<?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">JBiSE</journal-id><journal-title-group><journal-title>Journal of Biomedical Science and Engineering</journal-title></journal-title-group><issn pub-type="epub">1937-6871</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jbise.2017.105021</article-id><article-id pub-id-type="publisher-id">JBiSE-76400</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></subj-group></article-categories><title-group><article-title>
 
 
  Comparison of Mathematical Equations Applicable to Tolerance of Total Body Irradiation in Humans and Decay of Isotopes, Uranium and Thorium: Differences and Similarity
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sung</surname><given-names>Jang Chung</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Morristown-Hamblen Healthcare System, Morristown, TN, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>05</month><year>2017</year></pub-date><volume>10</volume><issue>05</issue><fpage>273</fpage><lpage>286</lpage><history><date date-type="received"><day>March</day>	<month>2,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>May</month>	<year>21,</year>	</date><date date-type="accepted"><day>May</day>	<month>24,</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>
 
 
  A clear and exact quantitative relationship between dose of total body irradiation and mortality in humans is still not known because of lack of human data that would enable us to determine LD
  <sub>50</sub> for humans in total body irradiation. Analysis of human data has been primarily from radiation accidents, radiotherapy and the atomic bomb victims. The author published the general mathematical equations of LD
  <sub>50 </sub>constructed on the basis of data presented by Cerveny, MacVittie and Young, employing the probacent formula model. In this study, the author compared the equations of tolerance of total body irradiation and decay of isotopes, uranium and thorium. Differences and similarity in these equations of the two groups are presented. The significance of similarity is specially described.
 
</p></abstract><kwd-group><kwd>Total Body Irradiation; Formula of LD50</kwd><kwd> Decay of Isotopes</kwd><kwd> Half-Life of  Isotopes</kwd><kwd> Safety in Radiotherapy and Space Flight</kwd><kwd> Probacent Model</kwd><kwd> Ultron-Logotron Theory</kwd><kwd> Theory of Everything</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>A clear and exact quantitative relationship between dose of total body irradiation and mortality in humans is still not known because of lack of human data that would enable us to determine LD<sub>50</sub> for humans in total body irradiation. Analysis of human data has been primarily from radiation accidents, radiotherapy and the atomic bomb victims [<xref ref-type="bibr" rid="scirp.76400-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.76400-ref9">9</xref>] .</p><p>The author published a mathematical equation of LD<sub>50</sub> constructed on the basis of the data published by Cerveny, MacVittie and Young [<xref ref-type="bibr" rid="scirp.76400-ref1">1</xref>] .</p><p>In decay of isotopes, an empirically constructed law is currently used to estimate their physical changes [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref11">11</xref>] . It seems to the author that there are no articles in the literatures that compare the equations of total body irradiation in humans and decay of isotopes such as LD<sub>50</sub> in humans and half-life in isotopes [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref11">11</xref>] . In this study, the author compared these equations for humans and isotopes, uranium and thorium, and attempted to clarify differences and similarity in the equations of both groups.</p><sec id="s1_1"><title>1.1. General Mathematical Formula of the Probacent-Probability Equation in Biological Phenomena</title><p>The author published a general mathematical formula, Equation (1) that calculates probabilities of mortality or survival as a function of intensity of stimulus and duration of exposure in humans and other living organisms exposed to hazardous environments or noxious agents, overcoming the risk in biological phenomena [<xref ref-type="bibr" rid="scirp.76400-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref16">16</xref>] .</p><disp-formula id="scirp.76400-formula90"><label>(1a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x2.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula91"><label>(1b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x3.png"  xlink:type="simple"/></disp-formula><p>where i is intensity of stimulus, external stressor or noxious agent; t is duration of exposure; a, b, c, d and n are constants. P is ‘probacent’ (abbreviation of percent probability), a relative amount of internal stress caused by an external stressor or a relative amount of loss of reserve for survival. Probacent values of 0, 50 and 100 correspond to (mean-5 SD), mean and (mean + 5 SD), respectively; the unit of ‘probacent’ is 0.1 SD. In addition, 0, 50 and 100 probacents seem to correspond to 0, 50 and 100 percent probability, respectively in mathematical prediction problems in terms of percentage. Q is mortality probability (%). Survival probability (%) is (100 ? Q). Equation (1) can be used for survival probability problems.