<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1103038</article-id><article-id pub-id-type="publisher-id">OALibJ-71423</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Gravitational Wave and Transparent Crystal Black Hole
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhiliang</surname><given-names>Cao</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Henry</surname><given-names>Gu Cao</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Wayne State University, Detroit, MI, USA</addr-line></aff><aff id="aff2"><addr-line>Northwestern University, Evanston, IL, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>williamcao12252000@yahoo.com(ZC)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>18</day><month>10</month><year>2016</year></pub-date><volume>03</volume><issue>10</issue><fpage>1</fpage><lpage>8</lpage><history><date date-type="received"><day>September</day>	<month>5,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>October</month>	<year>15,</year>	</date><date date-type="accepted"><day>October</day>	<month>19,</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>
 
 
  This paper uses the results of the latest Unified Field Theory (UFT) and the experimental results of the recent experiments of gravitational wave to study the configuration of a black hole. We conclude that a black hole has no singularity state. Instead, particles in a black hole form a stable system. Topologically, octahedron particles form sphere with two poles. A black hole always releases energy at the poles. If a black hole has an accretion disk, the particles from disk will wrap around the black hole, twist upwards, accelerated by out-going black hole energy at the poles, and ejected out at the top of a pole to form a black hole jet. The predictions made in the paper provide valuable insight regarding the inner workings of the black hole. We hope that our work can help future studies regarding gravitational waves, black hole, and dark energy.
 
</p></abstract><kwd-group><kwd>Dark Matter</kwd><kwd> Astronomy</kwd><kwd> Black Hole</kwd><kwd> Gravitational Wave</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Unified Field Theory (UFT) [<xref ref-type="bibr" rid="scirp.71423-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.71423-ref11">11</xref>] considers that gravity is the result of space-time distortion by energy. It supports the gravity equation as follow:</p><disp-formula id="scirp.71423-formula196"><graphic  xlink:href="http://html.scirp.org/file/71423x2.png"  xlink:type="simple"/></disp-formula><p>In recent test results [<xref ref-type="bibr" rid="scirp.71423-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.71423-ref16">16</xref>] , the final mass of the combined mass of merged black hole is 62 solar masses. If V = C, the frequency calculated based on the above equations will be: 521 Hz.</p><p>For the twin black holes, the frequency is doubled: 1042 Hz.</p><p>The actual test result [<xref ref-type="bibr" rid="scirp.71423-ref16">16</xref>] (<xref ref-type="fig" rid="fig1">Figure 1</xref>) is that the max frequency is 336 Hz.</p><p>Assume that the rotation speed is:</p><disp-formula id="scirp.71423-formula197"><graphic  xlink:href="http://html.scirp.org/file/71423x3.png"  xlink:type="simple"/></disp-formula><p>and:</p><disp-formula id="scirp.71423-formula198"><graphic  xlink:href="http://html.scirp.org/file/71423x4.png"  xlink:type="simple"/></disp-formula><p>The frequency is changed to:</p><disp-formula id="scirp.71423-formula199"><graphic  xlink:href="http://html.scirp.org/file/71423x5.png"  xlink:type="simple"/></disp-formula><p>According to the test result, the twin black hole failed to maintain the orbit. In 4 cycles, they collided.</p><disp-formula id="scirp.71423-formula200"><graphic  xlink:href="http://html.scirp.org/file/71423x6.png"  xlink:type="simple"/></disp-formula><p>When two black holes merge, the circulation speed is:</p><disp-formula id="scirp.71423-formula201"><graphic  xlink:href="http://html.scirp.org/file/71423x7.png"  xlink:type="simple"/></disp-formula><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Gravitational wave experiment results.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71423x8.png"/></fig></fig-group><p>When particles circling around the black hole:</p><disp-formula id="scirp.71423-formula202"><graphic  xlink:href="http://html.scirp.org/file/71423x9.png"  xlink:type="simple"/></disp-formula><p>or:</p><disp-formula id="scirp.71423-formula203"><graphic  xlink:href="http://html.scirp.org/file/71423x10.