p>Equation (1.10) represents an important aspect of the assertion. The charged particles of the accelerated mass cannot exceed the speed of light, thus, variable inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x62.png" xlink:type="simple"/></inline-formula> must vary proportionally to the acceleration number<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x63.png" xlink:type="simple"/></inline-formula>; where the values c, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x64.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x65.png" xlink:type="simple"/></inline-formula> are constant. At this juncture, one solves for variable inertial mass<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x66.png" xlink:type="simple"/></inline-formula>. Variable inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x67.png" xlink:type="simple"/></inline-formula> is such that:</p><disp-formula id="scirp.66431-formula99"><label>(1.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x68.png"  xlink:type="simple"/></disp-formula><p>Equation (1.11) can be expressed such that:</p><disp-formula id="scirp.66431-formula100"><label>(1.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x69.png"  xlink:type="simple"/></disp-formula><p>The premise of the assertion is the correlation of the acceleration of a cloud of charged particles and gravitation, therefore Newtonian gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x70.png" xlink:type="simple"/></inline-formula> is given such that [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] :</p><disp-formula id="scirp.66431-formula101"><label>(1.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x71.png"  xlink:type="simple"/></disp-formula><p>The density of the accelerated cloud of charged particles is denoted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x72.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x73.png" xlink:type="simple"/></inline-formula> is the discrete number of charged particles in the cloud per unit volume (V) as displayed below.</p><disp-formula id="scirp.66431-formula102"><label>(1.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x74.png"  xlink:type="simple"/></disp-formula><p>This implies that:</p><disp-formula id="scirp.66431-formula103"><label>(1.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x75.png"  xlink:type="simple"/></disp-formula><p>where M is the source mass in gravitational force<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x76.png" xlink:type="simple"/></inline-formula>. In the task of defining gravitation in terms of the varying inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x77.png" xlink:type="simple"/></inline-formula> associated with the accelerated cloud of charged particles, again, consider Newtonian gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x78.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula104"><label>(1.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x79.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x80.png" xlink:type="simple"/></inline-formula> are the spatial coordinates in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x81.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x82.png" xlink:type="simple"/></inline-formula>), mass M in Equation (1.16) (or Newtonian gravitational force) is substituted according to expression 1.15 (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x83.png" xlink:type="simple"/></inline-formula>). Newtonian gravitational force can then be expressed such that:</p><disp-formula id="scirp.66431-formula105"><label>(1.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x84.png"  xlink:type="simple"/></disp-formula><p>Mass value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x85.png" xlink:type="simple"/></inline-formula> is the mass of the particle at distance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x86.png" xlink:type="simple"/></inline-formula> under the influence of the gravitational force produced by the cloud of accelerated charged particles. Substituting the value of inertial mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x87.png" xlink:type="simple"/></inline-formula> into Equation (1.17); gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x88.png" xlink:type="simple"/></inline-formula> can then be expressed such that:</p><disp-formula id="scirp.66431-formula106"><label>(1.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x89.png"  xlink:type="simple"/></disp-formula><p>Therefore, the accelerating force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x90.png" xlink:type="simple"/></inline-formula> acting on the charged particles is oriented in the direction of travel while the force of gravity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x91.png" xlink:type="simple"/></inline-formula> generated by the particles is orthogonal to the direction of travel and therefore force<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x92.png" xlink:type="simple"/></inline-formula>. Section 2 will introduce the correlation of the gravitational space-time curve associated with the gravitational field generated by the accelerated charged particles.</p></sec><sec id="s3"><title>3. Gravitation Produced by Accelerated Charged Particles and Einstein’s Field Equations</title><p>The gravitational field generated by the cloud of accelerated particles on the verge of the speed of light inherently produces a space-time curve. Therefore the mathematical description of the space-time curve produced by the accelerated charged particles is given by Einstein’s field equation. Consider the function of expression (2.0) below.</p><disp-formula id="scirp.66431-formula107"><label>(2.0)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x93.png"  xlink:type="simple"/></disp-formula><p>The function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula> is a surjective or “onto” map from the domain composed of the Cartesian product <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula> to the codomain of n-dimensional real numbers <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x96.