Gb. Ray et al., HOW FAR CAN PROTEINS BEND THE FECO UNIT - DISTAL POLAR AND STERIC EFFECTS IN HEME-PROTEINS AND MODELS, Journal of the American Chemical Society, 116(1), 1994, pp. 162-176
Resonance Raman (RR) spectra are reported for structurally defined CO
adducts of two sterically constrained Fe(II) porphyrins: PocPiv, in wh
ich three of the pivaloylamino pickets of ''picket fence'' porphyrin ,
15,20-tetrakis[o-(pivaloylamino)phenyl]porphyrin) are attached to a be
nzene cap by single methylene groups, and C2-Cap, in which a benzene c
ap is attached by carboxylate links and a pair of methylene groups to
the four hydroxyl groups of 5,10,15,20-tetrakis(o-hydroxyphenyl)porphy
rin. Although the X-ray crystal structures of the two adducts show ver
y similar FeCO geometries, involving a small amount of bending and til
ting, their vibrational frequencies and RR enhancement patterns are ve
ry different. Relative to unconstrained porphyrins, the C-0 and Fe-C s
tretching (nu(CO) and nu(FeC)) frequencies show increased Fe-->CO back
-bonding for PocPiv but decreased back-bonding for C2-Cap. The Fe-C-O
bending mode (deltaF(FeCO)) is activated for PocPiv but not for C2-Cap
. These contrasting patterns can be attributed to the different polar
interactions of the bound CO in the two adducts. In the PocPiv adduct,
the 0 atom is in close contact with one of the amide NH groups; this
positive polar interaction increases back-bonding. In the C2-Cap adduc
t, the linker arms have ester and ether, rather than amide, groups and
there is a close contact between the CO and the benzene pi-cloud; thi
s negative polar environment decreases back-bonding. In addition the c
ap interaction may compress the FeC bond in C2-Cap, as evidenced by a
nu(FeC) frequency elevation from the value expected on the basis of th
e back-bonding decrease. The extensive vibrational data on CO adducts
of heme proteins and on sterically constrained synthetic porphyrins ar
e reexamined in the light of these results. Essentially all of the dat
a are consistent with expected polar effects in the binding pocket. Po
sitive distal polar interactions (1) increase nu(FeC) and decrease nu(
CO) along a back-bonding correlation that depends only on the nature o
f the trans axial ligand, (2) diminish the intensity of the nu(FeC) RR
band (attributed to a reduction in the Fe-C bond displacement between
the ground and excited states), and (3) activate the FeCO bending mod
e (by perturbing the 4-fold electronic symmetry via off-axis interacti
ons). A recent proposal that the RR band usually assigned to delta(FeC
O) actually arises from the bending mode overtone is discussed and is
rejected on the basis of comparisons with transition metal carbonyls f
or which thorough vibrational analyses are available. Elimination of p
ositive polar interactions reverses all three of these effects. The en
ergetics of the small FeCO distortions seen in the PocPiv and C2-Cap a
dducts are evaluated and are found to account for most of the CO affin
ity reductions of these constrained porphyrins. The polar interactions
appear to contribute only a small part of the overall energy, even th
ough they have a dominant effect on the vibrational frequency variatio
n. It is argued that large sterically-induced FeCO distortions are pre
cluded by the prohibitive energy cost, especially in proteins, where t
he available steric force is limited by the conformational flexibility
of the polypeptide. Somewhat greater FeCO bending than has so far bee
n observed in models is indicated for one of the substates, A3, of the
CO adduct of myoglobin. This effect is suggested to arise from a dono
r interaction with an imidazole lone pair, consistent with the distal
histidine tautomer determined by neutron diffraction. Even in this cas
e, however, the IR frequency precludes FeCO angles as small as 120-140
-degrees, values reported from early determinations of MbCO crystal st
ructures containing disordered CO. The dominant MbCO substates in solu
tion, A1,2, are indicated to have a significant polar interaction with
the distal histidine, in the alternate tautomer to the one seen in th
e neutron structure, and probably have nearly linear FeCO units, consi
stent with the most recent X-ray structure determination of a nondisor
dered crystal form.