</p><p>An actual example of the relationship between the external stressor and the internal stress is the case of carbon monoxide poisoning in humans [<xref ref-type="bibr" rid="scirp.76400-ref17">17</xref>] . P values in the formula, Equations (2) and (3) express the carboxyhemoglobin levels in blood (the amount of internal stress) caused by inspired carbon monoxide in air (the external stressor) at rest (Equation (2)) and at light work(Equation (3)), respectively.</p><disp-formula id="scirp.76400-formula92"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x4.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula93"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x5.png"  xlink:type="simple"/></disp-formula><p>where C is concentration of CO in air (%) and t is duration of exposure (minute).</p><p>Equation (1) is fundamentally based on Gaussian normal distribution.</p><p>Equation (4) represents a general formula that expresses the probability of survival and mortality of US adult population, 2001 [<xref ref-type="bibr" rid="scirp.76400-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref18">18</xref>] . Data on the survival, mortality and life expectancy reported by the National Center for Health Statistics [<xref ref-type="bibr" rid="scirp.76400-ref19">19</xref>] are used to construct the equations.</p><disp-formula id="scirp.76400-formula94"><label>(4a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x6.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula95"><label>(4b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x7.png"  xlink:type="simple"/></disp-formula><p>where P is probacent; t is age; Q is mortality (%); a, b and γ are constants. Survival probability (%),<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-9102398x8.png" xlink:type="simple"/></inline-formula>. The above distribution of Gaussian normal distribution becomes Weibull distribution if γ value = 1.</p><p>In general, as the first step of calculation in order to determine the constants, a, b and γ in Equation (4a), P-values are obtained from experimental data or clinical data, consulting the table of conversion of percent probability into probacent (see the author’s previous publications [<xref ref-type="bibr" rid="scirp.76400-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref16">16</xref>] ), then the constants can be determined with insertion of P-values into Equation (4a).</p><p>As the second step of calculation to obtain Q-values, a computer program of nonintegral calculation (Equation (6)) written by the author [<xref ref-type="bibr" rid="scirp.76400-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref18">18</xref>] is used because the computer cannot perform integral. The program is written on the basis of an approximation equation, Equation 6 for a specific integral equation, Equation (5) [<xref ref-type="bibr" rid="scirp.76400-ref19">19</xref>] .</p><disp-formula id="scirp.76400-formula96"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x9.png"  xlink:type="simple"/></disp-formula><p>The digital computer used the following equation as an approximation for 0 ≤ X&lt;∞.</p><disp-formula id="scirp.76400-formula97"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x10.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula98"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x11.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula99"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x12.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula100"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x13.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula101"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x14.png"  xlink:type="simple"/></disp-formula><p>Mathematical transformation of Equation (4b) to Equation (6) is described in the author’s previous publication [<xref ref-type="bibr" rid="scirp.76400-ref13">13</xref>] and its detail is presented in the author’s book [<xref ref-type="bibr" rid="scirp.76400-ref20">20</xref>] .</p><p>Equation (7) of death rate D is derivable from Equation (4a) (see the author’s previous publication [<xref ref-type="bibr" rid="scirp.76400-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref16">16</xref>] and Appendix of the current article).</p><disp-formula id="scirp.76400-formula102"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x15.png"  xlink:type="simple"/></disp-formula><p>where D is death rate, t is age; A, B and c are constants.</p><p>Formulas of death rate (D) for US older adults are expressed by Equations (8) and (9).