<?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.2017.81011</article-id><article-id pub-id-type="publisher-id">JMP-73760</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>
 
 
  Introduction of the Tensor Which Satisfied Binary Law
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Koji</surname><given-names>Ichidayama</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>716-0002 Okayama, Japan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>12</month><year>2016</year></pub-date><volume>08</volume><issue>01</issue><fpage>126</fpage><lpage>132</lpage><history><date date-type="received"><day>December</day>	<month>29,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>January</month>	<year>20,</year>	</date><date date-type="accepted"><day>January</day>	<month>23,</month>	<year>2017</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><html>
 <head></head>
 
  P: For every coordinate system, there is no immediate reason for preferring certain systems of co-ordinates to others. If we don’t recognize that P is establishment, we must recognize to existence of the absolute coordinate system. Therefore, we must recognize that P is establishment. Nevertheless, I got conclusion that P isn’t es-tablishment for all coordinate systems 
  <img src="Edit_1bcd5865-8c04-45ec-937a-a162e0a42dbe.bmp" alt="" />. If P is establishment, this is the trouble. As against, I got conclusion that if we consider “Binary Law” for all coordinate systems 
  <img src="Edit_1bcd5865-8c04-45ec-937a-a162e0a42dbe.bmp" alt="" style="white-space:normal;" />, P is establishment for all coordinate systems 
  <img src="Edit_1bcd5865-8c04-45ec-937a-a162e0a42dbe.bmp" alt="" style="white-space:normal;" />. If we consider Binary Law for all coordinate systems 
  <img src="Edit_1bcd5865-8c04-45ec-937a-a162e0a42dbe.bmp" alt="" style="white-space:normal;" />, we must consider Binary Law for the coordinate systems using into Tensor, too. So, I decided to report for the Tensor which satisfied Binary Law.
 
</html></p></abstract><kwd-group><kwd>Tensor</kwd><kwd> Covariant Derivative</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Definition 1. For every coordinate system, there is no immediate reason for pre- ferring certain systems of co-ordinates to others.</p><p>Definition 2. I named <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x6.png" xlink:type="simple"/></inline-formula> “Binary Law”.</p><p>Definition 3. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x7.png" xlink:type="simple"/></inline-formula>is established.</p><p>Definition 4. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x8.png" xlink:type="simple"/></inline-formula>is established.</p><p>Definition 5. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x9.png" xlink:type="simple"/></inline-formula>is established.</p><p>Definition 6. Convariant and contravariant tensor of the first rank <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x10.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x11.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.73760-ref1">1</xref>] .</p><p>Definition 7. Tensor of rank zero <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x12.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x13.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.73760-ref1">1</xref>] .</p><p>Definition 8. If tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x14.png" xlink:type="simple"/></inline-formula> satisfied<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x15.png" xlink:type="simple"/></inline-formula>, this tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x16.png" xlink:type="simple"/></inline-formula> was named sym- metric tensor [<xref ref-type="bibr" rid="scirp.73760-ref1">1</xref>] .</p><p>Definition 9. Convariant differentiation for Convariant Bector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x17.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x18.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.73760-ref1">1</xref>] .</p><p>Definition 10. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x19.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x20.png" xlink:type="simple"/></inline-formula> are establishment [<xref ref-type="bibr" rid="scirp.73760-ref2">2</xref>] .</p><p>Definition 11. Convariant differentiation for contravariant bector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x21.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x22.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.73760-ref2">2</xref>] .</p><p>Definition 12. Convariant differentiation for Scalar <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x23.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x24.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.73760-ref2">2</xref>] .</p></sec><sec id="s2"><title>2. About Reason to Take Binary Law into Consideration</title><p>We will have to receive existence of the absolute coordinate system if Definition 1 is not established. Therefore, we must accept establishment of Definition 1.</p><p>Proposition 1. Definition 1 is not established for all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x25.png" xlink:type="simple"/></inline-formula></p><p>Proof: All coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x26.png" xlink:type="simple"/></inline-formula> thinks about <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x27.png" xlink:type="simple"/></inline-formula> in a standard and can divide it into two next groups.</p><disp-formula id="scirp.73760-formula8"><graphic  xlink:href="http://html.scirp.org/file/11-7503039x28.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula9"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x29.png"  xlink:type="simple"/></disp-formula><p>I think that I change the coordinate systems of the standard <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x30.png" xlink:type="simple"/></inline-formula> of (1) for all coordi- nate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x31.png" xlink:type="simple"/></inline-formula> sequentially now. By the way, the difference cannot occur between each conclusion to be provided here if Definition 1 is established. This reason is that all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x32.png" xlink:type="simple"/></inline-formula> has a privilege of the equality each other if Definition 1 is established. At first (1) gets an invariable conclusion for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x33.png" xlink:type="simple"/></inline-formula> exchange. Therefore, at least (1) must get an invariable conclusion for the next <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x34.png" xlink:type="simple"/></inline-formula> exchange if Definition 1 is established. Here, I get</p><disp-formula id="scirp.73760-formula10"><graphic  xlink:href="http://html.scirp.org/file/11-7503039x35.