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SDA development

SDA development. Description of sda-4.23 Description of sda-5a - Sda for docking. Brownian dynamics simulations. Give the diffusional rate k 1 (upper estimate for catalytic rate). k 1   k -1. k 2   k -2. E. +. S. E:S. ES. . E. +. P.

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SDA development

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  1. SDA development • Description of sda-4.23 • Description of sda-5a • - Sda for docking

  2. Brownian dynamics simulations Give the diffusional rate k1 (upper estimate for catalytic rate) k1   k-1 k2   k-2 E + S E:S ES  E + P Best predictions are for relative rates when post-diffusional step (2) is the same/similar

  3. Brownian Dynamics simulations • start a number of trajectories from b-surface • monitor reaction •  - fraction of reactive trajectories • rigid proteins • atomic level description • no overlaps • electrostatic forces • steps ~ 0.5 Å, ~1 ps A B b-surface B c-surface

  4. Brownian dynamics simulation forcefield 110-130 150 1000 300 exclusion check

  5. Boltzmann factor calculations (sdabf) • one protein is fixed • the other - placed on the grid points and rotated randomly • electrostatic interaction energy between the proteins computed • positions with low energy stored • stored conformations clustered

  6. Electrostatic interaction energies Where qki – effective (fit to reproduce its electrostatic potential) charges of protein k, ri=(xi,yi,zi) charge coordinates, - electrostatic potential of protein l computed by solving Poisson-Boltzmann equation numerically

  7. Electrostatic desolvation energies Where qi – charges, xi– charge coordinates, - electrostatic potential computed by solving Poisson-Boltzmann equation numerically

  8. Electrostatic desolvation energy computations 12 charges 1=0 2

  9. Electrostatic desolvation energy computations 2 treatments of the surface of proteins in electrostatics: nmap -molecular surface – interior is inside analytically computed molecular surface, obtained by rolling solvent probe vdw - van der Waals surface – interior is inside Van der Waals surfaces of atoms Solvent probe, any point which can be inside it is a solvent Ds grid factor 1.7 Ds grid factor 4.2

  10. Protein-protein simulation results • Mutation and ionic strength dependence of rates are reproduced by simulations better than the rate differences for different proteins • Association in the case “3hfm” (HyHEL-10:HEL) is far from diffusional control • Formation of 2 contacts at 6 A separation should be required in order to association to occur

  11. Buried area Elcock & McCammon, Biophys.J. (2001) 80, 613  ~ 25 cal/mole/Å2

  12. Buried area/sda5 • Using buried area term makes BD simulations: • better • more realistic interaction energy description • worse • because flexibility should now to be taken into account, but it is not • longer : • Plastocyanin-cytf case – factor of 100, when typical sda4 encounter times are ~ 10 ns, sda5 encounter times are ~ 1000 ns ~ experimental complex lifetime • Longer living complexes will be even more longer to simulate (barnase-barstar with  =13 cal/mole/Å2 ~ 1 min per run, estimated for  =25 cal/mole/Å2 ~ 1 min *106 per run)

  13. Buried area/sda5 • Using buried area term makes BF sampling: • better • more realistic interaction energy description • worse • because flexibility should now to be taken into account, but it is not • longer : • not significantly, but BF samplings are long anyway

  14. Buried area/sda5 • Some expectations (?) • If electrostatic desolvation is used, then buried area = hydrophobic desolvation should be used too • Using buried area term in docking will give realistic energy values, but not good docked complexes • Using buried area term in BD simulations should give more realistic encounter times, but worse quantitative estimates for rate constants

  15. E12= Ecoul + Edes + Ehyd E12= Ecoul + Edes E12= Ecoul

  16. Docking using restraints • SDABFCW  - previous version of sampling program SDABF which compute energies only when restraints are satisfied and writes sorted low-energy complexes • SDA5DOCK - new version of SDABF, which computes buried area as a sum of accessible areas of atoms of the protein 2 which lay on the skin of the protein 1 .  The main results here are that applying restraints (constraints) is very efficient in reducing sampling time.

  17. Docking using restraints • SDAW - Brownian dynamics simulations with the possibility of writing low-energy complexes, which satisfy pre-defined restraints. (There are no forces resulted from restraints, restraints are only used in deciding if the complex should be stored.) • This method can be much faster than systematic search of low energy complexes, when comparable sampling accuracy is achieved.  For example, in case of www-domain/peptide case: systematic sampling with 1.5 A sampling grid spacing takes ~ 4 hours, while sdaw simulations (giving even lower energy complexes) ~ 20 min.  Sampling accuracy of BD is also much better - sqrt(6Dt)~0.3 A. However, docking by sdaw has obviously different meaning than systematic sampling. •  Apparent drawback is that many complexes are stored which are very similar.  Realistic is to write out 1000 complexes for further analysis, but the number of low-energy conformations found during BD is much larger.  Therefore, it might be necessary to add some clustering during BD simulations in order to not write similar complexes. • Restraints can be applied in atom-based fashion.  One test was done with ww-domain/peptide docking case, when CG_TRP_38 was restricted to be within 5A to any heavy atom of the peptide.  This requires 540 reaction pairs to be checked.  The same simulation was done when CB_TRP_38 was restricted to be within 8 A to any CB of the peptide, which requires 7 pairs to be checked.  The simulations with 540 pairs (77 times more than 7) took only 6 times more computing time.

  18. Docking using restraints • SDAWB - Brownian dynamics simulations with the possibility of biasing dynamics by pre-defined restraints and writing low-energy complexes, satisfying pre-defined restraints.  The difference here is that the dynamics is biased by applying Metropolis procedure favourng the motions resulting in better satisfaction of restraints.  Biasing is done along the 1-contact (any one of defined pairs) distance restraint with piecewise linear function constant at large and small contact distances and changing linearly inbetween. •  The performance of the algorithm is not very well tested.  It should have some advantages compared to SDAW, but its performance probably depends on the parameters of the biasing function.

  19. Octave‘s results

  20. Octave‘s results

  21. Octave‘s results

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