</p><p>Age group of 60 - 85 years:</p><disp-formula id="scirp.76400-formula103"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x16.png"  xlink:type="simple"/></disp-formula><p>Age group of 85 - 100 years:</p><disp-formula id="scirp.76400-formula104"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x17.png"  xlink:type="simple"/></disp-formula><p>The probacent formula model has been applied to data in the biomedical literature; to express a relationship among plasma acetaminophen concentration, time after ingestion and occurrence of hepatotoxicity in man [<xref ref-type="bibr" rid="scirp.76400-ref21">21</xref>] ; to express survival probability in patients with heart transplantation [<xref ref-type="bibr" rid="scirp.76400-ref22">22</xref>] ; to express survival probability in patients with malignant melanoma [<xref ref-type="bibr" rid="scirp.76400-ref23">23</xref>] and to express relationship among age, height and weight, and percentile in Saudi and US children of ages 6 - 16 years [<xref ref-type="bibr" rid="scirp.76400-ref24">24</xref>] .</p><p>Mehta and Joshi [<xref ref-type="bibr" rid="scirp.76400-ref25">25</xref>] successfully applied the probacent-probability equation model to use model-derived data as an input for radiation risk evaluation of Indian adult population in their studies.</p></sec><sec id="s1_2"><title>2.2. Equations of Tolerance of Total Body Irradiation in Humans</title><p>To my knowledge, there seem to be no general mathematical models in the literature that express the quantitative relationship among dose rate of radiation, duration of exposure and mortality and/or LD<sub>50</sub> of lethal dose for humans in ionizing total body irradiation.</p><p>Data on LD<sub>5</sub>, LD<sub>10</sub>, LD<sub>50</sub>, LD<sub>90</sub> and LD<sub>95</sub> versus dose rate shown in a table of animal-model predictions of lethal radiation doses to humans published by Cerveny, MacVittie and Young [<xref ref-type="bibr" rid="scirp.76400-ref1">1</xref>] are used to construct predictive formulas. A general formula Equation (10) to express the relationship among dose rate, duration of exposure and mortality in humans exposed to total body irradiation is constructed, employing the general probcent model, Equation (4a) where the constant γ = 1 in Equation (10).</p><disp-formula id="scirp.76400-formula105"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x18.png"  xlink:type="simple"/></disp-formula><p>where D is dose rate (rad/min); t is duration of exposure (min); A and B are constants.</p><p>Equations (11)-(15) express relationships among dose rate in rad/min, duration of exposure in minutes and mortality probability in percentage, employing Equation (10) [<xref ref-type="bibr" rid="scirp.76400-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref27">27</xref>] .</p><p>Various lethal dose values, LD<sub>5</sub>, LD<sub>10</sub>, LD<sub>50</sub>, LD<sub>90</sub> and LD<sub>95</sub>in ionizing total body irradiation in humans can be calculated from these equations.</p><disp-formula id="scirp.76400-formula106"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x19.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula107"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x20.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula108"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x21.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula109"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x22.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula110"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x23.png"  xlink:type="simple"/></disp-formula><p>where D is dose rate (rad/min) and t is duration of exposure (minute).</p><p>If the duration of exposure, time t is given or at any given time t, then the dose rate D<sub>50</sub> and lethal dose LD<sub>50</sub> (a product of D<sub>50</sub> x t) can be expressed by Equations (16) and (17), respectively.</p><disp-formula id="scirp.76400-formula111"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x24.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula112"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x25.png"  xlink:type="simple"/></disp-formula><p><xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref> illustrate the results and reveal a close agreement between formula-derived and animal-model-predicted data on lethal radiation doses, LD<sub>5-95</sub> for humans in the total body irradiation (p &gt; 0.995 in χ&#178; test). The lines representing Equations (11)-(15) in <xref ref-type="fig" rid="fig1">Figure 1</xref> are straight lines with different slopes.</p><p>There is a remarkable agreement between formula-predicted and published estimated LD<sub>50</sub> and mortality probabilities [<xref ref-type="bibr" rid="scirp.76400-ref26">26</xref>] .