Difference between revisions of "Structure-based mutation analysis Gaucher Disease"
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#OPLS-AA/L all-atom force field |
#OPLS-AA/L all-atom force field |
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+ | <figure id="fig:runtim"> |
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− | ==== AMBER03 ==== |
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+ | [[File:runtime.png|thumb|400px|left|<caption> Runtime of minimization with Gromacs for different nsteps by using the OPLS-AA/L force field and the wildtype structure 2nt0_A.</caption>]] |
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+ | </figure> |
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+ | <br style="clear:both;"> |
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− | nstep=50 |
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− | |||
− | step=50 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m7.446s |
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− | user 0m13.230s |
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− | sys 0m1.070s |
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+ | In <xr id="fig:runtim"/> we showed the runtime plot for different setting of nstep(from 50 to 5000). |
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− | nstep=100 |
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− | step=100 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m13.987s |
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− | user 0m25.860s |
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− | sys 0m1.530s |
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− | nstep=200 |
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− | step=200 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m27.186s |
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− | user 0m51.340s |
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− | sys 0m2.540s |
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− | nstep=300 |
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− | Step=300 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m40.664s |
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− | user 1m16.690s |
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− | sys 0m3.860s |
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− | nstep=400 |
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− | step=360 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m48.479s |
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− | user 1m32.195s |
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− | nstep=500 |
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− | step=360 |
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− | real 0m48.481s |
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− | sys 0m4.190s |
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− | nstep=600 |
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− | nstep=1000 |
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− | step=360 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m48.475s |
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− | user 1m31.650s |
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− | sys 0m4.720s |
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− | nstep=1500 |
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− | nstep=2000 |
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− | step=360 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m48.694s |
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− | user 1m31.450s |
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− | sys 0m4.990s |
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− | nstep=2500 |
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− | nstep=3000 |
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− | nstep=5000 |
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− | step=360 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m48.743s |
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− | user 1m32.050s |
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− | sys 0m4.550s |
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− | |||
− | ==== CHARMM27 ==== |
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− | |||
− | |||
− | nstep=50 |
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− | |||
− | step=50 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | |||
− | real 0m7.292s |
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− | user 0m12.950s |
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− | sys 0m1.050s |
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− | |||
− | |||
− | |||
− | nstep=100 |
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− | |||
− | step=100 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | |||
− | real 0m7.292s |
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− | real 0m13.785s |
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− | user 0m25.850s |
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− | sys 0m1.180s |
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− | |||
− | nstep=200 |
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− | |||
− | step=200 |
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− | Reached the maximum number of steps before reaching Fmax < |
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− | real 0m26.843s |
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− | user 0m50.240s |
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− | sys 0m2.660s |
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− | |||
− | nstep=300 |
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− | |||
− | Step=300 |
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− | Reached the maximum number of steps before reaching Fmax < |
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− | real 0m39.990s |
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− | user 1m15.850s |
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− | sys 0m3.470s |
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− | |||
− | |||
− | nstep=400 |
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− | |||
− | Step=348 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m46.322s |
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− | user 1m27.650s |
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− | sys 0m4.150s |
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− | |||
− | |||
− | nstep=500 |
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− | Step=348 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m46.158s |
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− | user 1m27.400s |
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− | sys 0m4.280s |
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− | |||
− | nstep=600 |
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− | nstep=700 |
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− | nstep=800 |
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− | nstep=900 |
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− | nstep=1000 |
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− | Step=348 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m46.121s |
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− | user 1m27.680s |
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− | sys 0m3.860s |
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− | |||
− | nstep=1500 |
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− | nstep=2000 |
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− | Step=348 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m45.345s |
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− | user 1m28.090s |
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− | sys 0m4.012s |
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− | nstep=2500 |
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− | nstep=3000 |
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− | nstep=5000 |
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− | Step=348 |
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− | Stepsize too small, or no change in energy. |
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− | real 0m46.013s |
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− | user 1m27.993s |
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− | sys 0m4.432s |
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− | |||
− | ==== OPLS-AA/L ==== |
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− | |||
− | nstep=50 |
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− | |||
