<?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">IJG</journal-id><journal-title-group><journal-title>International Journal of Geosciences</journal-title></journal-title-group><issn pub-type="epub">2156-8359</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijg.2015.66049</article-id><article-id pub-id-type="publisher-id">IJG-57394</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Application of Commensurability in Earthquake Prediction
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>oujin</surname><given-names>Su</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>Hui</surname><given-names>Hu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Seismological Bureau of Yunnan Province, Kunming, China</addr-line></aff><aff id="aff2"><addr-line>Yunnan Observatory, Chinese Academy of Sciences, Kunming, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>suyoujin0818@sina.com(OS)</email>;<email>huhui@mail.ynao.ac.cn(HH)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>06</month><year>2015</year></pub-date><volume>06</volume><issue>06</issue><fpage>619</fpage><lpage>624</lpage><history><date date-type="received"><day>2</day>	<month>May</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>22</month>	<year>June</year>	</date><date date-type="accepted"><day>25</day>	<month>June</month>	<year>2015</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 article introduces application of the expanding commensurability in earthquake prediction. The results show that most of the world’s major earthquake occurred at their commensurable points of time axis. An EQ 7.0 occurred in Lushan of China on 2013-04-20 and an EQ 8.2 occurred in Iquique of northern Chile on 2014-04-01 all occurred at their commensurable points of time axis. This once again proves that the commensurability provides an important scientific basis
   
  for the prediction of major earthquakes, which will occur in the area in future.
 
</p></abstract><kwd-group><kwd>Commensurability</kwd><kwd> Orders in the Natural World</kwd><kwd> Earthquake Prediction</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Earthquake (EQ) research, especially EQ prediction, is accepted as a worldwide difficult scientific problem [<xref ref-type="bibr" rid="scirp.57394-ref1">1</xref>] . People have made arduous and unremitting efforts for searching for the effective methods of EQ prediction for a very long time. However, most of the basic concepts and systems of methods do not break away from the system of quantitative analysis of the inertial system so that the problem of prediction of serious natural disasters like EQs has not been solved. A Chinese famous geophysicist, Weng Wenbo (1912-1994) studies the Titius-Bode law [<xref ref-type="bibr" rid="scirp.57394-ref2">2</xref>] and firstly pointed out that the occurrence time of EQ has the commensurability and applied the principle of the commensurability which was firstly proposed in astronomy to the prediction of major natural disasters such as earthquakes, droughts and water-loggings, etc., thereby developed it into the theory of prediction which have been widely used in the prediction of disasters [<xref ref-type="bibr" rid="scirp.57394-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.57394-ref7">7</xref>] . Based on this theory, the occurrence of a few EQs, droughts and water-loggings, and other natural disasters were successfully predicted.</p></sec><sec id="s2"><title>2. Commensurability and Its Expansion</title><p>Commensurability of the word was first proposed by the German famous astronomer Titius who found and proposed it in the study of the average distance between the planets within the solar system to the sun. Later, another famous German astronomer Bode made further studies. This is the famous Titius-Bode Law. From Titius- Bode law the distance of the planet n from the sun can be expressed as:</p><disp-formula id="scirp.57394-formula603"><label>, (1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2800834x5.png"  xlink:type="simple"/></disp-formula><p>It also can be written as the following form:</p><disp-formula id="scirp.57394-formula604"><label>, (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2800834x6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x7.png" xlink:type="simple"/></inline-formula> is the distance of the planet n to the sun, reckoned in astronomical unit, and n is the number of the planets away from the sun to the far side. For Mercury, the number n is not 1, instead it is taken as −∞. β is the commensurable value for the planets in the solar system [<xref ref-type="bibr" rid="scirp.57394-ref8">8</xref>] .</p><p>Just as the famous geophysicist Weng Wenbo [<xref ref-type="bibr" rid="scirp.57394-ref9">9</xref>] pointed out that the commensurability is one of the orders in the natural world. The Equation (2) itself brings to light the distribution law of the matter in a space region, and for time domain the commensurability can be expressed as:</p><disp-formula id="scirp.57394-formula605"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2800834x8.png"  xlink:type="simple"/></disp-formula><p>Here k is an integer. If the above relation is tenable, then the data set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x9.png" xlink:type="simple"/></inline-formula> is commensurable. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x10.png" xlink:type="simple"/></inline-formula>is the commensurable value of the data set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x11.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x12.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x13.png" xlink:type="simple"/></inline-formula>. If k is equal to 1, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x14.png" xlink:type="simple"/></inline-formula> is the period of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x15.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.57394-ref10">10</xref>] .</p></sec><sec id="s3"><title>3. Prediction Practice</title><sec id="s3_1"><title>3.1. Forecast by Weng Wenbo on the EQ Ms7.4 in California of United States on June 28, 1992</title><p>Before 1992 Weng Wenbo made a few forecasts of EQs occurring in United States, most of these forecasts corresponded quite well with the later occurred actual events [<xref ref-type="bibr" rid="scirp.57394-ref11">11</xref>] . As example, on January 17, 1992, according to a request from Prof. Cecil H. Green, Director of American Geophysical Unit, and upon obtaining ratification from senior authorities, Weng Wenbo presented his forecast report to Prof. Green [<xref ref-type="bibr" rid="scirp.57394-ref12">12</xref>] ;</p><p>Time: June 19 1992</p><p>Magnitude: 6.8</p><p>Place: Broad region of San Francisco</p><p>The predicted EQ occurred on June 28, 1992. Its magnitude Ms7.4, was only Ms0.6 greater in magnitude, and the occurrence date was only 9 days later than the date stated by the forecast report of Weng Wenbo [<xref ref-type="bibr" rid="scirp.57394-ref13">13</xref>] .</p></sec><sec id="s3_2"><title>3.2. Prediction on the Wenchuan EQ 8.0 and Lushan EQ 7.0 in China and the Iquique EQ 8.2 in Chile of 2014</title><p>The Wenchuan EQ Ms8.0 occurred in Sichuan province of China on May 12, 2008. It caused greatest heavy losses of the life and property in China in recent history. Before the EQ, Long Xiaoxia et al. based on the commensurability using the following commensurable equations with five elements rather precisely predicted that a strong EQ might occur in 2008 [<xref ref-type="bibr" rid="scirp.57394-ref14">14</xref>] :</p><disp-formula id="scirp.57394-formula606"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2800834x16.png"  xlink:type="simple"/></disp-formula><p>The EQ catalogue used by Long Xiaoxia et al. is given in <xref ref-type="table" rid="table1">Table 1</xref>. From <xref ref-type="table" rid="table1">Table 1</xref> the commensurable value of the EQs occurrence is equal to 2.44 years. Taking k = 5 we obtain:</p><disp-formula id="scirp.57394-formula607"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2800834x17.png"  xlink:type="simple"/></disp-formula><p>Its error which is the opposite of the occurrence date of the earthquake is 27 days. Its relative error is 0.03.</p><p>An EQ 7.0 occurred in Lushan of Sichuan province, China on 2013-04-20. Similar, on the basis of the <xref ref-type="table" rid="table1">Table 1</xref> we obtain:</p><disp-formula id="scirp.57394-formula608"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2800834x18.png"  xlink:type="simple"/></disp-formula><p>It occurred just at the commensurable point equal to 2 times of its time axis. Its absolute error is 22 days. Its relative error also is 0.03.</p><p>An EQ 8.2 in Iquique, northern Chile, occurred on 2014-04-01. By the research of Engdahl and Villasenor [<xref ref-type="bibr" rid="scirp.57394-ref15">15</xref>] the catalogues of EQs of M ≥ 7.0 have been complete and reliable since 1900. Therefore we have analyzed the EQs of M ≥ 7.0 in Chile since 1900.0, and found its commensurable value is 0.59 years (see <xref ref-type="table" rid="table2">Table 2</xref>). So,</p><disp-formula id="scirp.57394-formula609"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-2800834x19.png"  xlink:type="simple"/></disp-formula><p>It occurred just at the commensurable point equal to 7 times of its time axis. Its absolute error is 11 days. Its relative error is 0.05.</p><p>On the basis of many years’ research for commensurability according to the commensurable principle, we compiled a Fortran program for commensurable analyses of the data. By means of the Fortran program our analyzed results have been all given in the tables. The two tables all are directly output results by computer.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Commensurability of earthquakes in Sichuan-Yunnan region since 1900.0</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >Earthquakes date</th><th align="center" valign="middle"  colspan="2"  >X<sub>i</sub> − X<sub>i</sub><sub>−1</sub></th><th align="center" valign="middle" >KΔX</th><th align="center" valign="middle"  colspan="2"  >X<sub>i</sub> − KΔX</th></tr></thead><tr><td align="center" valign="middle" >No.