Calculation of Reduction Potential of FAD in MCAD using Combined DFTB/MM Simulations
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Transcript of Calculation of Reduction Potential of FAD in MCAD using Combined DFTB/MM Simulations
Calculation of Reduction Potential of FAD in MCAD using Combined DFTB/MM Simulations
Sudeep Bhattacharyay, Marian Stankovich, and Jiali Gao
Overview
Objective
Methods of calculation and strategies
Results
Future Directions
Flavoenzymes
Mediates electron transfer
Flavin ring shuttles between reduced and oxidized states
Protein environment controls the reduction potential of FAD
Coupled electron-proton transfer
pKa from experiment often misleading if that is observed through a observable signature belonging to a particular redox state
Need to predict correctly through simulation
Requires accuracy in a) reduction potential calculation and b) pKa calculation
Acyl-CoA Dehydrogenases (CAD) in Electron Transfer
Ghisla, S. et al. Eur J Biochem, 2004. 271, 494-508.
Medium chain acyl-CoA Dehydrogenase (MCAD)
FAD is reoxidized
FAD is reduced
MCAD: Structural Information
All -domainExtends into the other dimer
N CAll -domainTwo orthogonal
-sheets
Forms homotetrameric structure
Active site is formed at protein-protein interface
One FAD (cofactor) and one acyl-CoA (substrate) bind to the active site
Each active site work independent of the other
Passes electron to electron transfering protein (ETF) when it binds to MCADETF
N
NN
NO
O
H
H
CH3
CH3
H R
CoA
S
C
O
CC
C5H11
H
H
H
H
Glu376
O
O
(-)
Scheme 1
-hydride transfer on to the flavin nitrogen
NN
-proton abstraction by the catalytic base Glu376
OO
Potentials of mean force computation of MCAD demonstrate a STEPWISE mechanism
Both proton and hydride transfer CONTRIBUTE TO THE OVERALL CATALYTIC RATE in wild-type
Effect of PROTEIN ENVIRONMENT on the two steps can be investigated independently
A very attractive enzyme system to work with i.e. to TUNE the two reaction barriers
Need to know the effect of protein environment on the two processes
Bhattacharyya S. et al. (2005) Biochemistry,44,16549
A Tale of Two Quasi-independent Processes
R256Q
T168A wt-transient intermediate
Reduction of Flavin
blue (neutral)semiquinone
red (anionic)semiquinone
FAD + 2e + 2H+ FADH2
Experimental Mid-point Potentials Values
MCAD-bound FAD
blue (neutral)semiquinone
red (anionic)semiquinone
-98.6 kcal/mol
-99.3 kcal/mol
Gustafson et al. (1986) J. Biol. Chem. 261, 7733-7741
-197.6 kcal/mol
Mancini-Samuelson et al. (1998) Biochemistry, 37, 14605-14612
yellow
Methods and Strategies
Hybrid QM/MM methods; calculation of electron and proton affinities
Thermodynamic integration through FEP
Dual topology single coordinate method
Boundary condition
Electron and proton affinities
Model Reactionsa,b B3LYP/6-31+G(d,p)H (kcal/mol)
SCC-DFTB
H (kcal/mol)
AM1(Gaussian)
H (kcal/mol)
FAD + e¯ FAD¯ -44.3 -37.3 -63.5
FAD¯ + e¯ FAD2- +53.4 +58.2 48.3
FAD + 2e¯ FAD2- +9.1 +20.9 -15.1
FAD2- + H+ FADH¯ -436.5 -442.3 -420.0
FAD + 2e¯ + H+ FADH¯ -427.4 -421.4 -435.1
FADH + e¯ FADH¯ -49.4 -50.3 -57.2
FAD¯ + H+ FADH -333.7 -333.7 -314.3
FADH¯+ H+ FADH2 -331.7 -331.4 -320.2
FAD + 2e¯ + 2H+ FADH2 -759.1 -752.8 -755.3
N
N N
N
O
O
H
CH3
CH3
CH3
Free Energy Perturbation
Potential energy of a hybrid system: Uhybrid = (1-λ)UA + λUB
λ is a coupling parameter varied from 0-1 (0.1, 0.2, ….)