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] . Map <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x97.png" xlink:type="simple"/></inline-formula> has a domain of the number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x98.png" xlink:type="simple"/></inline-formula> of charged particles in the density of the cloud of accelerated particles which is an element of natural numbers (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x99.png" xlink:type="simple"/></inline-formula>) and the acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x100.png" xlink:type="simple"/></inline-formula> which is an element of real numbers (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x101.png" xlink:type="simple"/></inline-formula>). Map <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x102.png" xlink:type="simple"/></inline-formula> is expressed as shown below [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] .</p><disp-formula id="scirp.66431-formula108"><label>(2.01)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x103.png"  xlink:type="simple"/></disp-formula><p>The symbol <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula> denotes the field function to which the space-time curve or manifold is defined [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] . In more technical terms, the field <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula> represents the differential manifold to which the metric tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula> is defined on [<xref ref-type="bibr" rid="scirp.66431-ref4">4</xref>] . Thus function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula> is a map from the set of Minkowski coordinates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.66431-ref4">4</xref>] in set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x110.png" xlink:type="simple"/></inline-formula>) to the codomain of the set of points and displacements in set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x111.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x112.png" xlink:type="simple"/></inline-formula>) which is the set of points and displacements on the n-dimensional differential manifold or space-time curve surface. Where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x113.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x114.png" xlink:type="simple"/></inline-formula>) is a partial derivative operator in respect to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x115.png" xlink:type="simple"/></inline-formula>, the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x116.png" xlink:type="simple"/></inline-formula> is a map such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula109"><label>(2.02)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x117.png"  xlink:type="simple"/></disp-formula><p>The equivalence of function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x118.png" xlink:type="simple"/></inline-formula> and function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x119.png" xlink:type="simple"/></inline-formula> imply a composition of functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x120.png" xlink:type="simple"/></inline-formula>. Thus, Equation (2.0) expresses the composition map such that:</p><disp-formula id="scirp.66431-formula110"><label>(2.03)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x121.png"  xlink:type="simple"/></disp-formula><p>Thus, for every value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula> in the domain of map <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula> there exist a value a (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula>) such that a is an element of set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x126.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x127.png" xlink:type="simple"/></inline-formula>), hence the “onto” or surjective mapping. Expression 2.0 is the correspondence of the number of particles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x128.png" xlink:type="simple"/></inline-formula> and acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x129.png" xlink:type="simple"/></inline-formula> to solutions of Einstein’s field equation which are defined on a space-time manifold or set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x130.png" xlink:type="simple"/></inline-formula>. It will now be shown that the function of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x131.png" xlink:type="simple"/></inline-formula> correspond to given solutions of the Einstein Field equations. Let function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x132.png" xlink:type="simple"/></inline-formula> equal a value such that:</p><disp-formula id="scirp.66431-formula111"><label>(2.04)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x133.png"  xlink:type="simple"/></disp-formula><p>where A and B are arbitrary values, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x134.png" xlink:type="simple"/></inline-formula>is the metric tensor, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x135.png" xlink:type="simple"/></inline-formula> is an element of the set of values on the n-dimensional differential manifold <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x136.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x137.png" xlink:type="simple"/></inline-formula>. The Einstein tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x138.png" xlink:type="simple"/></inline-formula> is set equal function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x139.png" xlink:type="simple"/></inline-formula> such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula112"><label>(2.05)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x140.png"  xlink:type="simple"/></disp-formula><p>The Einstein tensor is given such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula113"><label>(2.06)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x141.png"  xlink:type="simple"/></disp-formula><p>[where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x142.png" xlink:type="simple"/></inline-formula> is the Ricci tensor, R is the scalar constant, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x143.png" xlink:type="simple"/></inline-formula> is the differential commutator for computing curvature [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] . This implies that the values of A and B in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x144.png" xlink:type="simple"/></inline-formula> are such that:</p><p><img data-original="http://html.scirp.org/file/1-7502714x145.png" />,<img data-original="http://html.scirp.org/file/1-7502714x146.png" /> (2.07)</p><p>As a second example, function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x147.png" xlink:type="simple"/></inline-formula> is now set equal to the stress-energy tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x148.png" xlink:type="simple"/></inline-formula> for a perfect fluid as shown below.