<?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">IJMPCERO</journal-id><journal-title-group><journal-title>International Journal of Medical Physics, Clinical Engineering and Radiation Oncology</journal-title></journal-title-group><issn pub-type="epub">2168-5436</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijmpcero.2022.112009</article-id><article-id pub-id-type="publisher-id">IJMPCERO-116673</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Calculation of Mass Stopping Power and Range of Protons as Well as Important Radiation Quantities in Some Biological Human Bodyparts (Water, Muscle, Skeletal and Bone, Cortical)
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ahlam</surname><given-names>S. Almutairi</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>Khalda</surname><given-names>T. Osman</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Physics, College of Science, Qassim University, Buraydah, Saudi Arabia</addr-line></aff><aff id="aff1"><addr-line>Department of Physics, College of Science, Qassim University, AL-Rass, Saudi Arabia</addr-line></aff><pub-date pub-type="epub"><day>20</day><month>04</month><year>2022</year></pub-date><volume>11</volume><issue>02</issue><fpage>99</fpage><lpage>112</lpage><history><date date-type="received"><day>26,</day>	<month>February</month>	<year>2022</year></date><date date-type="rev-recd"><day>18,</day>	<month>April</month>	<year>2022</year>	</date><date date-type="accepted"><day>21,</day>	<month>April</month>	<year>2022</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>
 
 
  In this work, the electronic mass stopping power and the range of protons in some biological human body parts
   
  (
  Water, Muscle,
   
  Skeletal and Bone, Cortical)
   
  were calculated in the energy range of protons 0.04 to 200 MeV using the theory of Bethe-Bloch formula as giving in the references. All these calculations were done using
   
  Matlab program. The data related to the densities, average atomic number to mass number <inline-formula><inline-graphic xlink:href="dit_40d7d8ce-6604-4dd4-9eb8-194a2c0dceb6.png" xlink:type="simple"/></inline-formula>
  
   and excitation energies for the present tissues and substances were collected from ICRU Report
   
  44
   
  (1989). The present results for electronic mass stopping powers and ranges were compared with the data of PSTAR and good agreements were found between them,
   
  especially at energies between 1
   
  -
   
  200
   
  MeV for stopping power and 4
   
  -
   
  200
   
  MeV for the range.
   
  Also in this study, several important quantities in the field of radiation, such as thickness, linear energy transfer (LET), absorbed dose, equivalent dose, and effective dose of the protons in the given biological
   
  human body parts
   
  were calculated
   
  at protons energy 0.04
   
  -
   
  200
   
  MeV.
 
