Investigations of optical line shapes and kinetic hole burning in myoglobin.

We present the results of an extensive investigation of the optical line shapes of deoxymyoglobin (Mb), the ligand-bound form (MbCO), and the low-temperature photoproduct (Mb*). The thermal properties and the pH dependence of the Soret band and the near infrared band III (approximately 760 nm) are analyzed, taking into account the underlying vibrational properties of the absorption bands. The strong temperature dependence associated with the Soret band of MbCO and band III of Mb indicates significant coupling to low-frequency modes that may not be directly observed in the resonance Raman spectra. On the basis of analogous line-shape studies in a variety of heme systems, we assign the low-frequency coupling in MbCO to torsional motions of the CO molecule. The low-frequency mode coupled to band III (approximately 70 cm-1) is found to lie quite close to the value for the heme-doming motion (approximately 50 cm-1) calculated by using the kinetically determined value of the force constant (17 N/m). Significant inhomogeneous broadening in the Soret region of Mb and Mb* is found to be due to a "nonkinetic" coordinate that we associate with the orientation of the proximal histidine. A "kinetic" coordinate, associated with the equilibrium displacement of the iron atom from the porphyrin plane (a) is found to contribute to the inhomogeneous broadening of both the Soret band and band III. The relaxation of the heme as the system evolves from from Mb* to Mb is followed optically as a function of temperature, and a sharp transition temperature is found at 185 K. The blue shifts of the Soret band and band III as Mb* evolves to Mb are found to be nearly identical (delta v*ABS approximately 140 cm-1) and attributed to changes in the mean value of a between Mb* (a*0) and Mb (a0 = 0.45 A). A simple quadratic model for the coordinate coupling that simultaneously accounts for the observed shift, delta v*ABS, the low-temperature kinetics and the kinetic hole burning predicts a*0 = 0.2 +/- 0.05 A and EA = 16 +/- 2 kJ/mol for the room temperature Arrhenius barrier height at the heme. A simple quantitative method for the analysis of kinetic hole-burning experiments is also developed and applied to recent studies involving quaternary and subunit-specific hemoglobin structures.     

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.     

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.     

Investigation of laser-induced long-lived states of photolyzed MbCO

We present evidence from resonance Raman and absorption measurements that the extended exposure of MbCO to CW laser light at low temperatures alters the CO rebinding kinetics and leads to a significantly increased population of very long lived states of photolyzed MbCO. This optical "pumping" process is observed for samples frozen in both aqueous buffer and glycerol/buffer and exhibits power law behavior with a very weak temperature dependence. A comparison of the nonexponential rebinding kinetics of CO molecules from the pumped states with the rebinding observed in flash photolysis experiments suggests that the pumped states are distinct geminate states, not observed in flash photolysis experiments. Thus, a four-state model, with two geminate states, is implicated for MbCO. Pumped states may represent "separated geminate pair" states with the CO molecule still in the heme pocket or possibly trapped within a cavity on its way through the protein matrix, consistent with molecular dynamics simulations. The possibility of significant deoxyheme relaxation from a less domed to a more domed configuration, as a result of the multiple photolysis events associated with the pumping process, is also explored. However, the small changes observed in the Soret band line shape and position subsequent to pumping at T less than 180 K tend to rule out this explanation for the pumping process. Since the yield for creating a pumped state is small (e.g., less than 10(-7) for T greater than 100 K), pumping can be observed only after extended illumination and is absent in flash photolysis measurements, even after multiple flashes. At higher temperatures (T greater than 180 K), the escape of the CO molecule to the solvent is observed. Our data are consistent with a "phase transition" of the protein that is coupled to the surrounding matrix. The protein fluctuations are quenched below approximately 185 K for a solvent composed of 70% glycerol and below approximately 260 K for aqueous buffer. We also present the first large amplitude measurements of CO rebinding from the protein exterior, observed below 200 K after freezing the sample under laser illumination.     

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.     

Pressure effects on the proximal heme pocket in myoglobin probed by Raman and near-infrared absorption spectroscopy.