</p><p>The t values in Equations (13), (16) and (17) seem to mathematically correspond to the half-life of isotopes in decay. The half-life t<sub>1/2</sub> (=T<sub>1/2</sub>) (the duration of</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Relationship among dose rate of radiation, duration of exposure and lethal radiation dose (LD<sub>5-95</sub>) in total body irradiation in humans. The abscissa represents duration of exposure in minutes (log scale). The ordinate represents dose rate in rad/min (log scale). Data points indicate lethal doses of LD<sub>5-95</sub> and appear to fall on the five formula- predicted straight lines in each group, respectively (see text)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-9102398x26.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Comparison of formula-derived and animal-model-predicted lethal radiation doses to humans</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Lethal</th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="3"  >Dose Rate (Gy/minute)</th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >Dose</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >LD5</td><td align="center" valign="middle"  colspan="2"  >Formula-derived</td><td align="center" valign="middle" >194</td><td align="center" valign="middle" >176.9</td><td align="center" valign="middle" >156.4</td><td align="center" valign="middle" >142.7</td><td align="center" valign="middle" >130</td><td align="center" valign="middle" >115</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  >Model-derived</td><td align="center" valign="middle" >194</td><td align="center" valign="middle" >177</td><td align="center" valign="middle" >156</td><td align="center" valign="middle" >143</td><td align="center" valign="middle" >130</td><td align="center" valign="middle" >115</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >LD10</td><td align="center" valign="middle"  colspan="2"  >Formula-derived</td><td align="center" valign="middle" >210</td><td align="center" valign="middle" >192.3</td><td align="center" valign="middle" >171.3</td><td align="center" valign="middle" >156.9</td><td align="center" valign="middle" >143.8</td><td align="center" valign="middle" >128</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  >Model-derived</td><td align="center" valign="middle" >210</td><td align="center" valign="middle" >192</td><td align="center" valign="middle" >171</td><td align="center" valign="middle" >157</td><td align="center" valign="middle" >144</td><td align="center" valign="middle" >128</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >LD50</td><td align="center" valign="middle"  colspan="2"  >Formula-derived</td><td align="center" valign="middle" >275</td><td align="center" valign="middle" >256.6</td><td align="center" valign="middle" >234.1</td><td align="center" valign="middle" >218.4</td><td align="center" valign="middle" >203.9</td><td align="center" valign="middle" >186</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  >Model-derived</td><td align="center" valign="middle" >275</td><td align="center" valign="middle" >257</td><td align="center" valign="middle" >234</td><td align="center" valign="middle" >218</td><td align="center" valign="middle" >204</td><td align="center" valign="middle" >186</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >LD90</td><td align="center" valign="middle"  colspan="2"  >Formula-derived</td><td align="center" valign="middle" >341</td><td align="center" valign="middle" >321.1</td><td align="center" valign="middle" >296.7</td><td align="center" valign="middle" >279.3</td><td align="center" valign="middle" >263.1</td><td align="center" valign="middle" >243</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  >Model-derived</td><td align="center" valign="middle" >341</td><td align="center" valign="middle" >321</td><td align="center" valign="middle" >297</td><td align="center" valign="middle" >279</td><td align="center" valign="middle" >263</td><td align="center" valign="middle" >243</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >LD95</td><td align="center" valign="middle"  colspan="2"  >Formula-derived</td><td align="center" valign="middle" >360</td><td align="center" valign="middle" >339.1</td><td align="center" valign="middle" >313.4</td><td align="center" valign="middle" >295.2</td><td align="center" valign="middle" >278.1</td><td align="center" valign="middle" >257</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  >Model-derived</td><td align="center" valign="middle" >360</td><td align="center" valign="middle" >339</td><td align="center" valign="middle" >313</td><td align="center" valign="middle" >295</td><td align="center" valign="middle" >278</td><td align="center" valign="middle" >257</td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>Formula-derived lethal radiation doses are calculated from Equations (11)-(15), obtaining total dose (rad) by dose rate (rad/minute) D multiplied by duration of exposure, time t (minute). p &gt; 0.995 in χ&#178; test.</p><p>exposure for 50% survival, 50% life expectancy) can be expressed by Equation (18) and (19).