Fluorescence study of the conformational properties of myoglobin structure. 3. pH-dependent changes in porphyrin and tryptophan fluorescence of the complex of sperm whale apomyoglobin with protoporphyrin IX; the role of the porphyrin macrocycle and iron in formation of native myoglobin structure

The porphyrin and tryptophan fluorescence of sperm whale apomyoglobin complexed with protoporphyrin IX has been studied in the pH range 2-13. It has been shown that the fluorescence and absorption spectra of protoporphyrin incorporated into the heme crevice remain constant in the pH range 5.5-10.8 but change significantly at pH less than 5.5 and pH greater than 10.8, due to the acid and alkaline denaturation, respectively, of the complex accompanied by dissociation of protoporphyrin IX. At the same pH ranges, the quantum yield of tryptophanyl fluorescence increases sharply as a result of removal of protoporphyrin, acting as a quencher, from the complex. Other parameters of tryptophanyl fluorescence (maximum position, halfwidth and spectrum shape) change in the alkaline region as well. In the acidic pH range, these parameters change only at pH less than 4.3, indicating that the Trp surroundings are more stable to denaturation than the heme crevice region. Between pH 5.5 and 10.9, where the complex of apomyoglobin with protoporphyrin IX is in its native state, the main parameters of tryptophan fluorescence remain unchanged except for the ratio I325/I350 which diminishes at pH greater than 9.5. Its alteration precedes the alkaline denaturation of the complex and can be explained by a local conformational change induced by the break of the 'salt bridges' essential for the maintenance of the native Mb structure in the N-terminal region. The fluorescence data obtained for apomyoglobin, myoglobin and the complex between protoporphyrin IX and apomyoglobin enable one to compare their structures and to evaluate the role of the porphyrin macrocycle and the iron atom in the formation of the native myoglobin structure and its functioning.     

Intramolecular conformational transitions "random coil-helix-folded structure" in polypeptides.

A general theory has been developed for conformational intramolecular transitions in a single macromolecule with a high degree of polymerization (an infinite length model) capable of forming two types of ordered structures: the α-helix and the folded β-structure, as well as acquiring the random coil conformation. The phase diagram analysis of this system has shown that the regular β-structure state is separated from all other states of the chain by the phase boundary line. Any intersection of the phase boundary is a phase transition which can be either of the first order or second order, depending on values of the energy parameters of the system. Mechanisms of intramolecular rearrangements: β-structure–random coil and α-helix–β-structure have been discussed. It has been shown that there exist two different mechanisms for each of these rearrangements, and the regions of parameter variation corresponding to each mechanism have been specified.     

Disorder-to-order conformational transitions in protein structure and its relationship to disease

Function in proteins largely depends on the acquisition of specific structures through folding at physiological time scales. Under both equilibrium and non-equilibrium states, proteins develop partially structured molecules that being intermediates in the process, usually resemble the structure of the fully folded protein. These intermediates, known as molten globules, present the faculty of adopting a large variety of conformations mainly supported by changes in their side chains. Taking into account that the mechanism to obtain a fully packed structure is considered more difficult energetically than forming partially “disordered” folding intermediates, evolution might have conferred upon an important number of proteins the capability to first partially fold and—depending on the presence of specific partner ligands—switch on disorder-to-order transitions to adopt a highly ordered well-folded state and reach the lowest energy conformation possible. Disorder in this context can represent segments of proteins or complete proteins that might exist in the native state. Moreover, because this type of disorder-to-order transition in proteins has been found to be reversible, it has been frequently associated with important signaling events in the cell. Due to the central role of this phenomenon in cell biology, protein misfolding and aberrant disorder-to-order transitions have been at present associated with an important number of diseases.     

S-nitrosylation-induced conformational change in blackfin tuna myoglobin

S-nitrosylation is a post-translational protein modification that can alter the function of a variety of proteins. Despite the growing wealth of information that this modification may have important functional consequences, little is known about the structure of the moiety or its effect on protein tertiary structure. Here we report high-resolution x-ray crystal structures of S-nitrosylated and unmodified blackfin tuna myoglobin, which demonstrate that in vitro S-nitrosylation of this protein at the surface-exposed Cys-10 directly causes a reversible conformational change by "wedging" apart a helix and loop. Furthermore, we have demonstrated in solution and in a single crystal that reduction of the S-nitrosylated myoglobin with dithionite results in NO cleavage from the sulfur of Cys-10 and rebinding to the reduced heme iron, showing the reversibility of both the modification and the conformational changes. Finally, we report the 0.95-A structure of ferrous nitrosyl myoglobin, which provides an accurate structural view of the NO coordination geometry in the context of a globin heme pocket.     

A method for the experimental study of DNA conformational transitions in fibers

The method proposed for the study of DNA conformational transitions is based on the proportionality, experimentally observed, between the length of a DNA fiber and the axial rise per nucleotide characterizing the molecular helix. Precise curves for the A-B and B-C transitions as a function of the relative humidity are obtained by using X-ray fiber data and measurements of fiber dimensions. It is thus shown that the A-B transition is a cooperative process between two different states, whereas the B-C transition can be considered as a progressive change of conformation. The present method is applied on two natural DNAs differing in base composition so that the effect of the nucleotide content on the conformational changes can be estimated.     