</p></abstract><kwd-group><kwd>Biological Human Bodyparts</kwd><kwd> Protons</kwd><kwd> Range</kwd><kwd> MatLab</kwd><kwd> PSTAR</kwd><kwd> Electronic Mass Stopping Power</kwd><kwd> LET</kwd><kwd> Absorbed Dose</kwd><kwd> Effective and Equivalent Dose</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In many fields, such as radiation dosimetry, radiation biology, and many others, radiation chemistry, radiotherapy, and nuclear physics, the stopping power, energy loss, rangestraggling, and equivalent dose rate of ions in the air, tissue, and polymers are very important. The use of protons or heavier ions as an alternative to external photon beams in radiotherapy is increasing, with the reason being that they preserve the target dose, ensure a higher dose delivered to the tumor, and can transfer energy in the form of a point shot through diseased tissue due to the Bragg curve [<xref ref-type="bibr" rid="scirp.116673-ref1">1</xref>]. The stopping power of charged particles has been measured using a variety of ways, including direct energyloss measurements through films, backscattering from thick substrates with deposited absorbing layers, gamma resonance shift measurements, self-supporting methods, and indirect verification of the stopping power based on alpha energy losses in the air have all been reported as methods for measuring the stopping power of charged particles. [<xref ref-type="bibr" rid="scirp.116673-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.116673-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.116673-ref4">4</xref>].</p><p>In the present work, the electronic mass stopping power and range of proton in some biological human body parts (Water, Muscle, Skeletaland Bone, Cortical) are calculated using the Bethe-Bloch formula as reported in the references.</p><p>As it is known in any therapeutic unit with protons, it needs to calculate the absorbed dose, the equivalent dose to the tissue, and the effective dose according to the energy of the protons. Therefore, in this work, a variety of radiation quantities such as thickness, absorbed dose, equivalent dose, and effective dose of the protons in Water, Muscle, Skeletal and Bone, Cortical were also computed in proton energy range 0.04 - 200 MeV.</p></sec><sec id="s2"><title>2. Methods</title><sec id="s2_1"><title>2.1. Calculations of Electronic Mass Stopping Power</title><p>Bethe was the first person to use quantum mechanical studies on stopping power. The Bethe theory of stopping power is valid when the projectile’s velocity surpasses the Bohr velocity. In Bethe’s theory, the goal is assumed to be charged particle. In Bethe’s approach to energy loss, the Born approximation is employed to represent inelastic collisions between heavy particles and atomic electrons. In this theory, the projectile heavy particle is as assumed to be structureless, whereas the target nucleus is assumed to be infinitely massive [<xref ref-type="bibr" rid="scirp.116673-ref4">4</xref>]. For the energy range 0.04 - 200 MeV, the Bethe mass stopping power equation [<xref ref-type="bibr" rid="scirp.116673-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.116673-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.116673-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.116673-ref7">7</xref>] was used:</p><p>− d E ρ d x = 5.08 &#215; 10 − 31 z 2 n β 2 ρ [ F ( β ) − ln I ] (1)</p><p>where β is v/c wherev is the proton velocity and c is light velocity,I is the mean excitation energy and F(β) is given by</p><p>F ( β ) = ln 1.02 &#215; 10 6 β 2 1 − β 2 − β 2 (2)</p><p>n is calculated using the following relation:</p><p>n = N a v ρ 〈 Z A 〉 (3)</p><p>where N<sub>a</sub> Avogadro number, ρ is the density of substances and Ζ/A is the ratio of atomic number to the mass number of substances. The basic data for human body tissues are given in <xref ref-type="table" rid="table1">Table 1</xref>. The calculated mass stopping power of protons for Water, Muscle, Skeletal and Bone, Cortical are based on Bethe equation after substituting the constants from <xref ref-type="table" rid="table1">Table 1</xref>. In <xref ref-type="table" rid="table2">Table 2</xref> the compositions of the human tissues are given [<xref ref-type="bibr" rid="scirp.116673-ref8">8</xref>].</p></sec><sec id="s2_2"><title>2.2. Calculations of Range</title><p>The range of a heavy particle is the straight distance it travels within the target. Light particles like electrons and positrons scatter widely throughout the path of targets due to their low mass, making it difficult to determine their journey duration. The path length of light particles has been calculated with remarkable success using Monte Carlo methods, which are based on a broad class of computational algorithms. On the other hand, heavy particles like protons have a practically straight line path length. The range of protons can be calculated using numerical integration methods. The Continuous Slowing Down Approximation (CSDA), on the other hand, is a straightforward and extensively used method for finding a variable’s range. This study used a simple and standard method for calculating the range of heavy particles such as protons in the targets. The CSDA approach uses incident particles to constantly lose energy in the route of the targets. neglects energy loss fluctuations. The range, R for an incident proton in the CSDA method is given as [<xref ref-type="bibr" rid="scirp.116673-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.116673-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.116673-ref7">7</xref>]:</p><p>R = ∫ E 0 E f d E M S ( E ) (4)</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Basic data for calculating mass stopping powers</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >I (eV)</th><th align="center" valign="middle" >n (electrons/m<sup>3</sup>)</th><th align="center" valign="middle" >〈 Z / A 〉</th><th align="center" valign="middle" >Density ρ (g/m<sup>3</sup>)</th><th align="center" valign="middle" >Substances</th></tr></thead><tr><td align="center" valign="middle" >75</td><td align="center" valign="middle" >3.341 &#215; 10<sup>29</sup></td><td align="center" valign="middle" >0.555</td><td align="center" valign="middle" >1,000,000</td><td align="center" valign="middle" >Water</td></tr><tr><td align="center" valign="middle" >74.6</td><td align="center" valign="middle" >3.476 &#215;10<sup>29</sup></td><td align="center" valign="middle" >0.550</td><td align="center" valign="middle" >1,050,000</td><td align="center" valign="middle" >Muscle, Skeletal</td></tr><tr><td align="center" valign="middle" >112</td><td align="center" valign="middle" >5.894 &#215;10<sup>29</sup></td><td align="center" valign="middle" >0.51</td><td align="center" valign="middle" >1,920,000</td><td align="center" valign="middle" >Bone, Cortical</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Elemental composition of Water, Muscle, Skeletal and Bone, Cortical tissues</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Composition</th><th align="center" valign="middle" >Substances</th></tr></thead><tr><td align="center" valign="middle" >H(0.111898), O(0.888102)</td><td align="center" valign="middle" >Water</td></tr><tr><td align="center" valign="middle" >C(0.143000), N(0.034000), H(0.102000), O(0.710000), Na(0.001000), P(0.002000), k(0.004000), Cl(0.001000), S(0.003000)</td><td align="center" valign="middle" >Muscle, Skeletal</td></tr><tr><td align="center" valign="middle" >C(0.155000), N(0.042000), H(0.034000), O(0.435000), Na(0.001000), P(0.103000), S(0.003000), Ca(0.225000), Mg(0.002000)</td><td align="center" valign="middle" >Bone, Cortical</td></tr></tbody></table></table-wrap><p>where, E 0 is the initial energy of incident charged particle in material, E f is the final energy of incident charged particle in material and M S ( E ) is the mass stopping power.</p></sec><sec id="s2_3"><title>2.3. Calculations of Thickness, Absorbed Dose, Equivalent Dose and Effective Dose</title><p>Thickness of proton in the tissue or substance is given by</p><p>T = R ρ (5)</p><p>where R (in g/cm<sup>2</sup>) is the range and is ρ the density of the tissue or substance [<xref ref-type="bibr" rid="scirp.116673-ref9">9</xref>]</p><p>Absorbed dose in (in rad): It is the transfer of an amount of energy of 100 erg per gram of the absorbent material when protons pass over it and is given by the following relation: [<xref ref-type="bibr" rid="scirp.116673-ref9">9</xref>]</p><p>D = E 1   grm 1.6 &#215; 10 − 13     J 1   MeV 10 7     erg 1   J 1   rad 100   erg gram (6)</p><p>where E is the proton energy.</p><p>Equivalent dose: is given by</p><p>H T = ∑ R W R &#215; D (7)</p><p>where D is the absorbed dose and W R is the weighting factor of radiation (proton) [<xref ref-type="bibr" rid="scirp.116673-ref9">9</xref>]</p><p>Effective dose: is given by</p><p>E = ∑ T W T H T (8)</p><p>where W T is the weighting factor of tissue or substance [<xref ref-type="bibr" rid="scirp.116673-ref9">9</xref>];</p><p>where W T = 0.12 for Water, Muscle, Skeletal and Bone, Cortical and W R = 5 for protons [<xref ref-type="bibr" rid="scirp.116673-ref10">10</xref>].