</p><disp-formula id="scirp.76400-formula113"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x27.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula114"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x28.png"  xlink:type="simple"/></disp-formula><p>The formulas of the above equations, LD<sub>50</sub> and mortality probability in lethal radiation exposure for humans might be helpful in preventing radiation hazard and injury, and further for safety in radiotherapy.<sub> </sub></p></sec><sec id="s1_3"><title>2.3. Equations of Decay in Radioisotopes, Uranium and Thorium</title><p>All radioactive decay in any isotopes follow the experimental law expressed by Equation (20) [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref28">28</xref>] .</p><disp-formula id="scirp.76400-formula115"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x29.png"  xlink:type="simple"/></disp-formula><p>where N<sub>0</sub> is the number of radioisotope atoms which have not decayed at present. N is the number of remaining atoms after time t. Consequently, the rate of decay each second is proportional to the number present and expressed by Equation (21).</p><disp-formula id="scirp.76400-formula116"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x30.png"  xlink:type="simple"/></disp-formula><p>The constant λ represents the probability that any given nucleus will decay in any given unit interval of time. λ is independent of the age of the nucleus of radioisotopes. λ values of uranium and thorium are 0.154 &#180; 10<sup>9</sup> years and 0.049 &#180; 10<sup>9</sup> years, respectively.</p><p>The half-life, T<sub>1/2</sub>, of any radioisotopes is given by Equation (22).</p><disp-formula id="scirp.76400-formula117"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x31.png"  xlink:type="simple"/></disp-formula><p>The half-life T<sub>1/2</sub> of uranium-238 and thorium-232 is 4.5 billion years and 14.1 billion years, respectively.</p><p>Equation (23) expresses a relationship between half-life and energy of emitted alpha particle from isotopes.</p><disp-formula id="scirp.76400-formula118"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x32.png"  xlink:type="simple"/></disp-formula><p>where E is the energy of emitted alpha particle, A (slope) and B (intercept) are constants. Equation (24) is the equation for thorium-232 [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] . If empirical data on half-life T<sub>1/2</sub> against E<sup>-1/2</sup>( in terms of E) of uranium or thorium are plotted on a log-log scale graph paper, each data of the two groups show a straight line, respectively [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref29">29</xref>] .</p><disp-formula id="scirp.76400-formula119"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x33.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s2"><title>2. Differences in Equations of Total Body Irradiation in Humans and Decay in Isotopes</title><p>General equations of tolerance of total body irradiation in humans (A group) and decay of isotopes, uranium and thorium (B group) are compared as follows:</p><p>1. Mortality</p><p>Mortality in humans:</p><disp-formula id="scirp.76400-formula120"><label>(A1a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x34.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula121"><label>(A1b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x35.png"  xlink:type="simple"/></disp-formula><p>Decay in isotopes:</p><disp-formula id="scirp.76400-formula122"><label>(B1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x36.png"  xlink:type="simple"/></disp-formula><p>2. Survival probability (S):</p><p>Survival probability in humans:</p><disp-formula id="scirp.76400-formula123"><label>(A2a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x37.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula124"><label>(A1b) (A2b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x38.png"  xlink:type="simple"/></disp-formula><p>Remaining probability after Decay in isotopes:</p><disp-formula id="scirp.76400-formula125"><label>(B2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x39.png"  xlink:type="simple"/></disp-formula><p>3. Death rate</p><p>Death rate in humans:</p><disp-formula id="scirp.76400-formula126"><label>(A3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x40.png"  xlink:type="simple"/></disp-formula><p>Decay rate:</p><disp-formula id="scirp.76400-formula127"><label>(B3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x41.png"  xlink:type="simple"/></disp-formula><p>The above comparison indicates clear differences in the equations of both groups, (A) and (B). The differences are considered to be due to the differences between non-uniformity vs uniformity in their structural organizations and sensitivities against the external stressor and/or internal stress of both groups under observations. Structural organizations of human bodies are complex and their sensitivities under observations are non-uniform. In contrast, the structural organization of radioisotope atoms is considered to be uniform and their sensitivity (response) against yet unknown internal stress or external stressor is uniform.