Journal:JBSD:5
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<StructureSection load='' size='450' side='right' scene='Journal:JBSD:5/Cv/2' caption=''> | <StructureSection load='' size='450' side='right' scene='Journal:JBSD:5/Cv/2' caption=''> | ||
=== Influence of divalent magnesium ion on DNA: molecular dynamics simulation studies === | === Influence of divalent magnesium ion on DNA: molecular dynamics simulation studies === | ||
- | <big>Sanchita Mukherjee and Dhananjay Bhattacharyya</big><ref> | + | <big>Sanchita Mukherjee and Dhananjay Bhattacharyya</big><ref>doi 10.1080/07391102.2012.713780</ref> |
<hr/> | <hr/> | ||
<b>Molecular Tour</b><br> | <b>Molecular Tour</b><br> | ||
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In order to get the positions of the magnesium ion with respect to DNA throughout the simulation, an average structure of DNA has been calculated first and then the positions of the magnesium ions were mapped on the average structure following periodic boundary condition with appropriate box dimension at each time step. To get the flavor of most occupied positions of Mg<sup>2+</sup> in the entire box we divided the box into (2Å)<sup>3</sup> grids and calculated the frequency of the ion in each grid throughout the simulation time. The grids with high frequencies are taken to predict the most likely positions of Mg<sup>2+</sup>. This gives an opportunity to visualize the positions and restrictions of the ion movements with respect to the DNA. The highest frequency for the <scene name='Journal:JBSD:5/Cv/4'>decamer</scene> is seen in the minor groove with grid frequency equivalent to that of 3 ns, but this corresponds to the initial crystal structure position of the ion. When it moves out of the minor groove high frequency is seen in major groove also (~1 ns) with more grids in number in the vicinity of major groove. The coordinated Mg<sup>2+</sup> site corresponds to the highest frequency region around the <scene name='Journal:JBSD:5/Cv/5'>dodecamer</scene>. Both major and minor grooves of the dodecamer contain high frequency (equivalent to about 800 ps) points corresponding to the presence of Mg<sup>2+</sup>. It is worth noting that high frequency points are also larger in number for major groove due to availability of more space in the major groove. This implies diminished movement of bulky magnesium in narrow minor groove and more flexible movement in wider major groove and could reason straightaway the preference of major groove. | In order to get the positions of the magnesium ion with respect to DNA throughout the simulation, an average structure of DNA has been calculated first and then the positions of the magnesium ions were mapped on the average structure following periodic boundary condition with appropriate box dimension at each time step. To get the flavor of most occupied positions of Mg<sup>2+</sup> in the entire box we divided the box into (2Å)<sup>3</sup> grids and calculated the frequency of the ion in each grid throughout the simulation time. The grids with high frequencies are taken to predict the most likely positions of Mg<sup>2+</sup>. This gives an opportunity to visualize the positions and restrictions of the ion movements with respect to the DNA. The highest frequency for the <scene name='Journal:JBSD:5/Cv/4'>decamer</scene> is seen in the minor groove with grid frequency equivalent to that of 3 ns, but this corresponds to the initial crystal structure position of the ion. When it moves out of the minor groove high frequency is seen in major groove also (~1 ns) with more grids in number in the vicinity of major groove. The coordinated Mg<sup>2+</sup> site corresponds to the highest frequency region around the <scene name='Journal:JBSD:5/Cv/5'>dodecamer</scene>. Both major and minor grooves of the dodecamer contain high frequency (equivalent to about 800 ps) points corresponding to the presence of Mg<sup>2+</sup>. It is worth noting that high frequency points are also larger in number for major groove due to availability of more space in the major groove. This implies diminished movement of bulky magnesium in narrow minor groove and more flexible movement in wider major groove and could reason straightaway the preference of major groove. | ||
- | Occupancy is defined as the simulation time during which a counterion was within a specific cutoff distance from a DNA atom in case of hydrated ions. The occupancy values were calculated for all the surface atoms of DNA to detect the highly preferred sites for magnesium. We found phosphate oxygen of the 4th residue in decamer to have the maximum occupancy (corresponding to 2 ns). We could select 28 such atoms having significant occupancy values in case of the <scene name='Journal:JBSD:5/Cv/ | + | Occupancy is defined as the simulation time during which a counterion was within a specific cutoff distance from a DNA atom in case of hydrated ions. The occupancy values were calculated for all the surface atoms of DNA to detect the highly preferred sites for magnesium. We found phosphate oxygen of the 4th residue in decamer to have the maximum occupancy (corresponding to 2 ns). We could select 28 such atoms having significant occupancy values in case of the <scene name='Journal:JBSD:5/Cv/17'>decamer</scene>. It indicates that the phosphate oxygen atoms come in close contact maximally while some nitrogen (N7) and base oxygen also have significant occupancy. Few non-polar hydrogen atoms are also seen to make water mediated contacts with the hydrated Mg<sup>2+</sup> ions. Similar high occupancy in the <scene name='Journal:JBSD:5/Cv/16'>dodecamer</scene> is seen for O1P of the 9th residue. Quit a few N7 atoms, O4, O3’ and O2 are also found near Mg<sup>2+</sup> for significant durations. Guanine 2-amino group also was found close to the hexahydrates. |
</StructureSection> | </StructureSection> |
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- ↑ Mukherjee S, Bhattacharyya D. Influence of divalent magnesium ion on DNA: molecular dynamics simulation studies. J Biomol Struct Dyn. 2012 Sep 10. PMID:22963740 doi:10.1080/07391102.2012.713780
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