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2"><title>2. Results</title><sec id="s2_1"><title>2.1. Black Hole Internal Structure</title><p>The structural formula [<xref ref-type="bibr" rid="scirp.71423-ref12">12</xref>] for proton is (in unit of electron mass):</p><disp-formula id="scirp.71423-formula204"><graphic  xlink:href="http://html.scirp.org/file/71423x11.png"  xlink:type="simple"/></disp-formula><p>In order to resist gravitational pressure in a black hole shell, the particle has to be stable. When the mass of the particle in unit of electron mass is divisible by strong interaction energy 137 instead of (2 &#215; 3 &#215; 5)<sup>2</sup>, the particle is perfectly in resonance with strong force and most stable (in unit of electron mass). The known particles do not have such characteristics. Since the know particles have three axes in <xref ref-type="fig" rid="fig2">Figure 2</xref>, the formula will start with:</p><disp-formula id="scirp.71423-formula205"><graphic  xlink:href="http://html.scirp.org/file/71423x12.png"  xlink:type="simple"/></disp-formula><p>A stable strong interacted axis is neutral. Since component with mass of 137 is charged. To make it both divisible and neutral, X can be:</p><p>2n &#215; 137<sup>(2m−1)</sup> or n &#215; 137<sup>(2m)</sup></p><p>n, m = 1, 2, 3, …</p><p>3 &#215; X:</p><p>3 &#215; (2n &#215; 137<sup>(2m−1)</sup>) or 3 &#215; (n &#215; 137<sup>(2m)</sup>)</p><p>i.e.:</p><p>…</p><p>3 &#215; (4 &#215; 137<sup>2</sup>)</p><p>3 &#215; (3 &#215; 137<sup>2</sup>)</p><p>3 &#215; (2 &#215; 137<sup>2</sup>)</p><p>3 &#215; (137<sup>2</sup>)</p><p>3 &#215; (128 &#215; 137)</p><p>3 &#215; (64 &#215; 137)</p><p>3 &#215; (32 &#215; 137)</p><p>3 &#215; (16 &#215; 137)</p><p>3 &#215; (8 &#215; 137)</p><p>3 &#215; (4 &#215; 137)</p><p>3 &#215; (2 &#215; 137)</p></sec><sec id="s2_2"><title>2.2. Dark Matter</title><p>Any structure in following formula (in unit of electron mass):</p><disp-formula id="scirp.71423-formula206"><graphic  xlink:href="http://html.scirp.org/file/71423x13.png"  xlink:type="simple"/></disp-formula><p>Can silently interact with any structure in above formula without releasing energy:</p><disp-formula id="scirp.71423-formula207"><graphic  xlink:href="http://html.scirp.org/file/71423x14.png"  xlink:type="simple"/></disp-formula><p>Three different particles:</p><disp-formula id="scirp.71423-formula208"><graphic  xlink:href="http://html.scirp.org/file/71423x15.png"  xlink:type="simple"/></disp-formula><p>The interaction without releasing energy leads to the “dark” character of the above structures.</p><p>When the neighboring particles share the same structure, they are in resonance. The neighbor particles in a shell should have the same structure.</p><p>The particles do not bind together with strong force. They form perfect crystal layers with no friction between layers. In <xref ref-type="fig" rid="fig3">Figure 3</xref>, the crystal planes are parallel to the surface of the black hole.</p></sec><sec id="s2_3"><title>2.3. Particle Orientation and Sphere</title><p>When a particle moves down toward the core of a black hole, the gravity accelerates the particle. It will collide with a particle and stops. If one of the axis of the octahedron dark particle is parallel to the axis of the black hole, the collision does not cause particles to spin. Therefore, one of the axis of the octahedron dark particle is parallel to the axis of the black hole.</p><p>Two neighboring particles vertical to the black hole axis are colliding due to the heat. For the same reason, their axes are lined up, one axis along Longitude, and one axis along Latitude.</p><p>We predict that the movements vertical to the axis are heat movements. A simple movement can be in form of vibration along axes. Such heat vibration vertical to the axis create spheres. The heat vibration generates pressure in the spheres and cancels out gravity introduced pressure within a sphere.</p><p>A stable black hole has no pressure between shells in the stable areas.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Particles in black hole</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71423x16.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Black hole crystal</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71423x17.png"/></fig></sec><sec id="s2_4"><title>2.4. Particle Speed in the Sphere and Heat</title><p>The internal collision of the sphere at the equator should cancel out the gravity of half sphere.</p><p>Assume that:</p><p>D: density.</p><p>r<sub>p</sub>: 0.84 &#215; 10<sup>−16</sup> m, radius of particle.</p><p>r: radius of sphere.</p><p>Gravity:</p><disp-formula id="scirp.71423-formula209"><graphic  xlink:href="http://html.scirp.org/file/71423x18.png"  xlink:type="simple"/></disp-formula><p>Collision:</p><disp-formula id="scirp.71423-formula210"><graphic  xlink:href="http://html.scirp.org/file/71423x19.png"  xlink:type="simple"/></disp-formula><p>or:</p><disp-formula id="scirp.71423-formula211"><graphic  xlink:href="http://html.scirp.org/file/71423x20.png"  xlink:type="simple"/></disp-formula><p>If the Sun becomes a black hole, it will be the smallest black hole ever found. The radius:</p><disp-formula id="scirp.71423-formula212"><graphic  xlink:href="http://html.scirp.org/file/71423x21.png"  xlink:type="simple"/></disp-formula><p>The smallest radius is the radius of proton, or:</p><disp-formula id="scirp.71423-formula213"><graphic  xlink:href="http://html.scirp.org/file/71423x22.png"  xlink:type="simple"/></disp-formula><p>V reaches to the maximum speed:</p><disp-formula id="scirp.71423-formula214"><graphic  xlink:href="http://html.scirp.org/file/71423x23.png"  xlink:type="simple"/></disp-formula><p>Black holes are very cold indeed.