− | step=50 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m6.063s |
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− | user 0m10.750s |
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− | sys 0m0.840s |
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− | |||
− | |||
− | nstep=100 |
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− | |||
− | step=100 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m11.513s |
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− | user 0m20.940s |
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− | sys 0m1.340s |
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− | |||
− | |||
− | nstep=200 |
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− | |||
− | step=200 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m22.378s |
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− | user 0m41.760s |
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− | sys 0m2.110s |
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− | |||
− | |||
− | nstep=300 |
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− | |||
− | Step=300 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m32.959s |
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− | user 1m1.960s |
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− | sys 0m3.180s |
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− | |||
− | |||
− | nstep=400 |
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− | |||
− | Step=400 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m43.790s |
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− | user 1m22.880s |
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− | sys 0m3.950s |
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− | |||
− | nstep=500 |
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− | |||
− | step=500 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 0m54.252s |
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− | user 1m43.040s |
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− | sys 0m4.720s |
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− | |||
− | |||
− | nstep=600 |
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− | |||
− | step=600 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 1m5.020s |
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− | user 2m3.660s |
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− | sys 0m5.490s |
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− | |||
− | |||
− | nstep=700 |
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− | |||
− | step=700 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 1m15.570s |
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− | user 2m24.260s |
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− | sys 0m6.150s |
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− | |||
− | nstep=800 |
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− | |||
− | step=800 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 1m26.511s |
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− | user 2m44.730s |
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− | sys 0m7.480s |
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− | |||
− | nstep=900 |
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− | |||
− | step=900 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 1m36.966s |
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− | user 3m5.360s |
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− | sys 0m7.810s |
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− | |||
− | |||
− | nstep=1000 |
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− | |||
− | step=1000 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 1m47.718s |
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− | user 3m25.940s |
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− | sys 0m8.560s |
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− | |||
− | |||
− | nstep=1100 |
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− | |||
− | step=1100 |
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− | Reached the maximum number of steps before reaching Fmax < 1 |
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− | real 1m58.514s |
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− | user 3m46.010s |
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− | sys 0m9.730s |
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− | |||
− | |||
− | nstep=1500 |
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− | step=1177 |
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− | Stepsize too small, or no change in energy. |
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− | real 2m6.700s |
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− | user 4m2.190s |
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− | sys 0m10.110s |
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− | |||
− | nstep=2000 |
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− | |||
− | step=1177 |
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− | Stepsize too small, or no change in energy. |
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− | real 2m6.707s |
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− | user 4m2.040s |
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− | sys 0m10.470s |
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− | |||
− | |||
− | nstep=2500 |
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− | nstep=3000 |
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− | |||
− | nstep=5000 |
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− | |||
− | step=1177 |
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− | Stepsize too small, or no change in energy. |
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− | real 2m6.734s |
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− | user 4m2.126s |
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− | sys 0m10.340s |
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=== Mutations === |
=== Mutations === |
Revision as of 17:32, 25 June 2012
The aim of this task was to carry out a thorough analysis of ten mutations and to classify them as disease-causing and non-disease causing. Technical details are reported in our protocol.
Contents
Cystral structure
<figtable id="tab:mutations">
PDB | Res [Å] | R value | Coverage | pH |
---|---|---|---|---|
2nt0 | 1.80 | 0.18 | 96% (40-536) | 4.5 |
3gxi | 1.84 | 0.19 | 96% (40-536) | 5.5 |
2v3f | 1.95 | 0.15 | 96% (40-536) | 6.5 |
2v3d | 1.96 | 0.16 | 96% (40-536) | 6.5 |
1ogs | 2.00 | 0.18 | 96% (40-536) | 4.6 |
The 5 crystral structures of glycosylceramidase with the highest resolution. The physiological lysosomal pH value is 4.5. 2nt0 was selected for the analysis. </figtable>
Mutations
<figtable id="tab:mutations">
Nr | Pos P04062 |
Pos 2nt0_A |
From | To | Disease causing |
---|---|---|---|---|---|
1 | 99 | 60 | H | R | No |
2 | 211 | 172 | V | I | No |
3 | 150 | 111 | E | K | Yes |
4 | 236 | 197 | L | P | Yes |
5 | 248 | 209 | W | R | Yes |
6 | 509 | 470 | L | P | No |
7 | 351 | 312 | W | C | Yes |
8 | 423 | 384 | A | D | Yes |
9 | 482 | 443 | D | N | No |
10 | 83 | 44 | R | S | No |
Mutations used for the structure-based mutation analysis. </figtable>
<figure id="fig:mutations">
</figure>
SCWRL
We employed SCWRL <ref name="scwrl">Qiang Wang, Adrian A. Canutescu, and Roland L. Dunbrack, Jr.(2008). SCWRL and MolIDE: Computer programs for side-chain conformation prediction and homology modeling. Nat Protoc.</ref> for substituting the wildtype residues listed in <xr id="tab:mutations"/> by the corresponding mutatant residues which are chosen from a rotamer library. <xr id="fig:scwrl"/> denotes the results.
<figure id="fig:scwrl">
Rotamers of SNPs from <xr id="tab:mutations"/>. Blue: wildtype; Red: rotamer SCWRL; In brackets: energy(mutant)-energy(wildtype). </figure>
None of rotamers chosen by SCWRL clashed with another side-chain or the backbone. The only mutation which led to a structural change was L470P. Here, the insertion of proline interrupted the beta-sheet. The hydrogen bonding network changed in case of mutation number 1, 5, 7, and 8 (cf. <xr id="tab:scwrl"/>). W209R introduces a hydrophilic arginine which forms a hydrogen bond to T180. Although not predicted by SCWRL, the arginine might impact the protein structure. W312C is located next to the active site (cf. <xr id="fig:mutations"/>) and there exists a hydrogen bond to E340. Substitution the hydrophobic tryptohphane by a hydrophlic cysteine in the vicinity of the active site might account for the disease-causing effect of this mutation.
