Exposure of frozen solutions of oxyhe
moglobin to
mages/gifchars/ga
mma.gif" BORDER=0 >-irradiation at 77 K yields EPR- andENDOR-active, one-electron-reduced oxyhe
me centers which retain the confor
mation of the dia
magneticprecursor. EPR spectra have been collected for the centers produced in hu
man HbO
2 and isolated
mages/gifchars/alpha.gif" BORDER=0>O
2and
mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">O
2 chains, as well as
mages/gifchars/alpha.gif" BORDER=0>O
2mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">(Zn),
mages/gifchars/alpha.gif" BORDER=0>(Zn)
mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">O
2, and
mages/gifchars/alpha.gif" BORDER=0>O
2mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">(Fe
3+) hybrids, each in frozen buffer and infrozen glasses that for
m in the presence of glycols and sugars and also in the presence of IHP. Thesereveal two spectroscopically distinct classes of such ferrihe
me centers (
g1 mages/entities/le.gif"> 2.25), denoted A and B.Averaged over
many si
milar sites, the A-center has a rho
mbic EPR signal with a
g-tensor,
gA = [2.248(4),2.146(1), 1.966(1)]; the B-center exhibits a less anisotropic EPR signal,
gB = [2.216(3), 2.118(2), 1.966(1)].Early
measure
ment had suggested that, in the cryoreduced HbO
2 tetra
mer, the two centers corresponded to the two different chains [Sy
mons, M. C. R., and Petersen, R. L. (1978)
Proc. R. Soc. London,Ser. B 201, 285-300]. However, the present EPR and ENDOR results show that the two signals insteadreflect the fact that the parent oxyhe
mes exist in two
major confor
mational substates and that this is truefor
both mages/gifchars/alpha.gif" BORDER=0>O
2 and
mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">O
2 subunits:
mages/gifchars/alpha.gif" BORDER=0>O
2A (
minor species) and
mages/gifchars/alpha.gif" BORDER=0>O
2B (
major species);
mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">O
2A(
major species)and
mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">O
2B (
minor species). Si
milar behavior is seen for MbO
2 [Kappl, R., H&ou
ml;hn-Berlage, M., H&uu
ml;tter
mann,J., Bartlett, N., and Sy
mons, M. C. R. (1985)
Biochim. Biophys. Acta 827, 327-343]. The A/B
g-tensorsof
mages/gifchars/alpha.gif" BORDER=0>O
2 and
mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">O
2 chains vary little with the environ
ment of the chains, while the relative populations ofthe substates depend greatly on glycols and IHP. These results suggest a quaternary influence on theoxyhe
me distal pocket of
mages/gifchars/alpha.gif" BORDER=0> chains and that the glycol-induced changes in the substate populations of theR-state HbO
2 tetra
mer are largely associated with the
mages/gifchars/alpha.gif" BORDER=0>O
2 subunit.
1H ENDOR spectra fro
m the distalhistidine proton hydrogen-bonded to the peroxo ligand show very different isotropic coupling for the A-and B-centers. Analysis of the spectroscopic data suggests that the A- and B-centers represent differentorientations of the oxyhe
me O
2 ligand relative to the distal histidine. It is likely that the A and Bconfor
mational substates in the
mages/gifchars/alpha.gif" BORDER=0>O
2 and
mages/gifchars/beta2.gif" BORDER=0 ALIGN="
middle">O
2 subunits differ not only in their tertiary structures but intheir affinities for O
2.