<?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">JBPC</journal-id><journal-title-group><journal-title>Journal of Biophysical Chemistry</journal-title></journal-title-group><issn pub-type="epub">2153-036X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jbpc.2020.112002</article-id><article-id pub-id-type="publisher-id">JBPC-100407</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Water Molecules in Carbon 70, (H&lt;sub&gt;2&lt;/sub&gt;O)&lt;sub&gt;3&lt;/sub&gt;@C&lt;sub&gt;70&lt;/sub&gt;
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>M.</surname><given-names>Baskar</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>N.</surname><given-names>Sathyan</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Central Forensic Science Laboratory, Directorate of Forensic Science Services, Ministry of Home Affairs, Govt. of India, Bhopal, India</addr-line></aff><aff id="aff2"><addr-line>Humanity and Science Department, KG Reddy College of Engineering &amp;amp; Technology, Moinabad, Telangana, India</addr-line></aff><pub-date pub-type="epub"><day>22</day><month>05</month><year>2020</year></pub-date><volume>11</volume><issue>02</issue><fpage>15</fpage><lpage>25</lpage><history><date date-type="received"><day>21,</day>	<month>April</month>	<year>2020</year></date><date date-type="rev-recd"><day>22,</day>	<month>May</month>	<year>2020</year>	</date><date date-type="accepted"><day>25,</day>	<month>May</month>	<year>2020</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>
 
 
  Endohedral fullerene studies are the fascinating one, particularly with Car
  bon
   
  60 and Carbon 70. Water molecules inside fullerenes alter their cage structure
  , reorientations make them to play a lot in charge distribution. In this line we are presenting our work on Carbon 70 with three water molecules inside. Ab initio SCF<b> </b>calculations are carried out for the fullerene Carbon 70 and Carbon 70 with three water molecules. Carbon 70 is a rugby ball structure, when three water molecules are added inside it, dissociation of charges takes place. Unusual flip flop circular hydrogen bond formation takes place inside Carbon 70. The dipole moment of endohedral C<sub>70</sub> with three water molecules has been found to be 0.53 Debye, 0.49 Debye and 0.71 Debye respectively for STO-3G, 3-21G and 6-31G basis sets. Total energies for this molecule are reported in addition to the Hydrogen bond length and bond angles of the three water molecules trapped inside C<sub>70</sub>.
 
</p></abstract><kwd-group><kwd>Carbon 70</kwd><kwd> (H&lt;sub&gt;2&lt;/sub&gt;O)&lt;sub&gt;3&lt;/sub&gt;@C&lt;sub&gt;70&lt;/sub&gt;: Endohedral Fullerene</kwd><kwd> &lt;i&gt;Ab Initio&lt;/i&gt;</kwd><kwd> Self Consistent Field</kwd><kwd> Dipole Moment</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Theoretical predictions of buckyball molecules appeared in literature between 1960 and 1970. Carbon 70 was discovered in 1985 by Robert Curl, Harold Kroto and Richard Smalley using laser evaporation of graphite. They found C<sub>n</sub> clusters (n &gt; 20) of which the most common were C<sub>60</sub> and C<sub>70</sub>. For this discovery they have been awarded Nobel Prize in 1996. Carbon 70 molecule, which is one type of fullerene is a cage like fused ring structure, resembles like a rugby ball. C<sub>70</sub> is made by 25 hexagons and 12 pentagons. Endohedral fullerenes also called as endofullerenes are fullerenes that have additional atoms, ions, clusters enclosed within their inner spheres. First lanthanum C<sub>60</sub> complex was synthesized in 1985 and called as La@C<sub>60</sub> [<xref ref-type="bibr" rid="scirp.100407-ref1">1</xref>]. C<sub>60</sub> with one water molecule [<xref ref-type="bibr" rid="scirp.100407-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref4">4</xref>] and three water molecule [<xref ref-type="bibr" rid="scirp.100407-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref6">6</xref>] are reported. Also, C<sub>70</sub> with two water molecules [<xref ref-type="bibr" rid="scirp.100407-ref7">7</xref>] is also reported. In this work three water molecules that are included inside C<sub>70</sub> are reported and can be called as (H<sub>2</sub>O)<sub>3</sub>@C<sub>70</sub>. Calculations are carried out at SCF ab-initio STO-3G, 3-21G and 6-31G basis sets.