</td><td align="center" valign="middle" >YMD</td><td align="center" valign="middle" >(year)</td><td align="center" valign="middle" >(year)</td><td align="center" valign="middle" >K</td><td align="center" valign="middle" >(year)</td><td align="center" valign="middle" >(year)</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >19131221</td><td align="center" valign="middle" >1913.97</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >19170731</td><td align="center" valign="middle" >1917.57</td><td align="center" valign="middle" >3.60</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >1.16</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >19230324</td><td align="center" valign="middle" >1923.22</td><td align="center" valign="middle" >5.65</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4.88</td><td align="center" valign="middle" >0.77</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >19250316</td><td align="center" valign="middle" >1925.20</td><td align="center" valign="middle" >1.98</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−0.46</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >19330825</td><td align="center" valign="middle" >1933.64</td><td align="center" valign="middle" >8.44</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >7.32</td><td align="center" valign="middle" >1.12</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >19360427</td><td align="center" valign="middle" >1936.32</td><td align="center" valign="middle" >2.68</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >0.24</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >19410516</td><td align="center" valign="middle" >1941.37</td><td align="center" valign="middle" >5.05</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4.88</td><td align="center" valign="middle" >0.17</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >19420201</td><td align="center" valign="middle" >1942.08</td><td align="center" valign="middle" >0.71</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.71</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >19480525</td><td align="center" valign="middle" >1948.40</td><td align="center" valign="middle" >6.32</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >7.32</td><td align="center" valign="middle" >−1.00</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >19500203</td><td align="center" valign="middle" >1950.09</td><td align="center" valign="middle" >1.69</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−0.75</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >19520930</td><td align="center" valign="middle" >1952.75</td><td align="center" valign="middle" >2.66</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >0.22</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >19550414</td><td align="center" valign="middle" >1955.28</td><td align="center" valign="middle" >2.53</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >0.09</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >19601109</td><td align="center" valign="middle" >1960.85</td><td align="center" valign="middle" >5.57</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4.88</td><td align="center" valign="middle" >0.69</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >19670830</td><td align="center" valign="middle" >1967.66</td><td align="center" valign="middle" >6.81</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >7.32</td><td align="center" valign="middle" >−0.51</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >19700105</td><td align="center" valign="middle" >1970.01</td><td align="center" valign="middle" >2.35</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−0.09</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >19710428</td><td align="center" valign="middle" >1971.32</td><td align="center" valign="middle" >1.31</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−1.13</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >19730206</td><td align="center" valign="middle" >1973.09</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−0.67</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >19740511</td><td align="center" valign="middle" >1974.35</td><td align="center" valign="middle" >1.26</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−1.18</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >19760823</td><td align="center" valign="middle" >1976.64</td><td align="center" valign="middle" >2.29</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−0.15</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >19790315</td><td align="center" valign="middle" >1979.20</td><td align="center" valign="middle" >2.56</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >0.12</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >19810124</td><td