FT-Infrared spectroscopic studies of the iron ligand CO stretch mode of iNOS oxygenase domain: effect of arginine and tetrahydrobiopterin

The iron ligand CO stretch vibration mode of the inducible nitric oxide synthase oxygenase domain (iNOSox) has been studied from 20 to 298 K. iNOSox in the absence of arginine reveals a temperature-dependent equilibrium of two major conformational substates with CO stretch bands centered at about 1945 and 1954 cm(-)(1). This behavior is not qualitatively changed when tetrahydrobiopterin (H(4)B) is bound. Arginine binding changes significantly the spectrum by formation of a sharp CO stretch mode band at about 1905 cm(-)(1) and indicates the formation of a hydrogen bond to the CO ligand. For temperatures lower than 250 K, the stretch vibration frequency decreases almost linearly with decreasing temperature and indicates that the coupling between the CO ligand and the arginine/protein in the active site via the hydrogen bond is very strong. Flashphotolysis of the CO ligand carried out at 25 K revealed the CO stretch mode of the photodissociated CO ligand trapped in the heme pocket. There is a negative linear relation between the stretch vibration frequencies of the photodissociated and the iron-bound CO indicating that the photodissociated ligand stays near the heme.     

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.     

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.     

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.     

Assignment of heme and distal amino acid resonances in the 1H-NMR spectra of the carbon monoxide and oxygen complexes of sperm whale myoglobin

Assignments of resonances of the heme and distal amino acid protons in spectra of the CO and O2 complexes of sperm whale myoglobin are reported. These resonances provide information on the conformation of the heme pocket. For oxymyoglobin, the assignments of the heme meso protons disagree with those proposed previously on the basis of partial deuteration experiments. Rapid ring flips about the C beta-C gamma bond are detected for Phe-CD1. Recent claims for two conformational substates of valine-E11 in carbonmonoxymyoglobin (Bradbury, J.H. and Carver, J.A. (1984) Biochemistry 23, 4905-4913) are shown to be in error. The pK of His-97 (FG3) in carbonmonoxymyoglobin has been determined (pK = 5.9). This residue appears to influence many spectroscopic properties of myoglobin. The distal His-E7 in carbonmonoxymyoglobin has pK less than 5.0. Differences in the heme pocket conformation in the CO complexes of myoglobin and leghemoglobin are discussed. These differences may be influential in O2 and CO association reactions.     

Structure and ligand binding properties of leucine 29(B10) mutants of human myoglobin.

Site-specific mutants of human myoglobin (Mb) have been prepared, in which Leu29 (B10) is replaced by Ala(L29A) or Ile(L29I), in order to examine the influence of this highly conserved residue in the hydrophobic clusters of the heme distal site on the heme environmental structure and ligand binding properties of Mb. Structural characterizations of these recombinant Mbs are studied by electronic absorption, infrared (IR), one- and two-dimensional proton nuclear magnetic resonance spectroscopies, and ligand-binding kinetics by laser photolysis measurements under ambient and high pressures (up to 2000 bar). Multiple split carbon monoxide (CO) stretch bands in the IR spectra of mutant Mbs exhibit a relative decrease of the 1945 cm-1 band (approximately 50%) which is associated with an upright binding geometry of CO, accompanied by an increase of the tilted CO conformer at 1932 cm-1. On the basis of these results, replacement of Leu29(B10) by Ala or Ile appears to allow bound CO to rotate from a conformation pointing toward the beta meso carbon of the heme group to the one pointing toward the alpha meso carbon atom, presumably filling the space left by removal of the delta 2 carbon atom of Leu29(B10). These substitutions cause the rate constants for CO and O2 association to decrease almost 3-5-fold. Present results show that CO and O2 bindings to the heme iron of Mb are controlled by Leu29(B10) by influencing the structure of close vicinity of the heme and the geometry of iron-bound ligand. Further, mutant Mbs (Leu72(E15)----Ala and Leu104 (G5)----Ala) which have altered residues in another hydrophobic clusters around proximal and distal site are also examined.     

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.     

Inhomogeneous broadening in spectral bands of carbonmonoxymyoglobin. The connection between spectral and functional heterogeneity.

The rebinding kinetics of CO to myoglobin after flash photolysis is nonexponential in time below approximately 180 K; the kinetics is governed by a distribution of enthalpic barriers. This distribution results from inhomogeneities in the protein conformation, referred to as conformational substates. Hole-burning experiments on the Soret and IR CO-stretch bands test the assumption that an inhomogeneous distribution of conformational substates results in inhomogeneously broadened spectra. CO was slowly photolyzed at different wavelengths in the Soret band at 10 K. Both the Soret band and the CO-stretch band A1, centered at 1,945 cm-1, shift during photolysis, demonstrating that different wavelengths excite different parts of the distributed population. We have also done kinetic hole-burning experiments by measuring peak shifts in the Soret and A1 bands as the CO molecules rebind. The shifts indicate that the spectral and enthalpic distributions are correlated. In the A1 band, the spectral and enthalpic distributions are highly correlated while in the Soret the correlation is weak. From the peak shifts in the spectral and kinetic hole-burning experiments the inhomogeneous broadening is estimated to be approximately 15% of the total width in the Soret band and approximately 60% in A1. We have previously measured the tilt angle alpha between the bound CO and the heme normal (Ormos, P., D. Braunstein, H. Frauenfelder, M. K. Hong, S.-L. Lin, T. B. Sauke, and R. D. Young. 1988. Proc. Natl. Acad. Sci. USA. 85:8492-8496) and observed a wave number dependence of the tilt angles within the CO-stretch A bands. Thus the spectral and enthalpic distributions of the A bands are coupled to a heterogeneity of the structure.     