The influence of high pressure on the heme protein conformation of myoglobin in different ligation states is studied using Raman spectroscopy over the temperature range from 30 to 295 K. Photostationary experiments monitoring the oxidation state marker bands demonstrate the change of rebinding rate with pressure. While frequency changes of vibrational modes associated with rigid bonds of the porphyrin ring are <1 cm(-1), we investigate a significant shift of the iron-histidine mode to higher frequency with increasing pressure (approximately 3 cm(-1) for deltaP = 190 MPa in Mb). The observed frequency shift is interpreted structurally as a conformational change affecting the tilt angle between the heme plane and the proximal histidine and the out-of-plane iron position. Independent evidence for iron motion comes from measurements of the redshift of band III in the near-infrared with pressure. This suggests that at high pressure the proximal heme pocket and the protein are altered toward the bound state conformation, which contributes to the rate increase for CO binding. Raman spectra of Mb and photodissociated MbCO measured at low temperature and variable pressure further support changes in protein conformation and are consistent with glasslike properties of myoglobin below 160 K.     

Ligand binding to heme proteins. V. Light-induced relaxation in proximal mutants L89I and H97F of carbonmonoxymyoglobin.

We have studied the proximal mutants L89I and H97F of MbCO with FTIR and temperature-derivative spectroscopy at temperatures between 10 and 160 K. The mutations give rise only to minor alterations of the stretch spectra of the bound and photodissociated CO ligand. The most pronounced difference is a larger population in the A3 substate at approximately 1930 cm-1 in the mutants. The barrier distributions, as determined by temperature-derivative spectroscopy, are very similar to native MbCO after short illumination. Extended illumination leads to substantial increases of the rebinding barriers in native MbCO and the proximal mutants. A larger fraction of light-relaxed states is found in the proximal mutants, implying that the conformational energy landscape has been modified to more easily allow light-induced transitions. These and other spectroscopic data imply that the large changes in the binding properties are brought about by a light-induced conformational relaxation involving the structure at the heme iron. Similarities with spectral hole-burning studies and physical models are discussed.     

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.     

Ligand binding and protein relaxation in heme proteins: a room temperature analysis of NO geminate recombination

Ultrafast absorption spectroscopy is used to study heme-NO recombination at room temperature in aqueous buffer on time scales where the ligand cannot leave its cage environment. While a single barrier is observed for the cage recombination of NO with heme in the absence of globin, recombination in hemoglobin and myoglobin is nonexponential. Examination of hemoglobin with and without inositol hexaphosphate points to proximal constraints as important determinants of the geminate rebinding kinetics. Molecular dynamics simulations of myoglobin and heme-imidazole subsequent to ligand dissociation were used to investigate the transient behavior of the Fe-proximal histidine coordinate and its possible involvement in geminate recombination. The calculations, in the context of the absorption measurements, are used to formulate a distinction between nonexponential rebinding that results from multiple protein conformations (substates) present at equilibrium or from nonequilibrium relaxation of the protein triggered by a perturbation such as ligand dissociation. The importance of these two processes is expected to depend on the time scale of rebinding relative to equilibrium fluctuations and nonequilibrium relaxation. Since NO rebinding occurs on the picosecond time scale of the calculated myoglobin relaxation, a time-dependent barrier is likely to be an important factor in the observed nonexponential kinetics. The general implications of the present results for ligand binding in heme proteins and its time and temperature dependence are discussed. It appears likely that, at low temperatures, inhomogeneous protein populations play an important role and that as the temperature is raised, relaxation effects become significant as well.     

Dioxygen replacement reaction in myoglobin

The replacement reaction of myoglobin (Mb), MbCO + O2 leads to MbO2 + CO leads to MbCO + O2, has been studied with flash photolysis in the temperature range from 140 to 320 K and the time range from 2 mus to 200 s. In a fraction of the Mb, the photodissociated CO remains within the protein; rebinding is not affected by the presence of O2 and occurs with rates that are identical with the ones observed earlier in solvents containing only CO. In the remaining fraction CO migrates into the solvent and Mb combines preferentially with oxygen. The rate of the subsequent replacement of O2 by CO permits calculation of the oxygen dissociation rate ko2; ko2 has been determined from 260 to 320 K. The measurements support a multibarrier model.     

Two-dimensional distributions of activation enthalpy and entropy from kinetics by the maximum entropy method.

The maximum entropy method (MEM) is used to numerically invert the kinetics of ligand rebinding at low temperatures to obtain the underlying two-dimensional distribution of activation enthalpies and entropies, g(H,S). A global analysis of the rebinding of carbon monoxide (CO) to myoglobin (Mb), monitored in the Soret band at temperatures from 60 to 150 K, is performed using a Newton-Raphson optimization algorithm. The MEM approach describes the data much better than traditional least-squares analyses, reducing chi 2 by an order of magnitude. The MEM resolves two barrier distributions suggestive of rebinding to different bound conformations of MbCO, the so-called A1 and A3 substates, whose activation barriers have been independently estimated from kinetics monitored in the infrared. The distribution corresponding to A3 possesses higher activation entropies, also consistent with infrared measurements. Within an A substate, correlations of S and H are recovered qualitatively from simulated data but can be difficult to obtain from experimental data. When the rebinding measured at 60 K is excluded from the inversion, two peaks are no longer clearly resolved. Thus, data of very high quality are required to unambiguously determine the kinetic resolvability of subpopulations and the shape of the barrier distribution for a single A substate.     

