Journal:JBSD:5

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<b>Molecular Tour</b><br>
<b>Molecular Tour</b><br>
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The polyelectrolyte behavior is one of the most important physicochemical properties of DNA. This behavior is dependent on the interaction of counterions with DNA, which plays a crucial role in stabilizing the double helix. Two B-DNA crystal structures, namely PDB ID 1D49, d(CGATTAATCG) containing one crystallographic hexahydrated magnesium ion and PDB ID 436D, d(CGCGAATTCGCG) with five crystallographic magnesium ions, among which one is coordinated to a phosphate oxygen and rest of them hexahydrated, were obtained from PDB. These systems were then neutralized with required number of sodium ions solvated with water molecules. Molecular dynamics simulations are carried out for each of them for 100 ns to understand dynamics of DNA and especially the magnesium ions around the DNA. In [[384d]] the six <font color='red'><b>water oxygen atoms (in red)</b></font> near the <span style="color:lime;background-color:black;font-weight:bold;">Mg<sup>2+</sup> ions (colored in green)</span> <scene name='Journal:JBSD:5/Cv/3'>are of highly distorted geometry</scene>.
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The polyelectrolyte behavior is one of the most important physicochemical properties of DNA. This behavior is dependent on the interaction of counterions with DNA, which plays a crucial role in stabilizing the double helix. Two B-DNA crystal structures, namely PDB ID [[1d49]], d(CGATTAATCG) containing one crystallographic hexahydrated magnesium ion and PDB ID [[436d]], d(CGCGAATTCGCG) with five crystallographic magnesium ions, among which one is coordinated to a phosphate oxygen and rest of them hexahydrated, were obtained from PDB. These systems were then neutralized with required number of sodium ions solvated with water molecules. Molecular dynamics simulations are carried out for each of them for 100 ns to understand dynamics of DNA and especially the magnesium ions around the DNA. In [[384d]] the six <font color='red'><b>water oxygen atoms (in red)</b></font> near the <span style="color:lime;background-color:black;font-weight:bold;">Mg<sup>2+</sup> ions (colored in green)</span> <scene name='Journal:JBSD:5/Cv/3'>are of highly distorted geometry</scene>.
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.

Revision as of 10:50, 22 July 2012

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