Free energy change ΔG = ∫(∂G(λ)/ ∂λ) dλ = ∫∂U(λ)/ ∂λ)dλ
0
1 1
0
Cartesian coordinates of the QM system kept invariant in the two states
Change of chemical state of the system without any major change of the cartesian coordinate
State A State B
Thermodynamic integration method
QM/MM Interactions
With same number of atoms in the two chemical states
Utot (R) = │ĤQM+ĤelQM/MM │ + Uvan
QM/MM (R) + UbondedQM/MM (R) + UMM (R)
electronic energy van der Waals bonded energy of the of the QM system MM atoms
+ the electrostatic interaction energy
Only the electrostatic term contributes to the free energy derivative as the two states have same cartesian coordinate
Gλ
(R;λ) = UA/MM(RQM ,RMM ) + UB/MM(RQM ,RMM )
Li, G. et al. J. Phys. Chem. B (2003) 107, 8643
Thermodynamic SchemesFEP for reduction potential calculation
E-FAD (ox) E-FAD(red)
FEP for pKa calculation
ΔGRd/Ox
ΔGRd/Ox is obtained from a single FEP calculation
AH.E(aq)
[A¯ -D].E(aq)
Aˉ .E(aq) + D(g)
Aˉ .E(aq) + H+ (aq)
Aˉ.E(aq) + H+ (g)
G solvH+
G E
AH/A¯G(1)
G(2)
G = 0.0
G E = G(1) + G(2) + Gsolv
AH/A¯ H+
Li, G. et al. J. Phys. Chem. B (2003) 107, 14521
Representations of Atoms
N3
N1 N10
N5
O4
O2
H
H
CH3
CH3
HB
HOOH
HO
P1
O
OO
P2
O
O
O5*
O5'
N1
N3
N9 N7
NH2
O
HO
HO
H
H
H
H
44a
10a
65a
7
899a
1'2'
3'
4'
5'
(-)
(-)
5*
4*
2*
3*
1*
8
2
4 5
6
2
QM atoms are treated by SCC-DFTB MM atoms by CHARMM forcefield QM/MM boundary treated with
generalized hybrid orbital (GHO) method or link atom method
Stochastic boundary or general solvent boundary
Stochastic Boundary Conditions
Reaction centeraverage of the coordinates of atoms treated by QM
Reaction zoneupto 24 Å
Buffer zone 24 - 30 Å
Reservoir zonebeyond 30 Å
• 30 Å water sphere added around the active site center
• Deleting all atoms beyond 45 Å
• Reaction zone : Newtonian Mechanics
• Buffer zone: Langevin’s equation of motion Friction coefficient and a harmonic restoring force with a gradiant: Scaled to 0 at reaction zone boundary
• Reservoir zone provides a static forcefield
45 Å
30 Å
Which Route ?
FAD + 2e + 2H+ FADH2 FAD FADˉ • FAD2ˉ
FADH• FADHˉ
e e
H+
H+
e
FADH2
H+
Model Reactionsa,b B3LYP/6-31+G(d,p)
H (kcal/mol)
SCC-DFTB
H (kcal/mol)
AM1(Gaussian)
H (kcal/mol)
FAD + e¯ FAD¯ -44.3 -37.3 -63.5
FAD¯ + e¯ FAD2- +53.4 +58.2 48.3
FAD + 2e¯ FAD2- +9.1 +20.9 -15.1
FAD2- + H+ FADH¯ -436.5 -442.3 -420.0
FAD¯ + H+ FADH -333.7 -333.7 -314.3
FADH + e¯ FADH¯ -49.4 -50.4 -57.2
FAD¯ + e¯ + H+ FADH
-383.1 -384.1 -371.7
FADH¯+ H+ FADH2 -331.7 -331.4 -320.2
FAD + 2e¯ + 2H+ FADH2
-759.1 -752.8 -755.3
Calculations using Stochastic Boundary Condition
FADˉ• + e FAD2-FAD + e FADˉ•
ΔG1Rd/Ox (FEP) = -79.64 kcal/mol
ΔG (Born Correction) =-5.46 kcal/mol ΔG1
Rd/Ox = -85.1 kcal/mol
ΔG1Rd/Ox (FEP) = -69.7 kcal/mol
ΔG (Born Correction) =-16.4 kcal/mol ΔG2
Rd/Ox = -86.1 kcal/mol
Calculated Reduction Potential
Enzyme mid-point reduction potential for MCAD-bound FAD
Em = -145 mV G = -197.9 kcal/mol