</p><disp-formula id="scirp.66431-formula114"><label>(2.08)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x149.png"  xlink:type="simple"/></disp-formula><p>The Stress-energy tensor is given such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula115"><label>(2.09)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x150.png"  xlink:type="simple"/></disp-formula><p>[where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x151.png" xlink:type="simple"/></inline-formula> is the Lagrangian for the Klein-Gordon equation [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] ] This implies that the values of A and B in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x152.png" xlink:type="simple"/></inline-formula> are such that:</p><p><img data-original="http://html.scirp.org/file/1-7502714x153.png" />,<img data-original="http://html.scirp.org/file/1-7502714x154.png" /> (2.10)</p><p>Due to the equivalence of function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x155.png" xlink:type="simple"/></inline-formula> and function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x156.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x157.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x158.png" xlink:type="simple"/></inline-formula>; this Implies that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x159.png" xlink:type="simple"/></inline-formula>;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x160.png" xlink:type="simple"/></inline-formula> (2.11)</p><p>Therefore the components of the Einstein tensor and the stress-energy tensor reside in the codomain of function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x161.png" xlink:type="simple"/></inline-formula>. This paper presents two derivations of Einstein’s field equations that express the equivalence of the functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x162.png" xlink:type="simple"/></inline-formula>. Therefore, there are two descriptions of the space-time curve generated by the cloud of accelerated charged particles using two separate aspects of Einstein’s field equations. The first description is the Schwarzchild aspect and the second is the stress-energy aspect as will be formulated in the next section.</p></sec><sec id="s4"><title>4. The Schwarzchild and Stress-Energy Description of a Space-Time Curve Generated by a Cloud of Accelerated Particles</title><p>Section 3 will introduce two formulations linking the number of particles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x163.png" xlink:type="simple"/></inline-formula> and acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x164.png" xlink:type="simple"/></inline-formula> to solutions to Einstein’s field equations, hence, validating the equivalence of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x165.png" xlink:type="simple"/></inline-formula>. The formulation begins with the Schwarzchild description.</p><p>The Schwarzchild descritption</p><p>In reference to this hypothetical description, accelerated charged particles traveling at velocities bordering the speed of light generate a gravitational field on a spherically symmetric body, hence, the need to formulate a description using the Schwarzchild metric. The Schwarzchild radius is given such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula116"><label>(3.0)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x166.png"  xlink:type="simple"/></disp-formula><p>Gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x167.png" xlink:type="simple"/></inline-formula> of Equation (1.18) is expressed in terms of the Schwarzchild radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x168.png" xlink:type="simple"/></inline-formula> as shown below.</p><disp-formula id="scirp.66431-formula117"><label>(3.01)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x169.png"  xlink:type="simple"/></disp-formula><p>Gravitational potential energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x170.png" xlink:type="simple"/></inline-formula> is conventionally obtained by evaluating the integral in respect to Schwarzchild radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x171.png" xlink:type="simple"/></inline-formula> giving a value such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula118"><label>(3.02)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x172.png"  xlink:type="simple"/></disp-formula><p>The maximum value of kinetic energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x173.png" xlink:type="simple"/></inline-formula> for a particle of mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x174.png" xlink:type="simple"/></inline-formula> in the fluid with a maximum velocity at the speed of light c is given such that [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] :</p><disp-formula id="scirp.66431-formula119"><label>(3.03)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x175.png"  xlink:type="simple"/></disp-formula><p>As is conventionally performed, kinetic energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x176.png" xlink:type="simple"/></inline-formula> is set equal to gravitational potential energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x177.png" xlink:type="simple"/></inline-formula> as shown below [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula120"><label>(3.04)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x178.png"  xlink:type="simple"/></disp-formula><p>This equivalence can be expressed as [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] :</p><disp-formula id="scirp.66431-formula121"><label>(3.05)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x179.png"  xlink:type="simple"/></disp-formula><p>Solving for the Schwarzchild radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x180.png" xlink:type="simple"/></inline-formula> gives the radius in terms of the number of particles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x181.png" xlink:type="simple"/></inline-formula> and acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x182.png" xlink:type="simple"/></inline-formula> as shown below [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula122"><label>(3.06)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x183.png"  xlink:type="simple"/></disp-formula><p>The Schwarzchild metric is given such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula123"><label>(3.07)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x184.png"  xlink:type="simple"/></disp-formula><p>The functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x185.