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.     

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.     

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.     

Photochemistry in dried polymer films incorporating the deionized blue membrane form of bacteriorhodopsin.

The preparation and photochemical properties of dried deionized blue membrane (dIbR600; lambdamax approximately 600 nm, epsilon approximately 54, 760 cm-1 M-1, f approximately 1.1) in polyvinyl alcohol films are studied. Reversible photoconversion from dIbR600 to the pink membrane (dIbR485; lambdamax approximately 485 nm) is shown to occur in these films under conditions of strong 647-nm laser irradiation. The pink membrane analog, dIbR485, has a molar extinction coefficient of approximately 39,000 cm-1 M-1 (f approximately 1.2). The ratio of pink --> blue and blue --> pink quantum efficiencies is 33 +/- 5. We observe an additional blue-shifted species (dIbR455, lambdamax approximately 455 nm) with a very low oscillator strength (f approximately 0.6, epsilon approximately 26,000 cm-1 M-1). This species is the product of fast thermal decay of dIbR485. Molecular modeling indicates that charge/charge and charge/dipole interactions introduced by the protonation of ASP85 are responsible for lowering the excited-state all-trans --> 9-cis barrier to approximately 6 kcal mol-1 while increasing the corresponding all-trans --> 13-cis barrier to approximately 4 kcal mol-1. Photochemical formation of both 9-cis and 13-cis photoproducts are now competitive, as is observed experimentally. We suggest that dIbR455 may be a 9-cis, 10-s-distorted species that partially divides the chromophore into two localized conjugated segments with a concomitant blue shift and decreased oscillator strength of the lambdamax absorption band.     

High pressure fourier transform infrared (FT-IR) spectroscopic studies on inducible nitric oxide (NO) synthase active site: a comparison to cytochrome p450CAM.

High pressure Fourier transform infrared (FT-IR) spectroscopy is performed for the first time to analyse the active site of inducible nitric oxide synthase (iNOSox) using the carbon monoxide (CO) heme iron ligand stretch mode (nuCO) as spectroscopic probe. A membrane-driven sapphire anvil high-pressure cell is used. Three major conformational substates exist in substrate-free iNOSox which are characterized by nuCO at approximately 1936, 1945 and 1952 cm(-1). High pressure favors the 1936 cm(-1) substate with a volume difference to the 1945 substate of approximately -21 cm3/mol. The pressure induced cytochrome P420 formation with a reaction volume of approximately -80 cm3/mol is observed. Arginine binding produces a very low nuCO at approximately 1905 cm(-1) caused by the H-bond from the substrate to CO. nuCO for the substates in the substrate-free and arginine-bound proteins shift linearly with pressure which is qualitatively similar to the observation on cytochrome P450cam. The slightly smaller positive slope of the shift in substrate-free iNOSox compared to substrate-free P450cam is interpreted as a slightly lesser compressible heme pocket. In contrast, the significant slower negative slope for arginine-bound iNOSox compared to camphor-bound P450cam results from the different kind of interactions to the CO ligand (electrostatic interaction in P450cam, H-bond in iNOSox).     

The early folding kinetics of apomyoglobin.

The folding pathway of apomyoglobin has been experimentally shown to have early kinetic intermediates involving the A, B, G, and H helices. The earliest detected kinetic events occur on a ns to micros time scale. We show that the early folding kinetics of apomyoglobin may be understood as the association of nascent helices through a network of diffusion-collision-coalescence steps G + H <--> GH + A <--> AGH + B <--> ABGH obtained by solving the diffusion-collision model in a chemical kinetics approximation. Our reproduction of the experimental results indicates that the model is a useful way to analyze folding data. One prediction from our fit is that the nascent A and H helices should be relatively more helix-like before coalescence than the other apomyoglobin helices.     

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.     

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.     

Electrogenicity of the sodium transport pathway in the Na,K-ATPase probed by charge-pulse experiments.