</p></sec><sec id="s2_4"><title>2.4. The Percentage Error of Difference</title><p>The percentage error of difference for the mass stopping power and range of protons in given biological human body parts is calculated by</p><p>% error = PSTARresult − Presentresult PSTARresult &#215; 100 (9)</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>The results of mass stopping power and range of protons in some biological human body parts (Water, Muscle, Skeletal and Bone, Cortical) are given in <xref ref-type="table" rid="table3">Table 3</xref>. In Figures 1-3 the mass stopping power of biological human body parts and their compositions are plotted using MathLab program and it is noted that the mass stopping power of all substances and tissues is approximately equal to t the average values of its compositions. The comparison between the present calculated electronic mass stopping powers and that of PSTAR program [<xref ref-type="bibr" rid="scirp.116673-ref8">8</xref>] are</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Values of electronicmass stopping power (in MeV cm<sup>2</sup>/g) of Water, Muscle, Skeletal and Bone, Cortical tissues</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="9"  >Mass stopping power (in MeV cm<sup>2</sup>/g)</th><th align="center" valign="middle"  rowspan="3"  >Proton energy (MeV)</th></tr></thead><tr><td align="center" valign="middle"  colspan="3"  >Bone, Cortical</td><td align="center" valign="middle"  colspan="3"  >Muscle, Skeletal</td><td align="center" valign="middle"  colspan="3"  >Water</td></tr><tr><td align="center" valign="middle" >Error%</td><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This Work</td><td align="center" valign="middle" >Error%</td><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This Work</td><td align="center" valign="middle" >Error%</td><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This work</td></tr><tr><td align="center" valign="middle" >172.21</td><td align="center" valign="middle" >648.4</td><td align="center" valign="middle" >−468.188</td><td align="center" valign="middle" >63.31</td><td align="center" valign="middle" >763.9</td><td align="center" valign="middle" >280.2840</td><td align="center" valign="middle" >60.29</td><td align="center" valign="middle" >732.4</td><td align="center" valign="middle" >290.8147</td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >74.09</td><td align="center" valign="middle" >708.7</td><td align="center" valign="middle" >183.5666</td><td align="center" valign="middle" >13.65</td><td align="center" valign="middle" >835.5</td><td align="center" valign="middle" >721.4194</td><td align="center" valign="middle" >8.91</td><td align="center" valign="middle" >805</td><td align="center" valign="middle" >733.2987</td><td align="center" valign="middle" >0.06</td></tr><tr><td align="center" valign="middle" >44.71</td><td align="center" valign="middle" >726</td><td align="center" valign="middle" >401.4380</td><td align="center" valign="middle" >3.39</td><td align="center" valign="middle" >854.5</td><td align="center" valign="middle" >825.5114</td><td align="center" valign="middle" >−1.33</td><td align="center" valign="middle" >826</td><td align="center" valign="middle" >837.0064</td><td align="center" valign="middle" >0.08</td></tr><tr><td align="center" valign="middle" >32.51</td><td align="center" valign="middle" >718.4</td><td align="center" valign="middle" >484.8158</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >842.8</td><td align="center" valign="middle" >836.9089</td><td align="center" valign="middle" >−3.87</td><td align="center" valign="middle" >816.1</td><td align="center" valign="middle" >847.7091</td><td align="center" valign="middle" >0.1</td></tr><tr><td align="center" valign="middle" >14.46</td><td align="center" valign="middle" >580.5</td><td align="center" valign="middle" >496.5740</td><td align="center" valign="middle" >−3.46</td><td align="center" valign="middle" >669.4</td><td align="center" valign="middle" >692.5518</td><td align="center" valign="middle" >−5.912</td><td align="center" valign="middle" >661.3</td><td align="center" valign="middle" >700.4432</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >4.74</td><td align="center" valign="middle" >394</td><td align="center" valign="middle" >375.3311</td><td align="center" valign="middle" >−3.64</td><td align="center" valign="middle" >466.3</td><td align="center" valign="middle" >483.2825</td><td align="center" valign="middle" >−3.51</td><td align="center" valign="middle" >471.9</td><td align="center" valign="middle" >488.4735</td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >307</td><td align="center" valign="middle" >299.7432</td><td align="center" valign="middle" >−3.41</td><td align="center" valign="middle" >363.2</td><td align="center" valign="middle" >375.5942</td><td align="center" valign="middle" >−3.14</td><td align="center" valign="middle" >368</td><td align="center" valign="middle" >379.5403</td><td align="center" valign="middle" >0.6</td></tr><tr><td align="center" valign="middle" >1.47</td><td align="center" valign="middle" >254.9</td><td align="center" valign="middle" >251.1486</td><td align="center" valign="middle" >−3.37</td><td align="center" valign="middle" >300</td><td align="center" valign="middle" >310.1025</td><td align="center" valign="middle" >−3.10</td><td align="center" valign="middle" >303.9</td><td align="center" valign="middle" >313.3203</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >1.07</td><td align="center" valign="middle" >219.6</td><td align="center" valign="middle" >217.2573</td><td align="center" valign="middle" >−10.25</td><td align="center" valign="middle" >241</td><td align="center" valign="middle" >265.7017</td><td align="center" valign="middle" >−2.93</td><td align="center" valign="middle" >260.8</td><td align="center" valign="middle" >268.4361</td><td align="center" valign="middle" >1.0</td></tr><tr><td align="center" valign="middle" >1.13</td><td align="center" valign="middle" >135.5</td><td align="center" valign="middle" >133.9751</td><td align="center" valign="middle" >−2.16</td><td align="center" valign="middle" >156.8</td><td align="center" valign="middle" >160.1849</td><td align="center" valign="middle" >−2.02</td><td align="center" valign="middle" >158.6</td><td align="center" valign="middle" >161.8006</td><td align="center" valign="middle" >2.0</td></tr><tr><td align="center" valign="middle" >2.21</td><td align="center" valign="middle" >81.42</td><td align="center" valign="middle" >79.6218</td><td align="center" valign="middle" >−0.76</td><td align="center" valign="middle" >93.01</td><td align="center" valign="middle" >93.7174</td><td align="center" valign="middle" >−0.65</td><td align="center" valign="middle" >94.04</td><td align="center" valign="middle" >94.6491</td><td align="center" valign="middle" >4.0</td></tr><tr><td align="center" valign="middle" >2.97</td><td align="center" valign="middle" >59.76</td><td align="center" valign="middle" >57.9867</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >67.83</td><td align="center" valign="middle" >67.7684</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >68.58</td><td align="center" valign="middle" >68.4376</td><td align="center" valign="middle" >6.0</td></tr><tr><td align="center" valign="middle" >3.52</td><td align="center" valign="middle" >47.77</td><td align="center" valign="middle" >46.0890</td><td align="center" valign="middle" >0.69</td><td align="center" valign="middle" >54</td><td align="center" valign="middle" >53.6292</td><td align="center" valign="middle" >0.81</td><td align="center" valign="middle" >54.60</td><td align="center" valign="middle" >54.1565</td><td align="center" valign="middle" >8.0</td></tr><tr><td align="center" valign="middle" >3.99</td><td align="center" valign="middle" >40.08</td><td align="center" valign="middle" >38.4770</td><td align="center" valign="middle" >1.18</td><td align="center" valign="middle" >45.17</td><td align="center" valign="middle" >44.6350</td><td align="center" valign="middle" >1.31</td><td align="center" valign="middle" >45.67</td><td align="center" valign="middle" >45.0727</td><td align="center" valign="middle" >10.0</td></tr><tr><td align="center" valign="middle" >5.93</td><td align="center" valign="middle" >23.07</td><td align="center" valign="middle" >21.7030</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >25.78</td><td align="center" valign="middle" >24.9752</td><td align="center" valign="middle" >3.27</td><td align="center" valign="middle" >26.07</td><td align="center" valign="middle" >25.2182</td><td align="center" valign="middle" >20.0</td></tr><tr><td align="center" valign="middle" >7.57</td><td align="center" valign="middle" >16.67</td><td align="center" valign="middle" >15.4082</td><td align="center" valign="middle" >4.83</td><td align="center" valign="middle" >18.56</td><td align="center" valign="middle" >17.6633</td><td align="center" valign="middle" >4.93</td><td align="center" valign="middle" >18.76</td><td align="center" valign="middle" >17.8345</td><td align="center" valign="middle" >30.0</td></tr><tr><td align="center" valign="middle" >9.17</td><td align="center" valign="middle" >13.26</td><td align="center" valign="middle" >12.0447</td><td align="center" valign="middle" >6.42</td><td align="center" valign="middle" >14.72</td><td align="center" valign="middle" >13.7744</td><td align="center" valign="middle" >6.54</td><td align="center" valign="middle" >14.88</td><td align="center" valign="middle" >13.9076</td><td align="center" valign="middle" >40.0</td></tr><tr><td align="center" valign="middle" >10.60</td><td align="center" valign="middle" >11.11</td><td align="center" valign="middle" >9.9320</td><td align="center" valign="middle" >7.89</td><td align="center" valign="middle" >12.31</td><td align="center" valign="middle" >11.3390</td><td align="center" valign="middle" >8.05</td><td align="center" valign="middle" >12.45</td><td align="center" valign="middle" >11.4484</td><td align="center" valign="middle" >50.0</td></tr><tr><td align="center" valign="middle" >12.01</td><td align="center" valign="middle" >9.63</td><td align="center" valign="middle" >8.4736</td><td align="center" valign="middle" >9.37</td><td align="center" valign="middle" >10.66</td><td align="center" valign="middle" >9.6615</td><td align="center" valign="middle" >9.51</td><td align="center" valign="middle" >10.78</td><td align="center" valign="middle" >9.7547</td><td align="center" valign="middle" >60.0</td></tr><tr><td align="center" valign="middle" >13.42</td><td align="center" valign="middle" >8.55</td><td align="center" valign="middle" >7.4023</td><td align="center" valign="middle" >10.78</td><td align="center" valign="middle" >9.45</td><td align="center" valign="middle" >8.4315</td><td align="center" valign="middle" >10.86</td><td align="center" valign="middle" >9.55</td><td align="center" valign="middle" >8.5127</td><td align="center" valign="middle" >70.0</td></tr><tr><td align="center" valign="middle" >14.77</td><td align="center" valign="middle" >7.72</td><td align="center" valign="middle" >6.5800</td><td align="center" valign="middle" >12.21</td><td align="center" valign="middle" >8.53</td><td align="center" valign="middle" >7.4886</td><td align="center" valign="middle" >12.29</td><td align="center" valign="middle" >8.62</td><td align="center" valign="middle" >7.5606</td><td align="center" valign="middle" >80.0</td></tr><tr><td align="center" valign="middle" >16.04</td><td align="center" valign="middle" >7.06</td><td align="center" valign="middle" >5.9276</td><td align="center" valign="middle" >13.57</td><td align="center" valign="middle" >7.8</td><td align="center" valign="middle" >6.7414</td><td align="center" valign="middle" >13.63</td><td align="center" valign="middle" >7.88</td><td align="center" valign="middle" >6.8062</td><td align="center" valign="middle" >90.0</td></tr><tr><td align="center" valign="middle" >17.36</td><td align="center" valign="middle" >6.53</td><td align="center" valign="middle" >5.3965</td><td align="center" valign="middle" >14.93</td><td align="center" valign="middle" >7.21</td><td align="center" valign="middle" >6.1338</td><td align="center" valign="middle" >14.94</td><td align="center" valign="middle" >7.28</td><td align="center" valign="middle" >6.1927</td><td align="center" valign="middle" >100.