Dynamics and reactivity of HbXL99 alpha. A cross-linked hemoglobin derivative

Resonance Raman spectroscopy, transient absorption, and fluroescence techniques have been employed to investigate the structure and dynamics of the alpha-cross-linked hemoglobin derivative, HbXL99 alpha. The resonance Raman spectra of the deoxy form of HbXL99 alpha are identical to those of native NbA (VFe-His approximately 222 cm-1), which exhibit a T-state (low affinity) structure regardless of solvent conditions. The resonance Raman spectra of the transient heme photoproduct resulting from CO photolysis from HbXL99 alpha appear to have structures intermediate between deoxy-T and ligand-bound R structures (VFe-His approximately 222 cm-1). Time-resolved resonance Raman data of HbXL99 alpha-CO show that complete CO recombination occurs after approximately 5 ms, with only a small amount of the CO-bound species reforming within approximately 200 ns (geminate recombination). Transient absorption spectra of HbXL99 alpha-O2 indicate that the extent of sub-nanosecond geminate recombination of O2 is also reduced in the cross-linked derivative relative to native HbA. The decrease in tryptophan fluorescence of HbXL99 alpha upon oxygenation further indicates that tertiary structural changes at the alpha 1-beta 2 interface upon ligation are apparently reduced, but not eliminated in the cross-linked derivative relative to HbA.     

Structural characterization of the proximal and distal histidine environment of cytoglobin and neuroglobin

Cytoglobin (Cgb) and neuroglobin (Ngb) are the first examples of hexacoordinated globins from humans and other vertebrates in which a histidine (His) residue at the sixth position of the heme iron is an endogenous ligand in both the ferric and ferrous forms. Static and time-resolved resonance Raman and FT-IR spectroscopic techniques were applied in examining the structures in the heme environment of these globins. Picosecond time-resolved resonance Raman (ps-TR3) spectroscopy of transient five-coordinate heme species produced by the photolysis of carbon monoxide (CO) adducts of Cgb and Ngb showed Fe-His stretching (nu(Fe-His)) bands at 229 and 221 cm(-1), respectively. No time-dependent shift in the nu(Fe-His) band of Cgb and Ngb was detected in the 20-1000 ps time domain, in contrast to the case of myoglobin (Mb). These spectroscopic data, combined with previously reported crystallographic data, suggest that the structure of the heme pocket in Cgb and Ngb is altered upon CO binding in a manner different from that of Mb and that the scales of the structural alteration are different for Cgb and Ngb. The structural property of the heme distal side of the ligand-bound forms was investigated by observing the sets of (nu(Fe-CO), nu(C-O), delta(Fe-C-O)) and (nu(Fe-NO), nu(N-O), delta(Fe-N-O)) for the CO and nitric oxide (NO) complexes of Cgb and Ngb. A comparison of the spectra of some distal mutants of Cgb (H81A, H81V, R84A, R84K, and R84T) and Ngb (H64A, H64V, K67A, K67R, and K67T) showed that the CO adducts of Cgb and Ngb contained three conformers and that the distal His (His81 in Cgb and His64 in Ngb) mainly contributes to the interconversion of the conformers. These structural characteristics of Cgb and Ngb are discussed in relation to their ligand binding and physiological properties.     

Picosecond resonance Raman evidence for unrelaxed heme in the (carbonmonoxy)myoglobin photoproduct

An actively and passively mode-locked Nd:YAG laser, producing 30-ps pulses of 1-mJ energy at 532 nm, has been used to photolyze (carbonmonoxy)myoglobin (MbCO) and generate its resonance Raman spectrum, which was recorded with a vidicon multichannel analyzer. The photoproduct spectrum was obtained by subtraction of the MbCO spectrum, obtained at lower incident power levels. Comparison with the spectrum of deoxyMb, obtained with the same apparatus, revealed frequency downshifts of approximately 4 cm-1, for bands at 1604, 1554, and 1542 cm-1, which are identified with porphyrin skeletal modes v10, v19, and v11. These frequencies are known to correlate inversely with the core size of the porphyrin ring, and the shifts imply a larger core size for the photoproduct than for deoxyMb. Similar shifts have been observed for the (carbonmonoxy)hemoglobin (HbCO) photoproduct; in that case, the shifts persist for longer than 20 ns, whereas they are absent in the MbCO photoproduct spectrum within 7 ns of photolysis. The unrelaxed state of the heme group region is therefore suggested to be maintained by protein forces, which relax more rapidly for Mb than Hb. This may reflect a tighter coupling in Hb of the out-of-plane movement of the Fe atom with the proximal histidine-containing F helix.     