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula11"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x36.png"  xlink:type="simple"/></disp-formula><p>by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x37.png" xlink:type="simple"/></inline-formula> exchange from (1). Therefore, (2) must be equal with (1) if Definition 1 is established. By the way, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x38.png" xlink:type="simple"/></inline-formula>of (1) is equal with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x39.png" xlink:type="simple"/></inline-formula> of (2), but <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x40.png" xlink:type="simple"/></inline-formula> of (1) is not equal with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x41.png" xlink:type="simple"/></inline-formula> of (2). In other words, (2) is not equal with (1). Therefore, Definition 1 is not established for all coor- dinate systems<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x42.png" xlink:type="simple"/></inline-formula>.</p><p>-End Proof</p><p>Establishment of Proposition 1 is a problem in thinking that Definition 1 must be established. Therefore, I aim at getting establishment of Definition 1 for all coordinate systems<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x43.png" xlink:type="simple"/></inline-formula>.</p><p>Proposition 2. If all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x44.png" xlink:type="simple"/></inline-formula> satisfies <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x45.png" xlink:type="simple"/></inline-formula>, Definition 1 is established for all coordinate systems<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x46.png" xlink:type="simple"/></inline-formula>.</p><p>Proof: I get</p><disp-formula id="scirp.73760-formula12"><graphic  xlink:href="http://html.scirp.org/file/11-7503039x47.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula13"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x48.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula14"><graphic  xlink:href="http://html.scirp.org/file/11-7503039x49.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula15"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x50.png"  xlink:type="simple"/></disp-formula><p>from (1), (2) if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x51.png" xlink:type="simple"/></inline-formula> satisfies</p><disp-formula id="scirp.73760-formula16"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x52.png"  xlink:type="simple"/></disp-formula><p>(3) is equal with (4) here. In other words, (2) is equal with (1) if all coordinate sys- tems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x53.png" xlink:type="simple"/></inline-formula> satisfies (5). Therefore, Definition 1 is established for all coordi- nate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x54.png" xlink:type="simple"/></inline-formula> if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x55.png" xlink:type="simple"/></inline-formula> satisfies (5).</p><p>-End Proof</p><p>Proposition 3. If all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x56.png" xlink:type="simple"/></inline-formula> satisfies <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x57.png" xlink:type="simple"/></inline-formula>, all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x58.png" xlink:type="simple"/></inline-formula> shifts to only two of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x59.png" xlink:type="simple"/></inline-formula></p><p>Proof: If all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x60.png" xlink:type="simple"/></inline-formula> satisfies (5), I get <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x61.png" xlink:type="simple"/></inline-formula> than all coordinate systems<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x62.png" xlink:type="simple"/></inline-formula>.</p><p>-End Proof</p><p>Proposition 4. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x63.png" xlink:type="simple"/></inline-formula> is established, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x64.png" xlink:type="simple"/></inline-formula>is esta- blished.</p><p>Proof: I get</p><disp-formula id="scirp.73760-formula17"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x65.png"  xlink:type="simple"/></disp-formula><p>from (5), (7) if I assume establishment of</p><disp-formula id="scirp.73760-formula18"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x66.png"  xlink:type="simple"/></disp-formula><p>when (5) is established. Because (6) includes contradiction,</p><disp-formula id="scirp.73760-formula19"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x67.png"  xlink:type="simple"/></disp-formula><p>is established when (5) is established.</p><p>-End Proof</p><p>Proposition 5. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x68.png" xlink:type="simple"/></inline-formula> is established, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x69.png" xlink:type="simple"/></inline-formula> are established.</p><p>Proof: When (5) is established, (8) is established from Proposition 4. Therefore, I get</p><disp-formula id="scirp.73760-formula20"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x70.png"  xlink:type="simple"/></disp-formula><p>from (8), (10) if I assume establishment of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x71.png" xlink:type="simple"/></inline-formula> when (5) is established. I can rewrite <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x72.