-85 -86 -56 -30
Estimated ΔGtotal = -256 kcal/mol; Overestimated energy ~ 60 kcal/mol
Possible reason for this overestimation
Long-range electrostatic interactions
FAD + 2e + 2H+ FADH2
(E-FAD2- /E-FADH-) (E-FADH- /E-FADH2)ΔGtotal = ΔG1
Rd/Ox + ΔG2Rd/Ox + G + G
Test Calculations
Stochastic boundary set up with net charge of the complex set to zero
General solvent boundary condition
Matching with experimental results
Treating Solvation with General Solvent Boundary Potential (GSBP)
Inner region atoms (ligand + part of enzyme + solvent) treated explicitly
Outer region: Atoms of enzyme are treated explicitly but the solvent is represented as a continuous dielectric medium
Im, W. et al. J. Chem. Phys. 2001, 114, 2924
Setup of Zones in GSBP
Reaction center
Inner region atoms (ligand + part of enzyme + solvent) treated explicitly (< 16 Å)
Water atoms deleted beyond 18 Å Charges of residues beyond 20 Å set to 0 Protein atom fixed beyond 20 Å Outer region: Atoms of enzyme are treated explicitly but the solvent
is represented as a continuous dielectric medium
Inner zone upto 16 Å
Buffer zone upto 18 Å
Secondary buffer (18-20) Å
Reservoir zone > 20 Å
Protein atoms which have 1-3 connections with reservoir zone are kept fixed
Compared Values of Free Energy Changes
Reaction
Stochastic boundary
with neutralized charge
G(kcal/mol)
General solvent
boundarypotential
G(kcal/mol)
E-FAD E-FADˉ· -57.46 -64.1
E-FADˉ· E-FAD2- -53.07 -46.4
E-FAD2- E-FADHˉ -47.9 -53
FEP for Electron Additions
-120
-100
-80
-60
-40
-20
0
0 0.2 0.4 0.6 0.8 1
l
dU
/dl (
kc
al/
mo
l)
-120
-100
-80
-60
-40
-20
0
20
0 0.2 0.4 0.6 0.8 1
l
dU
/dl
(kc
al/
mo
l)
E-FAD E-FADˉ· E-FADˉ· E-FAD2-
ΔG1Rd/Ox (FEP) = -51.0 kcal/mol
ΔG (Born Correction) =-5.46 kcal/mol ΔG1
Rd/Ox = -57.46 kcal/mol
ΔG2Rd/Ox (FEP) = -36.67 kcal/mol
ΔG (Born Correction) =-16.4 kcal/mol ΔG2
Rd/Ox = -53.07 kcal/mol
Calculations for Proton Additions
100
140
180
220
260
0 0.2 0.4 0.6 0.8 1
l
du/dl
(kca
l/mol)
100
140
180
220
260
0 0.2 0.4 0.6 0.8 1l
dU
/dl
(kc
al/m
ol)
E-FAD2- + H+ E-FADHˉ E-FADH- + H+ E-FADH2
ΔG2 (FEP) = -164.1kcal/molE(H+) a, self interaction energy of H-atom
= -141.9 kcal/molΔG b( H+ solvation) = 262.4 kcal/molΔG (Born Correction) =5.46 kcal/mol ΔG2
(total) = -38.15 kcal/mol
(E-FADH-- /E-FADH2)ΔG1 (FEP) = -184.8 kcal/molE(H+) a, self interaction energy of H-atom
= -141.9 kcal/molΔG b ( H+ solvation) = 262.4 kcal/molΔG (Born Correction) =16.4 kcal/mol ΔG1
(total) = -47.9 kcal/mol
(E-FAD2- /E-FADH-)
a Zhou, H. et al. Chemical Physics (2002) 277, 91 b Zhan, C. et al. P. Phys. Chem. A (2001) 105, 11534
FEP Electron Addition
-120
-100
-80
-60
-40
-20
0
0 0.2 0.4 0.6 0.8 1
l
dU
/dl
(kc
al/m
ol)
FAD FADˉ • FAD2ˉ
FADH• FADHˉ
e e
H+ H+
e
FADH2
H+
√√
√
√? E-FADH· E-FADHˉ
ΔG1Rd/Ox (FEP) = -55.47 kcal/mol
ΔG (Born Correction) =-5.46 kcal/mol ΔG1
Rd/Ox = -60.93 kcal/mol
√
Computed Free Energy Changes