Kinetic, structural, and spectroscopic identification of geminate states of myoglobin: a ligand binding site on the reaction pathway

Elementary steps or geminate states in the reaction of gaseous ligands with transport proteins delineate the trajectory of the ligand and its rebinding to the heme. By use of kinetic studies of the 765-nm optical "conformation" band, three geminate states were identified for temperatures less than approximately 100 K. MbCO, which is accumulated by photolysis between 1.2 and approximately 10 K, was characterized by our previous optical and X-ray absorption studies [Chance, B., Fischetti, R., & Powers, L. (1983) Biochemistry 22, 3820-3829]. Between 10 and approximately 100 K, geminate states that are also identified that have recombination rates of approximately 10(3) s-1 and approximately 10(-5) s-1 (40 K). Thus, it is possible to maintain a steady-state nearly homogeneous population of the slowest recombining geminate state, Mb, by regulated continuous illumination (optical pumping). Both X-ray absorption and resonance Raman studies under similar conditions of optical pumping show that the heme structure around the iron in Mb is similar to that of MbCO. In both geminate states, the iron-proximal histidine distance remains unchanged (+/- 0.02 A) from that of MbCO while the iron to pyrrole nitrogen average distance has not fully relaxed to that of the deoxy state. In MbCO the CO remains close to iron but not bound, and the Fe...CO angle, which is bent in MbCO (127 +/- 4 degrees C), is decreased by approximately 15 degrees [Powers, L., Sessler, J. L., Woolery, G. L., & Chance, B. (1984) Biochemistry 23, 5519-5523]. The CO molecule in Mb, however, has moved approximately 0.7 A further from iron. Computer graphics modeling of the crystal structure of MbCO places the CO in a crevice in the heme pocket that is just large enough for the CO molecule end-on. Above approximately 100 K resonance Raman studies show that this structure relaxes to the deoxy state.     

The formation of hydrogen bond in the proximal heme pocket of HemAT-Bs upon ligand binding

HemAT-Bs is the heme-based O(2) sensor responsible for aerotaxis control in Bacillus subtilis. In this study, we measured the time-resolved resonance Raman spectra of full-length HemAT-Bs wild-type (WT) and Y133F in the deoxy form and the photoproduct after photolysis of CO-bound form. In WT, the nu(Fe-His) band for the 10 ps photoproduct was observed at higher frequency by about 2 cm(-1) compared with that of the deoxy form. This frequency difference is relaxed in hundreds of picoseconds. This time-dependent frequency shift would reflect the conformational change of the protein matrix. On the other hand, Y133F mutant did not show such a substantial nu(Fe-His) frequency shift after photolysis. Since a hydrogen bond to the proximal His induces an up-shift of the nu(Fe-His) frequency, these results indicate that Tyr133 forms a hydrogen bond to the proximal His residue upon the ligand binding. We discuss a functional role of this hydrogen bond formation for the signal transduction in HemAT-Bs.     

Ligand binding to heme proteins: II. Transitions in the heme pocket of myoglobin.

Phenomena occurring in the heme pocket after photolysis of carbonmonoxymyoglobin (MbCO) below about 100 K are investigated using temperature-derivative spectroscopy of the infrared absorption bands of CO. MbCO exists in three conformations (A substrates) that are distinguished by the stretch bands of the bound CO. We establish connections among the A substates and the substates of the photoproduct (B substates) using Fourier-transform infrared spectroscopy together with kinetic experiments on MbCO solution samples at different pH and on orthorhombic crystals. There is no one-to-one mapping between the A and B substates; in some cases, more than one B substate corresponds to a particular A substate. Rebinding is not simply a reversal of dissociation; transitions between B substates occur before rebinding. We measure the nonequilibrium populations of the B substates after photolysis below 25 K and determine the kinetics of B substate transitions leading to equilibrium. Transitions between B substates occur even at 4 K, whereas those between A substates have only been observed above about 160 K. The transitions between the B substates are nonexponential in time, providing evidence for a distribution of substates. The temperature dependence of the B substate transitions implies that they occur mainly by quantum-mechanical tunneling below 10 K. Taken together, the observations suggest that the transitions between the B substates within the same A substate reflect motions of the CO in the heme pocket and not conformational changes. Geminate rebinding of CO to Mb, monitored in the Soret band, depends on pH. Observation of geminate rebinding to the A substates in the infrared indicates that the pH dependence results from a population shift among the substates and not from a change of the rebinding to an individual A substate.     