align="center" valign="middle" >1981.06</td><td align="center" valign="middle" >1.86</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >−0.58</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >19881106</td><td align="center" valign="middle" >1988.84</td><td align="center" valign="middle" >7.78</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >7.32</td><td align="center" valign="middle" >0.46</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >19890425</td><td align="center" valign="middle" >1989.31</td><td align="center" valign="middle" >0.47</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.47</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >19950712</td><td align="center" valign="middle" >1995.52</td><td align="center" valign="middle" >6.21</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >7.32</td><td align="center" valign="middle" >−1.11</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >19960203</td><td align="center" valign="middle" >1996.09</td><td align="center" valign="middle" >0.57</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.57</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >20080512</td><td align="center" valign="middle" >2008.36</td><td align="center" valign="middle" >12.27</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >12.20</td><td align="center" valign="middle" >0.07</td></tr><tr><td align="center" valign="middle"  colspan="3"  >Commensurable value</td><td align="center" valign="middle"  colspan="4"  >2.44</td></tr><tr><td align="center" valign="middle"  colspan="3"  >Mean</td><td align="center" valign="middle"  colspan="4"  >−0.031</td></tr><tr><td align="center" valign="middle"  colspan="3"  >Standard deviation (σ<sub>n</sub><sub>−1</sub>)</td><td align="center" valign="middle"  colspan="4"  >0.717</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Commensurability of EQs in Chile since 1900.0</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >Earthquakes date</th><th align="center" valign="middle"  colspan="2"  >X<sub>i</sub> − X<sub>i</sub><sub>−1</sub></th><th align="center" valign="middle" >KΔX</th><th align="center" valign="middle" >X<sub>i</sub> − KΔX</th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >No.</td><td align="center" valign="middle" >YMD</td><td align="center" valign="middle" >(year)</td><td align="center" valign="middle" >(year)</td><td align="center" valign="middle" >K</td><td align="center" valign="middle" >(year)</td><td align="center" valign="middle" >(year)</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >19040319</td><td align="center" valign="middle" >1904.21</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >19060817</td><td align="center" valign="middle" >1906.62</td><td align="center" valign="middle" >2.41</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >0.05</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >19060830</td><td align="center" valign="middle" >1906.66</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >19061226</td><td align="center" valign="middle" >1906.98</td><td align="center" valign="middle" >0.32</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >−0.27</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >19090608</td><td align="center" valign="middle" >1909.43</td><td align="center" valign="middle" >2.45</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >0.09</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >19100906</td><td align="center" valign="middle" >1910.67</td><td align="center" valign="middle" >1.24</td><td align="center" valign="middle" >2.</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >0.06</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >19110915</td><td align="center" valign="middle" >1911.70</td><td align="center" valign="middle" >1.03</td><td align="center" valign="middle" >2.</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >−0.15</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >19140130</td><td align="center" valign="middle" >1914.07</td><td align="center" valign="middle" >2.37</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >19180520</td><td align="center" valign="middle" >1918.38</td><td align="center" valign="middle" >4.31</td><td align="center" valign="middle" >7.</td><td align="center" valign="middle" >4.13</td><td align="center" valign="middle" >0.18</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >19181204</td><td align="center" valign="middle" >1918.92</td><td align="center" valign="middle" >0.54</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >−0.05</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >19221107</td><td align="center" valign="middle" >1922.85</td><td align="center" valign="middle" >3.93</td><td align="center" valign="middle" >7.