Difference between revisions of "Molecular Dynamics Simulations Analysis Gaucher Disease"
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+ | Technical details can be found in our [[Gaucher_Task10_Protocol|protocol]]. |
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== A brief check of results == |
== A brief check of results == |
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+ | We briefly checked the length of the MD simulations via <tt>gmxcheck</tt>. Since we used the AGroS paramter <tt>-lengthMD 10</tt>, we expected the MD simulation to be 10 ns long. <tt>gmxcheck</tt> reported for each simulation 2001 frames and a time step of 5 ps per frame which amounts to the expected length of 2001*5ps=10ns. |
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− | We briefly checked the length of the MD simulations via gmxcheck: |
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− | <pre> |
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− | gmxcheck -f traj.xtc |
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− | </pre> |
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− | Since we used the AGroS paramter <tt>-lengthMD 10</tt>, we expected the MD simulation to be 10ns long. <tt>gmxcheck</tt> reported for each simulation 2001 frames and a time step of 5ps per frame which amounts to the expected length of 2001*5ps=10ns. |
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We further investigated the runtime of the MD simulation by looking at the log files. The simulation of the WT took approximately twice as long as the other two mutations since we used only 16 instead of 32 cores. Performing a MD simulation over 1s would take more than 100000 years if the same hardware were used than we did. |
We further investigated the runtime of the MD simulation by looking at the log files. The simulation of the WT took approximately twice as long as the other two mutations since we used only 16 instead of 32 cores. Performing a MD simulation over 1s would take more than 100000 years if the same hardware were used than we did. |
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== Visualization == |
== Visualization == |
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+ | For getting a first impression of the MD simulations, we visualized the structures stored in the trajectory files. A course grained animation of the three simulations with 29 frames is shown in <xr id="fig:viz"/>. Altogether, the animations indicate that all three simulations terminated successfully without sever structural changes. Based on the visual inspection, we could not detect any rearrangements which would suggest a malign effect of one of the mutations. However, the active site residue E235 and E340 might be more flexible in L470P compared to the wildtype. |
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|<figure id="fig:gif_L470P">[[File:L470P.gif|thumb|300px|<caption>L470P</caption>]]</figure> |
|<figure id="fig:gif_L470P">[[File:L470P.gif|thumb|300px|<caption>L470P</caption>]]</figure> |
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|<figure id="fig:gif_W209R">[[File:W209R.gif|thumb|300px|<caption>W209R</caption>]]</figure> |
|<figure id="fig:gif_W209R">[[File:W209R.gif|thumb|300px|<caption>W209R</caption>]]</figure> |
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− | <caption align=" |
+ | <caption align="below">Visualization of the MD simulations. Red: the active site residues E235 and E340; Blue: the mutated residue.</caption> |
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== Quality assurance == |
== Quality assurance == |
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+ | We checked the quality of the MD simulations regarding the convergence of the pressure, temperature, potential energy, and total energy. Strongly fluctuating thermodynamic parameters and insufficiently converging parameters might hint at problems during the MD simulations or a lacking equilibration. |
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+ | <xr fig="id:qual_pres"/> shows the development of the pressure along the MD simulations. In all three cases, the pressure fluctuates between -200 and 200 bar but the average pressure of 1 bar does not change. In contrast the the wildtype which exhibits a negative drift, the pressure slightly increases in case of L470P and W209R. |
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<caption align="bottom">Development of the pressure during the MD simulation. In brackets: average/total-drift.</caption> |
<caption align="bottom">Development of the pressure during the MD simulation. In brackets: average/total-drift.</caption> |
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+ | The temperature of 297.9 K remains constant and varies by only +/- 2 K (<xr id="fig:qual_temp"/>). |
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<caption align="bottom">Development of the temperature during the MD simulation. In brackets: average/total-drift.</caption> |
<caption align="bottom">Development of the temperature during the MD simulation. In brackets: average/total-drift.</caption> |
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+ | Both the potential energy and the total energy reduces at the beginning of the MD simulations. L470P shows the strongest shift towards the negative range, i.e. the stability of the structure increases most. |
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<caption align="bottom">Development of the total energy during the MD simulation. In brackets: average/total-drift.</caption> |
<caption align="bottom">Development of the total energy during the MD simulation. In brackets: average/total-drift.</caption> |
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+ | Self-interactions between periodic images are unphysical and might disturb the MD simulations. We therefore checked the minimal distance to adjacent cells by taking (a) only C-alpha atoms and (b) also side-chain atoms into account (<xr id="fig:mindist"/>). |
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+ | In all three simulations, the minimal distance slightly decreases but does not falls below the cut-off distance of 2 nm. If only C-alpha atoms are taking into account, the minimal distance is bout 0.5 nm higher compared to using all protein atoms. This corresponds to an average side-chain length of 5 A. For W209R, the minimal distance drops below 2 nm at 9180 ps but then increases again such that this event does not impact the MD simulation. |
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Revision as of 17:08, 23 July 2012
Technical details can be found in our protocol.