Investigations of photolysis and rebinding kinetics in myoglobin using proximal ligand replacements

We use laser flash photolysis and time-resolved Raman spectroscopy of CO-bound H93G myoglobin (Mb) mutants to study the influence of the proximal ligand on the CO rebinding kinetics. In H93G mutants, where the proximal linkage with the protein is eliminated and the heme can bind exogenous ligands (e.g., imidazole, 4-bromoimidazole, pyridine, or dibromopyridine), we observe significant effects on the CO rebinding kinetics in the 10 ns to 10 ms time window. Resonance Raman spectra of the various H93G Mb complexes are also presented to aid in the interpretation of the kinetic results. For CO-bound H93G(dibromopyridine), we observe a rapid large-amplitude geminate phase with a fundamental CO rebinding rate that is approximately 45 times faster than for wild-type MbCO at 293 K. The absence of an iron proximal ligand vibrational mode in the 10 ns photoproduct Raman spectrum of CO-bound H93G(dibromopyridine) supports the hypothesis that proximal ligation has a significant influence on the kinetics of diatomic ligand binding to the heme.     

Low pH myoglobin photoproducts.

Recently, there has been interest in determining the conditions under which the iron-histidine bond ruptures in myoglobin at low pH, so that the effect of proximal heme ligation can be studied. A 220-cm-1 Raman mode, assigned to iron-histidine stretching, is clearly visible after photolysis of aqueous MbCO samples below pH4 at room temperature (Sage et al. Biochemistry. 30:1237-1247). In contrast, Iben et al. (Biophys. J. 59:908-919) do not observe this mode upon photolysis of a pH3 MbCO sample in a glycerol/water glass at low temperature. In order to account for both the low temperature and the room temperature experiments, Iben et al. suggest a scheme involving an unusual protonation state of the proximal histidine. Here, we discuss some inconsistencies in their explanation of the room temperature results and offer instead a simple modification of an earlier model. In addition, circular dichroism data are presented that indicate partial unfolding of MbCO in aqueous solution below pH4, and raise questions about the claim of Iben et al. that MbCO remains folded in 75% glycerol at pH3.     

Resonance Raman investigation of the effects of copper binding to iron-mesoporphyrin.histidine-rich glycoprotein complexes.

Histidine-rich glycoprotein (HRG) binds both hemes and metal ions simultaneously with evidence for interaction between the two. This study uses resonance Raman and optical absorption spectroscopies to examine the heme environment of the 1:1 iron-mesoporphyrin.HRG complex in its oxidized, reduced and CO-bound forms in the absence and presence of copper. Significant perturbation of Fe(3+)-mesoporphyrin.HRG is induced by Cu2+ binding to the protein. Specifically, high frequency heme resonance Raman bands indicative of low-spin, six-coordinate iron before Cu2+ binding exhibit monotonic intensity shifts to bands representing high-spin, five-coordinate iron. The latter coordination is in contrast to that found in hemoglobin and myoglobin, and explains the Cu(2+)-induced decrease and broadening of the Fe(3+)-mesoporphyrin.HRG Soret band concomitant with the increase in the high-spin marker band at 620 nm. After dithionite reduction, the Fe(2+)-mesoporphyrin.HRG complex displays high frequency resonance Raman bands characteristic of low-spin heme and no iron-histidine stretch, which together suggest six-coordinate iron. Furthermore, the local heme environment of the complex is not altered by the binding of Cu1+. CO-bound Fe(2+)-mesoporphyrin.HRG exhibits bands in the high and low frequency regions similar to those of other CO-bound heme proteins except that the iron-CO stretch at 505 cm-1 is unusually broad with delta nu approximately 30 cm-1. The dynamics of CO photolysis and rebinding to Fe(2+)-mesoporphyrin.HRG are also distinctive. The net quantum yield for photolysis at 10 ns is low relative to most heme proteins, which may be attributed to very rapid geminate recombination. A similar low net quantum yield and broad iron-CO stretch have so far only been observed in a dimeric cytochrome c' from Chromatium vinosum. Furthermore, the photolytic transient of Fe(2+)-mesoporphyrin.HRG lacks bands corresponding to high-spin, five-coordinate iron as is found in hemoglobin and myoglobin under similar experimental conditions, suggesting iron hexacoordination before CO recombination. These data are consistent with a closely packed distal heme pocket that hinders ligand diffusion into the surrounding solvent.     