</p></sec><sec id="s2"><title>2. Methods of Calculation</title><p>Computations of Self Consistent Field ab-initio calculations are carried out with STO-3G, 3-21G and 6-31G basis sets. Computations package, Firefly [<xref ref-type="bibr" rid="scirp.100407-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref9">9</xref>] and Avogadro [<xref ref-type="bibr" rid="scirp.100407-ref10">10</xref>] are used.</p></sec><sec id="s3"><title>3. Results</title><p>The structure of fullerene C<sub>70</sub> and the structure of Carbon 70 with three waters molecules inside are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> respectively. Optimized geometry calculations are carried out at SCF ab-initio STO-3G, 3-21G and 6-31G basis sets. Total energies of these molecules are given in <xref ref-type="table" rid="table1">Table 1</xref> in atomic units.</p><p>Optimized C<sub>70</sub> with 3 water molecules at 3-21G basis set is reported in the <xref ref-type="fig" rid="fig2">Figure 2</xref>. Cyclic hydrogen bonds involving flipping action inside Carbon 70 with 3 water molecules at 3-21G basis set with bond lengths and oxygen angles is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The bond length of one oxygen atom to the hydrogen atom of other water molecule and vice versa is 1.52 &#197;, 1.53 &#197; and 1.64 &#197; and the angle with respect to the oxygen of each water molecule is 57.55˚, 64.96˚ and 57.48˚ respectively.</p><p>Structure of C<sub>70</sub> with 3 H2O molecules optimised at 3-21G basis set</p><p>Cyclic water molecules having anchored and deflected with one hydrogen atom in each molecule, angles formed among water molecules after optimisation at 3-21G basis set are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>. The angles in respect of anchored and deflected hydrogen atom in each water molecule are 49.41˚, 79.65˚ and 50.93˚, 60.67˚, 61.88˚ and 57.46˚ respectively. The angle of water molecule is of 109.82˚, 105.69˚ and 107.15˚.</p><p>The optimized structure at 6-31G basis set of C<sub>70</sub> with 3 water molecules reported and the conformation of water molecules with hydrogen bonding in cyclic manner along with their bond lengths and oxygen bond angles are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, <xref ref-type="fig" rid="fig6">Figure 6</xref>(a) and <xref ref-type="fig" rid="fig6">Figure 6</xref>(b) respectively. The bond length of one oxygen atom to the hydrogen atom of other water molecule and vice versa is 1.63 &#197;, 1.63 &#197; and 1.70 &#197; and the angle with respect to the oxygen of each water molecule is 57.64˚, 65.85˚ and 56.51˚ respectively.</p><p>Structure of C<sub>70</sub> with 3 H2O molecules optimised at 6-31G basis set</p><p>Cyclic water molecules having anchored and deflected with one hydrogen atom in each molecule and the angles formed among water molecules after optimized at 6-31G basis set. The angles in respect of anchored and deflected hydrogen atom in each water molecule are 49.08˚, 85.29˚ and 45.63˚, 60.76˚, 61.24˚ &amp; 58.00˚ and the angle of water molecule is of 112.17˚, 107.37˚ and 109.48˚ respectively shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>(a) and <xref ref-type="fig" rid="fig7">Figure 7</xref>(b).</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Total energy of the molecules in atomic units (AU)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Molecules</th><th align="center" valign="middle" >STO-3G Basis Set</th><th align="center" valign="middle" >3-21 G Basis set</th><th align="center" valign="middle" >6-31 G Basis set</th></tr></thead><tr><td align="center" valign="middle" >CARBON 70</td><td align="center" valign="middle" >−2618.357389</td><td align="center" valign="middle" >−2843.170273</td><td align="center" valign="middle" >2649.574118</td></tr><tr><td align="center" valign="middle" >(H<sub>2</sub>O)<sub>3</sub>@C<sub>70</sub></td><td align="center" valign="middle" >−2635.636499</td><td align="center" valign="middle" >−2862.366387</td><td align="center" valign="middle" >−2877.425062</td></tr></tbody></table></table-wrap></sec><sec id="s4"><title>4. Discussion</title><p>The pentagons and hexagons of the rugby ball structure of fullerene C<sub>70</sub> as shown <xref ref-type="fig" rid="fig1">Figure 1</xref> are adopted to have the usual bond lengths and bond angles as reported