</td><td align="center" valign="middle" >4.13</td><td align="center" valign="middle" >−0.20</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >19221111</td><td align="center" valign="middle" >1922.86</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >19250515</td><td align="center" valign="middle" >1925.36</td><td align="center" valign="middle" >2.50</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >0.14</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >19270414</td><td align="center" valign="middle" >1927.28</td><td align="center" valign="middle" >1.92</td><td align="center" valign="middle" >3.</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >0.15</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >19281201</td><td align="center" valign="middle" >1928.92</td><td align="center" valign="middle" >1.64</td><td align="center" valign="middle" >3.</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >−0.13</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >19310318</td><td align="center" valign="middle" >1931.20</td><td align="center" valign="middle" >2.28</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >−0.08</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >19330223</td><td align="center" valign="middle" >1933.14</td><td align="center" valign="middle" >1.94</td><td align="center" valign="middle" >3.</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >0.17</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >19360713</td><td align="center" valign="middle" >1936.53</td><td align="center" valign="middle" >3.39</td><td align="center" valign="middle" >6.</td><td align="center" valign="middle" >3.54</td><td align="center" valign="middle" >−0.15</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >19390125</td><td align="center" valign="middle" >1939.06</td><td align="center" valign="middle" >2.53</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >0.17</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >19390418</td><td align="center" valign="middle" >1939.29</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.23</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >19401004</td><td align="center" valign="middle" >1940.76</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >2.</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >19420708</td><td align="center" valign="middle" >1942.51</td><td align="center" valign="middle" >1.75</td><td align="center" valign="middle" >3.</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >−0.02</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >19430314</td><td align="center" valign="middle" >1943.20</td><td align="center" valign="middle" >0.69</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >0.10</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >19430406</td><td align="center" valign="middle" >1943.26</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.06</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >19450913</td><td align="center" valign="middle" >1945.70</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >0.08</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >19460802</td><td align="center" valign="middle" >1946.58</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >19490420</td><td align="center" valign="middle" >1949.29</td><td align="center" valign="middle" >2.71</td><td align="center" valign="middle" >5.</td><td align="center" valign="middle" >2.95</td><td align="center" valign="middle" >−0.24</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >19490425</td><td align="center" valign="middle" >1949.31</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.02</td></tr><tr><td align="center" valign="middle" >29</td><td align="center" valign="middle" >19530506</td><td align="center" valign="middle" >1953.34</td><td align="center" valign="middle" >4.03</td><td align="center" valign="middle" >7.</td><td align="center" valign="middle" >4.13</td><td align="center" valign="middle" >−0.10</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >19600521</td><td align="center" valign="middle" >1960.38</td><td align="center" valign="middle" >7.04</td><td align="center" valign="middle" >12.</td><td align="center" valign="middle" >7.08</td><td align="center" valign="middle" >−0.04</td></tr><tr><td align="center" valign="middle" >31</td><td align="center" valign="middle" >19600522</td><td align="center" valign="middle" >1960.39</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >32</td><td align="center" valign="middle" >19600522</td><td align="center" valign="middle" >1960.39</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.00</td></tr><tr><td align="center" valign="middle" >33</td><td align="center" valign="middle" >19600620</td><td align="center" valign="middle" >1960.46</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.07</td></tr><tr><td align="center" valign="middle" >34</td><td align="center" valign="middle" >19601202</td><td align="center" valign="middle" >1960.92</td><td align="center" valign="middle" >0.46</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >−0.13</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >19620214</td><td align="center" valign="middle" >1962.12</td><td align="center" valign="middle" >1.20</td><td align="center" valign="middle" >2.