Spectroscopic studies of myoglobin at low pH: heme structure and ligation

We explore heme structure and ligation subsequent to a low-pH conformational transition in sperm whale myoglobin. Below pH 4.0, the iron-histidine bond breaks in metMb and deoxyMb. In MbCO, the majority of the iron-histidine bonds remain intact down to pH 2.6; however, the observation of a weak Fe-CO mode at 526 cm-1 indicates that a small fraction of the sample has the histidine replaced by a weak ligand, possibly water. The existence of a sterically hindered CO subpopulation in MbCO and the continued association of the four-coordinate heme with the protein in deoxyMb suggest that the heme pocket remains at least partially intact in the acid-induced conformation. The global pH-dependent conformational change described here is clearly distinguished from the local "closed" to "open" transition described previously in MbCO [Morikis et al. (1989) Biochemistry 28, 4791-4800]. Further observations of the four-coordinate heme state yield insights on the mechanism of heme photoreduction and the assignment of the 760-nm band in deoxyMb.     

UV resonance Raman studies of alpha-nitrosyl hemoglobin derivatives: relation between the alpha 1-beta 2 subunit interface interactions and the Fe-histidine bonding of alpha heme.

Human alpha-nitrosyl beta-deoxy hemoglobin A, alpha(NO)beta(deoxy), is considered to have a T (tense) structure with the low O(2) affinity extreme and the Fe-histidine (His87) (Fe-His) bond of alpha heme cleaved. The Fe-His bonding of alpha heme and the intersubunit interactions at the alpha 1-beta 2 contact of alpha(NO)-Hbs have been examined under various conditions with EPR and UV resonance Raman (UVRR) spectra excited at 235 nm, respectively. NOHb at pH 6.7 gave the UVRR spectrum of the R structure, but in the presence of inositol-hexakis-phosphate (IHP) for which the Fe-His bond of the alpha heme is broken, UVRR bands of Trp residues behaved half-T-like while Tyr bands remained R-like. The half-ligated nitrosylHb, alpha(NO)beta(deoxy), in the presence of IHP at pH 5.6, gave T-like UVRR spectra for both Tyr and Trp, but binding of CO to its beta heme (alpha(NO)beta(CO)) changed the UVRR spectrum to half-T-like. Binding of NO to its beta heme (NOHb) changed the UVRR spectrum to 70% T-type for Trp but almost R-type for Tyr. When the pH was raised to 8.2 in the presence of IHP, the UVRR spectrum of NOHb was the same as that of COHb. EPR spectra of these Hbs indicated that the Fe-His bond of alpha(NO) heme is partially cleaved. On the other hand, the UVRR spectra of alpha(NO)beta(deoxy) in the absence of IHP at pH 8.8 showed the T-like UVRR spectrum, but the EPR spectrum indicated that 40-50% of the Fe-His bond of alpha hemes was intact. Therefore, it became evident that there is a qualitative correlation between the cleavage of the Fe-His bond of alpha heme and T-like contact of Trp-beta 37. We note that the behaviors of Tyr and Trp residues at the alpha 1-beta 2 interface are not synchronous. It is likely that the behaviors of Tyr residues are controlled by the ligation of beta heme through His-beta 92(F8)-->Val-beta 98(FG5)-->Asp-beta 99(G1 )-->Tyr-alpha 42(C7) or Tyr-beta 145(HC2).     