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.     

A cooperative oxygen binding hemoglobin from Mycobacterium tuberculosis. Stabilization of heme ligands by a distal tyrosine residue

The homodimeric hemoglobin (HbN) from Mycobacterium tuberculosis displays an extremely high oxygen binding affinity and cooperativity. Sequence alignment with other hemoglobins suggests that the proximal F8 ligand is histidine, the distal E7 residue is leucine, and the B10 position is occupied by tyrosine. To determine how these heme pocket residues regulate the ligand binding affinities and physiological functions of HbN, we have measured the resonance Raman spectra of the O(2), CO, and OH(-) derivatives of the wild type protein and the B10 Tyr --> Leu and Phe mutants. Taken together these data demonstrate a unique distal environment in which the heme bound ligands strongly interact with the B10 tyrosine residue. The implications of these data on the physiological functions of HbN and another heme-containing protein, cytochrome c oxidase, are considered.     

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.     

The effects of E7 and E11 mutations on the kinetics of ligand binding to R state human hemoglobin

Association and dissociation rate constants for O2, CO, and methyl isocyanide binding to native and distal pocket mutants of R state human hemoglobin were measured using ligand displacement and partial photolysis techniques. Individual rate constants for the alpha and beta subunits were resolved by comparisons between the kinetic behavior of the native and mutant proteins. His-E7 was replaced with Gly and Gln in both alpha and beta subunits and with Phe in beta subunits alone. In separate experiments Val-E11 was replaced with Ala, Leu, and Ile in each globin chain. The parameters describing ligand binding to R state alpha subunits are sensitive to the size and polarity of the amino acids at positions E7 and E11. The distal histidine in this subunit inhibits the bimolecular rate of binding of both O2 and CO, sterically hinders bound CO and methyl isocyanide, and stabilizes bound O2 by hydrogen bonding. The Val-E11 side chain in alpha chains also appears to be part of the kinetic barrier to O2 and CO binding since substitution with Ala causes approximately 10-fold increases in the association rate constants for the binding of these diatomic ligands. However, substitution of Val-E11 by Ile produces only small decreases in the rates of ligand binding to alpha subunits. For R state beta subunits, the bimolecular rates of O2 and CO binding are intrinsically large, approximately 2-5-fold greater than those for alpha subunits, and with the exception of Val-E11----Ile mutation, little affected by substitutions at either the E7 or E11 positions. For the beta Val-E11----Ile mutant the association rate and equilibrium constants for all three ligands decreased 10-50-fold. All of these results agree with Shaanan's conclusions that the distal pocket in liganded beta subunits is more open whereas in alpha subunits bound ligands are more sterically hindered by adjacent distal residues (Shaanan, B. (1983) J. Mol. Biol. 171, 31-59). In the case of O2 binding to alpha subunits, the unfavorable steric effects are compensated by the formation of a hydrogen bond between the nitrogen atom of His-E7 and bound dioxygen.     

Compressibility and uncoupling of cytochrome P450cam: high pressure FTIR and activity studies

The effect of the hydrostatic pressure on the CO ligand stretch vibration in cytochrome P450cam-CO bound with various substrates is studied by FTIR. The vibration frequency is linearily shifted to lower values with increasing pressure. The slope of the shift gives the isothermal compressibility of the heme pocket and is found to be related to the high-spin state content in an opposite direction to that previously observed from the pressure-induced shift of the Soret band. This opposite behaviour is explained by the dual effect of heme pocket water molecules both on the CO ligand and on electrostatic potentials produced by the protein at the distal side. The latter effect disturbs ligand-distal side contacts which are needed for a specific proton transfer in oxygen activation when dioxygen is the ligand. Their loss results in uncoupled H(2)O(2) formation.     

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.     

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.     