</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >0.02</td></tr><tr><td align="center" valign="middle" >36</td><td align="center" valign="middle" >19650328</td><td align="center" valign="middle" >1965.23</td><td align="center" valign="middle" >3.11</td><td align="center" valign="middle" >5.</td><td align="center" valign="middle" >2.95</td><td align="center" valign="middle" >0.16</td></tr><tr><td align="center" valign="middle" >37</td><td align="center" valign="middle" >19661228</td><td align="center" valign="middle" >1966.98</td><td align="center" valign="middle" >1.75</td><td align="center" valign="middle" >3.</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >−0.02</td></tr><tr><td align="center" valign="middle" >38</td><td align="center" valign="middle" >19671221</td><td align="center" valign="middle" >1967.97</td><td align="center" valign="middle" >0.99</td><td align="center" valign="middle" >2.</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >−0.19</td></tr><tr><td align="center" valign="middle" >39</td><td align="center" valign="middle" >19710709</td><td align="center" valign="middle" >1971.51</td><td align="center" valign="middle" >3.54</td><td align="center" valign="middle" >6.</td><td align="center" valign="middle" >3.54</td><td align="center" valign="middle" >0.00</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >19740818</td><td align="center" valign="middle" >1974.62</td><td align="center" valign="middle" >3.11</td><td align="center" valign="middle" >5.</td><td align="center" valign="middle" >2.95</td><td align="center" valign="middle" >0.16</td></tr><tr><td align="center" valign="middle" >41</td><td align="center" valign="middle" >19750510</td><td align="center" valign="middle" >1975.35</td><td align="center" valign="middle" >0.73</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >0.14</td></tr><tr><td align="center" valign="middle" >42</td><td align="center" valign="middle" >19811016</td><td align="center" valign="middle" >1981.79</td><td align="center" valign="middle" >6.44</td><td align="center" valign="middle" >11.</td><td align="center" valign="middle" >6.49</td><td align="center" valign="middle" >−0.05</td></tr><tr><td align="center" valign="middle" >43</td><td align="center" valign="middle" >19811107</td><td align="center" valign="middle" >1981.85</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.06</td></tr><tr><td align="center" valign="middle" >44</td><td align="center" valign="middle" >19831004</td><td align="center" valign="middle" >1983.75</td><td align="center" valign="middle" >1.90</td><td align="center" valign="middle" >3.</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >0.13</td></tr><tr><td align="center" valign="middle" >45</td><td align="center" valign="middle" >19850303</td><td align="center" valign="middle" >1985.16</td><td align="center" valign="middle" >1.41</td><td align="center" valign="middle" >2.</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >0.23</td></tr><tr><td align="center" valign="middle" >46</td><td align="center" valign="middle" >19850304</td><td align="center" valign="middle" >1985.17</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >47</td><td align="center" valign="middle" >19850409</td><td align="center" valign="middle" >1985.26</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.09</td></tr><tr><td align="center" valign="middle" >48</td><td align="center" valign="middle" >19870305</td><td align="center" valign="middle" >1987.17</td><td align="center" valign="middle" >1.91</td><td align="center" valign="middle" >3.</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >0.14</td></tr><tr><td align="center" valign="middle" >49</td><td align="center" valign="middle" >19870305</td><td align="center" valign="middle" >1987.17</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.00</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >19870808</td><td align="center" valign="middle" >1987.60</td><td align="center" valign="middle" >0.43</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >−0.16</td></tr><tr><td align="center" valign="middle" >51</td><td align="center" valign="middle" >19880119</td><td align="center" valign="middle" >1988.05</td><td align="center" valign="middle" >0.45</td><td align="center" valign="middle" >1.</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >−0.14</td></tr><tr><td align="center" valign="middle" >52</td><td align="center" valign="middle" >19880205</td><td align="center" valign="middle" >1988.09</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >53</td><td align="center" valign="middle" >19950730</td><td align="center" valign="middle" >1995.57</td><td align="center" valign="middle" >7.48</td><td align="center" valign="middle" >13.</td><td align="center" valign="middle" >7.67</td><td align="center" valign="middle" >−0.19</td></tr><tr><td align="center" valign="middle" >54</td><td align="center" valign="middle" >19971015</td><td align="center" valign="middle" >1997.78</td><td align="center" valign="middle" >2.21</td><td align="center" valign="middle" >4.