Spectroscopic and photothermal study of myoglobin conformational changes in the presence of sodium dodecyl sulfate

Interactions between sodium dodecyl sulfate (SDS) and horse heart myoglobin (Mb) at surfactant concentrations below the critical micelle concentration have been studied using steady-state and transient absorption spectroscopies and photoacoustic calorimetry. SDS binding to Mb induces a heme transition from high-spin five-coordinate to low-spin six-coordinate in met- and deoxyMb, with the distal His residue likely to be the sixth ligand. The transition is complete at an SDS concentration of approximately 350 microM and approximately 700 microM for met- and deoxyMb, respectively. DeltaG(H(2)O) and m values determined from equilibrium SDS-induced unfolding curves indicate similar stability of met- and deoxyMb toward unfolding; however, the larger m value for the deoxyMb equilibrium intermediate indicates that its structure differs from that of metMb. Results from transient absorption spectroscopy show that CO rebinding to Fe(2+)-Mb in the presence of SDS is a biphasic process with the rate constant of the first process approximately 5.5 x 10(3) s(-1), whereas the second process displays a rate similar to that for CO rebinding to native Mb (k(obs) = 7.14 x 10(2) s(-1)) at 1 mM CO. Results of photoacoustic calorimetry show that CO dissociation from deoxyMb occurs more than 10 times faster in the presence of SDS than in native Mb. These data suggest that the heme binding pocket is more solvent-exposed in the SDS-induced equilibrium intermediate relative to native Mb, which is likely due to the electrostatic and hydrophobic interactions between surfactant molecules and the protein matrix.     

Fluorescence study of the thyroxine-dependent conformational changes in human serum transthyretin.

Fluorescence studies of transthyretin (TTR) were conducted to detect structural changes associated with the environment of its two tryptophans, induced by binding of thyroxine (T4). Non-radiative tryptophans relaxation rate has an activation energy of 6.4 kcal/mol for TTR, which is decreased to 4.4 kcal/mol for TTR-T4 complex. The maximum fluorescence wavelength was red-shifted as the excitation wavelength was increased. T4 changed the magnitude of this shift. T4 binding per se changed the emission maximum reflecting different environments of the tryptophans. Double-quenching experiments also showed that T4 produces changes in the tryptophans environments. These findings were interpreted as the result of structural alterations in the protein matrix induced by T4 which contribute in part to explain the negative cooperativity associated with the occupancy of the second binding site.     

Comparative study of the conformational transitions of frog and rabbit phosphorylases B

1. Conformational motility of the purified muscle glycogen phosphorylase B from two species of vertebrates (rabbit and frog) was investigated by the Hydrogen-Exchange method and Infrared Spectometry. 2. The experimental results of the 1H-2H exchange were expressed in terms of the probability P of exposure to isotopic solvent of phosphorylase peptide groups and in terms of the corresponding changes in standard free energy delta Go. 3. The combined methods used didn't show considerable differences of the protein conformations in the physiological pH region but rabbit phosphorylase was only characterized by rather more compact structure in comparison with frog phosphorylase.     

Salt-induced conformational transitions in chromatin. A flow linear dichroism study

The chromatin structure in solution has been studied by the flow linear dichroism method (LD) in a wide range of ionic strengths. It is found that increasing the ionic strength from 0.25 mM Na2EDTA, pH 7.0 to 100 mM NaCl leads to a strong reduction of the LD amplitude of chromatin and inversion of the LD sign from negative to positive at 2 mM NaCl. Chromatin exhibits a positive LD maximum value at 10-20 mM NaCl. These data enable us to conclude that in very low ionic strength (0.25 mM Na2EDTA) the nucleosome discs are oriented with their flat faces more or less parallel to the chromatin filament axis. Increasing ionic strength up to 20 mM NaCl leads to reorientation of the nucleosome discs and to formation of chromatin structures with nucleosome flat faces inclined to the fibril axis. A conformational transition of that kind is not revealed in H1-depleted chromatin. The condensation of the chromatin filaments with increasing concentration of NaCl from 20 mM to 100 mM slightly influences the orientation of the nucleosomes.     