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.9553</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >5.6294</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >5.6835</td><td align="center" valign="middle" >110.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.5826</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >5.2036</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >5.2536</td><td align="center" valign="middle" >120.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.2632</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.8391</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.8856</td><td align="center" valign="middle" >130.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.9864</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.5234</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.5667</td><td align="center" valign="middle" >140.0</td></tr><tr><td align="center" valign="middle" >23.44</td><td align="center" valign="middle" >4.89</td><td align="center" valign="middle" >3.7440</td><td align="center" valign="middle" >21.06</td><td align="center" valign="middle" >5.38</td><td align="center" valign="middle" >4.2470</td><td align="center" valign="middle" >21.18</td><td align="center" valign="middle" >5.44</td><td align="center" valign="middle" >4.2877</td><td align="center" valign="middle" >150.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.5298</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.0029</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.0413</td><td align="center" valign="middle" >160.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.3392</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.7858</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.8221</td><td align="center" valign="middle" >170.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.1683</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.5912</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.6257</td><td align="center" valign="middle" >180.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.0142</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.4159</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.4486</td><td align="center" valign="middle" >190.0</td></tr><tr><td align="center" valign="middle" >28.85</td><td align="center" valign="middle" >4.04</td><td align="center" valign="middle" >2.8745</td><td align="center" valign="middle" >26.64</td><td align="center" valign="middle" >4.44</td><td align="center" valign="middle" >3.2570</td><td align="center" valign="middle" >26.77</td><td align="center" valign="middle" >4.49</td><td align="center" valign="middle" >3.2882</td><td align="center" valign="middle" >200.0</td></tr></tbody></table></table-wrap><p>shown in Figures 4-6 angood agreements between two results are observed in energy range 1 - 200 MeV.</p><p>In <xref ref-type="table" rid="table4">Table 4</xref> the ranges of protons in some Biological human body parts (Water, Muscle, Skeletal and Bone, Cortical) are given. In Figures 7-9 a comparison between present results of ranges and that of PSTAR data are shown in energy</p><p>range 0.1 - 200 MeV and good agreements are observed. In <xref ref-type="table" rid="table5">Table 5</xref> and <xref ref-type="table" rid="table6">Table 6</xref> the thickness, LET, absorbed dose, effective and equivalent dose are given. In <xref ref-type="table" rid="table7">Table 7</xref> and <xref ref-type="table" rid="table8">Table 8</xref>, the empirical formulae for calculating mass stopping powers and ranges for protons in some biological human body parts (Water, Muscle Skeletal and Bone, Cortical) are given with the percentage difference error.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In this work, calculations of mass stopping power and range of protons incident</p><p>on the three different biological human parts (Water, Muscle, Skeletal and Bone, Cortical) have been done and the following conclusions are drawn:</p><p>1) The mass stopping power of the Water, Muscle, Skeletal and Bone, and Cortical is equal to the average value of mass stopping power of their compositions in energy range 0.04 - 200 MeV.</p><p>2) Values for mass stopping power and ranges of protons in Water, Muscle, Skeletal and Bone, Cortical are in good agreement with the data of PSTAR program. The percentage value of error difference was between 0.09% - 28.88% for</p><p>mass stopping power and was between 3.99% - 79.47% for range at proton energy ranging 0.04 - 200 MeV.</p><p>3) It was also observed that the maximum value of mass stopping power was at 0.1 MeV and after that, the mass stopping power start to decrease with increasing proton energy as expected.</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Values of range (in g/cm<sup>2</sup>) of Water, Muscle, Skeletal and Bone, Cortical tissues</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="9"  >Range (g/cm<sup>2</sup>)</th><th align="center" valign="middle"  rowspan="3"  >Proton energy (MeV)</th></tr></thead><tr><td align="center" valign="middle"  colspan="3"  >Bone, Cortical</td><td align="center" valign="middle"  colspan="3"  >Muscle, Skeletal</td><td align="center" valign="middle"  colspan="3"  >Water</td></tr><tr><td align="center" valign="middle" >Error%</td><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This Work</td><td align="center" valign="middle" >Error%</td><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This Work</td><td align="center" valign="middle" >Error%</td><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This Work</td></tr><tr><td align="center" valign="middle" >74.27</td><td align="center" valign="middle" >7.86 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >2.022 &#215; 1<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >78.25</td><td align="center" valign="middle" >6.96 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >1.514 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >79.47</td><td align="center" valign="middle" >7.25 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >1.488 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >75.06</td><td align="center" valign="middle" >1.06 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >3.991 &#215; 1<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >67.93</td><td align="center" valign="middle" >9.39 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >3.011 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >72.48</td><td align="center" valign="middle" >9.78 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >2.691 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >0.06</td></tr><tr><td align="center" valign="middle" >51.75</td><td align="center" valign="middle" >1.34&#215;10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >6.465 &#215; 1<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >58.08</td><td align="center" valign="middle" >1.17 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >4.905 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >60.12</td><td align="center" valign="middle" >1.21 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >4.825 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >0.08</td></tr><tr><td align="center" valign="middle" >41.61</td><td align="center" valign="middle" >1.61 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >9.400 &#215; 1<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >48.84</td><td align="center" valign="middle" >1.40 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >7.162 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >51.41</td><td align="center" valign="middle" >1.45 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >7.046 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >0.1</td></tr><tr><td align="center" valign="middle" >3.99</td><td align="center" valign="middle" >3.13 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >3.005 &#215; 1<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >14.39</td><td align="center" valign="middle" >2.71 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >2.320 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >18.43</td><td align="center" valign="middle" >2.80 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >2.284 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >30.41</td><td align="center" valign="middle" >7.37 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >9.611 &#215; 1<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >−18.39</td><td align="center" valign="middle" >6.35 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >7.518 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >−10.33</td><td align="center" valign="middle" >6.42 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >7.407 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >0.4</td></tr><tr><td align="center" valign="middle" >−46.15</td><td align="center" valign="middle" >0.0013</td><td align="center" valign="middle" >0.0019</td><td align="center" valign="middle" >−25.0</td><td align="center" valign="middle" >0.0012</td><td align="center" valign="middle" >0.0015</td><td align="center" valign="middle" >−36.36</td><td align="center" valign="middle" >0.0011</td><td