Rates of energy transfer between tryptophans and hemes in hemoglobin, assuming that the heme is a planar oscillator.

Using the Förster equations we have estimated the rate of energy transfer from tryptophans to hemes in hemoglobin. Assuming an isotropic distribution of the transition moments of the heme in the plane of the porphyrin, we computed the orientation factors and the consequent transfer rates from the crystallographic coordinates of human oxy- and deoxy-hemoglobin. It appears that the orientation factors do not play a limiting role in regulating the energy transfer and that the rates are controlled almost exclusively by the intrasubunit separations between tryptophans and hemes. In intact hemoglobin tetramers the intrasubunit separations are such as to reduce lifetimes to 5 and 15 ps/ns of tryptophan lifetime. Lifetimes of several hundred picoseconds would be allowed by the intersubunit separations, but intersubunits transfer becomes important only when one heme per tetramer is absent or does not accept transfer. If more than one heme per tetramer is absent lifetimes of more than 1 ns would appear.     

Fluorescence and energy transfer of tryptophans in Aplysia myoglobin.

The fluorescence decay of tryptophan residues in apo and met Aplysia limacina myoglobin and sperm whale myoglobin were measured in aqueous solution at 10 degrees-15 degrees C. In all species, multiexponential behavior was observed in which the individual components displayed unique frequency-dependent emission characteristics. The results suggest that the tryptophan fluorescence in all met samples are quenched by rapid Forster energy transfer to the heme as predicted from the crystal geometry. Fluorescence from the apo protein is similar to that in solutions of free tryptophans. In addition, the fluorescence properties of the reversible thermal denaturation of Aplysia limacina met myoglobin was investigated between 25 degrees and 75 degrees C.     

Energy transfer between tryptophans and aromatic ligands in apomyoglobin

The binding of three aromatic molecules to apomyoglobin has been investigated. In each case equilibrium dialysis studies and tryptophan fluorescence quenching studies indicate that a one to one complex has been formed. The fluorescence quenching studies further suggest that the binding of the aromatic molecules is at the heme site with possible involvement of the arginine CD3. Xenon, which is known to quench the fluorescence of aromatic hydrocarbons, is found to be bound to apomyoglobin-aromatic molecule complexes and quenches the emission of the aromatic molecule in the complexes. Oxygen quenches pyrene fluorescence in water solution but does not quench the pyrene fluorescence from the apomyoglobin-pyrene complex. This is explained by a slower rate of diffusion of oxygen to pyrene in the apomyoglobin-pyrene complex.     

Proton magnetic resonance study of the influence of heme 2,4 substituents on the exchange rates of labile protons in the heme pocket of myoglobin.

Four exchangeable protons with large hyperfine shifts are assigned in the heme pocket of sperm whale met-cyano myoglobin reconstituted with heme possessing acetyl groups, ethyl groups, bromines, and hydrogens at the 2,4 position, using both relaxation and chemical-shift data. The four protons arise from the ring NH's of the proximal (F8), distal (E7), and FG2 histidines, and the peptide NH of His F8. The similarity of all chemical shifts to those of the native protein as well as the invariance of the relaxation rates of the distal histidyl ring NH dictate essentially the same structure for the heme cavity of both native and reconstituted proteins. The exchange rates with bulk water of the four labile proteins in each modified protein were determined by saturation-transfer and line width methods. All four labile protons were found to have the same exchange rate as in the native protein for acetyl and ethyl 2,4 substituents; the two resolved labile protons in the derivative with 2,4 bromine were also unchanged. The reconstituted protein with hydrogens at the 2,4 position exhibited slower exchange rates for three of the four protons, indicating an increased dynamic stability of the heme pocket in the absence of bulky 2,4 substituents.     

Spectroscopic characterization of heme A reconstituted myoglobin.

The focus of this study was to examine the functional role of the unusual peripheral substitution of heme A. The effects of heme A stereochemistry on the reconstitution of the porphyrin have been examined in the heme A-apo-myoglobin complex using optical absorption and resonance Raman and electron paramagnetic resonance spectroscopies. The addition of one equivalent of heme A to apo-Mb produces a complex which displays spectroscopic signals consistent with a distribution of high- and low-spin heme chromophores. These results indicate that the incorporation of heme A into apo-Mb significantly perturbs the protein refolding.     