Dynamics of dioxygen and carbon monoxide binding to soybean leghemoglobin

The association of dioxygen and carbon monoxide to soybean leghemoglobin (Lb) has been studied by laser flash photolysis at temperatures from 10 to 320 K and times from 50 ns to 100 s. Infrared spectra of the bound and the photodissociated state were investigated between 10 and 20 K. The general features of the binding process in leghemoglobin are similar to the ones found in myoglobin. Below about 200 K, the photodissociated ligands stay in the heme pocket and rebinding is not exponential in time, implying a distributed enthalpy barrier between pocket and heme. At around 300 K, ligands migrate from the solvent through the protein to the heme pocket, and a steady state is set up between the ligands in the solvent and in the heme pocket. The association rate, lambda on, is mainly controlled by the final binding step at the heme, the bond formation with the heme iron. Differences between Lb and other heme proteins show up in the details of the various steps. The faster association rate in Lb compared to sperm whale myoglobin (Mb) is due to a faster bond formation. The migration from the solvent to the heme pocket is much faster in Lb than in Mb. The low-temperature binding (B----A) and the infrared spectra of CO in the bound state A and the photodissociated state B are essentially solvent-independent in Mb, but depend strongly on solvent in Lb. These features can be correlated with the x-ray structure.     

Conformational relaxation in hemoproteins: the cytochrome P-450cam case

Photodissociation of (CO)P-450(cam)(substrate) complexes was found to trigger a conformational relaxation process that interferes with ligand rebinding at temperatures as low as 140 K even though the protein conformational substates (CS(1)) remain frozen. To analyze the rebinding and relaxation kinetics, we developed a model that takes the distribution of relaxation rates explicitly into account and in which rebinding and relaxation rates are connected by a linear free energy relation. In all complexes heme relaxation occurs first and is probably faster than 100 ns even at 77 K. This is the only process found in substrate-free P-450(cam). Above 140 K and in the presence of a substrate, this initial, fast rebinding state (P) progressively relaxes to another state (P degrees ) in which rebinding is slower. The relaxation rate is independent of solvent rigidity and is governed by the protein's internal dynamics. Rebinding enthalpies in P and P degrees as well as the enthalpy shift brought about by relaxation correlate with the substrate propensity to block access to the iron site. In P degrees the barrier is higher because the substrate is closer to the heme normal and exerts more steric repulsion for CO binding. The relaxation process implies the return of substrate and heme to their ligand-free positions in which access to the heme is reduced.     

Dynamics of ligand binding to myoglobin.

Myoglobin rebinding of carbon monoxide and dioxygen after photodissociation has been observed in the temperature range between 40 and 350 K. A system was constructed that records the change in optical absorption at 436 nm smoothly and without break between 2 musec and 1 ksec. Four different rebinding processes have been found. Between 40 and 160 K, a single process is observed. It is not exponential in time, but approximately given by N(t) = (1 + t/to)-n, where to and n are temperature-dependent, ligand-concentration independent, parameters. At about 170 K, a second and at 200 K, a third concentration-independent process emerge. At 210 K, a concentration-dependent process sets in. If myoglobin is embedded in a solid, only the first three can be seen, and they are all nonexponential. In a liquid glycerol-water solvent, rebinding is exponential. To interpret the data, a model is proposed in which the ligand molecule, on its way from the solvent to the binding site at the ferrous heme iron, encounters four barriers in succession. The barriers are tentatively identified with known features of myoglobin. By computer-solving the differential equation for the motion of a ligand molecule over four barriers, the rates for all important steps are obtained. The temperature dependences of the rates yield enthalpy, entropy, and free-energy changes at all barriers. The free-energy barriers at 310 K indicate how myoglobin achieves specificity and order. For carbon monoxide, the heights of these barriers increase toward the inside; carbon monoxide consequently is partially rejected at each of the four barriers. Dioxygen, in contrast, sees barriers of about equal height and moves smoothly toward the binding site. The entropy increases over the first two barriers, indicating a rupturing of bonds or displacement of residues, and then smoothly decreases, reaching a minimum at the binding site. The magnitude of the decrease over the innermost barrier implies participation of heme and/or protein. The nonexponential rebinding observed at low temperatures and in solid samples implies that the innermost barrier has a spectrum of activation energies. The shape of the spectrum has been determined; its existence can be explained by assuming the presence of many conformational states for myoglobin. In a liquid at temperatures above about 230 K, relaxation among conformational states occurs and rebinding becomes exponential.     