align="center" valign="middle" >0.0015</td><td align="center" valign="middle" >0.6</td></tr><tr><td align="center" valign="middle" >−55.0</td><td align="center" valign="middle" >0.0020</td><td align="center" valign="middle" >0.0031</td><td align="center" valign="middle" >−41.18</td><td align="center" valign="middle" >0.0017</td><td align="center" valign="middle" >0.0024</td><td align="center" valign="middle" >−41.18</td><td align="center" valign="middle" >0.0017</td><td align="center" valign="middle" >0.0024</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >−60.71</td><td align="center" valign="middle" >0.0028</td><td align="center" valign="middle" >0.0045</td><td align="center" valign="middle" >−50.0</td><td align="center" valign="middle" >0.0024</td><td align="center" valign="middle" >0.0036</td><td align="center" valign="middle" >−45.83</td><td align="center" valign="middle" >0.0024</td><td align="center" valign="middle" >0.0035</td><td align="center" valign="middle" >1.0</td></tr><tr><td align="center" valign="middle" >−75</td><td align="center" valign="middle" >0.008</td><td align="center" valign="middle" >0.014</td><td align="center" valign="middle" >−53.33</td><td align="center" valign="middle" >0.0075</td><td align="center" valign="middle" >0.0115</td><td align="center" valign="middle" >−46.67</td><td align="center" valign="middle" >0.0075</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >2.0</td></tr><tr><td align="center" valign="middle" >−60.72</td><td align="center" valign="middle" >0.028</td><td align="center" valign="middle" >0.045</td><td align="center" valign="middle" >−55.42</td><td align="center" valign="middle" >0.024</td><td align="center" valign="middle" >0.0373</td><td align="center" valign="middle" >−50.00</td><td align="center" valign="middle" >0.024</td><td align="center" valign="middle" >0.036</td><td align="center" valign="middle" >4.0</td></tr><tr><td align="center" valign="middle" >−57.91</td><td align="center" valign="middle" >0.057</td><td align="center" valign="middle" >0.090</td><td align="center" valign="middle" >−48.60</td><td align="center" valign="middle" >0.050</td><td align="center" valign="middle" >0.0743</td><td align="center" valign="middle" >−48.98</td><td align="center" valign="middle" >0.049</td><td align="center" valign="middle" >0.073</td><td align="center" valign="middle" >6.0</td></tr><tr><td align="center" valign="middle" >−53.69</td><td align="center" valign="middle" >0.095</td><td align="center" valign="middle" >0.146</td><td align="center" valign="middle" >−45.78</td><td align="center" valign="middle" >0.083</td><td align="center" valign="middle" >0.1210</td><td align="center" valign="middle" >−45.12</td><td align="center" valign="middle" >0.082</td><td align="center" valign="middle" >0.119</td><td align="center" valign="middle" >8.0</td></tr><tr><td align="center" valign="middle" >−51.71</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >0.2124</td><td align="center" valign="middle" >−47.17</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >0.1766</td><td align="center" valign="middle" >−58.18</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >0.174</td><td align="center" valign="middle" >10.0</td></tr><tr><td align="center" valign="middle" >−41.46</td><td align="center" valign="middle" >0.48</td><td align="center" valign="middle" >0.679</td><td align="center" valign="middle" >−36.19</td><td align="center" valign="middle" >0.42</td><td align="center" valign="middle" >0.572</td><td align="center" valign="middle" >−34.76</td><td align="center" valign="middle" >0.42</td><td align="center" valign="middle" >0.566</td><td align="center" valign="middle" >20.0</td></tr><tr><td align="center" valign="middle" >−35.35</td><td align="center" valign="middle" >0.99</td><td align="center" valign="middle" >1.340</td><td align="center" valign="middle" >−32.92</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >1.183</td><td align="center" valign="middle" >−27.95</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >1.126</td><td align="center" valign="middle" >30.0</td></tr><tr><td align="center" valign="middle" >−30</td><td align="center" valign="middle" >1.67</td><td align="center" valign="middle" >2.171</td><td align="center" valign="middle" >−23.60</td><td align="center" valign="middle" >1.50</td><td align="center" valign="middle" >1.854</td><td align="center" valign="middle" >−23.99</td><td align="center" valign="middle" >1.48</td><td align="center" valign="middle" >1.835</td><td align="center" valign="middle" >40.0</td></tr><tr><td align="center" valign="middle" >−26.28</td><td align="center" valign="middle" >2.50</td><td align="center" valign="middle" >3.157</td><td align="center" valign="middle" >−20.85</td><td align="center" valign="middle" >2.24</td><td align="center" valign="middle" >2.707</td><td align="center" valign="middle" >−20.72</td><td align="center" valign="middle" >2.22</td><td align="center" valign="middle" >2.680</td><td align="center" valign="middle" >50.0</td></tr><tr><td align="center" valign="middle" >−23.51</td><td align="center" valign="middle" >3.47</td><td align="center" valign="middle" >4.286</td><td align="center" valign="middle" >−18.21</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >3.688</td><td align="center" valign="middle" >−18.54</td><td align="center" valign="middle" >3.08</td><td align="center" valign="middle" >3.651</td><td align="center" valign="middle" >60.0</td></tr><tr><td align="center" valign="middle" >−21.47</td><td align="center" valign="middle" >4.57</td><td align="center" valign="middle" >5.551</td><td align="center" valign="middle" >−16.52</td><td align="center" valign="middle" >4.11</td><td align="center" valign="middle" >4.789</td><td align="center" valign="middle" >−16.54</td><td align="center" valign="middle" >4.07</td><td align="center" valign="middle" >4.743</td><td align="center" valign="middle" >70.0</td></tr><tr><td align="center" valign="middle" >−19.73</td><td align="center" valign="middle" >5.80</td><td align="center" valign="middle" >6.944</td><td align="center" valign="middle" >−14.86</td><td align="center" valign="middle" >5.23</td><td align="center" valign="middle" >6.007</td><td align="center" valign="middle" >−15.09</td><td align="center" valign="middle" >5.17</td><td align="center" valign="middle" >5.950</td><td align="center" valign="middle" >80.0</td></tr><tr><td align="center" valign="middle" >−18.32</td><td align="center" valign="middle" >7.15</td><td align="center" valign="middle" >8.460</td><td align="center" valign="middle" >−13.72</td><td align="center" valign="middle" >6.45</td><td align="center" valign="middle" >7.335</td><td align="center" valign="middle" >−13.89</td><td align="center" valign="middle" >6.38</td><td align="center" valign="middle" >7.266</td><td align="center" valign="middle" >90.0</td></tr><tr><td align="center" valign="middle" >−17.12</td><td align="center" valign="middle" >8.62</td><td align="center" valign="middle" >10.096</td><td align="center" valign="middle" >−12.58</td><td align="center" valign="middle" >7.79</td><td align="center" valign="middle" >8.770</td><td align="center" valign="middle" >−12.84</td><td align="center" valign="middle" >7.70</td><td align="center" valign="middle" >8.689</td><td align="center" valign="middle" >100.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >11.845</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10.309</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10.214</td><td align="center" valign="middle" >110.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >13.706</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >11.949</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >11.840</td><td align="center" valign="middle" >120.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15.675</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >13.686</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >13.562</td><td align="center" valign="middle" >130.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >17.750</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15.519</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15.380</td><td align="center" valign="middle" >140.0</td></tr><tr><td align="center" valign="middle" >−13.35</td><td align="center" valign="middle" >17.58</td><td align="center" valign="middle" >19.927</td><td align="center" valign="middle" >−9.51</td><td align="center" valign="middle" >15.93</td><td align="center" valign="middle" >17.445</td><td align="center" valign="middle" >−9.71</td><td align="center" valign="middle" >15.76</td><td align="center" valign="middle" >17.290</td><td align="center" valign="middle" >150.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >22.205</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >19.463</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >19.291</td><td align="center" valign="middle" >160.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >24.581</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >21.571</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >21.382</td><td align="center" valign="middle" >170.