As expected, all mutations increased the energy of the model (cf. the energy difference in brackets in <xr id="fig:scwrl"/>). The energy increased most in case of L470P due to the break of the beta-sheet. A384D and W209R also made the model less stable which is caused by substituting an unpolar residue by a charged residue. All four mutations which increased the model energy most are disease-causing.
<figtable id="tab:scwrl">
Nr | Mutation | Wildtype | Mutatant | Clashes | Structural change | ||
---|---|---|---|---|---|---|---|
H-bonds | Hydrophobicity | H-bonds | Hydrophobicity | ||||
1 | H60R | T471 | Hydrophilic | G62 | Hydrophilic | No | No |
2 | V172I | Hydrophobic | Hydrophobic | No | No | ||
3 | E111K | Hydrophilic | Hydrophilic | No | No | ||
4 | L197P | Hydrophobic | Hydrophobic | No | No | ||
5 | W209R | Hydrophobic | T180 | Hydrophilic | No | No | |
6 | L470P | T482 | Hydrophobic | T482 | Hydrophobic | No | Yes |
7 | W312C | E340, C342, P316 | Hydrophobic | E340, C342 | Hydrophilic | No | No |
8 | A384D | Hydrophobic | V404 | Hydrophilic | No | No | |
9 | D443N | Hydrophilic | Hydrophilic | No | No | ||
10 | R44S | S13, Y487 | Hydrophilic | S13, Y487 | Hydrophilic | No | No |
Structure-based analysis of SNPs from <xr id="tab:mutations"/>. H-bonds: residues involved in forming hydrogen bonds (cut-off: 3.2 Å). </figtable>
We further noticed that SCRWL changed the backbone at some positions which led to different secondary structure assignments (<xr id="fig:scwrl_ss"/>). The positions at which the deviations could be observed were independent from the mutated sites.
<figure id="fig:scwrl_ss">
</figure>
FoldX
The superposition of the rotamer configurations predicted by FoldX and SCWRL are shown in <xr id="fig:foldx"/>. The predictions of both tools differed in case of four mutations. In case of H60R, the side-chain orientation of arginine predicted by FoldX forms two instead one hydrogen bonds to T741 and might therefore impact the protein structure more than the orientation of SCRWL. In case of A384D, the romater of FoldX might be more stable than the one of SCWRL since it has a higher distance to the surrounding residues. In case of D443N we prefer the prediction of SCWRL which is closer to the wildtype configuration. For the same reason we prefer the prediction of FoldX in case of R442. For the subsequent GROMACS analysis, we hence chose the FoldX model in case of mutation number 8 and 10 and the SCWRL models for all all other mutations.
<figure id="fig:foldx">
Rotamers of SNPs from <xr id="tab:mutations"/>. Blue: wildtype; Red: rotamer SCWRL; Orange: rotamer FoldX; In brackets: energy(mutant)-energy(wildtype). </figure>
A comprehensive list of the differences between the mutant and the wildtype models can be found here. The total energy increased in case of mutation number 4-8, and 10. Just as in case of SCWRL (cf. <xr id="fig:scwrl"/>), L470P, A384D, and W209R increased the energy of the model most. Since it is unlikely that mutations like V172I decrease the energy, we consider the energy calculations of SCWRL as more plausible.
Minimise
SCWRL models
<figure id="fig:minimise_scwrl_e">
Energy of the SCWRL mutant models compared to the SCWRL wildtype models over five iterations minimise. </figure>
<figure id="fig:minimise_scwrl_m">
Side-chain conformation of the SCWRL mutant models compared to the SCWRL wildtype models over five iterations Minimise. </figure>
FoldX models
<figure id="fig:minimise_foldx_mutations">
Side-chain optimization of FoldX models over five iterations minimise. Green: the input model. </figure>
Gromacs
Runtime analysis
To show the relationship between nsteps and runtime of 'mdrun', different nstep were chosen from 50 to 1000. Three different energy functions were selected:
- AMBER03 protein, nucleic AMBER94
- CHARMM27 all-atom force field (with CMAP)
- OPLS-AA/L all-atom force field
<figure id="fig:runtim">
</figure>
In <xr id="fig:runtim"/> we showed the runtime plot for different setting of nstep(from 50 to 5000).
Mutations
Mutation 1
Energy Average Err.Est. RMSD Tot-Drift ------------------------------------------------------------------------------- Bond 1624.88 820 5492.83 -5022.62 (kJ/mol) Angle 4289.66 76 402.822 -411.894 (kJ/mol) Potential -45289.6 2900 16896.6 -18817.6 (kJ/mol)
References
<references/>