1 / 19

Hybrid Quantum-Classical Molecular Dynamics of Enzyme Reactions

Hybrid Quantum-Classical Molecular Dynamics of Enzyme Reactions. Sharon Hammes-Schiffer Penn State University. Issues to be Explored. Fundamental nature of H nuclear quantum effects Zero point energy H tunneling Nonadiabatic effects Rates and kinetic isotope effects

Download Presentation

Hybrid Quantum-Classical Molecular Dynamics of Enzyme Reactions

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Hybrid Quantum-Classical Molecular Dynamics of Enzyme Reactions Sharon Hammes-Schiffer Penn State University

  2. Issues to be Explored • Fundamental nature of H nuclear quantum effects • Zero point energy • H tunneling • Nonadiabatic effects • Rates and kinetic isotope effects • Comparison to experiment • Prediction • Role of structure and motion of enzyme and solvent • Impact of enzyme mutations

  3. Billeter, Webb, Iordanov, Agarwal, SHS, JCP 114, 6925 (2001) Hybrid Quantum/Classical Approach Real-time mixed quantum/classical molecular dynamics simulations including electronic/nuclear quantum effects and motion of complete solvated enzyme • Elucidates relation between specific enzyme motions • and enzyme activity • Identifies effects of motion on both activation free energy and • dynamical barrier recrossings

  4. Two Levels of Quantum Mechanics • Electrons • Breaking and forming bonds • Empirical valence bond (EVB) potential • Warshel and coworkers • Nuclei • Zero point motion and hydrogen tunneling • H nucleus represented by 3D vibrational wavefunction • Mixed quantum/classical molecular dynamics • MDQT surface hopping method

  5. D A H D A H Empirical Valence Bond Potential EVB State 1 EVB State 2 Diagonalize • GROMOS forcefield • Morse potential for D-H and A-H bond • 2 parameters fit to reproduce experimental free • energies of activation and reaction

  6. Mixed quantum/classical nuclei • r: H nucleus, quantum • R: all other nuclei, classical • Calculate 3D H vibrational wavefunctions on grid Treat H Nucleus QM Fourier grid Hamiltonian multiconfigurational self-consistent-field (FGH-MCSCF) Webb and SHS, JCP 113, 5214 (2000) Partial multidimensional grid generation method Iordanov et al., CPL 338, 389 (2001)

  7. Calculation of Rates and KIEs • Equilibrium TST rate • Calculated from activation free energy • Generate adiabatic quantum free energy profiles • Nonequilibrium transmission coefficient • Accounts for dynamical re-crossings of barrier • Reactive flux scheme including nonadiabatic effects

  8. Collective reaction coordinate • Mapping potential to drive reaction over barrier • Thermodynamic integration to connect • free energy curves • Peturbation formula to include adiabatic • H quantum effects Calculation of Free Energy Profile

  9. Reactive flux approach for infrequent events • Initiate ensemble of trajectories at dividing surface • Propagate backward and forward in time Calculation of Transmission Coefficient  = 1/a for trajectories with a forward and a-1 backward crossings = 0 otherwise Keck, Bennett, Chandler, Anderson • MDQT surface hopping method to include vibrationally • nonadiabatic effects (excited vibrational states) • Tully, 1990; SHS and Tully, 1994

  10. Mixed Quantum/Classical MD • Classical molecular dynamics • Calculate adiabatic H quantum states • Expand time-dependent wavefunction • quantum probability for state n at time t • Solve time-dependent Schrödinger equation Hynes,Warshel,Borgis,Kapral, Laria,McCammon,van Gunsteren,Cukier,Tully

  11. Tully, 1990; SHS and Tully, 1994 • System remains in single adiabatic quantum state k • except for instantaneous nonadiabatic transitions • Probabilistic surface hopping algorithm: for large number • of trajectories, fraction in state n at time t is • Combine MDQT and reactive flux • [Hammes-Schiffer and Tully, 1995] • -Propagate backward with fictitious surface hopping • algorithm independent of quantum amplitudes • - Re-trace trajectory in forward direction to determine • weighting to reproduce results of MDQT MDQT

  12. LADH Alcohol Aldehyde/Ketone DHFR DHF THF NAD+ NADH + H+ NADPH + H+ NADP+ Systems Studied • Liver alcohol dehydrogenase • Dihydrofolate reductase

  13. Dihydrofolate Reductase Simulation system > 14,000 atoms • Maintains levels of THF required for biosynthesis of • purines, pyrimidines, and amino acids • Hydride transfer from NADPH cofactor to DHF substrate • Calculated KIE (kH/kD) is consistent with experimental value of 3 • Calculated rate decrease for G121V mutant consistent with • experimental value of 160 • k = 0.88 (dynamical recrossings occur but not significant)

  14. DHFR Productive Trajectory

  15. DHFR Recrossing Trajectory

  16. Network of Coupled Motions • Located in active site and exterior of enzyme • Equilibrium, thermally averaged motions • Conformational changes along collective reaction coordinate • Reorganization of environment to facilitate H- transfer • Occur on millisecond timescale of H- transfer reaction

  17. Strengths of Hybrid Approach • Electronic and nuclear quantum effects included • Motion of complete solvated enzyme included • Enables calculation of rates and KIEs • Elucidates fundamental nature of nuclear quantum effects • Provides thermally averaged, equilibrium information • Provides real-time dynamical information • Elucidates impact of mutations

  18. Limitations and Weaknesses • System size • LADH (~75,000 atoms), DHFR (~14,000 atoms) • Sampling • DHFR: 4.5 ns per window, 90 ns total • Potential energy surface (EVB) • not ab initio, requires fitting, only qualitatively accurate • Bottleneck: grid calculation of H wavefunctions • - must calculate energies/forces on grid for each MD time step • - scales as • - computationally expensive to include more quantum nuclei • Future US/UK and biomolecules/materials collaborations • Future requirements for HPC hardware and software

  19. Acknowledgements Pratul Agarwal Salomon Billeter Tzvetelin Iordanov James Watney Simon Webb Kim Wong DHFR: Ravi Rajagopalan, Stephen Benkovic Funding: NIH, NSF, Sloan, Dreyfus

More Related