experimentally. Due to the inclusion of water molecules as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>, C<sub>70</sub> structure is slightly modified and the formation of dipole moment is seen. Dipole moment has been found to be 0.53 Debye, 0.49 Debye and 0.71 Debye respectively for STO-3G, 3-21G and 6-31G basis sets. Dipole moment is the indication of conductivity and magnetism. Three water molecules inside C<sub>70</sub> interact with each other through hydrogen bonding. One hydrogen of the water molecule interact with Oxygen of other water molecule respectively through bonding in cyclic, which makes themselves as a cyclic water trimer. Water trimer exhibits ortho metastable configuration inside C<sub>70</sub>, rather para configuration when it is outside the rugby ball [<xref ref-type="bibr" rid="scirp.100407-ref11">11</xref>].</p><p>This study is in line with our previous work on circular and linear hydrogen bonds on molecules [<xref ref-type="bibr" rid="scirp.100407-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref15">15</xref>]. Fullerenes and Endohedral fullerenes will find a lot of applications in conductivity, magnetism, drug delivary, photovoltics and storing atoms and molecules. It seems to be finding applications in sensing, cosmetics and medicinal fields. This kind of studies will help to achieve the above applications.</p><p>3-21 G basis set Calculation on (H<sub>2</sub>O)<sub>3</sub>@C<sub>70</sub></p><p>One hydrogen atom of all the three water molecules (H-O-H) encapsulated in the endohedral fullerene is anchored with respect to H-O- in a triangle forming among themselves, as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a), in an angle H-H-H is 49.41˚, 79.65˚<sup> </sup>and 50.93˚ respectively which are altogether and considerably different from the same anchored angle of H-H-H in (H<sub>2</sub>O)<sub>3</sub>@C<sub>60</sub> [<xref ref-type="bibr" rid="scirp.100407-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref6">6</xref>] i.e. 61.89˚, 57.17˚ and 60.94˚. On the other hand, the other hydrogen atom is deflected in all the three water molecules with respect to -O-H and the angle between the deflected hydrogens is 60.67˚, 61.88˚ and 57.46˚ respectively, as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b), which are very little change similarities from the angle of H-H-H in (H<sub>2</sub>O)<sub>3</sub>@C<sub>60</sub> [<xref ref-type="bibr" rid="scirp.100407-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref6">6</xref>] i.e. 59.90˚, 60.26˚ and 59.84˚. The bond length between the deflected hydrogen atom of one water molecule and the oxygen of the second water molecule, deflected hydrogen of second water molecule and the oxygen of the third water molecule and deflected hydrogen of third water molecule and the oxygen of the first water molecule have been observed respectively as 1.52 &#197;, 1.53 &#197; and 1.64 &#197; as shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a). The ab-initio calculations of Fullerene C<sub>70</sub>, Water trimer and Water trimer encapsulated fullerene in three different levels of basis sets, STO-3G, 3-21G and 6-31G, using RHF have been taken place and their optimised and the total energy for stabilizing the molecules is presented as shown in the <xref ref-type="table" rid="table1">Table 1</xref>. Water molecules in the endohedral fullerene adopt an angle is 109.82˚, 105.69˚ and 107.15˚ and their bond length as defined in the <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) and <xref ref-type="table" rid="table2">Table 2</xref> respectively. The angles of each of the water molecules and their bond lengths are having little deviation from their corresponding experimental values for gas phase, O-H length is 0.95718 &#197; and the H-O-H angle is 104.474˚ [<xref ref-type="bibr" rid="scirp.100407-ref16">16</xref>] and liquid water, O-H length 0.991 &#197;, H-O-H angle 105.5˚ and 106.0˚ [<xref ref-type="bibr" rid="scirp.100407-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref18">18</xref>].