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Hybrid Quantum-Classical Molecular Dynamics of Hydrogen
Transfer Reactions in Enzymes
Sharon Hammes-Schiffer Penn State University
Enzymes• Catalyze chemical reactions: make them faster
enzymecofactor
substrate
chemicalreaction
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
Impact of Enzyme Motion
• Activation free energy barrier– equilibrium between transition state and reactant
• Dynamical re-crossings of free energy barrier– nonequilibrium dynamical effect
Hybrid Approach
Real-time mixed quantum/classical molecular dynamicssimulations including nuclear quantum effects andmotion of complete solvated enzyme
Billeter, Webb, Iordanov, Agarwal, SHS, JCP 114, 6925 (2001)
• Elucidates relation between specific enzyme motions and enzyme activity• Distinguishes between activation free energy and dynamical barrier recrossing effects
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
Empirical Valence Bond Potential
• GROMOS forcefield
• Morse potential for DH and AH bond• 2 parameters fit to reproduce experimental free
energies of activation and reaction
EVB State 1 EVB State 2
D AH D AH
1 nuc 12EVB nuc
12 2 nuc 12
( )( )
( )
V V
V V
RH R
R
EVB nuc g nuc( ) ( )VH R RDiagonalize
Treat H Nucleus QM• Mixed quantum/classical nuclei
r: H nucleus, quantum
R: all other nuclei, classical
• Calculate 3D H vibrational wavefunctions on grid
Fourier grid Hamiltonian multiconfigurationalself-consistent-field (FGH-MCSCF)Webb and SHS, JCP 113, 5214 (2000)
Partial multidimensional grid generation methodIordanov et al., CPL 338, 389 (2001)
( , ) ( ; ) ( ) ( ; )nH g n nT V r R r R R r R
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
† /
TSTBG k TBk T
kh e
dyn TSTk k
0 1
Calculation of Free Energy Profile• Collective reaction coordinate
• Mapping potential to drive
reaction over barrier
• Thermodynamic integration to connect free energy curves• Perturbation formula to include adiabatic H quantum effects
11 22 o( ) ( , ) ( , )V V R r R r R
map 11 22( , ; ) (1 ) ( , ) ( , )m m mV V V r R r R r R
map intmap0 ( ; ) [ ( ) ( ; )]( ; )
,
n m o mn m
m n
F VFe e e
R R
intmap map( ; ) ( , ; )m mV Ve C d e R r Rr r
Calculation of Transmission Coefficient
• Reactive flux approach for infrequent events– Initiate ensemble of trajectories at dividing surface– Propagate backward and forward in time
w = 1/ for trajectories with forward and -1 backward crossings = 0 otherwise
• MDQT surface hopping method to include vibrationally nonadiabatic effects (excited vibrational states) Tully, 1990; SHS and Tully, 1994
Mixed Quantum/Classical MD2
tot1
( , )2
cNI
H gI I
PH T V
M
r R
• 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
eff eff ( )II I IM V RF R R
( , ) ( ; ) ( ) ( ; )nH g n nT V r R r R R r R
( , , ) ( ) ( ; )n nn
t C t r R r R2
( ) :nC t
k k k j kjj
i C C i C R d kj k j Rd
Hynes,Warshel,Borgis,Ciccotti,Kapral,Laria,McCammon,van Gunsteren,Cukier
MDQT
• 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 • Incorporates zero point energy and H tunneling• Valid in adiabatic, nonadiabatic, and intermediate regimes
Tully, 1990; SHS and Tully, 1994
2( )nC t
MDQT Reactive Flux
• Reactive flux approach for infrequent events– Initiate ensemble of trajectories at dividing surface– Propagate backward and forward in time
• Extension for MDQT [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
Liver Alcohol Dehydrogenase
• Critical for key steps in metabolism• Relevant to medical complications of alcoholism• Experiments: Klinman (KIE, mutagenesis)• Other theory
– electronic structure: Houk, Bruice, Gready– molecular dynamics: Bruice– VTST-QM/MM: Truhlar, Gao, Hillier, Cui, Karplus
Alcohol Aldehyde/Ketone
NAD+ NADH + H+
LADH
LADH Simulation System
• 75140 atoms in rectangular periodic box• Two protein chains, co-enzymes, benzyl alcohol substrates• 22682 solvent (water molecules)
Crystal structure: Ramaswamy, Eklund, Plapp, 1994
Active Site of LADH• Proton transfer occurs prior to hydride transfer