EPR and ENDOR studies of cryoreduced compounds II of peroxidases and myoglobin. Proton-coupled electron transfer and protonation status of ferryl hemes

The nature of the [Fe(IV)-O] center in hemoprotein Compounds II has recently received considerable attention, as several experimental and theoretical investigations have suggested that this group is not necessarily the traditionally assumed ferryl ion, [Fe(IV)=O]2+, but can be the protonated ferryl, [Fe(IV)-OH]3+. We show here that cryoreduction of the EPR-silent Compound II by gamma-irradiation at 77 K produces Fe(III) species retaining the structure of the precursor [Fe(IV)=O]2+ or [Fe(IV)-OH]3+, and that the properties of the cryogenerated species provide a report on structural features and the protonation state of the parent Compound II when studied by EPR and 1H and 14N ENDOR spectroscopies. To give the broadest view of the properties of Compounds II we have carried out such measurements on cryoreduced Compounds II of HRP, Mb, DHP and CPO and on CCP Compound ES. EPR and ENDOR spectra of cryoreduced HRP II, CPO II and CCP ES are characteristic of low-spin hydroxy-Fe(III) heme species. In contrast, cryoreduced "globins", Mb II, Hb II, and DHP II, show EPR spectra having lower rhombicity. In addition the cryogenerated ferric "globin" species display strongly coupled exchangeable (1)H ENDOR signals, with A max approximately 20 MHz and a iso approximately 14 MHz, both substantially greater than for hydroxide/water ligand protons. Upon annealing at T > 180 K the cryoreduced globin compounds II relax to the low-spin hydroxy-ferric form with a solvent kinetic isotope effect, KIE > 6. The results presented here together with published resonance Raman and Mossbauer data suggest that the high-valent iron center of globin and HRP compounds II, as well as of CCP ES, is [Fe(IV)=O]2+, and that its cryoreduction produces [Fe(III)-O]+. Instead, as proposed by Green and co-workers, CPO II contains [Fe(IV)-OH]3+ which forms [Fe(III)-OH]2+ upon radiolysis. The [Fe(III)-O]+ generated by cryoreduction of HRP II and CCP ES protonate at 77 K, presumably because the heme is linked to a distal-pocket hydrogen bonding/proton-delivery network through an H-bond to the "oxide" ligand. The data also indicate that Mb and HRP compounds II exist as two major conformational substates.     

Molecular dynamics simulations of heme reorientational motions in myoglobin.

Molecular dynamics simulations of 2-ns duration were performed on carbonmonoxymyoglobin and deoxymyoglobin in vacuo to study the reorientational dynamics of the heme group. The heme in both simulations undergoes reorientations of approximately 5 degrees amplitude on a subpicosecond time scale, which produce a rapid initial decay in the reorientational correlation function to about 0.99. The heme also experiences infrequent changes in average orientation of approximately 10 degrees amplitude, which lead to a larger slow decay of the reorientational correlation function over a period of hundreds of picoseconds. The simulations have not converged with respect to these infrequent transitions. However, an estimate of the order parameter for rapid internal motions of the heme from those orientations which are sampled by the simulations suggests that the subnanosecond orientational dynamics of the heme accounts for at least 30% of the unresolved initial anisotropy decay observed in the nanosecond time-resolved optical absorption experiments on myoglobin reported by Ansari et al. in a companion paper (Ansari, A., C.M. Jones, E.R. Henry, J. Hofrichter, and W.A. Eaton. 1992. Biophys. J. 64:852-868.). A more complete sampling of the accessible heme orientations would most likely increase this fraction further. The simulation of the liganded molecule also suggests that the conformational dynamics of the CO ligand may contribute significantly to discrepancies between the ligand conformation as probed by x-ray diffraction and by infrared-optical photoselection experiments. The protein back-bone explores multiple conformations during the simulations, with the largest structural changes appearing in the E and F helices, which are in contact with the heme. The variations in the heme orientation correlate with the conformational dynamics of the protein on a time scale of hundreds of picoseconds, suggesting that the heme orientation may provide a useful probe of dynamical processes in the protein.     

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.     

Electron transfer between heme proteins and ceruloplasmin

Reduced cytochrome-c, reduced myoglobin and oxyhemoglobin respectively have been oxidized to oxidized cytochrome-c, metmyoglobin and methemoglobin by ceruloplasmin. Metmyoglobin and methemoglobin formation was stoichiometric while oxidized cytochrome-c reacted catalytically. Only 50% methemoglobin was formed which suggested that two hemes out of four could transfer electrons. Hydrogen peroxide was formed in the reaction of reduced cytochrome-c with ceruloplasmin.     