</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Bond length (&#197;) and Bond angles (˚) of three water molecules in C<sub>70</sub> encapsulated, optimized at 3-21G basis set and 6-31G basis set</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  >3-21 G basis set</th><th align="center" valign="middle"  colspan="2"  >6-31 G basis set</th></tr></thead><tr><td align="center" valign="middle" >Water Molecule</td><td align="center" valign="middle" >Bond Angle in ˚/ Bond Length in &#197;</td><td align="center" valign="middle" >Water Molecule</td><td align="center" valign="middle" >Bond Angle in ˚/ Bond Length in &#197;</td></tr><tr><td align="center" valign="middle" >H<sub>11</sub> − O<sub>1</sub> − H<sub>12 </sub> <sub> </sub></td><td align="center" valign="middle" >109.82˚ 107.15 0.96 0.99</td><td align="center" valign="middle" >H<sub>11</sub> − O<sub>1</sub> − H<sub>12 </sub> <sub> </sub></td><td align="center" valign="middle" >112.17˚ 0.94 0.96</td></tr><tr><td align="center" valign="middle" >H<sub>21</sub> − O<sub>2</sub> − H<sub>22</sub></td><td align="center" valign="middle" >105.69˚ 0.99 0.96</td><td align="center" valign="middle" >H<sub>21</sub> − O<sub>2</sub> − H<sub>22</sub></td><td align="center" valign="middle" >107.37˚ 0.96 0.95</td></tr><tr><td align="center" valign="middle" >H<sub>31</sub> − O<sub>3</sub> − H<sub>33</sub></td><td align="center" valign="middle" >107.15˚ 0.96 0.99</td><td align="center" valign="middle" >H<sub>31</sub> − O<sub>3</sub> − H<sub>33</sub></td><td align="center" valign="middle" >109.48˚ 0.96 0.94</td></tr><tr><td align="center" valign="middle" >O<sub>1</sub> − O<sub>2</sub> − O<sub>3</sub></td><td align="center" valign="middle" >57.55˚ 2.53 2.36</td><td align="center" valign="middle" >O<sub>1</sub> − O<sub>2</sub> − O<sub>3</sub></td><td align="center" valign="middle" >57.64˚ 2.57 2.35</td></tr><tr><td align="center" valign="middle" >O<sub>2</sub> − O<sub>3</sub> − O<sub>1 </sub> O<sub>3</sub> − O<sub>1</sub></td><td align="center" valign="middle" >64.96˚ 2.53</td><td align="center" valign="middle" >O<sub>2</sub> − O<sub>3</sub> − O<sub>1 </sub> O<sub>3</sub> − O<sub>1</sub></td><td align="center" valign="middle" >65.852˚ 2.38</td></tr><tr><td align="center" valign="middle" >O<sub>3</sub> − O<sub>1</sub> − O<sub>2 </sub></td><td align="center" valign="middle" >57.48˚</td><td align="center" valign="middle" >O<sub>3</sub> − O<sub>1</sub> − O<sub>2 </sub></td><td align="center" valign="middle" >56.51˚</td></tr><tr><td align="center" valign="middle" >O<sub>1</sub> − H<sub>21</sub></td><td align="center" valign="middle" >1.64</td><td align="center" valign="middle" >O<sub>1</sub> − H<sub>21</sub></td><td align="center" valign="middle" >1.70</td></tr><tr><td align="center" valign="middle" >O<sub>2</sub> − H<sub>31</sub></td><td align="center" valign="middle" >1.52</td><td align="center" valign="middle" >O<sub>2</sub> − H<sub>31</sub></td><td align="center" valign="middle" >1.63</td></tr><tr><td align="center" valign="middle" >O<sub>3</sub> − H<sub>11</sub></td><td align="center" valign="middle" >1.53</td><td align="center" valign="middle" >O<sub>3</sub> − H<sub>11</sub></td><td align="center" valign="middle" >1.63</td></tr><tr><td align="center" valign="middle" >H<sub>12</sub> − H<sub>22</sub> − H<sub>33</sub> <sub>Anchored</sub></td><td align="center" valign="middle" >49.41˚ 2.55 2.50</td><td align="center" valign="middle" >H<sub>12</sub> − H<sub>22</sub> − H<sub>33</sub> <sub>Anchored</sub></td><td align="center" valign="middle" >49.08˚ 3.29 2.36</td></tr><tr><td align="center" valign="middle" >H<sub>22</sub> − H<sub>33</sub> − H<sub>12 </sub> <sub>Anchored</sub></td><td align="center" valign="middle" >79.65˚ 3.23</td><td align="center" valign="middle" >H<sub>22</sub> − H<sub>33</sub> − H<sub>12 </sub> <sub>Anchored</sub></td><td align="center" valign="middle" >85.29˚ 2.50</td></tr><tr><td align="center" valign="middle" >H<sub>33</sub> − H<sub>12</sub> − H<sub>22 </sub> <sub>Anchored </sub></td><td align="center" valign="middle" >50.93˚</td><td align="center" valign="middle" >H<sub>33</sub> − H<sub>12</sub> − H<sub>22 </sub> <sub>Anchored</sub></td><td align="center" valign="middle" >45.63˚</td></tr><tr><td align="center" valign="middle" >H<sub>12</sub> − H<sub>22</sub> − H<sub>33</sub> <sub>Deflected</sub></td><td align="center" valign="middle" >60.87 1.89 1.81</td><td align="center" valign="middle" >H<sub>12</sub> − H<sub>22</sub> − H<sub>33</sub> <sub>Deflected</sub></td><td align="center" valign="middle" >60.76˚ 1.97 1.91</td></tr><tr><td align="center" valign="middle" >H<sub>22</sub> − H<sub>33</sub> − H<sub>12 </sub> <sub>Deflected</sub></td><td align="center" valign="middle" >61.88 1.87</td><td align="center" valign="middle" >H<sub>22</sub> − H<sub>33</sub> − H<sub>12 </sub> <sub>Deflected</sub></td><td align="center" valign="middle" >61.24˚ 1.96</td></tr><tr><td align="center" valign="middle" >H<sub>33</sub> − H<sub>12</sub> − H<sub>22 </sub> <sub>Deflected</sub></td><td align="center" valign="middle" >57.46</td><td align="center" valign="middle" >H<sub>33</sub> − H<sub>12</sub> − H<sub>22 </sub> <sub>Deflected</sub></td><td align="center" valign="middle" >58.00˚</td></tr></tbody></table></table-wrap><p>All the three water molecules are stabilized by interacting with their hydrogens among themselves and also with carbons of fullerenes C<sub>70</sub>. Four hydrogens of two water molecules are interacting with six membered ring of C<sub>70</sub> and two hydrogens of one water molecule is interacting with five membered ring of the C<sub>70</sub> as shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>(a). The overall optimized fullerene C<sub>70</sub> structure is related to oval in shape and the diameter of the fullerene alongside of the oval is 8.25 &#197; and their minimum diameter other than the oval side is 6.98 &#197; as shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>(b). The spatial orientation of atoms (anchored hydrogens, deviated hydrogens and oxygens) in all the three water molecules within C<sub>70</sub> are altogether are in different planes and parallel to each other.</p><p>The hydrogen atoms and oxygen atoms of all the three water molecules are stabilized by maximally interacting with six membered rings of the fullerene molecule in range of the distance from 2.5 &#197; to 2.9 &#197;. Graphical representations of the molecule are referred by Visual Molecular Dynamics software Package [<xref ref-type="bibr" rid="scirp.100407-ref19">19</xref>].</p><p>6-31 G basis set Calculation (H<sub>2</sub>O)<sub>3</sub>@C<sub>70</sub></p><p>One hydrogen atom of all the three water molecules (H-O-H) encapsulated in the endohedral fullerene is anchored with respect to H-O- in a triangle among themselves in an angle H-H-H is 49.08, 85.29˚ and 45.63˚ respectively which are about 12.81˚, 28.12˚ and 15.31˚ differ from the same angle of H-H-H in (H<sub>2</sub>O)<sub>3</sub>@C<sub>60</sub> [<xref ref-type="bibr" rid="scirp.100407-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref6">6</xref>] as shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>(b). On the other hand, the other hydrogen atom is deflected in all the three water molecules with respect to -O-H and the angle between the deflected hydrogens is 60.76˚, 61.24˚ and 58.00˚ respectively which are very little change similarities, as shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>, from the angle of H-H-H in (H<sub>2</sub>O)<sub>3</sub>@C<sub>60</sub> [<xref ref-type="bibr" rid="scirp.100407-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref6">6</xref>]. The bond length between the deflected hydrogen atom of one water molecule and the oxygen of the second water molecule, deflected hydrogen of second water molecule and the oxygen of the third water molecule and deflected hydrogen of third water molecule and the oxygen of the first water molecule have been observed respectively as 1.63 &#197;, 1.63 &#197; and 1.70 &#197; respectively as shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>(a). The ab-initio calculations of Fullerene C<sub>70</sub>, Water trimer and Water trimer encapsulated fullerene in three different levels of basis sets, STO-3G, 3-21G and 6-31G, using RHF have been taken place and their optimized and the total energy for stabilizing the molecules is presented as shown in the <xref ref-type="table" rid="table1">Table 1</xref>. Water molecules in the endohedral fullerene adopt an angle is 112.17˚, 107.34˚ and 109.48˚ and their bond length as defined in <xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="table" rid="table2">Table 2</xref>. All the three water molecules are stabilized by interacting with their hydrogens among themselves and also with carbons of fullerenes C<sub>70</sub>. Four hydrogens of two water molecules are interacting with six membered ring of C<sub>70</sub> and two hydrogens of one water molecule is interacting with partially with