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.73760-formula21"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x73.png"  xlink:type="simple"/></disp-formula><p>here. When (5) is established, I get</p><disp-formula id="scirp.73760-formula22"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x74.png"  xlink:type="simple"/></disp-formula><p>from Definition 3. Because (9) includes contradiction for (11),</p><disp-formula id="scirp.73760-formula23"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x75.png"  xlink:type="simple"/></disp-formula><p>is established when (5) is established.</p><p>Similary, I get</p><disp-formula id="scirp.73760-formula24"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x76.png"  xlink:type="simple"/></disp-formula><p>from (8), (14) if I assume establishment of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x77.png" xlink:type="simple"/></inline-formula> when (5) is established. I can rewrite <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x78.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.73760-formula25"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x79.png"  xlink:type="simple"/></disp-formula><p>here. When (5) is established, I get</p><disp-formula id="scirp.73760-formula26"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x80.png"  xlink:type="simple"/></disp-formula><p>from Definition 4. Because (13) includes contradiction for (15),</p><disp-formula id="scirp.73760-formula27"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x81.png"  xlink:type="simple"/></disp-formula><p>is established when (5) is established.</p><p>Similary, I get</p><disp-formula id="scirp.73760-formula28"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x82.png"  xlink:type="simple"/></disp-formula><p>from (8), (18) if I assume establishment of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x83.png" xlink:type="simple"/></inline-formula> when (5) is established. I can rewrite <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x84.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.73760-formula29"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x85.png"  xlink:type="simple"/></disp-formula><p>here. When (5) is established, I get</p><disp-formula id="scirp.73760-formula30"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x86.png"  xlink:type="simple"/></disp-formula><p>from Definition 5. Because (17) includes contradiction for (19),</p><disp-formula id="scirp.73760-formula31"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x87.png"  xlink:type="simple"/></disp-formula><p>is established when (5) is established. And, I get</p><disp-formula id="scirp.73760-formula32"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x88.png"  xlink:type="simple"/></disp-formula><p>from (12), (16), (20).</p><p>-End Proof</p></sec><sec id="s3"><title>3. About the Tensor Which Satisfied Binary Law</title><p>We will have to think about adaptation of the establishment of Binary Law for the coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x89.png" xlink:type="simple"/></inline-formula> in the tensor if we think about establishment of Binary Law for all coordinate systems<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x90.png" xlink:type="simple"/></inline-formula>. Therefore, I decided to report Tensor when all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x91.png" xlink:type="simple"/></inline-formula> satisfied Binary Law.</p><p>Proposition 6. If all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x92.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x93.png" xlink:type="simple"/></inline-formula>, Convariant and Contravariant Tensor of the first rank does not change the form of the equation.</p><p>Proof: I get</p><disp-formula id="scirp.73760-formula33"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x94.png"  xlink:type="simple"/></disp-formula><p>from Definition 6 if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x95.png" xlink:type="simple"/></inline-formula> satisfies (5). Definition 6 and (22) are equal here. Therefore, if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x96.png" xlink:type="simple"/></inline-formula> satisfied (5), Convariant and Contravariant Tensor of the first rank does not change the form of the equation.</p><p>-End Proof</p><p>Proposition 7. Tensor of the second rank becomes Symmetric Tensor if all coor- dinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x97.png" xlink:type="simple"/></inline-formula> satisfies <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x98.png" xlink:type="simple"/></inline-formula></p><p>Proof: I get</p><disp-formula id="scirp.73760-formula34"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x99.png"  xlink:type="simple"/></disp-formula><p>from Definition 7 if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x100.png" xlink:type="simple"/></inline-formula> satisfies (5). Definition 7 and (23) are equal here. We can use (12), (16), (20), (21) for (23) by considering Pro- position 5 here. And we can rewrite (23) by using (12), (16) for</p><disp-formula id="scirp.73760-formula35"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x101.png"  xlink:type="simple"/></disp-formula><p>Then, I get</p><disp-formula id="scirp.73760-formula36"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x102.png"  xlink:type="simple"/></disp-formula><p>from (23),(24). And we can rewrite (23) by using (20), (21) for</p><disp-formula id="scirp.73760-formula37"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x103.png"  xlink:type="simple"/></disp-formula><p>Then, I get</p><disp-formula id="scirp.73760-formula38"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x104.png"  xlink:type="simple"/></disp-formula><p>from (26). Therefore, Tensor of the second rank becomes Symmetric Tensor than consideration of Definition 8 when all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x105.png" xlink:type="simple"/></inline-formula> satisfies (5).</p><p>-End Proof</p><p>Proposition 8. If all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x106.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x107.png" xlink:type="simple"/></inline-formula>, The distance of two points be able to change oneself in connection with the metric of space.