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x186.png" xlink:type="simple"/></inline-formula> take on values of the Schwarzchild radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x187.png" xlink:type="simple"/></inline-formula> such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula124"><label>(3.08)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x188.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66431-formula125"><label>(3.09)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x189.png"  xlink:type="simple"/></disp-formula><p>[where r is the radius of the spherically symmetric body <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x190.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] ] The prime notation (') denotes that the variations in the metric correspond to the number of particles<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x191.png" xlink:type="simple"/></inline-formula> and acceleration number<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x192.png" xlink:type="simple"/></inline-formula>. The metric <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x193.png" xlink:type="simple"/></inline-formula> is set equal to the metric tensor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x194.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.66431-formula126"><label>(3.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x195.png"  xlink:type="simple"/></disp-formula><p>Expressing the value of metric tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x196.png" xlink:type="simple"/></inline-formula> gives the matrix expression of:</p><disp-formula id="scirp.66431-formula127"><label>(3.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x197.png"  xlink:type="simple"/></disp-formula><p>Therefore, the Einstein tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x198.png" xlink:type="simple"/></inline-formula> can be expressed such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula128"><label>(3.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x199.png"  xlink:type="simple"/></disp-formula><p>where the Ricci tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x200.png" xlink:type="simple"/></inline-formula> is expressed in terms of the differential commutator for computing curvature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x201.png" xlink:type="simple"/></inline-formula> such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula129"><label>(3.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x202.png"  xlink:type="simple"/></disp-formula><p>The requirement of the equivalence of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x203.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x204.png" xlink:type="simple"/></inline-formula>) is satisfied where function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x205.png" xlink:type="simple"/></inline-formula> is substituted by function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x206.png" xlink:type="simple"/></inline-formula> at time t, spherical radius r, and spherical angles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x207.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x208.png" xlink:type="simple"/></inline-formula> indicating the spherical coordinates of the Schwarzchild metric.</p><disp-formula id="scirp.66431-formula130"><label>(3.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x209.png"  xlink:type="simple"/></disp-formula><p>The stress-energy tensor description</p><p>A cloud of charged particles are again accelerated via an electromagnetic force (of any given source i.e. particle accelerator or subatomic charged particles emitted from a star) to the verge of the speed of light producing a gravitational field that is exerting on a fluid of particles of mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x210.png" xlink:type="simple"/></inline-formula> per unit volume. For the purpose of this derivation, the fluid is considered a perfect fluid. Thus, the stress energy tensor for a perfect fluid <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x211.png" xlink:type="simple"/></inline-formula> is expressed as shown below [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] .</p><disp-formula id="scirp.66431-formula131"><label>(3.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x212.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x213.png" xlink:type="simple"/></inline-formula> is the Lagrangian for the Klein-Gordon equation as shown below [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] .</p><disp-formula id="scirp.66431-formula132"><label>(3.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x214.png"  xlink:type="simple"/></disp-formula><p>The fluid 4-velocity denoted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x215.png" xlink:type="simple"/></inline-formula> varies along a geodesic embedded on the space-time manifold. Fluid velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x216.png" xlink:type="simple"/></inline-formula> progresses along a time-like curve and can be expressed in terms of the chain rule [<xref ref-type="bibr" rid="scirp.66431-ref5">5</xref>] as expressed below [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] .</p><disp-formula id="scirp.66431-formula133"><label>(3.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x217.png"  xlink:type="simple"/></disp-formula><p>The geodesic rule is acknowledged as shown below [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] .</p><disp-formula id="scirp.66431-formula134"><label>(3.