Molecular Dynamics Simulations Analysis Hemochromatosis
Hemochromatosis>>Task 10: Molecular dynamics simulations analysis
Contents
- 1 Short task description
- 2 Protocol
- 3 Molecular dynamics simulations for HFE
- 3.1 Calculation statistics
- 3.2 Trajectory visualization
- 3.3 Energies
- 3.4 Minimum distance between periodic boundary cells
- 3.5 RMSF for protein and C-alpha
- 3.6 Pymol analysis of average and bfactor
- 3.7 Radius of gyration
- 3.8 solvent accessible surface area
- 3.9 hydrogen-bonds between protein and protein / protein and water
- 3.10 Ramachandran plots
- 3.11 RMSD matrix
- 3.12 Internal RMSD
- 4 Conclusion
- 5 References
Short task description
Detailed description: Molecular dynamics simulations analysis
Protocol
A protocol with a description of the data acquisition and other scripts used for this task is available here.
Molecular dynamics simulations for HFE
Note: All pictures/graphs shown here are from the first run (in case of 1a6zC[wildtype]-pictures) or second run (in case of R224W- or C282S-mutation). The reason for this is described under LINKTOMINDISTTODO.
Calculation statistics
<figtable id="tab:simulation_stats"> Statistics of the MD simulations
| Input | Calc. time | Calc. speed | time to reach 1 s |
|---|---|---|---|
| Wildtype | 13h31:15 | 17.750 ns/day | 154350,8 years |
| C282S | 13h35:05 | 17.667 ns/day | 155075,9 years |
| R224W | 13h35:02 | 17.668 ns/day | 155067,1 years |
</figtable>
GMXcheck revealed for all calculations that all 2001 frames were calculated, resulting in a 10ns model.
Trajectory visualization
<figtable id="tab:traj_vis">
</figtable>
<xr id="tab:traj_vis"/> shows the trajectories for the three MD simulations (WT, R224W, and C282S). The wildtype and R224W mostly maintain the starting structure, though some bigger parts are shifted as a whole. In both cases the upper and lower helices of the MHC I domain seem to move closer together and the M1 domain (right part in the figure) shifts around, but retains its general structure. The trajectory for C282S exhibits much less movement as the previous two which are quite flexible. Towards the end of the simulation there is a deformation of the M1 domain which is most likely caused by the missing disulfide bond due to the mutation. This deformation presumably prevents the later (but crucial) binding of beta-2-microglobulin to HFE.
Energies
Pressure
<figtable id="tab:pressure">
</figtable>
The plots in <xr id="tab:pressure"/> show the pressures of the calculated systems over time. These show that, although the pressures differ greatly in some cases, the average is still at about 0 (with minor fluctuations).
Temperature
<figtable id="tab:temperature">
</figtable>
The next thing we calculated were the temperatures. For all three models they can be seen in <xr id="tab:temperature"/>. The maximal deviation from the average is about 4 degrees for all models.
Potential
<figtable id="tab:potential">
</figtable>
With gromacs we could also extract the potentials, as can be seen in <xr id="tab:potential"/>. As in the plots before the average fluctuates around the same value for all three models themselves. However, these points differ slightly:
The average potential of the wildtype and the C282S mutation tend to be around the same (~-9.195e+05) whereas the R224W mutation potential is slightly higher (~-9.19e+05).
Total energy
<figtable id="tab:total_energy">
</figtable>
In <xr id="tab:total_energy"/> the values of the total energies are denoted over the different states in time. Again we get an average with minor fluctuation at around the same value for each model.
All these plots show the same behavior with one exception: average around the same value and look different between the three models. This can be expected as minor changes can introduce or eradicate bindings, therefore changing the overall energies which then influence all further steps. The exception is the potential of the R224W mutation which is slightly higher than the other two models' potentials.
Minimum distance between periodic boundary cells
<figtable id="comparison">
</figtable>
The first calculations for the mutations resulted in the minimum distances of TABLETODO. As there should be at least 2 nm distance in between at all time one can see that the mutations show the opposite. Therefore it might be possible that the protein affects itself which is not desired. To see if this states were calculated just by chance (random fluctuations that built up over time into an undesired direction) we repeated the calculations for all three models.