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >27.054</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >23.767</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >23.560</td><td align="center" valign="middle" >180.0</td></tr><tr><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >29.622</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >26.050</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25.824</td><td align="center" valign="middle" >190.0</td></tr><tr><td align="center" valign="middle" >−11.78</td><td align="center" valign="middle" >28.88</td><td align="center" valign="middle" >32.283</td><td align="center" valign="middle" >−8.42</td><td align="center" valign="middle" >26.21</td><td align="center" valign="middle" >28.417</td><td align="center" valign="middle" >−8.65</td><td align="center" valign="middle" >25.93</td><td align="center" valign="middle" >28.172</td><td align="center" valign="middle" >200.0</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Thickness, LET, absorbed dose, equivalent dose and effective dose of proton in Water and Muscle, Skeletal</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >(MeV)</th><th align="center" valign="middle"  colspan="5"  >Water</th><th align="center" valign="middle"  colspan="5"  >Macles, Skeletal</th></tr></thead><tr><td align="center" valign="middle" >Thickness (cm)</td><td align="center" valign="middle" >LET (MeV/cm)</td><td align="center" valign="middle" >Absorbed Dose &#215; 10<sup>−</sup><sup>8</sup> (rad)</td><td align="center" valign="middle" >Equivalent Dose &#215; 10<sup>−</sup><sup>8</sup> (rem)</td><td align="center" valign="middle" >Effective Dose &#215; 10<sup>−</sup><sup>8</sup> (rem)</td><td align="center" valign="middle" >Thickness (cm)</td><td align="center" valign="middle" >LET (MeV/cm)</td><td align="center" valign="middle" >Absorbed Dose &#215; 10<sup>−</sup><sup>8</sup> (rad)</td><td align="center" valign="middle" >Equivalent Dose &#215; 10<sup>−</sup><sup>8</sup> (rem)</td><td align="center" valign="middle" >Effective Dose &#215; 10<sup>−</sup><sup>8</sup> (rem)</td></tr><tr><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >1.488 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >290.8147</td><td align="center" valign="middle" >0.064</td><td align="center" valign="middle" >0.320</td><td align="center" valign="middle" >0.034</td><td align="center" valign="middle" >1.441 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >294.298</td><td align="center" valign="middle" >0.064</td><td align="center" valign="middle" >0.320</td><td align="center" valign="middle" >0.034</td></tr><tr><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >2.691 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >733.2987</td><td align="center" valign="middle" >0.096</td><td align="center" valign="middle" >0.480</td><td align="center" valign="middle" >0.057</td><td align="center" valign="middle" >2.868 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >757.490</td><td align="center" valign="middle" >0.096</td><td align="center" valign="middle" >0.480</td><td align="center" valign="middle" >0.057</td></tr><tr><td align="center" valign="middle" >0.08</td><td align="center" valign="middle" >4.825 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >837.0064</td><td align="center" valign="middle" >0.128</td><td align="center" valign="middle" >0.640</td><td align="center" valign="middle" >0.076</td><td align="center" valign="middle" >4.671 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >866.787</td><td align="center" valign="middle" >0.128</td><td align="center" valign="middle" >0.640</td><td align="center" valign="middle" >0.076</td></tr><tr><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >7.046 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >847.7091</td><td align="center" valign="middle" >0.160</td><td align="center" valign="middle" >0.800</td><td align="center" valign="middle" >0.096</td><td align="center" valign="middle" >6.821 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >878.754</td><td align="center" valign="middle" >0.160</td><td align="center" valign="middle" >0.800</td><td align="center" valign="middle" >0.096</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >2.284 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >700.4432</td><td align="center" valign="middle" >0.320</td><td align="center" valign="middle" >1.600</td><td align="center" valign="middle" >0.192</td><td align="center" valign="middle" >2.210 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >727.179</td><td align="center" valign="middle" >0.320</td><td align="center" valign="middle" >1.600</td><td align="center" valign="middle" >0.192</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >7.407 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >488.4735</td><td align="center" valign="middle" >0.640</td><td align="center" valign="middle" >3.200</td><td align="center" valign="middle" >0.384</td><td align="center" valign="middle" >7.160 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >507.446</td><td align="center" valign="middle" >0.640</td><td align="center" valign="middle" >3.200</td><td align="center" valign="middle" >0.384</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.0015</td><td align="center" valign="middle" >379.5403</td><td align="center" valign="middle" >0.960</td><td align="center" valign="middle" >4.800</td><td align="center" valign="middle" >0.576</td><td align="center" valign="middle" >0.0014</td><td align="center" valign="middle" >394.373</td><td align="center" valign="middle" >0.960</td><td align="center" valign="middle" >4.800</td><td align="center" valign="middle" >0.576</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.0024</td><td align="center" valign="middle" >313.3203</td><td align="center" valign="middle" >1.280</td><td align="center" valign="middle" >6.400</td><td align="center" valign="middle" >0.768</td><td align="center" valign="middle" >0.0023</td><td align="center" valign="middle" >325.607</td><td align="center" valign="middle" >1.280</td><td align="center" valign="middle" >6.400</td><td align="center" valign="middle" >0.768</td></tr><tr><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0.0035</td><td align="center" valign="middle" >268.4361</td><td align="center" valign="middle" >1.600</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0.960</td><td align="center" valign="middle" >0.0034</td><td align="center" valign="middle" >278.986</td><td align="center" valign="middle" >1.600</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0.960</td></tr><tr><td align="center" valign="middle" >2.0</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >161.8006</td><td align="center" valign="middle" >3.200</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >1.920</td><td align="center" valign="middle" >0.0110</td><td align="center" valign="middle" >168.194</td><td align="center" valign="middle" >3.200</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >1.920</td></tr><tr><td align="center" valign="middle" >4.0</td><td align="center" valign="middle" >0.036</td><td align="center" valign="middle" >94.6491</td><td align="center" valign="middle" >6.400</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" >3.840</td><td align="center" valign="middle" >0.0356</td><td align="center" valign="middle" >98.403</td><td align="center" valign="middle" >6.400</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" >3.840</td></tr><tr><td align="center" valign="middle" >6.0</td><td align="center" valign="middle" >0.073</td><td align="center" valign="middle" >68.4376</td><td align="center" valign="middle" >9.600</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >5.760</td><td align="center" valign="middle" >0.0707</td><td align="center" valign="middle" >71.156</td><td align="center" valign="middle" >9.600</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >5.760</td></tr><tr><td align="center" valign="middle" >8.0</td><td align="center" valign="middle" >0.119</td><td align="center" valign="middle" >54.1565</td><td align="center" valign="middle" >12.800</td><td align="center" valign="middle" >64</td><td align="center" valign="middle" >7.680</td><td align="center" valign="middle" >0.1152</td><td align="center" valign="middle" >56.310</td><td align="center" valign="middle" >12.800</td><td align="center" valign="middle" >64</td><td align="center" valign="middle" >7.680</td></tr><tr><td align="center" valign="middle" >10.0</td><td align="center" valign="middle" >0.174</td><td align="center" valign="middle" >45.0727</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >9.600</td><td align="center" valign="middle" >0.1682</td><td align="center" valign="middle" >46.866</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >9.600</td></tr><tr><td align="center" valign="middle" >20.0</td><td align="center" valign="middle" >0.566</td><td align="center" valign="middle" >25.2182</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" >160</td><td align="center" valign="middle" >19.200</td><td align="center" valign="middle" >0.545</td><td align="center" valign="middle" >26.224</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" >160</td><td align="center" valign="middle" >19.200</td></tr><tr><td align="center" valign="middle" >30.0</td><td align="center" valign="middle" >1.126</td><td align="center" valign="middle" >17.8345</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >28.800</td><td align="center" valign="middle" >1.084</td><td align="center" valign="middle" >18.546</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >28.800</td></tr><tr><td align="center" valign="middle" >40.0</td><td align="center" valign="middle" >1.835</td><td align="center" valign="middle" >13.9076</td><td align="center" valign="middle" >64</td><td align="center" valign="middle" >320</td><td align="center" valign="middle" >38.400</td><td align="center" valign="middle" >1.765</td><td align="center" valign="middle" >14.463</td><td align="center" valign="middle" >64</td><td align="center" valign="middle" >320</td><td align="center" valign="middle" >38.400</td></tr><tr><td align="center" valign="middle" >50.0</td><td align="center" valign="middle" >2.680</td><td align="center" valign="middle" >11.4484</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >400</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >2.578</td><td align="center" valign="middle" >11.905</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >400</td><td align="center" valign="middle" >48</td></tr><tr><td align="center" valign="middle" >60.0</td><td align="center" valign="middle" >3.651</td><td align="center" valign="middle" >9.7547</td><td align="center" valign="middle" >96</td><td align="center" valign="middle" >480</td><td align="center" valign="middle" >57.600</td><td align="center" valign="middle" >3.512</td><td align="center" valign="middle" >10.144</td><td align="center" valign="middle" >96</td><td align="center" valign="middle" >480</td><td align="center" valign="middle" >57.600</td></tr><tr><td align="center" valign="middle" >70.0</td><td align="center" valign="middle" >4.743</td><td align="center" valign="middle" >8.5127</td><td align="center" valign="middle" >112</td><td align="center" valign="middle" >560</td><td align="center" valign="middle" >67.200</td><td