both the five and six membered ring of the C<sub>70</sub> as shown in <xref ref-type="fig" rid="fig9">Figure 9</xref>(a). The overall optimized fullerene C<sub>70</sub> structure optimized at 631-G is also related to oval in shape and the maximum diameter of the fullerene alongside of the oval is 8.26 &#197; and their maximum diameter other than the oval side is 6.98 &#197; as shown in <xref ref-type="fig" rid="fig9">Figure 9</xref>(b). The spatial orientation of atoms (i.e. anchored hydrogen, deviated hydrogen and oxygen) in all the three water molecules within C<sub>70</sub> are altogether existing in different planes and parallel to each other.</p><p>Comparison of optimised C<sub>70</sub> with three water molecules at 3-21G and 6-31G basis sets</p><p>Comparing the endohedral fullerene (H<sub>2</sub>O)<sub>3</sub>@C<sub>70</sub> structure at 3-21G and 6-31G basis sets, it is found that having maximum similarities. In contrary the water molecules adopts their position among themselves are meagerly deflective through their oxygen and hydrogen bonds as show in <xref ref-type="fig" rid="fig1">Figure 1</xref>0 &amp; <xref ref-type="fig" rid="fig1">Figure 1</xref>1. There is also a dissimilarity of their bond lengths. The orientations of the water molecules encapsulated in C<sub>60</sub> [<xref ref-type="bibr" rid="scirp.100407-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref6">6</xref>] with comparison of the water molecules encapsulated in C<sub>70</sub> optimized both at 3-21G and 6-31G basis sets are considerably different in their various angles and bond lengths as discussed. The hydrogen and oxygen bond deviations in respect of the water molecules optimized at 3-21G and 6-31G basis set is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>0 &amp; <xref ref-type="fig" rid="fig1">Figure 1</xref>1.</p><p>The spacial orientation of atoms (i.e. anchored hydrogen, deviated hydrogen and oxygen) in all the three water molecules within C<sub>70</sub> level are altogether existing in different planes and parallel to each other separately but high probable similarities could be observed among the water molecules at 3-21 G and 6-31 G by measuring the differences as detailed in <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>The length of deviations among bond lengths and angles of all the three water molecules in C<sub>70</sub> is as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>2 and in <xref ref-type="table" rid="table3">Table 3</xref>.</p></sec><sec id="s5"><title>5. Conclusion</title><p>SCF ab initio Calculations on fullerenes C<sub>70</sub> and endohedral fullerene (H<sub>2</sub>O)<sub>3</sub>@ C<sub>70</sub> shows a promising beginning to find out the structural reorientation in equilibrium geometries. Spacial orientations of atoms in water molecules within C<sub>70</sub> show three different planes. Charges need refinements. This result is in line with our previous ab-initio calculation with (H<sub>2</sub>O)<sub>3</sub>@C<sub>60</sub>. The study on seven endofullerene, M@C<sub>60</sub>), Where M = H2O, Li+, Na+, K+, Be2+, Mg2+, and Ca2+ were also reported [<xref ref-type="bibr" rid="scirp.100407-ref20">20</xref>] and concluded that all of the endofullerenes are more stable than pure C60. Coupled translational and rotational motions of H2 molecules in C<sub>70</sub> and C60 has been reported [<xref ref-type="bibr" rid="scirp.100407-ref21">21</xref>] with the predictions that at most two H2 molecules can stably occupy C<sub>70</sub> and just one can be accommodated by C<sub>60 </sub>which are</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Length of deviations in bond length and bond angles of trimer water molecules in C<sub>70</sub> encapsulated at 3-21G and 6-31G basis set</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Water Molecule</th><th align="center" valign="middle"  colspan="2"  >H−H</th><th align="center" valign="middle"  rowspan="2"  >O−O</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >0.10</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.15</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.15</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.92</td></tr></tbody></table></table-wrap><p>in accord with the experimental preparation of (H<sub>2</sub>)n@C<sub>70</sub> (n) 1, 2) 4 and H<sub>2</sub>@C<sub>60</sub> [<xref ref-type="bibr" rid="scirp.100407-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.100407-ref23">23</xref>]. At the same Experimental value of dipole moment of one water encapsulated fullerene also supports this kind of work, but a lot of experimental work should be carried out for further endeavours. This kind of studies will help endohedral fullerenes to achieve the applications in the field of sensors, super conductivity, medicine, magnetism, storing, photovoltic and drug delivery, etc.