A brief check of results
We briefly checked the length of the MD simulations via gmxcheck. Since we used the AGroS paramter -lengthMD 10, we expected the MD simulation to be 10 ns long. gmxcheck reported for each simulation 2001 frames and a time step of 5 ps per frame which amounts to the expected length of 2001*5ps=10ns.
We further investigated the runtime of the MD simulation by looking at the log files. The simulation of the WT took approximately twice as long as the other two mutations since we used only 16 instead of 32 cores. Performing a MD simulation over 1s would take more than 100000 years if the same hardware were used than we did.
<figtable id="tab:runtime">
Name | Runtime | ns/day | years/1s | |
---|---|---|---|---|
WT | 16h25:59 | 14.605 | 187536 | |
L470P | 9h20:49 | 25.677 | 106699 | |
W209R | 9h18:47 | 25.770 | 106314 |
Runtime of the MD simulations and the estimated runtime for a simulation length of 1s. </figtable> The computation of the energy term Coul(T) + LJ [W3-W3] accounted for most (47%) of the floating point operations.
Visualization
For getting a first impression of the MD simulations, we visualized the structures stored in the trajectory files. A course grained animation of the three simulations with 29 frames is shown in <xr id="fig:viz"/>. Altogether, the animations indicate that all three simulations terminated successfully without sever structural changes. Based on the visual inspection, we could not detect any rearrangements which would suggest a malign effect of one of the mutations. However, the active site residue E235 and E340 might be more flexible in L470P compared to the wildtype.
</figure> </figure> </figure><figure id="fig:gif_wt"> |
<figure id="fig:gif_L470P"> |
<figure id="fig:gif_W209R"> |
Quality assurance
We checked the quality of the MD simulations regarding the convergence of the pressure, temperature, potential energy, and total energy. Strongly fluctuating thermodynamic parameters and insufficiently converging parameters might hint at problems during the MD simulations or a lacking equilibration.
<xr fig="id:qual_pres"/> shows the development of the pressure along the MD simulations. In all three cases, the pressure fluctuates between -200 and 200 bar but the average pressure of 1 bar does not change. In contrast the the wildtype which exhibits a negative drift, the pressure slightly increases in case of L470P and W209R.
</figure> </figure> </figure><figure id="fig:qual_pres_wt"> |
<figure id="fig:qual_pres_L470P"> |
<figure id="fig:qual_pres_W209R"> |
The temperature of 297.9 K remains constant and varies by only +/- 2 K (<xr id="fig:qual_temp"/>).
</figure> </figure> </figure><figure id="fig:qual_temp_wt"> |
<figure id="fig:qual_temp_L470P"> |
<figure id="fig:qual_temp_W209R"> |
Both the potential energy and the total energy reduces at the beginning of the MD simulations. L470P shows the strongest shift towards the negative range, i.e. the stability of the structure increases most.
</figure> </figure> </figure><figure id="fig:qual_pot_wt"> |
<figure id="fig:qual_pot_L470P"> |
<figure id="fig:qual_pot_W209R"> |
<figure id="fig:qual_tot_wt"> |
<figure id="fig:qual_tot_L470P"> |
<figure id="fig:qual_tot_W209R"> |
Self-interactions between periodic images are unphysical and might disturb the MD simulations. We therefore checked the minimal distance to adjacent cells by taking (a) only C-alpha atoms and (b) also side-chain atoms into account (<xr id="fig:mindist"/>).
In all three simulations, the minimal distance slightly decreases but does not falls below the cut-off distance of 2 nm. If only C-alpha atoms are taking into account, the minimal distance is bout 0.5 nm higher compared to using all protein atoms. This corresponds to an average side-chain length of 5 A. For W209R, the minimal distance drops below 2 nm at 9180 ps but then increases again such that this event does not impact the MD simulation.
</figure> </figure> </figure><figure id="fig:mindist_wt"> |
<figure id="fig:mindist_tot_L470P"> |
<figure id="fig:mindist_tot_W209R"> |
RMSF
</figure> </figure> </figure><figure id="fig:rsmf_wt"> |
<figure id="fig:rsmf_L470P"> |
<figure id="fig:rsmf_W209R"> |
<figure id="fig:rsmf_c_wt"> |
<figure id="fig:rsmf_c_L470P"> |
<figure id="fig:rsmf_c_W209R"> |
<figure id="fig:rsmf_p_wt"> |
<figure id="fig:rsmf_p_L470P"> |
<figure id="fig:rsmf_p_W209R"> |
<figure id="fig:rsmf_avg_wt"> |
<figure id="fig:rsmf_avg_L470P"> |
<figure id="fig:rsmf_avg_W209R"> |