<figtable id="comparison">
</figtable>
The resulting minimal distances can be seen in TABLETODO. We therefore decided to use the model of the first calculation for the wildtype, and the models of the second calculation for the mutation types.
RMSF for protein and C-alpha
Protein based
<figtable id="tab:rmsf_prot">
</figtable>
In general the RMS fluctuations of all three models look similar. The most differing graph is the one of R224W which shows a major peak at residues 220-235 as well as only a small peak at around residue 20.
C-Alpha based
<figtable id="tab:rmsf_ca">
</figtable>
The c-alpha based RMSF shows the same behavior as the whole-protein-based ones: the major differences are at around residue 20 and 220-235 of the R224W mutation.
Statistical values
With the GIVENSCRIPTTODO we calculated the values for the t-Test:
1a6zC to R224W : 8.079405e-57**
1a6zC to C282S : 2.87453e-56**
R224W to C282S : 5.45069e-25**
Pymol analysis of average and bfactor
<figtable id="tab:avg_bfactor">
</figtable>
In these part we evaluate the model averages and b-factors of each position. Because it is an average over all timesteps this averaged structure can be impossible in nature.
As one can see there is a big change of b-factors when comparing the wildtype and both mutations we calculated. From both mutations the R224W one shows a bigger difference to the wildtype. As expected the positions "at the edges" and those not in a secondary structure tend to have higher fluctuations/higher b-factors. It is worth noting, that even the beta sheets on the right side of the R224W picture (position 180 and higher) have (compared to wildtype and C282S mutation) pretty high b-factors. Also one can see that a little helix is inserted into the average structure of the R224W average model (right part of the picture, high b-factor [red], position ~220-225).
Radius of gyration
<figtable id="tab:gyration_ca">
</figtable>
<figtable id="tab:gyration_prot">
</figtable>
These graphs show the radii of gyration in general als well as in each dimension. From start to end there is a slight increase in general gyrationradius for all models. However the fluctuation of the radius is the weakest for the wildtype and the C282S mutation. There seem to be most fluctuation in the R224W model. Also the R224W mutation has in general the highes radius of gyration.
Another striking difference between the models is the low radius of gyration in the Z dimension for the mutations, whereas this type of gyration is in the wildtype only low for the first ~3000ps. In exchange both mutations gain more radius of gyration in the Y dimension compared to the wildtype.
solvent accessible surface area
<figtable id="tab:sas">
</figtable>
The preceding graphs show the Solvent accessible surface. As the hydrophilic, total and D Gsolv values are very similar we will just talk about the hydrophobic values.
The most similar ones between those three are the wildtype and the R224W mutation which differ only in the strength of the fluctuation, of which the mutation has the higher one. Both fluctuate around about the same value.
The less similar one is the C282S hydrophobic curve. It shows about the same fluctuation strength as the wildtype but in general a decrease towards the end can be seen. Therefore this might be an indicator, that the hydrophobic residues turn to the inside, but we cant be sure as there is no increase in the other values.
<figtable id="tab:sas_res">
</figtable>
In the area per residue averaged over the trajectory no clear difference can be seen.
hydrogen-bonds between protein and protein / protein and water
Protein-Protein
<figtable id="tab:hbonds_pp">
</figtable>
The calculations show that in each of the three cases the number of bonds within the protein as well as their distances tend to stay the same.
Protein-Water
<figtable id="tab:hbonds_pw">
</figtable>
Although the inner-protein bonds seem to stay the same (see PREVIOUSSECTIONTODO), the bonds formed with hydrogen show a different behavior.
In case of the wildtype, both the number of hydrogen bonds as well as the number of pairs within 0.35nm are (compared to the rest) fairly low at first, rising in the first ~600ps. This may be an indication that at first a dense protein state is existent. Also from ~8000-8600ps there is a drop in the number of hydrogen bonds, whereas the number of pairs within 0.35nm does not show an equal behavior. Overall the numbers tend to be at the same level each after the first 600ps rise.
The R224W model shows a different behavior over time:
The first steps show a similar "both numbers low and rising till 600ps" behavior. But instead of having a fluctuation around one constant value there seems to be a slight decrease over time as well as bigger fluctuations. This affects both, the number of bonds as well as pairs within 0.35nm.