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors are acknowledging the support rendered by 1) Central Forensic Science Laboratory, Bharkheda Bondar, Bairagarh Kalan, Bhopal-462030, Madhya Pradesh, India and 2) Humanity &amp; Science Department, KG Reddy College of Engineering &amp; Technology, Moinabad-501504, Telangana, India.</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Baskar, M. and Sathyan, N. (2020) Water Molecules in Carbon 70, (H<sub>2</sub>O)<sub>3</sub>@C<sub>70</sub>. Journal of Biophysical Chemistry, 11, 15-25. https://doi.org/10.4236/jbpc.2020.112002</p></sec></body><back><ref-list><title>References</title><ref id="scirp.100407-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Chai, Y., Guo, T., Jin, C.M., et al. (1991) Fullerenes with Metal Inside. Journal of Physical Chemistry, 95, 7564-7568. https://doi.org/10.1021/j100173a002</mixed-citation></ref><ref id="scirp.100407-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Benno, M., Mamone, S. and Levitt, M.H. (2015) Electrical Detection of Ortho-Para Conversion in Fullerene-Encapsulated Water. Nature Communications, 6, Article No. 8112. https://doi.org/10.1038/ncomms9112</mixed-citation></ref><ref id="scirp.100407-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Kurotobi, K. and Murata, Y. (2003) A Single Molecule of Water Encapsulated in Fullerene C6060. Science, 333, 613. https://doi.org/10.1126/science.1206376</mixed-citation></ref><ref id="scirp.100407-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Xu, B.X. and Chen, X. (2013) Electrical-Driven Transport of Endohedral Fullerene Encapsulating a Single Water Molecule. Physical Review Letters, 110, Article ID: 156103. https://doi.org/10.1103/PhysRevLett.110.156103</mixed-citation></ref><ref id="scirp.100407-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Baskar, M., Sathyan, N. and Nair, T. (2018) Water Molecules in the Carbon C60 Confined Space. Journal of Biophysical Chemistry, 9, 15-21.  
https://www.scirp.org/journal/paperabs.aspx?paperid=88249  
https://doi.org/10.4236/jbpc.2018.92002</mixed-citation></ref><ref id="scirp.100407-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Baskar, M. and Sathyan, N. (2018) Water Molecules in the Carbon Confined Space (H2O)3@C60. Nanomedicine and Nanotechnology, 4, Article ID: 000158.</mixed-citation></ref><ref id="scirp.100407-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Zhang, R., Murata, M., Aharen, T., Wakamiya, A., Shimoaka, T., Hasegawa, T. and Murata, Y. (2016) Synthesis of a Distinct Water Dimer inside Fullerene C70. Nature Chemistry, 8, 435-441. https://doi.org/10.1038/nchem.2464</mixed-citation></ref><ref id="scirp.100407-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Granovsk, A.A. Firefly Version 8.2.0. 
http://classic.chem.msu.su/gran/firefly/index.html</mixed-citation></ref><ref id="scirp.100407-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Schmidt, M.W., Baldridge, K.K., Boatz, J.A., Elbert, S.T., Gordon, M.S., Jenson, J.H., Koseky, S., Matsunaja, N., Nguyen, K.A., Su, S., Wimdus, T.L., Dupvis, M. and Montgomery, J.A. (1993) General Atomic and Molecular Electronic Structure System. Journal of Computational Chemistry, 14, 1347-1363.  
https://doi.org/10.1002/jcc.540141112</mixed-citation></ref><ref id="scirp.100407-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Hanwell, M.D., Curtis, D.E., Lonie, D.C., et al. (2012) Avogadro: An Advanced Semantic Chemical Editor, Visualization, and Analysis Platform. Journal of Cheminformatics, 4, 17. https://doi.org/10.1186/1758-2946-4-17</mixed-citation></ref><ref id="scirp.100407-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Xantheas, S.S. and Dunning Jr., T.H. (1993) The Structure of the Water Trimer from ab Initio Calculations. The Journal of Chemical Physics, 98, 8037.  