Contribution of the heme propionate groups to the electron transfer and electrostatic properties of myoglobin

The role of the heme propionate groups in determining the electron transfer and electrostatic properties of myoglobin have been studied by thermodynamic, kinetic, and spectroscopic studies of horse heart myoglobin in which the heme propionate groups are esterified. Spectroelectrochemical analysis has established that the E_m,7 of dimethylester heme-substituted Mb (DME-Mb) (E_m,7 = 100.2(2) mV vs. NHE (Normal Hydrogen Electrode) (25 °C) is increased  40 mV relative to that of the native protein with ΔH° = −12.9(2) kcal/mol and ΔS° = −51.0(8) cal/mol/deg (pH 7.0, μ = 0.1 M (phosphate)). The second order rate constant for reduction of DME-metMb by Fe(EDTA)²⁻ is increased  > 400-fold relative to that for reduction of native metMb to a value of 1.34(2) × 10³ M⁻¹ s⁻¹ with ΔS^‡ = −13(1) cal/mol/deg and ΔH^‡ = 9.2(3) (pH 7.0, μ = 0.1 M (phosphate)). Analysis of the pH dependences of the reduction potential and rate constant for reduction by Fe(EDTA)²⁻ demonstrates that heme propionate esterification introduces significant changes into the electrostatic interactions in myoglobin. These changes are also manifested by differences in the pH dependences of the ¹H NMR spectra of native and DME-metMb that reveal shifts in pK_a values for specific His residues as the result of heme propionate esterification. In sum, the current results establish that heme propionate esterification not only affects the electron transfer properties of myoglobin but also influences the titration behavior of specific His residues.     

Conformation between the substrate-binding site and heme of cytochrome P-450 studied by excitation energy transfer

The conformation between the substrate-binding site and heme of cytochrome P-450 was studied by excitation energy transfer. Cytochrome P-450 was obtained from the hepatic microsomes of polychlorinated biphenyl-treated male rats, and ten polycyclic aromatic hydrocarbons were used as substrates. The energy transfer from the substrate to the heme of the enzyme was measured according to the F?rster equation. On the basis of the assumption that the substrates are bound at different positions in the plane of the same substrate-binding site, the position of the heme in relation to the substrate-binding site was determined in solution and in the presence of synthetic phospholipid. The results demonstrated that the distance between the substrate-binding site and the heme of cytochrome P-450 was greater when the enzyme was incorporated into micelles of phospholipid than when in solution, and that the conformational relationship of the substrate-binding site towards the heme was changed by an angle of 21 degrees on incorporation of the enzyme into phospholipid micelles.     

Mechanism of electron transfer between myoglobin derivatives and ferricytochrome C

Progress in the studies of the electron transport mechanism in biological systems is greatly hindered by the lack of detailed structural information about the components of these systems. That is why a study of electron transfer between protein molecules with the known spatial organization in model reactions in vitro is of great importance. In this respect the MbO2--Cyt C oxidation-reduction reaction offers unique possibilities. Studies of the effects of pH and ionic strength of the medium on the kinetics of this reaction in combination with chemical modification of single amino acid residues of Mb and Cyt C enabled us to identify those parts of the surface of haemoproteins where the molecules come into "active contact". A variation in the number or/and the arrangement of the charged groups at the "active sites" of the molecules induced by both changing the medium pH and chemical modification of some of these groups lowers markedly the probability of electron transfer in the system (e.g. His GH1 and His A10 in Mb) or blocks it entirely (acylation of Lys 72 (73) or Tyr 74 in Cyt C). Based on the results obtained and on the data of Mb and Cyt C X-ray analysis, the figures of spatial arrangement of the groups at the "active sites" of these molecules are presented.     

The effect of ligand dynamics on heme electronic transition band III in myoglobin.

Band III is a near-infrared electronic transition at ~13,000 cm(-1) in heme proteins that has been studied extensively as a marker of protein conformational relaxation after photodissociation of the heme-bound ligand. To examine the influence of the heme pocket structure and ligand dynamics on band III, we have studied carbon monoxide recombination in a variety of myoglobin mutants after photolysis at 3 K using Fourier transform infrared temperature-derivative spectroscopy with monitoring in three spectral ranges, (1) band III, the mid-infrared region of (2) the heme-bound CO, and (3) the photodissociated CO. Here we present data on mutant myoglobins V68F and L29W, which both exhibit pronounced ligand movements at low temperature. From spectral and kinetic analyses in the mid-infrared, a small number of photoproduct populations can be distinguished, differing in their distal heme pocket conformations and/or CO locations. We have decomposed band III into its individual photoproduct contributions. Each photoproduct state exhibits a different "kinetic hole-burning" (KHB) effect, a coupling of the activation enthalpy for rebinding to the position of band III. The analysis reveals that the heme pocket structure and the photodissociated CO markedly affect the band III transition. A strong kinetic hole-burning effect results only when the CO ligand resides in the docking site on top of the heme group. Migration of CO away from the heme group leads to an overall blue shift of band III. Consequently, band III can be used as a sensitive tool to study ligand dynamics after photodissociation in heme proteins.     