FTIR studies of internal proton transfer reactions linked to inter-heme electron transfer in bovine cytochrome c oxidase

FTIR difference spectroscopy is used to reveal changes in the internal structure and amino acid protonation states of bovine cytochrome c oxidase (CcO) that occur upon photolysis of the CO adduct of the two-electron reduced (mixed valence, MV) and four-electron reduced (fully reduced, FR) forms of the enzyme. FTIR difference spectra were obtained in D(2)O (pH 6-9.3) between the MV-CO adduct (heme a(3) and Cu(B) reduced; heme a and Cu(A) oxidized) and a photostationary state in which the MV-CO enzyme is photodissociated under constant illumination. In the photostationary state, part of the enzyme population has heme a(3) oxidized and heme a reduced. In MV-CO, the frequency of the stretch mode of CO bound to ferrous heme a(3) decreases from 1965.3 cm(-1) at pH* 相似文献   

Infrared absorption study of the heme pocket dynamics of carbonmonoxyheme proteins

The temperature dependencies of the infrared absorption CO bands of carboxy complexes of horseradish peroxidase (HRP(CO)) in glycerol/water mixture at pH 6.0 and 9.3 are interpreted using the theory of optical absorption bandshape. The bands' anharmonic behavior is explained assuming that there is a higher-energy set of conformational substates (CSS(h)), which are populated upon heating and correspond to the protein substates with disordered water molecules in the heme pocket. Analysis of the second moments of the CO bands of the carboxy complexes of myoglobin (Mb(CO)) and hemoglobin (Hb(CO)), and of HRP(CO) with benzohydroxamic acid (HRP(CO)+BHA), shows that the low energy CSS(h) exists also in the open conformation of Mb(CO), where the heme pocket is spacious enough to accommodate a water molecule. In the HRP(CO)+BHA and closed conformations of Mb(CO) and Hb(CO), the heme pocket is packed with BHA and different amino acids, the CSS(h) has much higher energy and is hardly populated even at the highest temperatures. Therefore only motions of these amino acids contribute to the band broadening. These motions are linked to the protein surface and frozen in the glassy matrix, whereas in the liquid solvent they are harmonic. Thus the second moment of the CO band is temperature-independent in glass and is proportional to the temperature in liquid. The temperature dependence of the second moment of the CO peak of HRP(CO) in the trehalose glass exhibits linear coupling to an oscillator. This oscillator can be a moving water molecule locked in the heme pocket in the whole interval of temperatures or a trehalose molecule located in the heme pocket.     

Infrared spectra of carbonyl hemoglobins: characterization of dynamic heme pocket conformers

The infrared spectra for carbon monoxide complexed to hemoglobins were examined in the C-O stretch region. Deconvolution of the spectra requires four bands and supports the presence of four distinct conformers at the ligand binding site. Most typical hemoglobins exhibit only one predominant conformer for each subunit represented by a band at 1951 cm-1 in contrast to myoglobins, which typically exist in two major conformations. Several hemoglobins with an enlarged heme pocket are shown to shift the C-O frequency into the higher frequency conformer regions. Many factors, including pH, temperature, solvents, and divalent metals, are also shown to be capable of expanding the heme pocket. Only very specific structural changes that can reduce the size of the heme pocket will result in the lower frequency conformers. The weighted averages of the multiple CO vibrational frequencies are linearly related to the single 13CO NMR chemical shift values and to the exponential of fast CO on-rates. Conformer interconversion occurs at a rate greater than 10(4) s-1. The infrared C-O stretch spectra provide qualitative and quantitative information on the structural dynamics, stability, and ligand binding properties of hemoglobins.     

EPR studies on the photoinduced intermediates of NO complexes in recombinant ferric-Mb trapped at low temperatures

The nitrosyl complex of ferric myoglobin is EPR-silent. Upon photolysis at low temperatures, the photoinduced intermediates trapped in the distal heme cavity exhibit new EPR spectra due to the interaction between the photodissociated NO (S=1/2) and the ferric high spin heme (S=5/2). In order to elucidate the effect of distal E7 (His64) and E11 (Val68) mutations upon the electronic structure of the metal center, its immediate environment, and its interaction with the photodissociated NO, EPR spectra of the photoproducts of the NO complexes of recombinant ferric Mb mutants were measured at 5 K. EPR spectra of the photoproducts were closely related to the size and/or the polarity of the distal pocket residues. The distal pocket of the E7 mutants seemed to be sterically crowded, even decreasing the side chain volume or changing its hydrophobicity by replacing amino acid at position 64. We have found that the mobility of the photodissociated NO molecule in the distal heme pocket was strongly governed by the nature of the amino acid residue at E11 position.     

Conformational substates and dynamic properties of carbonmonoxy hemoglobin

Heme pocket dynamics of human carbonmonoxy hemoglobin (HbCO) is studied by Fourier transform infrared spectroscopy. The CO stretching band at various temperatures in the interval 300-10 K is analyzed in terms of three taxonomic A substates; however, in HbCO the band attributed to the A(1) taxonomic substate accounts for approximately 90% of the total intensity in the pH range 8.8-4.5. Two different regimes as a function of temperature are observed: below 160 K, the peak frequency and the bandwidth of the A(1) band have constant values whereas, above this temperature, a linear temperature dependence is observed, suggesting the occurrence of transitions between statistical substates within the A(1) taxonomic substate in this protein. The relationship between the heme pocket dynamics (as monitored by the thermal behavior of the CO stretching band), the overall dynamic properties of the protein matrix (as monitored by the thermal behavior of Amide II and Amide I' bands) and the glass transition of the solvent (as monitored by the thermal behavior of the bending band of water) is also investigated. From this analysis, we derive the picture of a very soft heme pocket of hemoglobin characterized by rather large anharmonic terms and strongly coupled to the dynamic properties of the solvent.