Competition with Xenon Elicits Ligand Migration and Escape Pathways in Myoglobin

Evidence for ligand migration toward the xenon-binding cavities in myoglobin comes from a number of laser photolysis studies of MbO₂ including mutants and from cryo- and time-resolved crystallography of MbCO. To explore ligand migration in greater detail, we investigated the rebinding kinetics of both MbO₂ and MbCO under a xenon partial pressure ranging from 1 to 16 atm over the temperature range (293–77 K). Below 180 K xenon affects to a significant, but minor, extent the thermodynamic parameters for rebinding from the primary docking site in each Mb taxonomic substate. Above 200 K the ligand migrates to the proximal Xe1 site but when the latter is occupied by xenon a new kinetic process appears. It is attributed to rebinding from transient docking sites located on the path between the primary and the secondary docking site of both ligands. Ligand escape exhibits a more complicated pattern than expected. At room temperature O₂ and CO escape appears to take place exclusively from the primary site. In contrast, at T ≈ 250 K, roughly 50% of the CO molecules that have escaped from the protein originate from the Xe1 secondary site.     

Carboxy Mb at pH 3. Time-resolved resonance Raman study at cryogenic temperatures.

Cryogenic samples of MbCO at pH3 are studied using nanosecond and picosecond time-resolved resonance Raman spectroscopy. It is observed that under excitation conditions sufficient to completely photodissociate MbCO at pH7, the pH3 sample at 10 ns remains substantially unphotolyzed even at 15 K. The similarity in the optical and resonance Raman spectra of MbCO at pH3 with that of pH7 indicates that at pH3 the iron remains six-coordinate and low-spin. The Fe-CO stretch frequency is consistent with a more upright CO orientation. The absence of the v(Fe-His) band in the 30 ps photoproduct Raman spectrum suggests that the Fe-His(F8) bond is broken within 30 ps of photodissociation. Other Raman bands, though, are not consistent with a normal four-coordinate heme for the photoproduct, Mb*. Suggested possible interpretations include a four-coordinate heme highly perturbed by the close lying protonated proximal histidine or a five-coordinate heme with the Fe-His bond significantly weakened. The partial photolysis monitored at 30 ps and 100 K indicates either a significant amount of geminate recombination within 30 ps or low quantum yield or photolysis. The time course for CO recombination is monitored via the Raman spectra from 30 ps to 3 ns at 100 K and 160 K. Of the fraction of protein-ligand pairs that remain photodissociated at 30 ps, 50% recombine by approximately 250 ps at 100 K and 160 K, supporting the flash photolysis rebinding data of Cowen et al. (Cowen, B. R. 1990. Ph. D. thesis. University of Illinois at Urbana-Champaign; Cowen, B. R., D. Braunstein, H. Frauenfelder, P. J. Steinbach, and R. D. Young. 1989. Biophys. J. 55:55a. [Abstr.].) The conclusions from these resonance Raman studies are extended to solution phase studies at ambient temperatures.     

Ligand binding to heme proteins. VI. Interconversion of taxonomic substates in carbonmonoxymyoglobin.