align="center" valign="middle" >4.561</td><td align="center" valign="middle" >8.853</td><td align="center" valign="middle" >112</td><td align="center" valign="middle" >560</td><td align="center" valign="middle" >67.200</td></tr><tr><td align="center" valign="middle" >80.0</td><td align="center" valign="middle" >5.950</td><td align="center" valign="middle" >7.5606</td><td align="center" valign="middle" >128</td><td align="center" valign="middle" >640</td><td align="center" valign="middle" >76.800</td><td align="center" valign="middle" >5.721</td><td align="center" valign="middle" >7.863</td><td align="center" valign="middle" >128</td><td align="center" valign="middle" >640</td><td align="center" valign="middle" >76.800</td></tr><tr><td align="center" valign="middle" >90.0</td><td align="center" valign="middle" >7.266</td><td align="center" valign="middle" >6.8062</td><td align="center" valign="middle" >144</td><td align="center" valign="middle" >720</td><td align="center" valign="middle" >86.400</td><td align="center" valign="middle" >6.986</td><td align="center" valign="middle" >7.078</td><td align="center" valign="middle" >144</td><td align="center" valign="middle" >720</td><td align="center" valign="middle" >86.400</td></tr><tr><td align="center" valign="middle" >100.0</td><td align="center" valign="middle" >8.689</td><td align="center" valign="middle" >6.1927</td><td align="center" valign="middle" >160</td><td align="center" valign="middle" >800</td><td align="center" valign="middle" >96</td><td align="center" valign="middle" >8.353</td><td align="center" valign="middle" >6.440</td><td align="center" valign="middle" >160</td><td align="center" valign="middle" >800</td><td align="center" valign="middle" >96</td></tr><tr><td align="center" valign="middle" >110.0</td><td align="center" valign="middle" >10.214</td><td align="center" valign="middle" >5.6835</td><td align="center" valign="middle" >176</td><td align="center" valign="middle" >880</td><td align="center" valign="middle" >105.60</td><td align="center" valign="middle" >9.818</td><td align="center" valign="middle" >5.910</td><td align="center" valign="middle" >176</td><td align="center" valign="middle" >880</td><td align="center" valign="middle" >105.60</td></tr><tr><td align="center" valign="middle" >120.0</td><td align="center" valign="middle" >11.840</td><td align="center" valign="middle" >5.2536</td><td align="center" valign="middle" >192</td><td align="center" valign="middle" >960</td><td align="center" valign="middle" >115.20</td><td align="center" valign="middle" >11.380</td><td align="center" valign="middle" >5.463</td><td align="center" valign="middle" >192</td><td align="center" valign="middle" >960</td><td align="center" valign="middle" >115.20</td></tr><tr><td align="center" valign="middle" >130.0</td><td align="center" valign="middle" >13.562</td><td align="center" valign="middle" >4.8856</td><td align="center" valign="middle" >208</td><td align="center" valign="middle" >1040</td><td align="center" valign="middle" >124.80</td><td align="center" valign="middle" >13.034</td><td align="center" valign="middle" >5.081</td><td align="center" valign="middle" >208</td><td align="center" valign="middle" >1040</td><td align="center" valign="middle" >124.80</td></tr><tr><td align="center" valign="middle" >140.0</td><td align="center" valign="middle" >15.380</td><td align="center" valign="middle" >4.5667</td><td align="center" valign="middle" >224</td><td align="center" valign="middle" >1120</td><td align="center" valign="middle" >134.40</td><td align="center" valign="middle" >14.780</td><td align="center" valign="middle" >4.749</td><td align="center" valign="middle" >224</td><td align="center" valign="middle" >1120</td><td align="center" valign="middle" >134.40</td></tr><tr><td align="center" valign="middle" >150.0</td><td align="center" valign="middle" >17.290</td><td align="center" valign="middle" >4.2877</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >1200</td><td align="center" valign="middle" >144</td><td align="center" valign="middle" >16.615</td><td align="center" valign="middle" >4.459</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >1200</td><td align="center" valign="middle" >144</td></tr><tr><td align="center" valign="middle" >160.0</td><td align="center" valign="middle" >19.291</td><td align="center" valign="middle" >4.0413</td><td align="center" valign="middle" >256</td><td align="center" valign="middle" >1280</td><td align="center" valign="middle" >153.60</td><td align="center" valign="middle" >18.537</td><td align="center" valign="middle" >4.203</td><td align="center" valign="middle" >256</td><td align="center" valign="middle" >1280</td><td align="center" valign="middle" >153.60</td></tr><tr><td align="center" valign="middle" >170.0</td><td align="center" valign="middle" >21.382</td><td align="center" valign="middle" >3.8221</td><td align="center" valign="middle" >272</td><td align="center" valign="middle" >1360</td><td align="center" valign="middle" >163.20</td><td align="center" valign="middle" >20.544</td><td align="center" valign="middle" >3.975</td><td align="center" valign="middle" >272</td><td align="center" valign="middle" >1360</td><td align="center" valign="middle" >163.20</td></tr><tr><td align="center" valign="middle" >180.0</td><td align="center" valign="middle" >23.560</td><td align="center" valign="middle" >3.6257</td><td align="center" valign="middle" >288</td><td align="center" valign="middle" >1440</td><td align="center" valign="middle" >172.80</td><td align="center" valign="middle" >22.635</td><td align="center" valign="middle" >3.770</td><td align="center" valign="middle" >288</td><td align="center" valign="middle" >1440</td><td align="center" valign="middle" >172.80</td></tr><tr><td align="center" valign="middle" >190.0</td><td align="center" valign="middle" >25.824</td><td align="center" valign="middle" >3.4486</td><td align="center" valign="middle" >304</td><td align="center" valign="middle" >1520</td><td align="center" valign="middle" >182.40</td><td align="center" valign="middle" >24.809</td><td align="center" valign="middle" >3.586</td><td align="center" valign="middle" >304</td><td align="center" valign="middle" >1520</td><td align="center" valign="middle" >182.40</td></tr><tr><td align="center" valign="middle" >200.0</td><td align="center" valign="middle" >28.172</td><td align="center" valign="middle" >3.2882</td><td align="center" valign="middle" >320</td><td align="center" valign="middle" >1600</td><td align="center" valign="middle" >192</td><td align="center" valign="middle" >27.064</td><td align="center" valign="middle" >3.419</td><td align="center" valign="middle" >320</td><td align="center" valign="middle" >1600</td><td align="center" valign="middle" >192</td></tr></tbody></table></table-wrap><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> Thickness, LET, absorbed dose, equivalent dose and effective dose of proton in Bone, Cortical</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >E (MeV)</th><th align="center" valign="middle"  colspan="5"  >Bone, Cortical</th></tr></thead><tr><td align="center" valign="middle" >Thickness (cm)</td><td align="center" valign="middle" >LET (MeV/cm)</td><td align="center" valign="middle" >Absorbed Dose &#215; 10<sup>−</sup><sup>8</sup> (rad)</td><td align="center" valign="middle" >Equivalent Dose &#215; 10<sup>−</sup><sup>8</sup> (rem)</td><td align="center" valign="middle" >Effective Dose &#215; 10<sup>−</sup><sup>8</sup> (rem)</td></tr><tr><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >1.053 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >−898.921</td><td align="center" valign="middle" >0.064</td><td align="center" valign="middle" >0.320</td><td align="center" valign="middle" >0.034</td></tr><tr><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >2.078 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >352.447</td><td align="center" valign="middle" >0.096</td><td align="center" valign="middle" >0.480</td><td align="center" valign="middle" >0.057</td></tr><tr><td align="center" valign="middle" >0.08</td><td align="center" valign="middle" >3.367 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >770.761</td><td align="center" valign="middle" >0.128</td><td align="center" valign="middle" >0.640</td><td align="center" valign="middle" >0.076</td></tr><tr><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >4.896 &#215; 10<sup>−</sup><sup>5</sup></td><td align="center" valign="middle" >930.846</td><td align="center" valign="middle" >0.160</td><td align="center" valign="middle" >0.800</td><td align="center" valign="middle" >0.096</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.565 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >953.422</td><td align="center" valign="middle" >0.320</td><td align="center" valign="middle" >1.600</td><td align="center" valign="middle" >0.192</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >5.006 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >720.635</td><td align="center" valign="middle" >0.640</td><td align="center" valign="middle" >3.200</td><td align="center" valign="middle" >0.384</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >9.881 &#215; 10<sup>−</sup><sup>4</sup></td><td align="center" valign="middle" >575.506</td><td align="center" valign="middle" >0.960</td><td align="center" valign="middle" >4.800</td><td align="center" valign="middle" >0.576</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.0016</td><td align="center" valign="middle" >482.205</td><td align="center" valign="middle" >1.280</td><td align="center" valign="middle" >6.400</td><td align="center" valign="middle" >0.768</td></tr><tr><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0.0023</td><td align="center" valign="middle" >417.134</td><td align="center" valign="middle" >1.600</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0.960</td></tr><tr><td align="center" valign="middle" >2.0</td><td align="center" valign="middle" >0.0074</td><td align="center" valign="middle" >257.232</td><td align="center" valign="middle" >3.200</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >1.920</td></tr><tr><td align="center" valign="middle" >4.0</td><td