A charge-pulse technique was designed to measure charge movements in the Na-transport mode of the Na,K-ATPase in membrane fragments adsorbed to a planar lipid bilayer with high time resolution. 1) Na+ transport was measured as a function of membrane potential, and 2) voltage-dependent extracellular ion binding and release were analyzed as a function of Na+ concentration and membrane potential. The results could be fitted and explained on the basis of a Post-Albers cycle by simulations with a mathematical model. The minimal reaction sequence explaining the electrogenicity of the pump consists of the following steps: (Na3)E1-P <--> P-E2(Na3) <--> P-E2(Na2) <--> P-E2(Na) <--> P-E2. The conformational change, E1 to E2, is electrogenic (beta 0 < or = 0.1) and the rate-limiting step of forward Na+ transport with a rate constant of 25 s-1 (T = 20 degrees C). The first ion release step, P-E2(Na3) <--> P-E2(Na2), is the major charge translocating process (delta 0 = 0.65). It is probably accompanied by a protein relaxation in which the access structure between aqueous phase and binding site reduces the dielectric distance. The release of the subsequent Na+ ions has a significantly lower dielectric coefficient (delta1 = delta 2 = 0.2). Compared with other partial reactions, the ion release rates are fast (1400 s-1, 700 s-1, and 4000 s-1). On the basis of these findings, a refined electrostatic model of the transport cycle is proposed.     

Solution 1H nuclear magnetic resonance determination of the distal pocket structure of cyanomet complexes of genetically engineered sperm whale myoglobin His64 (E7)-->Val, Thr67 (E10)-->Arg. The role of distal hydrogen bonding by Arg67 (E10) in modulating ligand tilt.

Sequence-specific 2D methodology has been used to assign the 1H NMR signals for all active site residues in the paramagnetic cyano-met complexes of sperm whale synthetic double mutant His64[E7]-->Val/Thr67[E10]-->Arg (VR-met-MbCN) and triple mutant His64[E7]-->Val/Thr67[E10]-->Arg/Arg45[CD3]-->Asn (VRN-metMbCN). The resulting dipolar shifts for noncoordinated proximal side residues were used to quantitatively determine the orientation of the paramagnetic susceptibility tensor in the molecular framework for the two mutants, which were found indistinguishable but distinct from those of both wild-type and the His64[E7]-->Val single point mutant (V-metMbCN). The observed dipolar shifts for the E helix backbone protons and Phe43[CD1], together with steady-state nuclear Overhauser effect between the E helix and the heme, were analyzed to show that both the E helix and Phe43[CD1] move slightly closer to the iron to minimize the vacancy resulting from the His64[E7]-->Val substitution, as found in V-metMbCN (Rajarathnam, K., J. Qin, G.N. LaMar, M. L. Chiu, and S. G. Sligar. 1993. Biochemistry. 32:5670-5680). The dipolar shifts of the mutated Val64[E7] and Arg67[E10] allow the determination of their orientations relative to the heme, and the latter residue is shown to insert into the pocket and provide a hydrogen bond to the coordinated ligand, as found in the naturally occurring ValE7/ArgE10 genetic variant, Aplysia limacina Mb. The oxy-complex of both A. limacina Mb and VR-Mb, VRN-Mb have been proposed to be stabilized by this hydrogen bonding interaction (Travaglini Allocatelli, C. et al. 1993. Biochemistry. 32:6041-6049). The magnitude of the tilt of the major magnetic axes from the heme normal in VR-metMbCN and VRN-metMbCN, which is related to the tilt of the ligand, is the same as in wild-type or V-metMbCN, but the direction of tilt is altered from that in V-metMbCN. It is concluded that the change in the direction of the ligand tilt in both the double and triple mutants, as compared to WT metMbCN and V-metMbCN single mutant, is due to the attractive hydrogen-bonding between ArgE10 and the bound cyanide.     