The kinetic properties of the three taxonomic A substates of sperm whale carbonmonoxy myoglobin in 75% glycerol/buffer are studied by flash photolysis with monitoring in the infrared stretch bands of bound CO at nu(A0) approximately 1967 cm-1, nu(A1) approximately 1947 cm-1, and nu(A3) approximately 1929 cm-1 between 60 and 300 K. Below 160 K the photodissociated CO rebinds from the heme pocket, no interconversion among the A substates is observed, and rebinding in each A substate is nonexponential in time and described by a different temperature-independent distribution of enthalpy barriers with a different preexponential. Measurements in the electronic bands, e.g., the Soret, contain contributions of all three A substates and can, therefore, be only approximately modeled with a single enthalpy distribution and a single preexponential. The bond formation step at the heme is fastest for the A0 substate, intermediate for the A1 substate, and slowest for A3. Rebinding between 200 and 300 K displays several processes, including geminate rebinding, rebinding after ligand escape to the solvent, and interconversion among the A substates. Different kinetics are measured in each of the A bands for times shorter than the characteristic time of fluctuations among the A substates. At longer times, fluctuational averaging yields the same kinetics in all three A substates. The interconversion rates between A1 and A3 are determined from the time when the scaled kinetic traces of the two substates merge. Fluctuations between A1 and A3 are much faster than those between A0 and either A1 or A3, so A1 and A3 appear as one kinetic species in the exchange with A0. The maximum-entropy method is used to extract the distribution of rate coefficients for the interconversion process A0 <--> A1 + A3 from the flash photolysis data. The temperature dependencies of the A substate interconversion processes are fitted with a non-Arrhenius expression similar to that used to describe relaxation processes in glasses. At 300 K the interconversion time for A0 <--> A1 + A3 is 10 microseconds, and extrapolation yields approximately 1 ns for A1 <--> A3. The pronounced kinetic differences imply different structural rearrangements. Crystallographic data support this conclusion: They show that formation of the A0 substate involves a major change of the protein structure; the distal histidine rotates about the C(alpha)-C(beta) bond, and its imidazole sidechain swings out of the heme pocket into the solvent, whereas it remains in the heme pocket in the A1 <--> A3 interconversion. The fast A1 <--> A3 exchange is inconsistent with structural models that involve differences in the protonation between A1 and A3.     

Myoglobin mutants giving the largest geminate yield in CO rebinding in the nanosecond time domain.

We have measured the rebinding of carbon monoxide (CO) to some distal mutants of myoglobin (Mb) in the time range from 10(-8) to 10(-1) s by flash photolysis, in which the photodissociated CO rebinds to the heme iron without escaping to the solvent water from the protein matrix. We have found that the double mutants [His64-->Val/Val68-->Thr (H64V/V68T) and His64-->Val/Val68-->Ser (H64V/V68S)] have an extremely large geminate yield (70-80%) in water at 5 degreesC, in contrast to the 7% of the geminate yield of wild-type Mb. The CO geminate yields for these two mutants are the largest in those of Mb mutants reported so far, showing that the two mutants have a unique heme environment that favors CO geminate rebinding. Comparing the crystal structures and 1H-NMR and vibrational spectral data of H64V/V68T and H64V/V68S with those of other mutants, we discuss factors that may control the nanosecond geminate CO rebinding and CO migration in the protein matrix.     

Structural fluctuations of myoglobin from normal-modes,M?ssbauer,Raman, and absorption spectroscopy.

A normal-mode analysis of carbon monoxymyoglobin (MbCO) and deoxymyoglobin (Mb) with 170 water molecules is performed for (54)Fe and (57)Fe. A projection is defined that extracts iron out-of-plane vibrational modes and is used to calculate spectra that can be compared with those from resonance Raman scattering. The calculated spectra and the isotopic shift (57)Fe versus (54)Fe agree with the experimental data. At low temperatures the average mean square fluctuations (MSFs) of the protein backbone atoms agree with molecular dynamics simulation. Below 180 K the MSFs of the heme iron agree with the data from Mossbauer spectroscopy. The MSFs of the iron atom relative to the heme are an order of magnitude smaller than the total MSFs of the iron atom. They agree with the data from optical absorption spectroscopy. Thus the MSFs of the iron atom as measured by Mossbauer spectroscopy can be used to probe the overall motion of the heme within the protein matrix, whereas the Gaussian thermal line broadening of the Soret band and the resonance Raman bands can be used to detect local intramolecular iron-porphyrin motions.     

Dynamics of ligand rebinding to unfolded MbCO by guanidine HCl

Femtosecond vibrational spectroscopy was used to probe a functionally important dynamics and residual structure of myoglobin unfolded by 4 M guanidine HCl. The spectra of the dissociated CO indicated that the residual structure of unfolded myoglobin (Mb) forms a few hydrophobic cavities that could accommodate the dissociated ligand. Geminate rebinding (GR) of CO to the unfolded Mb is three-orders-of-magnitude faster and more efficient than the native Mb but similar to a model heme in a viscous solvent, suggesting that the GR of CO to heme is accelerated by the longer retention of the dissociated ligand near the Fe atom by the poorly-structured protein matrix of the unfolded Mb or viscous solvent. The inefficient GR of CO in native Mb, while dissociated CO is trapped in the primary heme pocket located near the active binding site, indicates that the tertiary structure of the pocket in native Mb plays a functionally significant role.