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x218.png"  xlink:type="simple"/></disp-formula><p>Hence the appropriate use of the Christoffel symbol <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x219.png" xlink:type="simple"/></inline-formula> applies as follows [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] .</p><disp-formula id="scirp.66431-formula135"><label>(3.19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x220.png"  xlink:type="simple"/></disp-formula><p>In substituting fluid velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x221.png" xlink:type="simple"/></inline-formula> for the differential notation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x222.png" xlink:type="simple"/></inline-formula> in Equation (3.15), the stress-energy tensor is expressed such that [<xref ref-type="bibr" rid="scirp.66431-ref3">3</xref>] :</p><disp-formula id="scirp.66431-formula136"><label>(3.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x223.png"  xlink:type="simple"/></disp-formula><p>Consider dynamic pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x224.png" xlink:type="simple"/></inline-formula> at fluid velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x225.png" xlink:type="simple"/></inline-formula> and fluid density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x226.png" xlink:type="simple"/></inline-formula> shown below.</p><disp-formula id="scirp.66431-formula137"><label>(3.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x227.png"  xlink:type="simple"/></disp-formula><p>At this juncture, fluid velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x228.png" xlink:type="simple"/></inline-formula> is substituted with the time-like partial derivative <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x229.png" xlink:type="simple"/></inline-formula> in dynamic pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x230.png" xlink:type="simple"/></inline-formula> as shown below [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula138"><label>(3.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x231.png"  xlink:type="simple"/></disp-formula><p>Or alternatively,</p><disp-formula id="scirp.66431-formula139"><label>(3.23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x232.png"  xlink:type="simple"/></disp-formula><p>Let dynamic pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x233.png" xlink:type="simple"/></inline-formula> equal the expression of the sums of components of partial pressure<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x234.png" xlink:type="simple"/></inline-formula>, where each component of pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x235.png" xlink:type="simple"/></inline-formula> is a part of the diagonal components of the 4 by 4 matrix of stress-energy tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x236.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x237.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.66431-formula140"><label>(3.24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x238.png"  xlink:type="simple"/></disp-formula><p>This implies that:</p><disp-formula id="scirp.66431-formula141"><label>(3.25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x239.png"  xlink:type="simple"/></disp-formula><p>Isolating the partial derivatives<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x240.png" xlink:type="simple"/></inline-formula>, gives:</p><disp-formula id="scirp.66431-formula142"><label>(3.26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x241.png"  xlink:type="simple"/></disp-formula><p>Substituting Equation (3.26) into Equation (3.20) (or the stress tensor), one obtains:</p><disp-formula id="scirp.66431-formula143"><label>(3.27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x242.png"  xlink:type="simple"/></disp-formula><p>Consider the unit vector u in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x243.png" xlink:type="simple"/></inline-formula> shown below [<xref ref-type="bibr" rid="scirp.66431-ref5">5</xref>] .</p><disp-formula id="scirp.66431-formula144"><label>(3.28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x244.png"  xlink:type="simple"/></disp-formula><p>Gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x245.png" xlink:type="simple"/></inline-formula> generated by accelerated particles is multiplied by unit vector giving a vector valued force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x246.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.66431-ref5">5</xref>] .</p><disp-formula id="scirp.66431-formula145"><label>(3.29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x247.png"  xlink:type="simple"/></disp-formula><p>Using the classical equation of pressure equal to force per unit area (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x248.png" xlink:type="simple"/></inline-formula>) [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] , components of pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x249.png" xlink:type="simple"/></inline-formula> is set equal to the components of the ratio of vector valued gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x250.png" xlink:type="simple"/></inline-formula> and spherically symmetric area <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x251.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x251.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x252.png" xlink:type="simple"/></inline-formula>) perpendicular to force as shown below.</p><disp-formula id="scirp.66431-formula146"><label>(3.30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x253.png"  xlink:type="simple"/></disp-formula><p>The sums of components of pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x254.png" xlink:type="simple"/></inline-formula> are equal to the sums of components <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x255.png" xlink:type="simple"/></inline-formula> such that:</p><disp-formula id="scirp.66431-formula147"><label>(3.31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x256.png"  xlink:type="simple"/></disp-formula><p>Substituting the value of Equation (3.31) into Equation (3.27) gives the stress energy tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x257.png" xlink:type="simple"/></inline-formula> such that:</p><disp-formula id="scirp.66431-formula148"><label>(3.32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x258.png"  xlink:type="simple"/></disp-formula><p>The stress energy tensor is set equal to the Einstein tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x259.