We generated atomic coordinates of an artificial protein that was recently
synthesized to model the central part of the native cytochrome b (Cb) subun
it consisting of a four-helix bundle with two hemes. Since no X-ray structu
re is available, the structural elements of the artificial Cb were assemble
d from scratch using all known chemical and structural information availabl
e and avoiding strain as much as possible. Molecular dynamics (MD) simulati
ons applied to this model protein exhibited root-mean-square deviations as
small as those obtained from MD simulations starting with the crystal struc
ture of the native Cb subunit. This demonstrates that the modeled structure
of the artificial Cb is relatively rigid and strain-free. The model struct
ure of the artificial Cb was used to determine the redox potentials of the
two hemes by calculating the electrostatic energies from the solution of th
e linearized Poisson-Boltzmann equation (LPBE). The calculated redox potent
ials agree within 20 meV with the experimentally measured values. The depen
dence of the redox potentials of the hemes on the protein environment was a
nalyzed. Accordingly, the total shift in the redox potentials is mainly due
to the low dielectric medium of the protein, the protein backbone charges,
and the salt bridges formed between the arginines and the propionic acid g
roups of the hemes. The difference in the shift of the redox potentials is
due to the interactions with the hydrophilic side chains and the salt bridg
es formed with the propionic acids of the hemes. For comparison and to test
the computational procedure, the redox potentials of the two hemes in the
native Cb from the cytochrome bc(1) (Cbc(1)) complex were also calculated.
Also in this case the computed redox potentials agree well with experiments
.