https://doi.org/10.1063/1.464558</mixed-citation></ref><ref id="scirp.100407-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Sathyan, N., Santhanam, V. and Sobhanadri, J. (1995) Ab Initio Calculations on Some Binary Systems Involving Hydrogen Bonds. Journal of Molecular Structure: THEOCHEM, 333, 179-189. https://doi.org/10.1016/0166-1280(94)03931-A</mixed-citation></ref><ref id="scirp.100407-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Sathyan, N., Santhanam, V., Madhurima, V. and Sobhanadri, J. (1995) Conformational Study on the Binary Mixture Acetone-Methanol Involving H-Bonding. Journal of Molecular Structure THEOCHEM, 342, 187-192.  
https://doi.org/10.1016/0166-1280(95)90115-9</mixed-citation></ref><ref id="scirp.100407-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Madhurima, V., Sathyan, N., Murthy, V.R.K. and Sobhanadri, J. (1998) Dielectric and Conformational Studies of Hydrogen Bonded Acetone and Acetonitrile System. Spectrochimica Acta Part A, 54, 299-304.  
https://doi.org/10.1016/S1386-1425(97)00235-7</mixed-citation></ref><ref id="scirp.100407-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Sathyan, N., Santhanam, V. and Sobhanadri, J. (1996) Conformational Analysis of N-Chloromethylenimine and Its Hydrogen-Bonded Dimers with Water from the Study of Nuclear Quadrupole Interactions. Zeitschrift für Naturforschung A, 51, 534-536. https://doi.org/10.1515/zna-1996-5-628</mixed-citation></ref><ref id="scirp.100407-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Isaacs, E.D., Shukla, A., Platzman, P.M., Hamann, D.R., Barbiellini, B., et al. (2000) Compton Scattering Evidence for Covalency of the Hydrogen Bond in Ice. Journal of Physics and Chemistry of Solids, 61, 403-406.  
https://doi.org/10.1016/S0022-3697(99)00325-X</mixed-citation></ref><ref id="scirp.100407-ref17"><label>17</label><mixed-citation publication-type="book" xlink:type="simple">Hasted, J.B. (1972) Liquid Water: Dielectric Properties. In: Franks, F., Ed., Water, a Comprehensive Treatise: The Physics and Physical Chemistry of Water, Vol. 1, Springer, Boston, 255-309. https://doi.org/10.1007/978-1-4684-8334-5_7</mixed-citation></ref><ref id="scirp.100407-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Ichikawa, K., Kamed, Y., Yamaguchi, T., Wakita, H. and Misawa, M. (1991) Neutron-Diffraction Investigation of the Intermolecular Structure of a Water Molecule in the Liquid Phase at High Temperatures. Molecular Physics, 73, 79-86.  
https://doi.org/10.1080/00268979100101071</mixed-citation></ref><ref id="scirp.100407-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Humphrey, W., Dalke, A. and Schulten, K. (1996) VMD: Visual Molecular Dynamics. Journal of Molecular Graphics, 14, 33-38.  
https://doi.org/10.1016/0263-7855(96)00018-5</mixed-citation></ref><ref id="scirp.100407-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">de Oliveira, O.V. and da Silva Gon&amp;#231alves, A. (2014) Quantum Chemical Studies of Endofullerenes (M@C60) Where M = H2O, Li+, Na+, K+, Be2+, Mg2+, and Ca2+. Computational Chemistry, 2, 51-58. https://doi.org/10.4236/cc.2014.24007</mixed-citation></ref><ref id="scirp.100407-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Sebastianelli, F., Xu, M.Z., Bacic, Z., Lawler, R. and Turro, N.J. (2010) Hydrogen Molecules inside Fullerene C70: Quantum Dynamics, Energetics, Maximum Occupancy, and Comparison with C60. Journal of the American Chemical Society, 132, 9826-9832. https://doi.org/10.1021/ja103062g</mixed-citation></ref><ref id="scirp.100407-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Komatsu, K., Murata, M. and Murata, Y. (2005) Encapsulation of Molecular Hydrogen in Fullerene C60 by Organic Synthesis. Science, 307, 238-240.  
https://doi.org/10.1126/science.1106185</mixed-citation></ref><ref id="scirp.100407-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Murata, M., Murata, Y. and Komatsu, K. (2006) Synthesis and Properties of Endohedral C60 Encapsulating Molecular Hydrogen. Journal of the American Chemical Society, 128, 8024-8033. https://doi.org/10.1021/ja061857k</mixed-citation></ref></ref-list></back></article>