Transient Raman study of horseradish peroxidase. Evidence for a lack of extensive heme pocket relaxation subsequent to carbon monoxide photolysis

Time-resolved resonance Raman spectroscopy is a valuable tool for the study of the dynamics of heme-protein interactions. In particular, the photolysis of a ligand by short laser pulses allows for the examination of the dynamic evolution of heme-protein interactions subsequent to ligand dissociation. To date, such studies have been confined largely to hemoglobins and myoglobins. Here we present the results of the first transient Raman study of a peroxidase. Resonance Raman spectra of horseradish peroxidase were obtained within 10 ns of ligand (CO) photolysis at a variety of pH values. We find that there is only minimal relaxation of the heme pocket of horseradish peroxidase in response to ligand photolysis. This relaxation is pH-dependent and most probably involves the heme vinyl substituents. Such behavior is in sharp contrast to the transient behavior of most hemoglobins and beef heart cytochrome oxidase.     

Structural dynamics of myoglobin: ligand migration among protein cavities studied by Fourier transform infrared/temperature derivative spectroscopy.

Fourier transform infrared (FTIR) spectroscopy in the CO stretch bands combined with temperature derivative spectroscopy (TDS) was used to characterize intermediate states obtained by photolysis of two sperm whale mutant myoglobins, YQR (L29(B10)Y, H64(E7)Q, T67(E10)R) and YQRF (with an additional I107(G8)F replacement). Both mutants assume two different bound-state conformations, A(0) and A(3), which can be distinguished by their different CO bands near 1965 and 1933 cm(-1). They most likely originate from different conformations of the Gln-64 side chain. Within each A substate, a number of photoproduct states have been characterized on the basis of the temperature dependence of recombination in TDS experiments. Different locations and orientations of the ligand within the protein can be distinguished by the infrared spectra of the photolyzed CO. Recombination from the primary docking site, B, near the heme dominates below 50 K. Above 60 K, ligand rebinding occurs predominantly from a secondary docking site, C', in which the CO is trapped in the Xe4 cavity on the distal side, as shown by crystallography of photolyzed YQR and L29W myoglobin CO. Another kinetic state (C") has been identified from which rebinding occurs around 130 K. Moreover, a population appearing above the solvent glass transition at approximately 180 K (D state) is assigned to rebinding from the Xe1 cavity, as suggested by the photoproduct structure of the L29W sperm whale myoglobin mutant. For both the YQR and YQRF mutants, rebinding from the B sites near the heme differs for the two A substates, supporting the view that the return of the ligand from the C', C", and D states is not governed by the recombination barrier at the heme iron but rather by migration to the active site. Comparison of YQR and YQRF shows that access to the Xe4 site (C') is severely restricted by introduction of the bulky Phe side chain at position 107.     

Ligand migration and protein fluctuations in myoglobin mutant L29W

We have determined eight X-ray structures of myoglobin mutant L29W at various experimental conditions. In addition, infrared spectroscopic experiments are presented, which are discussed in the light of the X-ray structures. Two distinct conformations of the CO-ligated protein were identified, giving rise to two stretching bands of heme-bound CO. If L29W MbCO crystals are illuminated around 180 K, a deoxy species is formed. The CO molecules migrate to the proximal side of the heme and remain trapped in the so-called Xe1 cavity upon temperature decrease to 105 K. The structure of this photoproduct is almost identical to the equilibrium high-temperature deoxy Mb structure. If the temperature is cycled to increasingly higher values, CO recombination is observed. Three intermediate structures have been determined during the rebinding process. Efficient recombination occurs only above 180 K, the characteristic temperature for the onset of protein dynamics. Rebinding is remarkably slow because bulky residues His64 and Trp29 block important migration pathways of the CO molecule.     