</p><p>If LD<sub>5</sub>, LD<sub>10</sub>, LD<sub>50</sub>, LD<sub>90</sub> and LD<sub>95</sub> against time (duration of exposure) are plotted on a log-log scale graph paper, those data reveal multiple straight lines (<xref ref-type="fig" rid="fig1">Figure 1</xref>). In contrary, the data on isotopes, uranium-238 and thrium-232 reveal a single straight line, respectively [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref11">11</xref>] .</p></sec><sec id="s3"><title>3. Similarity in Equations of Tolerance of Total Body Irradiation in Humans and Decay in Isotopes</title><p>The energy of the emitted alpha particle can be deduced by using Einstein’s formula (E = mc<sup>2</sup>).</p><disp-formula id="scirp.76400-formula128"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x42.png"  xlink:type="simple"/></disp-formula><p>where m<sub>p</sub> is the mass of the parent nucleus, m<sub>d</sub> is the mass of the daughter nucleus, and m<sub>a</sub> is the mass of the alpha particle (which is the He<sup>2</sup> nucleus).</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-9102398x43.png" xlink:type="simple"/></inline-formula>represents the lost energy of the parent nucleus that is equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-9102398x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-9102398x44.png" xlink:type="simple"/></inline-formula>. E reflects and is proportional to the amount of internal stress caused by yet unknown inherent factor or undetermined external stressor possibly such as cosmic radiation.</p><p>The relationship between dose rate D and duration of exposure t in total body irradiation in humans is expressed by Equation 26 [<xref ref-type="bibr" rid="scirp.76400-ref26">26</xref>] .</p><disp-formula id="scirp.76400-formula129"><label>(26) (same as (10))</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x45.png"  xlink:type="simple"/></disp-formula><p>The relationship between dose rate and half-life (50% life expectancy for 50% survival probability) is expressed by Equation (27).</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-9102398x46.png" xlink:type="simple"/></inline-formula>; (27) (same as (19))</p><p>The half-life (the duration of exposure for 50% survival, 50% life expectancy) is inversely proportional to the dose rate.</p><p>Equation (28) expresses the relationship between the half-life of isotopes and the energy of emitted alpha particle.</p><disp-formula id="scirp.76400-formula130"><label>(28) (same as (23))</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x47.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula131"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x48.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula132"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x49.png"  xlink:type="simple"/></disp-formula><p>If logT<sub>1/2</sub> versus logE in Equation (30) instead of Equation (29) are plotted on a log-log graph paper, the data points reveal virtually a straight line [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref11">11</xref>] as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> that illustrates a similar straight line representing the data points of logT<sub>1/2</sub> versus logD<sub>50</sub>. Consequently, Equation (27) for mortality in humans and Equation (30) for decay in isotopes reveal a similarity in their forms as well as in the straight lines in their graphic plottings. Both equations, Equations (27) and Equation (30) indicate a similar form. This result may indicate that the equation of decay of isotopes in quantum physics is derivable from the equation of mortality of total body irradiation in humans. The internal stress amount caused by the external stressor, total body irradiation reflects the dose rate. The energy of the emitted alpha particle reflects the internal stress amount in isotope atoms. The internal stress amount is thus common in both phenomena and seems to make the similarity in the forms of Equations (27) and (30).</p><p>The internal stress (energy) is proportional to the dose rate D<sub>50</sub> , and the internal stress of the isotope atom is reflected in the energy E of the emitted alpha particle. On the basis of the similarity in both Equations (27) and (30) and the straight line in both graphic plotting of both equations, Equation (27A) is assumed to express the above relation.</p><disp-formula id="scirp.76400-formula133"><label>(27A)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x50.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula134"><label>(27B)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x51.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula135"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x52.