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x260.png" xlink:type="simple"/></inline-formula>) to show the correspondence between the gravitational stress T (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x261.png" xlink:type="simple"/></inline-formula>) exerted on a perfect fluid which flows through a region of space-time and the curved geometry of that region of space-time to which the fluid travels. Thus, Equation (3.32) below gives a full description of the gravitational effects of the cloud of accelerated charged particles on both the dynamics of the fluid and the curved surface of the space-time maniflold.</p><disp-formula id="scirp.66431-formula149"><label>(3.32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x262.png"  xlink:type="simple"/></disp-formula><p>Conclusively, the stress-energy tensor describing the pressure exerted by the gravitational field produced by the accelerated charged particles on a perfect fluid correspond to the surjective map of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x263.png" xlink:type="simple"/></inline-formula> (or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x264.png" xlink:type="simple"/></inline-formula>). Therefore it has been effectively shown to correlate the variations in the number of particles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x265.png" xlink:type="simple"/></inline-formula> and acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x266.png" xlink:type="simple"/></inline-formula> to solutions to Einstein’s field equation.</p></sec><sec id="s5"><title>5. The Generation of Electromagnetic Force to Exert Sufficient Acceleration to Produce a Gravitational Field</title><p>It is of great importance to show the possibility and feasibility of accelerating a cloud of charged particles to an extent to where they actually produce a gravitational field in the real world. Thus, the Lorentz equation of electromagnetic force is applied to show this possibility. Lorentz force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x267.png" xlink:type="simple"/></inline-formula> is as shown below [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula150"><label>(4.0)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x268.png"  xlink:type="simple"/></disp-formula><p>The velocity vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x269.png" xlink:type="simple"/></inline-formula> is the velocity of each individual charged particle in the cloud density being accelerated by vector valued electromagnetic force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x269.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x270.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] . Where q is the individual charge of each particle in the cloud density. The x-component of particle velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x269.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x270.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x271.png" xlink:type="simple"/></inline-formula> is given as approximated velocity value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x269.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x270.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x271.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x272.png" xlink:type="simple"/></inline-formula> as shown below.</p><disp-formula id="scirp.66431-formula151"><label>(4.01)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x273.png"  xlink:type="simple"/></disp-formula><p>The vector value for the magnetic field is given such that:</p><disp-formula id="scirp.66431-formula152"><label>(4.02)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x274.png"  xlink:type="simple"/></disp-formula><p>The vector value for the electric field is given such that:</p><disp-formula id="scirp.66431-formula153"><label>(4.03)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x275.png"  xlink:type="simple"/></disp-formula><p>Carrying out the cross product of velocity vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x276.png" xlink:type="simple"/></inline-formula> and magnetic field vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x276.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x277.png" xlink:type="simple"/></inline-formula> give the orthogonal vector value shown below.</p><disp-formula id="scirp.66431-formula154"><label>(4.04)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x278.png"  xlink:type="simple"/></disp-formula><p>The value of Lorentz force vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x279.png" xlink:type="simple"/></inline-formula> at the given vector quantities of electric field<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x279.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x280.png" xlink:type="simple"/></inline-formula>, particle velocity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x279.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x280.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x281.png" xlink:type="simple"/></inline-formula>, and magnetic field <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x279.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x280.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x281.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x282.png" xlink:type="simple"/></inline-formula> are that of Equation (4.05) below.</p><disp-formula id="scirp.66431-formula155"><label>(4.05)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x283.png"  xlink:type="simple"/></disp-formula><p>The magnitude of electromagnetic force vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x284.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x284.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x285.png" xlink:type="simple"/></inline-formula>) takes on a value such that:</p><disp-formula id="scirp.66431-formula156"><label>(4.06)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x286.png"  xlink:type="simple"/></disp-formula><p>The magnitude of electromagnetic force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x287.png" xlink:type="simple"/></inline-formula> is set equal to force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x287.