align="center" valign="middle" >0.023</td><td align="center" valign="middle" >152.873</td><td align="center" valign="middle" >6.400</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" >3.840</td></tr><tr><td align="center" valign="middle" >6.0</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" >111.334</td><td align="center" valign="middle" >9.600</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >5.760</td></tr><tr><td align="center" valign="middle" >8.0</td><td align="center" valign="middle" >0.076</td><td align="center" valign="middle" >88.490</td><td align="center" valign="middle" >12.800</td><td align="center" valign="middle" >64</td><td align="center" valign="middle" >7.680</td></tr><tr><td align="center" valign="middle" >10.0</td><td align="center" valign="middle" >0.110</td><td align="center" valign="middle" >73.875</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >9.600</td></tr><tr><td align="center" valign="middle" >20.0</td><td align="center" valign="middle" >0.353</td><td align="center" valign="middle" >41.669</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" >160</td><td align="center" valign="middle" >19.200</td></tr><tr><td align="center" valign="middle" >30.0</td><td align="center" valign="middle" >0.698</td><td align="center" valign="middle" >29.583</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >28.800</td></tr><tr><td align="center" valign="middle" >40.0</td><td align="center" valign="middle" >1.131</td><td align="center" valign="middle" >23.125</td><td align="center" valign="middle" >64</td><td align="center" valign="middle" >320</td><td align="center" valign="middle" >38.400</td></tr><tr><td align="center" valign="middle" >50.0</td><td align="center" valign="middle" >1.644</td><td align="center" valign="middle" >19.069</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >400</td><td align="center" valign="middle" >48</td></tr><tr><td align="center" valign="middle" >60.0</td><td align="center" valign="middle" >2.232</td><td align="center" valign="middle" >16.269</td><td align="center" valign="middle" >96</td><td align="center" valign="middle" >480</td><td align="center" valign="middle" >57.600</td></tr><tr><td align="center" valign="middle" >70.0</td><td align="center" valign="middle" >2.891</td><td align="center" valign="middle" >14.212</td><td align="center" valign="middle" >112</td><td align="center" valign="middle" >560</td><td align="center" valign="middle" >67.200</td></tr><tr><td align="center" valign="middle" >80.0</td><td align="center" valign="middle" >3.616</td><td align="center" valign="middle" >12.633</td><td align="center" valign="middle" >128</td><td align="center" valign="middle" >640</td><td align="center" valign="middle" >76.800</td></tr><tr><td align="center" valign="middle" >90.0</td><td align="center" valign="middle" >4.406</td><td align="center" valign="middle" >11.380</td><td align="center" valign="middle" >144</td><td align="center" valign="middle" >720</td><td align="center" valign="middle" >86.400</td></tr><tr><td align="center" valign="middle" >100.0</td><td align="center" valign="middle" >5.258</td><td align="center" valign="middle" >10.361</td><td align="center" valign="middle" >160</td><td align="center" valign="middle" >800</td><td align="center" valign="middle" >96</td></tr><tr><td align="center" valign="middle" >110.0</td><td align="center" valign="middle" >6.169</td><td align="center" valign="middle" >9.514</td><td align="center" valign="middle" >176</td><td align="center" valign="middle" >880</td><td align="center" valign="middle" >105.60</td></tr><tr><td align="center" valign="middle" >120.0</td><td align="center" valign="middle" >7.138</td><td align="center" valign="middle" >8.798</td><td align="center" valign="middle" >192</td><td align="center" valign="middle" >960</td><td align="center" valign="middle" >115.20</td></tr><tr><td align="center" valign="middle" >130.0</td><td align="center" valign="middle" >8.164</td><td align="center" valign="middle" >8.185</td><td align="center" valign="middle" >208</td><td align="center" valign="middle" >1040</td><td align="center" valign="middle" >124.80</td></tr><tr><td align="center" valign="middle" >140.0</td><td align="center" valign="middle" >9.244</td><td align="center" valign="middle" >7.653</td><td align="center" valign="middle" >224</td><td align="center" valign="middle" >1120</td><td align="center" valign="middle" >134.40</td></tr><tr><td align="center" valign="middle" >150.0</td><td align="center" valign="middle" >10.378</td><td align="center" valign="middle" >7.188</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >1200</td><td align="center" valign="middle" >144</td></tr><tr><td align="center" valign="middle" >160.0</td><td align="center" valign="middle" >11.565</td><td align="center" valign="middle" >6.777</td><td align="center" valign="middle" >256</td><td align="center" valign="middle" >1280</td><td align="center" valign="middle" >153.60</td></tr><tr><td align="center" valign="middle" >170.0</td><td align="center" valign="middle" >12.802</td><td align="center" valign="middle" >6.411</td><td align="center" valign="middle" >272</td><td align="center" valign="middle" >1360</td><td align="center" valign="middle" >163.20</td></tr><tr><td align="center" valign="middle" >180.0</td><td align="center" valign="middle" >14.090</td><td align="center" valign="middle" >6.083</td><td align="center" valign="middle" >288</td><td align="center" valign="middle" >1440</td><td align="center" valign="middle" >172.80</td></tr><tr><td align="center" valign="middle" >190.0</td><td align="center" valign="middle" >15.428</td><td align="center" valign="middle" >5.787</td><td align="center" valign="middle" >304</td><td align="center" valign="middle" >1520</td><td align="center" valign="middle" >182.40</td></tr><tr><td align="center" valign="middle" >200.0</td><td align="center" valign="middle" >16.814</td><td align="center" valign="middle" >5.519</td><td align="center" valign="middle" >320</td><td align="center" valign="middle" >1600</td><td align="center" valign="middle" >192</td></tr></tbody></table></table-wrap><table-wrap id="table7" ><label><xref ref-type="table" rid="table7">Table 7</xref></label><caption><title> The empirical formulae for calculating mass stopping powers</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >the empirical formulae for calculating mass stopping powers</th><th align="center" valign="middle"  rowspan="3"  >Substances</th></tr></thead><tr><td align="center" valign="middle"  colspan="2"  >y = A 1 e x / t 1 + y ∘</td></tr><tr><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This work</td></tr><tr><td align="center" valign="middle" >A<sub>1</sub> = 5.60379 &#215; 10<sup>8</sup> t<sub>1</sub> = −0.03805, yₒ = 1.2486<sup> </sup> R<sup>2</sup> = 0.99998</td><td align="center" valign="middle" >A<sub>1</sub> = 7.13118 &#215; 10<sup>8</sup> t<sub>1</sub> = −0.03752, yₒ = 0.31402 R<sup>2</sup> = 0.99998</td><td align="center" valign="middle" >Water</td></tr><tr><td align="center" valign="middle" >A<sub>1</sub> = 5.2736 &#215; 10<sup>8</sup>, t<sub>1</sub> = −0.03784, yₒ = 1.08913<sup> </sup> R<sup>2</sup> = 0.99998</td><td align="center" valign="middle" >A<sub>1</sub> = 6.760 &#215; 10<sup>8</sup> t<sub>1</sub> = −0.03729, yₒ = 0.17554 R<sup>2</sup> = 0.99999</td><td align="center" valign="middle" >Muscle, Skeletal</td></tr><tr><td align="center" valign="middle" >A<sub>1</sub> = 2.99461 &#215; 10<sup>8</sup>, t<sub>1</sub> = −0.03638, yₒ = 0.71424<sup> </sup> R<sup>2</sup> = 1</td><td align="center" valign="middle" >A<sub>1</sub> = 3.12078 &#215; 10<sup>8</sup> t<sub>1</sub> = −0.03626, yₒ = −0.34842 R<sup>2</sup> = 1</td><td align="center" valign="middle" >Bone, Cortical</td></tr></tbody></table></table-wrap><table-wrap id="table8" ><label><xref ref-type="table" rid="table8">Table 8</xref></label><caption><title> The empirical formulae for calculating range</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >the empirical formulae for calculating Range</th><th align="center" valign="middle"  rowspan="3"  >Substances</th></tr></thead><tr><td align="center" valign="middle"  colspan="2"  >y = A 1 e x / t 1 + y ∘</td></tr><tr><td align="center" valign="middle" >PSTAR</td><td align="center" valign="middle" >This work</td></tr><tr><td align="center" valign="middle" >A<sub>1</sub> = 6.50318 &#215; 10<sup>−</sup><sup>15</sup> t<sub>1</sub> = 0.02013, yₒ = −0.05453 R<sup>2</sup> = 0.99988</td><td align="center" valign="middle" >A<sub>1</sub> = 2.33355 &#215; 10<sup>−</sup><sup>14</sup> t<sub>1</sub> = 0.02082, yₒ = −0.03587 R<sup>2</sup> = 0.9999</td><td align="center" valign="middle" >Water</td></tr><tr><td align="center" valign="middle" >A<sub>1</sub> = 5.65636 &#215; 10<sup>−</sup><sup>15</sup> t<sub>1</sub> = 0.01985, yₒ = −0.06137 R<sup>2</sup> = 0.99992</td><td align="center" valign="middle" >A<sub>1</sub> = 2.04888 &#215; 10<sup>−</sup><sup>14</sup> t<sub>1</sub> = 0.02053, yₒ = −0.03963 R<sup>2</sup> = 0.99996</td><td align="center" valign="middle" >Muscle, Skeletal</td></tr><tr><td align="center" valign="middle" >A<sub>1</sub> = 5.09688 &#215; 10<sup>−</sup><sup>15</sup> t<sub>1</sub> = 0.01844, yₒ = −0.04659 R<sup>2</sup> = 0.99988</td><td align="center" valign="middle" >A<sub>1</sub> = 2.054547 &#215; 10<sup>−</sup><sup>14</sup> t<sub>1</sub> = 0.01924, yₒ = −0.03062 R<sup>2</sup> = 99986</td><td align="center" valign="middle" >Bone, Cortical</td></tr></tbody></table></table-wrap><p>4) The empirical formulae suggested for mass stopping power are simple and accurate at proton energy (1 - 200 MeV) while the empirical formulae suggested for proton range give a good result compared to calculated values at proton energy (4 - 200 MeV).</p><p>5) Also in this study, some radiation quantities were calculated, such as linear energy transfer, adsorbed dose, and effective and equivalent dose that give good information to those interested in proton therapy.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors thank the Department of Physics, Qassim University, for their support and encouragement of this research.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Almutairi, A.S. and Osman, K.T. 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