</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >−0.15</td></tr><tr><td align="center" valign="middle" >55</td><td align="center" valign="middle" >19980130</td><td align="center" valign="middle" >1998.07</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >56</td><td align="center" valign="middle" >20050613</td><td align="center" valign="middle" >2005.44</td><td align="center" valign="middle" >7.37</td><td align="center" valign="middle" >12.</td><td align="center" valign="middle" >7.08</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >57</td><td align="center" valign="middle" >20100227</td><td align="center" valign="middle" >2010.15</td><td align="center" valign="middle" >4.71</td><td align="center" valign="middle" >8.</td><td align="center" valign="middle" >4.72</td><td align="center" valign="middle" >−0.01</td></tr><tr><td align="center" valign="middle"  colspan="3"  >Commensurable value</td><td align="center" valign="middle"  colspan="4"  >0.590</td></tr><tr><td align="center" valign="middle"  colspan="3"  >Mean</td><td align="center" valign="middle"  colspan="4"  >−0.027</td></tr><tr><td align="center" valign="middle"  colspan="3"  >Standard deviation (σ<sub>n−</sub><sub>1</sub>)</td><td align="center" valign="middle"  colspan="4"  >0.142</td></tr></tbody></table></table-wrap><p>From <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref> the results show that the EQs basically all occur at the commensurable point of its time axis, respectively. It also shows that the EQs occurrence is not accidental, and there is its pattern and inevitability, only the commensurable value is different for EQs occurred in different areas.</p><p>In the Tables, ΔX is the commensurable value of the studied region. K means that the EQ lies on K times of the commensurable value ΔX behind the latest recent EQ occurred in the area in its time axis. In the Tables, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-2800834x20.png" xlink:type="simple"/></inline-formula>is the time interval between major EQs occurring in the same area. For example, EQ No. 3 in <xref ref-type="table" rid="table1">Table 1</xref>, X<sub>3</sub> = 1923.22, X<sub>2</sub> = 1917.57, the time interval between the 3<sup>rd</sup> and 2<sup>nd</sup> EQ is 5.65 year (unit: years). The corresponding K value under EQ No. 3 is K<sub>3</sub> = 2, i.e. the 3rd EQ occurred on the second commensurable point in its time axis after the 2<sup>nd</sup> EQ. According to K<sub>3</sub> and the commensurable value, the predicting point equals to 1917.57 adding the product of 2 and the commensurable value (i.e. 1917.57 + 2ΔX = 1917.57 + 4.88). Its prediction error (i.e. the difference between the predicted point and actual time of occurrence of the third EQ) is 0.77 years.</p></sec></sec><sec id="s4"><title>4. Discussion and Conclusion</title><p>1) The commensurability revealed by Titius-Bode itself brings to light the distribution law of the matter in a space region, and the expanding commensurable theory proposed by Weng Wenbo reveals the time law of the occurrence of the events in a specified space region. It can be seen that the commensurability is present in various natural phenomena and has universality. It is helpful to study the complicated relationships among various matters, and thus merits further in-depth research.</p><p>2) The occurrence of the events seems to be a random accident. In fact, that is not the case. It is in the accident that the necessity resides. Therefore, the commensurability can provide a scientific basis for the prediction of events which may occur.</p><p>3) After commensurable value can be determined, K values should be used in order of K = 1, 2, 3, ・・・, i.e. when K = 1 is used but earthquake does not occur, then use K = 2, ・・・. The predicted point extrapolated in the time axis by the commensurable value is only a necessary condition, and therefore certain false forecasts are also inevitable, because the exact occurrence time is determined by multiple complex factors. In order to obtain precise prediction, this method must be used in collaboration with other relevant methods, taking the approach of comprehensive analysis.</p></sec><sec id="s5"><title>Acknowledgements</title><p>We extend heartfelt thanks to the referees for their valuable comments. Dr. Chen I-wan, British (ancestor Chinese), Former Advisor of Committee of Natural Hazard Prediction of China Geophysics Society gave us valuable discussion and help. We express our heartfelt thanks to him.</p><p>This work is supported by the tackle key project of the ministry of science and technology of P. R. China (2012BAK19B01).</p></sec></body><back><ref-list><title>References</title><ref id="scirp.57394-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Geller, R.J., Jackson, D.D., Kagan, Y.Y., et al. (1997) Earthquakes Cannot Be Predicted. Science, 275, 1616-1617.  
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