We present a microscopic model of carbon monoxide (CO) binding to myoglobin
which reproduces the experimentally observed Arrhenius pre-exponential fac
tor of 10(9) s(-1) and activation enthalpy distribution centered at 12 kJ/m
ol. The model is based on extensive ab initio calculations of CO interactin
g with a model heme-imidazole group which we performed using a fully quantu
m mechanical Hartree-Fock/density functional theory (HF/DFT) hybrid method.
We fit the HF/DFT calculated energies, obtained for over 1000 heme-CO stru
ctures with varied CO and iron positions and orientations for both high (S=
2) and low (S=0) spin states, to a model potential function which includes
a bonding interaction in both of the spin states, electrostatic, and anisot
ropic Lennard-Jones-type interactions. By combining the x-ray determined pr
otein structure with this potential and protein-CO interactions and interna
l heme interaction potentials obtained from established molecular dynamics
literature, we calculate the energy required for the CO to reach the spin c
rossing from the heme pocket. We find that the transition between the two s
pin states occurs when CO and iron have activation enthalpies of 8 kJ/mol a
nd 3 kJ/mol, respectively, which are necessary to move CO towards the iron
and the iron atom relative to the heme plane N-pyr. At the same time we fin
d that 1 kJ/mol is needed to move N-epsilon of His-64 and C-gamma of Val-68
relative to the heme group. The requirement that these motions be synchron
ized reduces the Arrhenius pre-exponential by a factor of 150 from the 10(1
2) s(-1) obtained from CO motion across the heme pocket, leaving a factor o
f similar to 6 to account for CO orientation and nonadiabaticity of the ele
ctronic spin change. The observed width of the enthalpy distribution is rep
roduced by assuming a Gaussian distribution of the heme positions with a st
andard deviation of 0.2 Angstrom. We characterize the conformational relaxa
tion by calculating an enthalpy barrier using x-ray structures of myoglobin
in both the MbCO photoproduct and deoxy conformations, and we find a small
difference, similar to 5 kJ/mol, between the two conformations. (C) 2000 A
merican Institute of Physics. [S0021-9606(00)01239-3].