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula136"><label>(27C)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x53.png"  xlink:type="simple"/></disp-formula><p>Equation (27C), (27) and (30) reveal a remarkable similar mathematical form.</p><p>The general formulas of the probacent-probability equation are experimentally (experimental data with animals) [<xref ref-type="bibr" rid="scirp.76400-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref31">31</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref32">32</xref>] and/or empirically (clinical data) constructed by the author and his coworkers [<xref ref-type="bibr" rid="scirp.76400-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref16">16</xref>] . Equations related to decay of isotopes are primarily empirically constructed [<xref ref-type="bibr" rid="scirp.76400-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref11">11</xref>] .</p><p>The probacent model is applicable to express the relationship between dose rate and survival time in mice exposed to total body irradiation (p-value&gt; 0.995 in χ&#178; test) [<xref ref-type="bibr" rid="scirp.76400-ref33">33</xref>] . The probacent model was applied to the data on low dose rate versus cancer mortality risk, published by the United Nations (UNSCEAR, 2010) and other investigators, to construct general formulas expressing a relationship between dose and solid cancer or leukemia mortality probability after exposure to acute low dose ionizing radiation in humans. There is a remarkable agreement between formula-derived and published values of low dose and solid cancer or leukemia mortality probability (P &gt; 0.997) [<xref ref-type="bibr" rid="scirp.76400-ref34">34</xref>] .</p><p>The probacent formula may provide a mathematical bridge connecting biology and quantum physics. The probacent formula gave a special momentum to the author to develop the hypothesis of the ultron-logotron theory related to mind and matter, consciousness and quantum physics (Theory of Everything), and further the possible deeper structure of leptons and quarks on the basis of quantum physics and Confucian philosophy [<xref ref-type="bibr" rid="scirp.76400-ref35">35</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref37">37</xref>] .</p><p>It has been recently discovered that electrons split into two separate parts: a spinon (a neutral magnet behaving as a tiny compass needle) and an orbiton carrying its electron motion (negative electrical charge) around the nucleus [<xref ref-type="bibr" rid="scirp.76400-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref39">39</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref40">40</xref>] . The spinon and orbiton seem to correspond to the neutral part of yin- and yang-ultrons composite and the negative part of yin-ultron as predicted in the ultron-logotron theory, respectively [<xref ref-type="bibr" rid="scirp.76400-ref37">37</xref>] . Yin- and yang-ultrons in a spinon are postulated to line up in a tiny series magnet arrangement with a south and a north pole in one direction that can generate spin. This substructure of electron suggests that a quark in a proton is likewise composed of two separable particles, a magnetic (of yin-and yang-ultrons composite) and an electrical particle (of yin- or yang-ultrons) [<xref ref-type="bibr" rid="scirp.76400-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref44">44</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref45">45</xref>] .</p><p>Hematopoietic cells of bone marrow, the intestinal tract, and the central nervous system are most vulnerable to radiation effects [<xref ref-type="bibr" rid="scirp.76400-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref41">41</xref>] . Death is caused by multi-organ failure. In case of relatively high doses, infection and hemorrhage are earliest contributing factors to death, resulting from the damage to the most sensitive hematopoietic cells in total body irradiation [<xref ref-type="bibr" rid="scirp.76400-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref42">42</xref>] .</p><p>It has been recently proven in neuroscience that radiation caused pathologic cell changes in neurons of brain [<xref ref-type="bibr" rid="scirp.76400-ref43">43</xref>] . The hazard of total body irradiation to astronauts in a possible future long space flight to the mars or other stars would be very significant and serious so that the problems regarding safety of astronauts should be investigated [<xref ref-type="bibr" rid="scirp.76400-ref43">43</xref>] .</p><p>Further research would be needed for verification of the author’s formulas related to tolerance of total body irradiation in humans.