Measurement of beta(1-->3)-glucans in occupational and home environments with an inhibition enzyme immunoassay.

beta (1-->3)-Glucans are known for their potent ability to induce nonspecific inflammatory reactions and are believed to play a role in bioaerosol-induced respiratory symptoms. An inhibition enzyme immunoassay (EIA) was developed for the quantitation of beta (1-->3)-glucans in dust samples from occupational and residential environments. Immunospecific rabbit antibodies were produced by immunization with bovine serum albumin-conjugated laminarin [beta (1-->3)-glucan] and affinity chromatography on epoxy-Sepharose-coupled beta (1-->3)-glucans. The laminarin-based calibration curve in the inhibition EIA ranged from approximately 40 to 3,000 ng/ml (15 to 85% inhibition). Another beta (1-->3)-glucan (curdlan) showed a similar inhibition curve but was three to five times less reactive on a weight basis. Pustulan, presumed to be a beta (1-->6)-glucan, showed a parallel dose-response curve at concentrations 10 times higher than that of laminarin. Control experiments with NaIO4 and beta (1-->3)-glucanase treatment to destroy beta (1-->6)- and beta (1-->3)-glucan structures, respectively, indicate that the immunoreactivity of pustulan in the assay was due to beta (1-->3)-glucan and not to beta (1-->6)-glucan structures. Other polysaccharides, such as mannan and alpha (1-->6)-glucan, did not react in the inhibition EIA. Beta (1-->3)-Glucan extraction of dust samples in water (with mild detergent) was performed by heat treatment (120 degrees C) because aqueous extracts obtained at room temperature did not contain detectable beta (1-->3)-glucan levels. The assay was shown to detect heat-extractable beta (1-->3)-glucan in dust samples collected in a variety of occupational and environmental settings. On the basis of duplicate analyses of dust samples, a coefficient of variation of approximately 25% was calculated. It was concluded that the new inhibition EIA offers a useful method for indoor beta (1-->3)-glucan exposure assessment.     

Purification and some properties of alpha-L-arabinofuranosidase from Bacillus subtilis 3-6.

alpha-L-Arabinofuranosidase (EC 3.2.1.55) was purified from culture supernatant of Bacillus subtilis 3-6. The enzyme had a molecular weight of 61,000 and displayed maximum activity at pH 7.0 and 60 degrees C. It released arabinose from O-alpha-L-arabinofuranosyl-(1-->3)-O-beta-D-xylopyranosyl-(1-->4)-D-x ylopyranos e (A1X2), O-beta-D-xylopyranosyl-(1-->4)-[O-alpha-L-arabinofuranosyl-(1-->3)]- O-beta-D-xylopyranosyl-(1-->4)-D-xylopyranose (A1X3), and arabinan, but not from O-beta-D-xylopyranosyl-(1-->2)-O-alpha-L- arabinofuranosyl-(1-->3)-O-beta-D-xylopyranosyl-(1-->4)-O-beta-D-xylopyr anosyl- (1-->4)-D-xylopyranose (A1X4), arabinoxylan, gum arabic, or arabinogalactan.     

Dehydration and crystallization of trehalose and sucrose glasses containing carbonmonoxy-myoglobin

We report a study wherein we contemporarily measured 1) the dehydration process of trehalose or sucrose glasses embedding carbonmonoxy-myoglobin (MbCO) and 2) the evolution of the A substates in saccharide-coated MbCO. Our results indicate that microcrystallization processes, sizeably different in the two saccharides, take place during dehydration; moreover, the microcrystalline structure is maintained unless the dry samples are equilibrated with a humidity >/=75% (>/=60%) at 25 degrees C for the trehalose (sucrose) sample. The evolution of the parameters that characterize the A substates of MbCO indicates that 1) the effects of water withdrawal are analogous in samples dried in the presence or in the absence of sugars, although much larger effects are observed in the samples without sugar; 2) the distribution of A substates is determined by the overall matrix structure and not only by the sample water content; and 3) the population of A0 substate (i. e., the substate currently put in relation with MbCO molecules having the distal histidine out of the heme pocket) is largely enhanced during the dehydration process. However, after rehumidification its population is largely decreased with respect to the values obtained, at similar water content, during the first dehydration run.     

Spectrally silent transitions in the bacteriorhodopsin photocycle.