– Experimental data– Electronic structure/classical forcefield calculations
Agarwal, Webb, SHS, JACS 122, 4803 (2000)
LADH Reaction
Free Energy Profile for LADH• Two EVB parameters fit to experimental free energies Plapp and coworkers, Biochemistry 32, 11186 (1993)• Nuclear quantum effects decrease free energy barrier
Hydrogen Vibrational Wavefunctions
Reactant
TS
Product
Ground state Excited state
Isotope Effects of H Wavefunctions at TS
Hydrogen
Deuterium
Tritium
KIE from Activation Free Energy
TST Calculations Experiment1
kH/kD 5.0 ± 1.8 3.78 ± 0.07
kD/kT 2.4 ± 0.8 1.89 ± 0.01
1Bahnson and Klinman, 1995
The Reactive Center
Equilibrium Averages of Properties
Real-Time Dynamical Trajectories
LADH Productive Trajectory
LADH Unproductive Trajectory
LADH Recrossing Trajectory
Transmission Coefficient
H = 0.95D = 0.98
• Values nearly unity dynamical effects not dominant
• Inverse KIE for
Calculations: kH/kD = 4.8 ± 1.8
Experiment: kH/kD = 3.78 ± 0.07
Correlation FunctionsNormalized weighted correlation between geometrical property and barrier re-crossing ()
Property CorrelationCD-CA distance 17.8%Zn-O distance 0.5%CD-O distance 5.0%VAL-203 C1-CA distance 5.6%VAL-203 C1-NH4 distance 5.2%VAL-203 C1-CD distance 0.2%C NAD+/NADH angle - 1.7%N NAD+/NADH angle 10.4%Standard deviation for random sample: 6.0%
Dihydrofolate Reductase
• Maintains levels of THF required for biosynthesis of purines, pyrimidines, and amino acids• Pharmacological applications• Experiments: Benkovic (kinetics, mutagenesis), Wright (NMR)• Previous theory
– electronic structure: Houk– QM/MM: Gready and coworkers– molecular dynamics: Radkiewicz and Brooks
DHF THF
NADPH + H+ NADP+
DHFR
DHFR Simulation System
• 14063 atoms in octahedral periodic box
• NADPH co-enzyme, DHF substrate
• 4122 solvent (water molecules)
Crystal structure: 1rx2, Sawaya and Kraut, Biochemistry 1997
DHFR Reaction
Free Energy Profile for DHFR
• Two EVB parameters fit to experimental free energies Fierke, Johnson and Benkovic, Biochemistry 1987
• kH/kD TST: 3.4 ± 0.8, experiment: 3.0 ± 0.4
Agarwal, Billeter, Hammes-Schiffer, JPC 106, 3283 (2002)
Transmission Coefficient for DHFR
H = 0.80D = 0.85
• Values less than unity
dynamical barrier recrossings significant
• Physical basis
− friction from environment
− not due to nonadiabatic transitions
DHFR Productive Trajectory
Motion in DHFR
• Conserved residues
(genomic analysis across 36
species, E. coli to human)• Effects of mutations on
hydride transfer rate:
large effects far from active site, non-additive double mutants• NMR: dynamic regions Wright and coworkers• MD: correlated regions Radkiewicz and Brooks
Agarwal, Billeter, Rajagopalan, Benkovic, Hammes-Schiffer, PNAS 2002
Hybrid Quantum-Classical Simulations• Systematic study of conserved residues• Calculated two quantities per distance
− thermally averaged change from reactant to TS (ms timescale of H─ transfer)− correlation to degree of barrier recrossing (fs-ps timescale of dynamics near TS)
DHF/NADPH Motion
Motions Near DHF/NADPH
Loop Motion
Network of Coupled Promoting Motions• Located in active site and exterior of enzyme• Contribute to collective reaction coordinate• Occur on millisecond timescale of H transfer reaction
G121V Mutant Free Energy Profile
Simulations: G121V has higher free energy barrier than WTExperiment: G121V rate 163 times smaller than WT
Gly
Val
G121V Mutant MotionsWT G121V
Summary of Hybrid Approach
• Generate free energy profiles and dynamical trajectories− Nuclear quantum effects included− Motion of complete solvated enzyme included
• Wealth of information– Rates and KIEs– Fundamental nature of nuclear quantum effects– Relation between specific enzyme motions and activity
(activation free energy and barrier re-crossings)– Impact of mutations– Network of coupled promoting motions
Acknowledgements
Pratul AgarwalSalomon BilleterTzvetelin IordanovJames WatneySimon Webb
DHFR: Ravi Rajagopalan, Stephen Benkovic
Funding: NSF, NIH, Sloan, Dreyfus