Dynamic analysis of efficient heme rotation in myoglobin by NMR spectroscopy.

Sperm whale myoglobin was reconstituted with 1,4,5,8-tetramethylhemin. The hyperfine-shifted proton NMR signals from the prosthetic group exhibit remarkable pattern changes around 15 degrees C, while the globin resonances are normal to obey the Curie law. The NMR anomaly specifically observed for the heme signals suggests a slow to rapid rotational transition of the hemin about the iron-histidine bond. The temperature-dependent pattern changes were quantitatively analyzed by a dynamic NMR method. Two sets of analyses with the heme-methyl and pyrrole-proton lines consistently afforded delta H not equal to = 16.3 kcal/mol, delta S not equal to = 14.0 e.u., delta G not equal to = 12.1 kcal/mol at 298 K, and a frequency of 90 degrees heme rotation 5600 s-1 at 20 degrees C. The relatively large activation entropy suggests that structural rearrangements at the direct heme vicinity are involved and that efficient heme rotation is accomplished by a number of fluctuative local heme-globin contacts within a conserved crevice structure.     

Substitution of the heme binding module in hemoglobin alpha- and beta-subunits. Implication for different regulation mechanisms of the heme proximal structure between hemoglobin and myoglobin

In our previous work, we demonstrated that the replacement of the "heme binding module," a segment from F1 to G5 site, in myoglobin with that of hemoglobin alpha-subunit converted the heme proximal structure of myoglobin into the alpha-subunit type (Inaba, K., Ishimori, K. and Morishima, I. (1998) J. Mol. Biol. 283, 311-327). To further examine the structural regulation by the heme binding module in hemoglobin, we synthesized the betaalpha(HBM)-subunit, in which the heme binding module (HBM) of hemoglobin beta-subunit was replaced by that of hemoglobin alpha-subunit. Based on the gel chromatography, the betaalpha(HBM)-subunit was preferentially associated with the alpha-subunit to form a heterotetramer, alpha(2)[betaalpha(HBM)(2)], just as is native beta-subunit. Deoxy-alpha(2)[betaalpha(HBM)(2)] tetramer exhibited the hyperfine-shifted NMR resonance from the proximal histidyl N(delta)H proton and the resonance Raman band from the Fe-His vibrational mode at the same positions as native hemoglobin. Also, NMR spectra of carbonmonoxy and cyanomet alpha(2)[betaalpha(HBM)(2)] tetramer were quite similar to those of native hemoglobin. Consequently, the heme environmental structure of the betaalpha(HBM)-subunit in tetrameric alpha(2)[betaalpha(HBM)(2)] was similar to that of the beta-subunit in native tetrameric Hb A, and the structural conversion by the module substitution was not clear in the hemoglobin subunits. The contrastive structural effects of the module substitution on myoglobin and hemoglobin subunits strongly suggest different regulation mechanisms of the heme proximal structure between these two globins. Whereas the heme proximal structure of monomeric myoglobin is simply determined by the amino acid sequence of the heme binding module, that of tetrameric hemoglobin appears to be closely coupled to the subunit interactions.     

X-ray absorption studies of myoglobin peroxide reveal functional differences between globins and heme enzymes

X-ray absorption studies of myoglobin peroxide show that although it is not identical with compound I or II of horseradish peroxidase [Chance, B., Powers, L., Ching, Y., Poulos, T., Yamazaki, I., & Paul, K. G. (1984) Arch. Biochem. Biophys. 235, 596-611], it has some structural features in common with both. As seen in compound I, the Fe-O distance is short, but the iron-pyrrole nitrogen distance is contracted with a longer iron-histidine distance like compound II. The iron has a higher oxidation state than Fe3+, suggesting an oxyferryl ion type species. Comparison of the structures of various peroxidase and myoglobin compounds points out systematic differences that may explain the catalytic activity of the pi cation radical as well as some of the differences between globins and heme enzymes.