The photocycle kinetics of bacteriorhodopsin were analyzed from 0 to 40 degrees C at 101 wavelengths (330-730 nm). The data can be satisfactorily approximated by eight exponents. The slowest component (half-time 20 ms at 20 degrees C) belongs to the 13-cis cycle. The residual seven exponentials that are sufficient to describe the all-trans photocycle indicate that at least seven intermediates of the all-trans cycle must exist, although only five spectrally distinct species (K, L, M, N, and O) have been identified. These seven exponentials and their spectra at different temperatures provide the basis for the discussion of various kinetic schemes of the relaxation. The simplest model of irreversible sequential transitions includes after the first K--> L step the quasiequilibria of L<-->M, M<-->N, and N<-->O intermediates. These quasiequilibria are controlled by rate-limiting dynamics of the protein and/or proton transfer steps outside the chromophore region. Thus there exists an apparent kinetic paradox (i.e., why is the number of exponents of relaxation (at least seven) higher than the number of distinct spectral intermediates (only five)), which can be explained by assuming that some of the transitions correspond to changes in the quasiequilibria between spectrally distinct intermediates (i.e., are spectrally silent).     

Structural studies of lipooligosaccharides from Haemophilus ducreyi ITM 5535, ITM 3147, and a fresh clinical isolate, ACY1: evidence for intrastrain heterogeneity with the production of mutually exclusive sialylated or elongated glycoforms.

The structures of the lipooligosaccharides (LOSs) from Haemophilus ducreyi ITM 5535 and ITM 3147 and a fresh clinical isolate, ACY1, have been investigated. Oligosaccharides were obtained from phenol-water-extracted LOS by mild acid hydrolysis and were studied by methylation analysis, fast atom bombardment and electrospray ionization mass spectrometry, and nuclear magnetic resonance spectroscopy. The major oligosaccharide obtained from all strains was a nonasaccharide with the structure beta-D-Galp-(1-->4)-beta-D-GlcNAcp-(1-->3)-beta-D-Galp-(1-->4)-D-a lpha-D-Hepp- (1-->6)-beta-D-Glcp-(1-->[L-alpha-D-Hepp-(1-->2)-L-alpha-D-Hepp - (1-->3)]4)-L-alpha-D-Hepp-Kdo (Kdo stands for 3-deoxy-D-manno-octulosonic acid) and is thus identical to that identified as the major oligosaccharide in H. ducreyi ITM 2665 (E. K. H. Schweda, A. C. Sundström, L. M. Eriksson, J.A. Jonasson, and A. A. Lindberg, J. Biol. Chem. 269:12040-12048, 1994). Electrospray ionization mass spectrometry on O-deacylated LOS from H. ducreyi ITM 5535 obtained after treatment with anhydrous hydrazine gave evidence for the presence of a sialylated major compound, Neu5Ac alpha(2-->3)-beta-D-Galp-(1-->4)-beta-D-GlcNAcp-(1-->3)-beta-D-Gal p- (1-->4)-D-alpha-D-Hepp-(1-->6)-beta-D-Glcp-(1-->[L-alpha-D-Hepp -(1-->2)-L- alpha-D-Hepp-(1-->3)]4)-L-alpha-D-Hepp-Kdo(P)-O-deacylated lipid A (Neu5Ac stands for N-acetylneuraminic acid). However, an even larger oligosaccharide could be isolated from all strains as a minor component, viz., the undecasaccharide beta-D-Galp-(1-->4)-beta-D-GlcNAcp-(1-->3)-beta-d-Galp-(1-->4)-beta-D-glcNAcp-(1-->3)-beta-D-Galp-(1-->4)-D-alpha-D-Hepp-(1-->6)-beta-D-Glcp-(1-->[L-alpha-D-Hepp-(1-->2)-L-alpha-D-Hepp-(1-->3)]4-L-alpha-D-Hepp-Kdo, which represents an N-acetyl lactosamine disaccharide unit elongation of the LOS outer core. No Sialylation of this latter minor component undecasaccharide was detected.     

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.     

Study of wild type and genetically modified reaction centers from Rhodobacter capsulatus: structural comparison with Rhodopseudomonas viridis and Rhodobacter sphaeroides.