Rebinding and relaxation in the myoglobin pocket

The infrared stretching bands of carboxymyoglobin (MbCO) and the rebinding of CO to Mb after photodissociation have been studied in the temperature range 10-300 K in a variety of solvents. Four stretching bands imply that MbCO can exist in four substates, A0-A3. The temperature dependences of the intensities of the four bands yield the relative binding enthalpies and and entropies. The integrated absorbances and pH dependences of the bands permit identification of the substates with the conformations observed in the X-ray data (Kuriyan et al., J. Mol. Biol. 192 (1986) 133). At low pH, A0 is hydrogen-bonded to His E7. The substates A0-A3 interconvert above about 180 K in a 75% glycerol/water solvent and above 270 K in buffered water. No major interconversion is seen at any temperature if MbCO is embedded in a solid polyvinyl alcohol matrix. The dependence of the transition on solvent characteristics is explained as a slaved glass transition. After photodissociation at low temperature the CO is in the heme pocket B. The resulting CO stretching bands which are identified as B substates are blue-shifted from those of the A substates. At 40 K, rebinding after flash photolysis has been studied in the Soret, the near-infrared, and the integrated A and B substates. All data lie on the same rebinding curve and demonstrate that rebinding is nonexponential in time from at least 100 ns to 100 ks. No evidence for discrete exponentials is found. Flash photolysis with monitoring in the infrared region shows four different pathways within the pocket B to the bound substates Ai. Rebinding in each of the four pathways B----A is nonexponential in time to at least 10 ks and the four pathways have different kinetics below 180 K. From the time and temperature dependence of the rebinding, activation enthalpy distributions g(HBA) and preexponentials ABA are extracted. No pumping from one A substate to another, or one B substate to another, is observed below the transition temperature of about 180 K. If MbCO is exposed to intense white light for 10-10(3) s before being fully photolyzed by a laser flash, the amplitude of the long-lived states increases. The effect is explained in terms of a hierarchy of substates and substate symmetry breaking. The characteristics of the CO stretching bands and of the rebinding processes in the heme pocket depend strongly on the external parameters of solvent, pH and pressure. This sensitivity suggests possible control mechanisms for protein reactions.     

Time-resolved magnetic circular dichroism spectroscopy of photolyzed carbonmonoxy cytochrome c oxidase (cytochrome aa3).

Nanosecond time-resolved magnetic circular dichroism (TRMCD) and time-resolved natural circular dichroism (TRCD) measurements of photolysis products of the CO complex of eukaryotic cytochrome c oxidase (CcO-CO) are presented. TRMCD spectra obtained at 100 ns and 10 microseconds after photolysis are diagnostic of pentacoordinate cytochrome a3Fe2+, as would be expected for simple photodissociation. Other time-resolved spectroscopies (UV-visible and resonance Raman), however, show evidence for unusual Fea3(2+) coordination after CO photolysis (Woodruff, W. H., O. Einarsdóttir, R. B. Dyer, K. A. Bagley, G. Palmer, S. J. Atherton, R. A. Goldbeck, T. D. Dawes, and D. S. Kliger. 1991. Proc. Nat. Acad. Sci. U.S.A. 88:2588-2592). Furthermore, time-resolved IR experiments have shown that photodissociated CO binds to CuB+ prior to recombining with Fea3(2+) (Dyer, R. B., O. Einarsdóttir, P. M. Killough, J. J. López-Garriga, and W. H. Woodruff. 1989. J. Am. Chem. Soc. 111:7657-7659). A model of the CcO-CO photolysis cycle which is consistent with all of the spectroscopic results is presented. A novel feature of this model is the coordination of a ligand endogenous to the protein to the Fe axial site vacated by the photolyzed CO and the simultaneous breaking of the Fe-imidazole(histidine) bond.     

Response of the local heme environment of (carbonmonoxy)hemoglobin to protein dehydration

The effects of protein dehydration upon the equilibrium and dynamic properties of the heme active site in human hemoglobin (HbA) have been probed by resonance Raman scattering. Spectra of equilibrium carbonmonoxy-HbA and the photolytic heme transient species generated within 10 ns of ligand photolysis have been obtained from thin films of protein in various stages of dehydration. These data provide detailed information concerning the response of the heme and its bonding interactions with both the proximal histidine and carbon monoxide as a function of protein hydration. For protein hydration levels of 0.4-1.0 g of H2O/g of protein, our results indicate that the C = O stretching mode of carbonmonoxy-HbA is dramatically affected by protein hydration levels, thus corroborating the infrared results of Brown et al. [Brown, W. E., Sutcliffe, J. W., & Pulsinelli, P. D. (1983) Biochemistry 22, 2914-2923]. However, we find that both heme skeletal modes and the Fe-C bond strength are largely insensitive to dehydration. Moreover, the proximal pocket geometry (as reflected in the behavior of the Fe-proximal histidine stretching mode) immediately following ligand photolysis was found to be very similar to that of R-state solution hemoglobin. At protein hydration levels below the theoretical monolayer limit, small changes in the resonance Raman spectra of both equilibrium HbCO and the transient heme species generated subsequent to ligand photolysis are detected. These include broadening of the Fe-C stretching mode in equilibrium HbCO and a small shift to lower frequency of the Fe-His mode in the photolytic transient species.(ABSTRACT TRUNCATED AT 250 WORDS)     