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x288.png" xlink:type="simple"/></inline-formula> corresponding to pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x287.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x288.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x289.png" xlink:type="simple"/></inline-formula> and cross sectional area <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x287.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x288.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x289.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x290.png" xlink:type="simple"/></inline-formula> (previously mentioned in section 1) to be acting on the cloud of charged particles as shown in Equation (4.07) below.</p><disp-formula id="scirp.66431-formula157"><label>(4.07)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x291.png"  xlink:type="simple"/></disp-formula><p>Recall that acceleration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x292.png" xlink:type="simple"/></inline-formula> corresponds to the force (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x292.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x293.png" xlink:type="simple"/></inline-formula>) per unit area (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x292.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x293.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x294.png" xlink:type="simple"/></inline-formula>) acting on the cloud of accelerated charged particles, which correspond to pressure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x292.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x293.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x294.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x295.png" xlink:type="simple"/></inline-formula> (where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x292.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x293.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x294.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x295.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x296.png" xlink:type="simple"/></inline-formula>). Recall that force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x292.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x293.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x294.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x295.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x296.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x297.png" xlink:type="simple"/></inline-formula> takes on a value such that:</p><disp-formula id="scirp.66431-formula158"><label>(4.08)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x298.png"  xlink:type="simple"/></disp-formula><p>The value of Equation (4.07) then becomes:</p><disp-formula id="scirp.66431-formula159"><label>(4.09)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x299.png"  xlink:type="simple"/></disp-formula><p>Equation (4.09) can be expressed such that:</p><disp-formula id="scirp.66431-formula160"><label>(4.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x300.png"  xlink:type="simple"/></disp-formula><p>The task is to obtain the required voltage at a given acceleration number<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x301.png" xlink:type="simple"/></inline-formula>, this will require one to solve Equation (4.10) for electric field E as shown below.</p><disp-formula id="scirp.66431-formula161"><label>(4.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x302.png"  xlink:type="simple"/></disp-formula><p>Recall that velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x303.png" xlink:type="simple"/></inline-formula> is the particles’ approximate velocity at 99% of the speed of light. Thus, velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x303.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x304.png" xlink:type="simple"/></inline-formula> is simply the product of the speed of light c and the value 0.99<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x303.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x304.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x305.png" xlink:type="simple"/></inline-formula>. The speed of light can then be distributed out of Equation (4.11), giving the value of Equation (4.12) such that:</p><disp-formula id="scirp.66431-formula162"><label>(4.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x306.png"  xlink:type="simple"/></disp-formula><p>The value of electrical field E is equal to the negative partial derivative of voltage V in respect to length x [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula163"><label>(4.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x307.png"  xlink:type="simple"/></disp-formula><p>Substituting this value (Equation (4.13)) into Equation (4.12) gives the differential equation shown below.</p><disp-formula id="scirp.66431-formula164"><label>(4.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x308.png"  xlink:type="simple"/></disp-formula><p>This can be rearranged such that:</p><disp-formula id="scirp.66431-formula165"><label>(4.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x309.png"  xlink:type="simple"/></disp-formula><p>The corresponding integrals in respect to voltage V and length x are expressed such that [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] :</p><disp-formula id="scirp.66431-formula166"><label>(4.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x310.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x311.png" xlink:type="simple"/></inline-formula> is unit length, evaluating the integrals give the value of voltage <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x312.png" xlink:type="simple"/></inline-formula> such that:</p><disp-formula id="scirp.66431-formula167"><label>(4.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x313.png"  xlink:type="simple"/></disp-formula><p>Length <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x314.png" xlink:type="simple"/></inline-formula> is set to unity (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x314.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x315.png" xlink:type="simple"/></inline-formula>), therefore voltage <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x314.