Reaction centers from the purple bacterium Rhodobacter (Rb.) capsulatus and from two mutants ThrL226-->Ala and IleL229-->Ser, modified in the binding protein pocket of the secondary quinone acceptor (QB), have been studied by flash-induced absorbance spectroscopy. In ThrL226-->Ala, the binding affinities for endogenous QB (ubiquinone 10) and UQ6 are found to be two to three times as high as the wild type. In contrast, in IleL229-->Ser, the binding affinity for UQ6 is decreased about three times compared to the wild type. In ThrL226-->Ala, a markedly increased sensitivity (approximately 30 times) to o-phenanthroline is observed. In Rhodopseudomonas viridis, where Ala is naturally in position L226, the sensitivity to o-phenanthroline is close to that observed in ThrL226-->Ala. We propose that the presence of Ala in position L226 is responsible for the high sensitivity to that inhibitor. The pH dependencies of the rate constants of P+QB- (kBP) charge recombination kinetics (P is a dimer of bacteriochlorophyll, and QB is the secondary quinone electron acceptor) show destabilization of QB- in ThrL226-->Ala and IleL229-->Ser, compared to the wild type. At low pH, similar apparent pK values of protonation of amino acids around QB- are measured in the wild type and the mutants. In contrast to Rb. sphaeroides, in the wild type Rb. capsulatus, kBP substantially increases in the pH range 7-10.(ABSTRACT TRUNCATED AT 250 WORDS)     

Quaternary structure dynamics and carbon monoxide binding kinetics of hemoglobin valency hybrids.

The kinetics of CO binding and changes in quaternary structure for symmetric valency hybrids of human hemoglobin have been extensively studied by laser photolysis techniques. Both alpha+beta and alpha beta+ hybrids were studied with five different ferric ligands, over a broad range of CO concentrations and photolysis levels. After full CO photolysis, the hybrid tetramers switch extensively and rapidly (< 200 microseconds) to the T quaternary structure. Both R --> T and T --> R transition rates for valency hybrid tetramers with 0 and 1 bound CO have been obtained, as well as the CO association rates for alpha and beta subunits in the R and T states. The results reveal submillisecond R reversible T interconversion, and, for the first time, the changes in quaternary rates and equilibria due to binding a single CO per tetramer have been resolved. The data also show significant alpha-beta differences in quaternary dynamics and equilibria. The allosteric constants do not vary with the spin states of the ferric subunits as predicted by the Perutz stereochemical model. For the alpha beta+CN hybrid the kinetics are heterogeneous and imply partial conversion to a T-like state with very low (seconds) R reversible T interconversion.     

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.     

Dynamics of carbon monoxide binding with neuronal nitric oxide synthase.

The dynamics of CO rebinding with neuronal NO synthase (nNOS) following laser flash photolysis have been investigated from 293 to 77 K in the absence and presence of its substrate L-arginine. The distribution functions of the rate parameters P(k) and of the activation enthalpy P(H) were determined using the maximum entropy method. In a fluid solvent near room temperature, bimolecular rebinding is biphasic, as previously reported by several groups. However, measurement of the rotational correlation time shows that the apparent biphasic rebinding is not relevant to the genuine dynamics of NOS. In addition to native dimeric nNOS, another species (possibly aggregated or partially unfolded conformation) with different hydrodynamic characteristics is responsible for the faster rebinding process. In a rigid environment at low temperature, the geminate internal rebinding is not affected by the presence of the nonnative species. nNOS exhibits a bimodal distribution of CO activation enthalpy with P(H) consisting of two distinct bands with temperature-dependent amplitudes down to 77 K. The similarity of these findings with those recently reported for cytochromes P-450 suggests a common hierarchical organization of conformational substates, with a splitting of each conformational substate into a doublet. Thus, thiolate-coordinated heme proteins are in clear contrast to histidine-coordinated oxygen-transport heme proteins. The present results with nNOS provide additional support to previous arguments incriminating the thiolate ligand as responsible for the splitting of conformational substates.