</p></sec><sec id="s4"><title>4. Conclusions</title><p>In this study, the mathematical equations applicable to tolerance of total body irradiation in humans and decay in isotopes, uranium and thorium are compared. The following differences and similarity as well as the significance in the equations of both groups are presented. A general formula of the probacent- probability equation is experimentally and empirically constructed and applicable as an approximation method to calculate probabilities of survival, mortality and death rate in humans and animals exposed to hazardous environments or noxious agents, overcoming the risk.</p><p>(1) Differences are present between the equations of tolerance of total body irradiation and decay of isotopes due to differences in uniformity of subjects under observations.</p><p>(2) There is a remarkable similarity between the forms of the equations of LD<sub>50</sub> of total body irradiation in humans and half-life of isotopes.</p><p>(3) The equation of decay of isotopes seems to be derivable from the equation of dose rate of total body irradiation in humans.</p><p>(4) The mathematical probacent model may provide a mathematical bridge connecting biology and quantum physics.</p><p>(5) The equation of tolerance of total body irradiation in humans would be hopefully helpful in radiotherapy and in case of astronauts in a possible future long space flight in estimating their safety.</p><p>(6) Electrons split into two particles, a neutral particle (spinon) and a particle with a negative electrical charge (orbiton) [<xref ref-type="bibr" rid="scirp.76400-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref39">39</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref40">40</xref>] as predicted in the author’s ultron-logotron theory. This substructure of electron suggests that a quark is likewise composed of two separable particles, a magnetic (of yin- and yang-ultrons composite) and an electrical particle (of yin-or yang-ul- trons) [<xref ref-type="bibr" rid="scirp.76400-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref44">44</xref>] [<xref ref-type="bibr" rid="scirp.76400-ref45">45</xref>] .</p><p>Further research would be needed for verification of the above findings and presentation.</p></sec><sec id="s5"><title>Cite this paper</title><p>Chung, S.J. (2017) Comparison of Mathematical Equations Applicable to Tolerance of Total Body Irradiation in Humans and Decay of Isotopes, Uranium and Thorium: Differences and Similarity. J. Biomedical Sci- ence and Engineering, 10, 273-286. https://doi.org/10.4236/jbise.2017.105021</p></sec><sec id="s6"><title>Appendix</title><p>Equation (31) is derived from Equation (4a) (see the author’s previous publication [<xref ref-type="bibr" rid="scirp.76400-ref14">14</xref>] .</p><disp-formula id="scirp.76400-formula137"><label>(4a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x54.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula138"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x55.png"  xlink:type="simple"/></disp-formula><p>where P is probacent; D is death rate, t is time (age), a, b, A’, B’, γ and c are constants.</p><disp-formula id="scirp.76400-formula139"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x56.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula140"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x57.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula141"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x58.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula142"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x59.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula143"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x60.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula144"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x61.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.76400-formula145"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-9102398x62.png"  xlink:type="simple"/></disp-formula><p>Equation (7) and Equation (32) are thus derived from Equation (4a).</p><disp-formula id="scirp.76400-formula146"><graphic  xlink:href="http://html.scirp.org/file/6-9102398x63.png"  xlink:type="simple"/></disp-formula><p>Submit or recommend next manuscript to SCIRP and we will provide best service for you:</p><p>Accepting pre-submission inquiries through Email, Facebook, LinkedIn, Twitter, etc.</p><p>A wide selection of journals (inclusive of 9 subjects, more than 200 journals)</p><p>Providing 24-hour high-quality service</p><p>User-friendly online submission system</p><p>Fair and swift peer-review system</p><p>Efficient typesetting and proofreading procedure</p><p>Display of the result of downloads and visits, as well as the number of cited articles</p><p>Maximum dissemination of your research work</p><p>Submit your manuscript at: http://papersubmission.scirp.org/</p><p>Or contact jbise@scirp.org</p></sec></body><back><ref-list><title>References</title><ref id="scirp.76400-ref1"><label>1</label><mixed-citation publication-type="book" xlink:type="simple">Cerveny, T.J., MacVittie, T.J. and Young, R.W. 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