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x315.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x316.png" xlink:type="simple"/></inline-formula> can be expressed such that:</p><disp-formula id="scirp.66431-formula168"><label>(4.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x317.png"  xlink:type="simple"/></disp-formula><p>Voltage <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x318.png" xlink:type="simple"/></inline-formula> is the product of electrical current I and resistance R (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x318.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x319.png" xlink:type="simple"/></inline-formula>) [<xref ref-type="bibr" rid="scirp.66431-ref2">2</xref>] .</p><disp-formula id="scirp.66431-formula169"><label>(4.19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x320.png"  xlink:type="simple"/></disp-formula><p>Equations ((4.18) and (4.19)) show the required voltage <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x321.png" xlink:type="simple"/></inline-formula> at acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x321.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x322.png" xlink:type="simple"/></inline-formula> to produce gravitational force fields and the corresponding space-time curves using a given density number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x321.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x322.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x323.png" xlink:type="simple"/></inline-formula> of charged particles at 99% if the speed of light. Thus the value of voltage <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x321.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x322.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x323.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x324.png" xlink:type="simple"/></inline-formula> or IR sufficient to produce an acceleration that will generate gravity can be shown to exist in the real world with the condition of the inequality below.</p><disp-formula id="scirp.66431-formula170"><label>(4.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x325.png"  xlink:type="simple"/></disp-formula><p>Voltage <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x326.png" xlink:type="simple"/></inline-formula> can be mapped to and corresponds to a gravitational force value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x326.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x327.png" xlink:type="simple"/></inline-formula> at the number of particles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x326.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x327.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x328.png" xlink:type="simple"/></inline-formula> and acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x326.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x327.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x328.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x329.png" xlink:type="simple"/></inline-formula> as shown below.</p><disp-formula id="scirp.66431-formula171"><label>(4.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x330.png"  xlink:type="simple"/></disp-formula><p>where gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x331.png" xlink:type="simple"/></inline-formula> is such that:</p><disp-formula id="scirp.66431-formula172"><label>(4.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7502714x332.png"  xlink:type="simple"/></disp-formula></sec><sec id="s6"><title>6. Conclusion: Experiment Proposal</title><p>The force associated with the Casimir effect describing vacuum energy was confirmed by an experiment conducted by physicist Steven Lamoreaux in 1996 [<xref ref-type="bibr" rid="scirp.66431-ref6">6</xref>] . The experiment was conducted in a vacuum between two metal plates [<xref ref-type="bibr" rid="scirp.66431-ref6">6</xref>] . The minutest value of force pulling the plates together was detected. Thus, in a similar manner, an experiment can be conducted where a cloud of charged particles are accelerated to within an infinitesimal fraction of the speed of light between two non-metal plates constructed of an electrically neutral material to avoid the detection of electromagnetic forces that can be confused with gravitational force. The equation of gravitational force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x333.png" xlink:type="simple"/></inline-formula> linking gravitation to acceleration number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x333.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x334.png" xlink:type="simple"/></inline-formula> and the number of particles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x333.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x334.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x335.png" xlink:type="simple"/></inline-formula> can be used to predict a pressure (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x333.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x334.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x335.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7502714x336.png" xlink:type="simple"/></inline-formula>) exerted on the electrically neutral plates. The experimental verification of the equations formulated in this paper will lead to further progress in generating gravitational fields and space-time curves based on any method of energy generation that produces electromagnetic energy used to sufficiently accelerate the charged particles. Lastly, the obvious implication to the generation of a gravitational field proportionally to energy produced is the possibility of generating artificial gravity without the use of centripetal force and the generation of space-time curves also science fictionally referred to as warp fields.</p></sec><sec id="s7"><title>Cite this paper</title><p>Edward A. Walker, (2016) Gravitational Space-Time Curve Generation via Accelerated Charged Particles. Journal of Modern Physics,07,863-874. doi: 10.4236/jmp.2016.79078</p></sec></body><back><ref-list><title>References</title><ref id="scirp.66431-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Manor, E. 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