Reaction
Stochastic Boundary with 0
chargeG
(kcal/mol)
E-FAD + e E-FAD¯· -57.46
E-FAD¯· + H+ E-FADH· -39.97
E-FAD¯· + e E-FAD2- -53.07
E-FAD2- + H+ E-FADH¯ -47.9
E-FADH¯ + H+ E-FADH2 -38.15
Enz-FADH· E-FADH2 -60.93
Summary
Gexpt
H+
Enz-FAD
Enz-FADH•
Enz-FAD¯• Enz-FAD2-
Enz-FADH¯
H+
e e-57.46 kcal/mol -53.07 kcal/mol
-47.9 kcal/mol
e
-60.93 kcal/mol
-98.6 kcal/mol - 39.97 kcal/mol
H+
Enz-FADH2
-197.9 kcal/mol
-38.15 kcal/mol
Gexpt
Gcomput
= -97.4 kcal/mol -7.0 kcal/mol
Overestimation ~ 6 kcal/mol
Gcomput
= -196.6 kcal/mol -6.3 kcal/mol
Overestimation ~ 6 kcal/mol
Conclusions
The two-electron two-proton reduction potential of FAD in MCAD was calculated Both reduction potential calculations yield results that are consistent to the
experimental values Computed 2e/2H+ reduction potential for FAD bound MCAD is -180 mV, which is
35 mV more negative than the experimental value The first reduction potential of MCAD-bound FAD was calculated to be ~ -103
kcal/mol compared to the experimentally observed value of -98.6 kcal/mol Computed second reduction potential for MCAD-bound FAD was ~ -105
kcal/mol, about 6 kcal/mol more negative than the experimentally observed value of -99.3 kcal/mol
This calculation shows that at neutral pH MCAD-bound FAD will be converted to the hydroquinone form FADH2 through a two electrons/two protons reduction
pKa calculation of E-FADH¯ and E-FADH2 show that both values are quite high: 35 and 27, respectively. The pKa of E-FADH• was calculated to be ~30
Future Directions Using the method to compute the reduction potential
and pKa of FAD and FMN in aqueous solution pka calculation of acyl-CoA substrate bound to MCAD
Acknowledgements
$ NIHProfessor Jiali Gao Professor Don G. Truhlar
Dr. Kowangho Nam Dr. Alessandro Cembran
Dr. Marian Stankovich Dr. Qiang Cui Dr. Haibo YuMinnesota Supercomputing Institute
FAD + 2e + 2H+ FADH2
Total = S1 + S2 + GS
(FAD2- /FADH2)
Em = -(Total)/nF + NHE ; n = number of electrons = 2F= Faraday constant = 23.06 kcal/mol
Total - nFNHE = -nFEm , F = 23.06 kcal/(mol.V)
nFNHE = -n4.43 F V = -2x 4.43 x 23.06 kcal/mol = -204.31 kcal/molFor FAD-MCAD: E0 = -0.145V
Thus Total - nFNHE = -nF x (-0.145) = -2 x 23.06 x (-0.145) kcal/mol
= 6.687 kcal/mol
Thus Total = (6.687 + nFNHE ) kcal/mol = (6.687 -204.31) kcal/mol
= -197.6 kcal/mol
Converting FAD Reduction Potential
For FAD bound MCAD: Mid point potential, E0 = -0.145VLenn, N. D. Stankovich, M. T. Liu, H. Biochemistry, 1990, 29, 3709
Calculating Absolute Reduction Potential
Standard Hydrogen Electrode (Normal Hydrogen Electrode) = Free energy change, EH
0 in the reaction
H+ (s) + e¯ ½H2 (g) EH0
For a general reduction process:
M (s) + e¯ M¯(s) EMM¯
Then combining the above 2 equations
½H2 (g) + M(s) M¯(s) + H+ (s) E0
=> EMM¯ = (E0 + EH0)
E0H = -4.43 eV
Irregular Solvent-Protein Interfaces
RinnerRexact
ΔRdiel= fixed atoms
Im, W. et al. J. Chem. Phys. 2001, 114, 2924