Ligand binding to a hemoprotein lacking the distal histidine. The myoglobin from aplysia limacina (Val(E7))

The time course of ligand recombination to the myoglobin from Aplysia limacina, which has Val(E7), was measured following photolysis by flashes of 35 ps to 300 ns with a time resolution of 10 ps or 1 ns. CO shows only biomolecular recombination. O2 has a small geminate reaction with a half-time of tens of picoseconds, but no nanosecond geminate reaction. NO has two picosecond relaxations with half-times of 70 ps (15%) and 1 ns (80%) and one nanosecond relaxation with a half-time of 4.6 ns. The biomolecular rates for O2 and NO are the same: 2 x 10(7) M-1 s-1. Methyl and ethyl isonitriles have a geminate reaction with a half-time of 35 ps. Ethyl isonitrile has, in addition, a nanosecond relaxation (25%) with a half-time of 100 ns. t-Butyl isonitrile has four geminate relaxations (10 ps, 35 ps, 1 ns, and 1 microseconds). Analysis of the results suggests much easier movement of ligand between the heme pocket and the exterior than in sperm whale myoglobin (His(E7]. The reactivity of the heme is little different, placing the effect of the differences from sperm whale myoglobin on the distal side of the heme.     

Structural heterogeneity of the Fe(2+)-N epsilon (HisF8) bond in various hemoglobin and myoglobin derivatives probed by the Raman-active iron histidine stretching mode.

We have examined the Fe(2+)-N epsilon (HisF8) complex in hemoglobin A (HbA) by measuring the band profile of its Raman-active nu Fe-His stretching mode at pH 6.4, 7.0, and 8.0 using the 441-nm line of a HeCd laser. A line shape analysis revealed that the band can be decomposed into five different sublines at omega 1 = 195 cm-1, omega 2 = 203 cm-1, omega 3 = 212 cm-1, omega 4 = 218 cm-1, and omega 5 = 226 cm-1. To identify these to the contributions from the different subunits we have reanalyzed the nu Fe-His band of the HbA hybrids alpha(Fe)2 beta(Co)2 and alpha(Co)2 beta(Fe)2 reported earlier by Rousseau and Friedman (D. Rousseau and J. M. Friedman. 1988. In Biological Application on Raman Spectroscopy. T. G. Spiro, editor, 133-216). Moreover we have reanalyzed other Raman bands from the literature, namely the nu Fe-His band of the isolated hemoglobin subunits alpha SH- and beta SH-HbA, various hemoglobin mutants (i.e., Hb(TyrC7 alpha-->Phe), Hb(TyrC7 alpha-->His), Hb M-Boston and Hb M-Iwate), N-ethylmaleimide-des(Arg141 alpha) hemoglobin (NES-des(Arg141 alpha)HbA) and photolyzed carbonmonoxide hemoglobin (Hb*CO) measured 25 ps and 10 ns after photolysis. These molecules are known to exist in different quaternary states. All bands can be decomposed into a set of sublines exhibiting frequencies which are nearly identical to those found for deoxyhemoglobin A. Additional sublines were found to contribute to the nu Fe-His band of NES-des(Arg141 alpha) HbA and the Hb*CO species. The peak frequencies of the bands are determined by the most intensive sublines. Moreover we have measured the nu Fe-His band of deoxyHbA at 10 K in an aqueous solution and in a 80% glycerol/water mixture. Its subline composition at this temperature depends on the solvent and parallels that of more R-like hemoglobin derivatives. We have also measured the optical charge transfer band III of deoxyHbA at room temperature and found, that at least three subbands are required to fit its asymmetric band shape. This corroborates the findings on the nu Fe-His band in that it is indicative of a heterogeneity of the Fe(2+)-N epsilon(HisF8) bond. Finally we measured the nu Fe-His band of horse heart deoxyMb at different temperatures and decomposed it into three different sublines. In accordance with what was obtained for HbA their intensities rather than their frequencies are temperature-dependent.(ABSTRACT TRUNCATED AT 400 WORDS)