</p><p>Proof: I get</p><disp-formula id="scirp.73760-formula39"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x108.png"  xlink:type="simple"/></disp-formula><p>from Definition 10 if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x109.png" xlink:type="simple"/></inline-formula> satisfies (5). I get</p><disp-formula id="scirp.73760-formula40"><graphic  xlink:href="http://html.scirp.org/file/11-7503039x110.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula41"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x111.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula42"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x112.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula43"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x113.png"  xlink:type="simple"/></disp-formula><p>from Definition 9 if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x114.png" xlink:type="simple"/></inline-formula> satisfies (5). By the way, we cannot handle (30), (31) according to Proposition 3. We can use (12), (16), (20), (21) for (29) by considering Proposition 5 here. And we must rewrite (29) by using (16) for</p><disp-formula id="scirp.73760-formula44"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x115.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula45"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x116.png"  xlink:type="simple"/></disp-formula><p>I decide not to handle (33) by consideration of (28) here. Well, I get conclution from (32) that if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x117.png" xlink:type="simple"/></inline-formula> satisfied (5), Scalar quantity be able to change oneself in connection with the metric of space. Here, This Scalar quantity expressed the all of quantity expressed as Scalar. Therefore, I get conclution that the distance of two points be able to change oneself in connection with the metric of space.</p><p>-End Proof</p><p>Proposition 9. If all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x118.png" xlink:type="simple"/></inline-formula> satisfied <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x119.png" xlink:type="simple"/></inline-formula>, convariant differentiation for Contravariant Bector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x120.png" xlink:type="simple"/></inline-formula> behave like a convariant differentiation for Scalar <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x121.png" xlink:type="simple"/></inline-formula></p><p>Proof: I get</p><disp-formula id="scirp.73760-formula46"><graphic  xlink:href="http://html.scirp.org/file/11-7503039x122.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula47"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x123.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula48"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x124.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula49"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x125.png"  xlink:type="simple"/></disp-formula><p>from Definition 11 if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x126.png" xlink:type="simple"/></inline-formula> satisfies (5). By the way, we cannot handle (35), (36) according to Proposition 3. We can use (12), (16), (20), (21) for (34) by considering Proposition 5 here. And we must rewrite (34) by using (21) for</p><disp-formula id="scirp.73760-formula50"><graphic  xlink:href="http://html.scirp.org/file/11-7503039x127.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73760-formula51"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x128.png"  xlink:type="simple"/></disp-formula><p>And, I can get</p><disp-formula id="scirp.73760-formula52"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x129.png"  xlink:type="simple"/></disp-formula><p>from (37) for consideration of (28). And we can rewrite (38) by using (21) for</p><disp-formula id="scirp.73760-formula53"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7503039x130.png"  xlink:type="simple"/></disp-formula><p>Because the second term of the right side of (38) does not exist here, we may adopt (38) and (39) description form of which. Well, I get conclution from (39), Definition 12 that if all coordinate systems <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x131.png" xlink:type="simple"/></inline-formula> satisfied (5), Convariant differentiation for Contravariant Bector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x132.png" xlink:type="simple"/></inline-formula> behave like a Convariant differentiation for Scalar<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x133.png" xlink:type="simple"/></inline-formula>.</p><p>-End Proof</p></sec><sec id="s4"><title>4. Discussion</title><p>About Definition 2:</p><p>I named (5) “Binary Law” by Proposition 3.</p><p>About Proposition 6:</p><p>Convariant and contravariant tensor of the first rank don’t change the formula whether it’s satisfied (5) or not.</p><p>About Proposition 8:</p><p>In (32), we can think that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x134.png" xlink:type="simple"/></inline-formula> expressed the distance of two points in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x135.png" xlink:type="simple"/></inline-formula> is</p><p>establishment and this is constant. And, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x136.png" xlink:type="simple"/></inline-formula>expresses the distance of two points in general and this is not constant.</p><p>About Proposition 9:</p><p>In (39), we can handle <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x137.png" xlink:type="simple"/></inline-formula> as tensor similarly<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7503039x138.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s5"><title>Cite this paper</title><p>Ichidayama, K. (2017) Introduction of the Tensor Which Satisfied Binary Law. Journal of Modern Physics, 8, 126-132. http://dx.doi.org/10.4236/jmp.2017.81011</p></sec></body><back><ref-list><title>References</title><ref id="scirp.73760-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Dirac, P.A.M. (1975) General Theory of Relativity. John Wiley and Sons, Inc., Hoboken.</mixed-citation></ref><ref id="scirp.73760-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Einstein, A. (1916) Die Grundlage der allgemeinen Relativit&amp;auml;tstheorie. Annalen der Physik, 49, 769.</mixed-citation></ref></ref-list></back></article>