CONFORMATIONAL SUBSTATES OF THE FE2-HIS F8 LINKAGE IN DEOXYMYOGLOBIN AND HEMOGLOBIN PROBED IN PARALLEL BY THE RAMAN BAND OF THE FE-HIS STRETCHING VIBRATION AND THE NEAR-INFRARED ABSORPTION-BAND-III()
H. Gilch et al., CONFORMATIONAL SUBSTATES OF THE FE2-HIS F8 LINKAGE IN DEOXYMYOGLOBIN AND HEMOGLOBIN PROBED IN PARALLEL BY THE RAMAN BAND OF THE FE-HIS STRETCHING VIBRATION AND THE NEAR-INFRARED ABSORPTION-BAND-III(), International journal of quantum chemistry, 59(4), 1996, pp. 301-313
We measured the nu(Fe-His) Raman band of horse heart deoxymyoglobin an
d human deoxyhemoglobin as a function of temperature between 10 and 30
0 K. A self-consistent spectral analysis of the deoxymyoglobin Raman b
and reveals that it is underlied by three different sublines with freq
uencies at Ohm(1) = 209 cm(-1), Ohm(2) = 217 cm(-1), and Ohm(3) = 225
cm(-1) and an identical half-width of 13 cm(-1). All these parameters
were found to be independent of temperature. These sublines were attri
buted to different conformational substates of the Fe2+-His F8 linkage
, which comprise different out-off-plane displacements of the heme iro
n and tilt angles of the Fe2+-N-epsilon(His F8) bond. The intensity ra
tio I-3/I-2 exhibits a van't Hoff behavior between 150 and 300 K, bend
s over in a region between 150 and 80 K, and remains constant at lower
temperature. In contrast, I-2/I-1 shows a maximum at 170 K and approa
ches a constant value at 80 K. These data can be fitted by a modified
van't Hoff expression, which accounts for the freezing into nonequilib
rium distributions of substrates in a temperature interval Delta T aro
und a distinct temperature T-f and also for the linear temperature dep
endence of the protein's specific heat. The fits to the above intensit
y ratios yield a freezing temperature of T-f = 117 K and a transition
region of Delta T = 55 K. The nu(Fe-His) Raman band of human deoxyhemo
globin was decomposed into seven sublines with frequencies at 195, 202
, 211, 218, 226, 234, and 240 cm(-1), with half-widths of 12 cm(-1). W
hile the low-frequency sublines are strong at 300 K, the high-frequenc
y sublines dominate the band at cryogenic temperatures. In comparison,
we also investigated the temperature dependence of the near-infrared
band III at 760 nm. Band III of deoxymyoglobin can be decomposed into
two subbands which are 165 cm(-1) apart. The ratio of their absorption
cross sections shows a temperature dependence which parallels that of
the ratio I-3/(I-2 + I-1) of the corresponding Raman sublines. Band I
II of deoxyhemoglobin was decomposed into three subbands, the absorpti
on cross sections of which also depend on temperature, similar to what
has been observed for the nu(Fe-His) subbands. These observations pro
vide strong evidence that the frequency positions of the subbands of b
and III and the nu(Fe-His) sublines are governed by the same coordinat
es. For both proteins investigated, the frequency positions and the ha
lf-widths of the band III subbands depend significantly on temperature
. This is rationalized in terms of an earlier proposed model (Cupane e
t al., Fur. Biophys. J. 21; 385 1993) which assumes that the correspon
ding electronic transition is coupled to a bath of low-frequency modes
. Our data indicate that these modes are harmonic below 130 K but beco
me anharmonic above this temperature. This onset of anharmonic motions
is interpreted as resulting from conformational transitions within th
e protein which affect the prostethic group via heme-protein coupling.
(C) 1996 John Wiley & Sons, Inc.