The calculated model of the C282S mutation shows a different behavior at start than both preceding described, but a similar behavior to the R224W mutation:
For the number of hydrogen bonds there are very high fluctuations at the first 1000ps (rising till 100ps, drop to 300ps, rise till 1000ps) with a slight overall decrease afterwards like for the R224W mutation. The number of pairs within 0.35nm seem to show a similar behavior, however because of the fluctuations this is not very clear.
Ramachandran plots
<figtable id="tab:ramachandran">
</figtable>
The ramachandran plots (cf. <xr id="tab:ramachandran"/>) seem to follow the rules for the allowed and forbidden regions with a few exceptions. What is noticable though is that all of the allowed regions are almost filled to the maximum (i.e. no trend towards certain regions). Another difference are the regions above and below the left-handed alpha helix area (Psi: 110 to 180 and -180 to -150; Phi: 50 to 80) which are missing in the R224W mutation and almost non-existant in the C282S mutation. Though these areas have no significant structural element associated with them. Apart from that the plots appear almost the same, although they are hard to analyse as the dots are spread over a wide area and not clustered within distinct regions.
RMSD matrix
<figtable id="tab:rmsd_matrix_prot">
</figtable>
<figtable id="tab:rmsd_matrix_mcb">
</figtable>
The RMSD matrices for the whole protein (cf. <xr id="tab:rmsd_matrix_prot"/>) and the mainchain and C-beta atoms (cf. <xr id="tab:rmsd_matrix_mcb"/>) are almost identical. The C-beta matrices have slighty lower RMSD values which is not surprising as only a subset of the atoms is taken into consideration. The small difference between the two matrix groups suggests that most of the structural changes are based on backbone rearrangements and not on orientational changes (rotations) of the residues.
The wildtype seems to periodically change between conformations as the RMSD goes up (green-yellow) and down (light blue) along the x-axis (time) for most of the different structural states (y-axis). The only noticable changes are in the at the beginning as the structure that is present in the first 1000ps seems to be quickly discarded (highest RMSD with the other states). Overall the changes are minor as the maximum RMSD is about 0.65 which is still considered quite low.
The R224W mutations appears to be very stable in the beginning, but has two structural changes towards the end. A moderate one between 6500-8000ps and a strong one between 9500-10000ps. For the rest of the time it has even less structural fluctuations than the wildtype.
The RMSD fluctuations for C282S exhibit an opposite behavior to R224W. There is a major structural change at 2000ps and some minor changes up to 3000ps. After 3000ps the structure remains almost the same until the end of the simulation. As the mutation is malign it can be assumed that it is a non-functional structure in which the proteins seems to be trapped.
Internal RMSD
<figtable id="tab:rmsd_vs_start">
</figtable>
<figtable id="tab:rmsd_vs_avg">
</figtable>
<xr id="tab:rmsd_vs_start"/> and <xr id="tab:rmsd_vs_avg"/> show the RMSD values for the different structural states compared to the starting and average structure respectively.
The first (against starting structure) in particular reflects what could already be seen in the RMSD matrix section. The wildtype quickly assumes what seems to be its average structure and then periodically fluctuates around it. R224W slowly deviates from the starting structure until 6500ps where it has a moderate structural change and a strong one later at around 9500ps. C282S has a strong deviation at 2000ps and then remains quite stable till the end.
When compared to the average structure the wildtype reaches its favored conformation at around 2000ps. There are some peaks around 4300ps, 5100ps, 7900ps, and 9100ps, but the RMSD alsways goes down afterwards. At the very end, though, is the highest peak which suggests a disruption of the structural equilibrium. This might be caused by the drop in the MinDist between the boundaries below 2nm at the end of the simulation and therefore be a result of unwanted interactions between the simulated proteins.
In contrast to the wildtype R224W has a higher RMSD to its average structure (0.3 compared to 0.2). This suggests a higher number of different states which are still quite similar to the starting structure (RMSD ~0.4). At the end of the simulation the equilibrium is disrupted (like in the wildtype simulation), but this time the reason is unkown as the minimum distance between boundaries is one of the highes values in this time period.
Of the three simulations C282S shows the most stable average structure. It is accomplished by two major structural changes at around 2000ps and 3000ps. After that C282S exhibits the lowest RMSD fluctuations of the trio.
Conclusion
References
<references/>