</p></sec></sec><sec id="s3"><title>3. Discussions</title><sec id="s3_1"><title>3.1. Unreachable Event Horizon</title><p>The spheres in the black hole create a stable system. Such system stops further crashing from happening and there will be no path to reach the event horizon. Instead, the escape energy is one half of the inertia energy, a stable black hole follows:</p><disp-formula id="scirp.71423-formula215"><graphic  xlink:href="http://html.scirp.org/file/71423x24.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_2"><title>3.2. Transparent Crystal</title><p>The structures:</p><disp-formula id="scirp.71423-formula216"><graphic  xlink:href="http://html.scirp.org/file/71423x25.png"  xlink:type="simple"/></disp-formula><p>are octahedron shaped.</p><p>Topologically, octahedron particle formed sphere <xref ref-type="fig" rid="fig4">Figure 4</xref> has two poles. An octahedron on the sphere has one axis vertical to the sphere, one axis along Longitude, and one axis along Latitude.</p><p>The Longitude effects are less in the areas close to two poles. The particles are mainly aligned with the axis of the black hole and the other two axes are aligned by external forces and form a perfect crystal.</p><p>The areas further away from the poles have disproportional crystal dislocations that lead to pressures between the shells and form unstable fault structures shaped as squared cylinders/cones. The pressure causes movements along the fault surface. The energy will be released continuously from fault surface as particles crash down toward the core of black hole along the fault surface.</p><p>For a single black hole [<xref ref-type="bibr" rid="scirp.71423-ref17">17</xref>] <xref ref-type="fig" rid="fig5">Figure 5</xref>, it has both cross shaped bright arms and circular features.</p><p>In black hole system [<xref ref-type="bibr" rid="scirp.71423-ref18">18</xref>] in <xref ref-type="fig" rid="fig6">Figure 6</xref>, the center pole areas may have ideal crystal surrounded by other cones which are directly map to the bright spots in the real image in <xref ref-type="fig" rid="fig6">Figure 6</xref> on the right.</p><p>Due to the gravity, photons release from the deep fault surface are red shifted, while photons from the upper level of black hole are blue (less red shifted).</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Octahedron particle sphere and fault cone</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71423x26.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Quasar 1 and defect cones near a pole</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71423x27.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Squared quasar and defect cones near a pole</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71423x28.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Black hole jet</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71423x29.png"/></fig></sec><sec id="s3_3"><title>3.3. Black Hole Jet</title><p>When there is an accretion disk, circling matter will touch the surface of black hole, where the vibration movements along a longitude convert the circling matter into layers of spheres wrapping around the black hole. The newly formed spheres twist upwards. When these particles reach a pole, they are accelerated by out-going black hole energy at the poles. The particles are continuously pulled into the new sphere from the rotating disk and ejected at the top of pole. This dynamic process forms a black hole jet <xref ref-type="fig" rid="fig7">Figure 7</xref>.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>We predict that:</p><p>1) A black hole is composed of dark particles structured as follows:</p><disp-formula id="scirp.71423-formula217"><graphic  xlink:href="http://html.scirp.org/file/71423x30.png"  xlink:type="simple"/></disp-formula><p>2) The black hole radius is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71423x31.png" xlink:type="simple"/></inline-formula>;</p><p>3) A black hole has a stable octahedron dark particle formed cold spheres. There is no pressure between the spheres;</p><p>4) These octahedron dark particles formed spheres have two poles and fault cones which emit black hole energy;</p><p>5) Particles circling a black hole wrap around the black hole and form spheres which are ejected out at the poles to form black hole jets.</p><p>Additional studies are warranted regarding fault cones, black hole jet, and interactions between two neighboring black holes.</p></sec><sec id="s5"><title>Cite this paper</title><p>Cao, Z.L. and Cao, H.G. (2016) Gravitational Wave and Trans- parent Crystal Black Hole. Open Access Li- brary Journal, 3: e3038. http://dx.doi.org/10.4236/oalib.1103038</p></sec></body><back><ref-list><title>References</title><ref id="scirp.71423-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Cao, Z.L. and Cao, H.G. (2013) Unified Field Theory and the Configuration of Particles. 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