Lipid-induced conformational transitions of beta-lactoglobulin

Bovine beta-lactoglobulin (betaLG) provides an excellent model protein system for beta-to-alpha conformational change, but its behavior varies when the change is induced by alcohols, surfactants, or lipid vesicles. Here the interaction and orientation of betaLG in association with various artificial lipid vesicles at neutral and acidic pH have been studied by use of several complementary spectroscopic techniques. Circular dichroism (CD) and Fourier transform infrared (FTIR) spectra demonstrated that betaLG acquires a non-native alpha-helical structure upon binding with anionic lipids, while zwitterionic lipids do not have a significant effect on its conformation. The degree of induced alpha-helix depends on the lipid concentration and is strongly affected by the charge of the protein and lipids as well as the ionic strength of the solution. Near-UV CD and Trp emission spectra revealed that the tertiary structure of lipid-bound betaLG is highly expanded but not completely disrupted. Fluorescence quenching together with a Trp emission blue shift showed that the Trp residues remain largely shielded from the solvent when interacting with DMPG, which would be consistent with at least some portions of betaLG having been inserted into the lipid membrane. The orientations of the alpha-helix and beta-sheet axes in membrane-bound betaLG were found to be parallel and perpendicular, respectively, to the membrane film normal, as determined by use of polarized attenuated total reflection (ATR) FTIR spectra. Our findings reveal that the lipid-induced beta-to-alpha transition in betaLG, accompanied by a substantial disruption in tertiary structure, is mainly driven by strong electrostatic interactions. Once the tightly packed betaLG is disrupted, hydrophobic residues become exposed and available for insertion into the lipid bilayer, where hydrophobic interaction with the lipids may play a role in stabilizing the helical components.     

Fluorescence conformational probe study of calcium release from sarcoplasmic reticulum

Sarcoplasmic reticulum isolated from rabbit skeletal muscle was labeled with a limited (0.625 nmol/mg sarcoplasmic reticulum protein) amount of the fluorescent thiol reagent N-(7-dimethylamino-4-methyl-3-coumarinyl)maleimide (DACM). The fluorescence intensity of the membrane-attached DACM decreased concurrently with (Ca2+ and caffeine)-induced Ca2+ release, depolarization-induced Ca2+ release and Ca2+-dependent dependent passive efflux of Ca2+. The decreased DACM fluorescence level initiated by a Ca2+ jump was subsequently reversed under passive efflux conditions when there was no ATP-dependent Ca2+ uptake, suggesting spontaneous closing of the channels. Therefore, the higher fluorescence level corresponds to a larger population of closed channels, whereas the lower level represents a larger population of opened channels. Under conditions when the Ca2+ release-coupled fluorescence change was maximal, a stoichiometric incorporation of DACM took place only into a 32-kDa protein. Furthermore, reconstituted vesicles, in which purified DACM-labeled 32-kDa protein was incorporated into unlabeled sarcoplasmic reticulum vesicles, were capable of both (Ca2+ and caffeine)-induced Ca2+ release and the release-coupled DACM fluorescence change. These results suggest that the 32-kDa protein is a constituent of the Ca2+ release channel or a protein which is in close contact with the channel.     

Geometry-based sampling of conformational transitions in proteins

The fast and accurate prediction of protein flexibility is one of the major challenges in protein science. Enzyme activity, signal transduction, and ligand binding are dynamic processes involving essential conformational changes ranging from small side chain fluctuations to reorientations of entire domains. In the present work, we describe a reimplementation of the CONCOORD approach, termed tCONCOORD, which allows a computationally efficient sampling of conformational transitions of a protein based on geometrical considerations. Moreover, it allows for the extraction of the essential degrees of freedom, which, in general, are the biologically relevant ones. The method rests on a reliable estimate of the stability of interactions observed in a starting structure, in particular those interactions that change during a conformational transition. Applications to adenylate kinase, calmodulin, aldose reductase, T4-lysozyme, staphylococcal nuclease, and ubiquitin show that experimentally known conformational transitions are faithfully predicted.     

Fluctuation domains in myoglobin. Fluorescence quenching studies

The dynamics of two domains in the myoglobin molecule, close to the heme and inside the protein medium including the surface, are investigated through the study of the fluorescence oxygen quenching of two probes imbedded in the heme pocket: zinc protoporphyrin IX (with a fluorescence lifetime of 2.1 ns) and metal-free protoporphyrin IX (with a fluorescence lifetime of 17.8 ns).     

Fluorescence studies on the interaction of myoglobin with mitochondria

To determine the nature and characteristic parameters of the myoglobin-mitochondrion interaction during oxymyoglobin (MbO₂) deoxygenation in the cell, we studied the quenching of the intrinsic mitochondrial flavin and tryptophan fluorescence by different liganded myoglobins in the pH range of 6–8, as well as the quenching of the fluorescence of the membrane probes 1,8-ANS and merocyanine 540 (M 540) embedded into the mitochondrial membrane. Physiologically active MbO₂ and oxidized metmyoglobin (metMb), which are unable to bind oxygen, were used as the quenchers. The absence of quenching of flavin and tryptophan fluorescence implies that myoglobin does not form quenching complexes with either electron transport chain proteins of the inner mitochondrial membrane or with outer membrane proteins. We found, however, that MbO₂ and metMb effectively quench 1,8-ANS and M 540 fluorescence in the pH range of 6–8. Characteristic parameters of 1,8-ANS and M 540 fluorescence quenching by the myoglobins (extent of quenching and quencher binding constant, K _m) are very similar, indicating that both probes are localized in phospholipid sites of the mitochondrial membrane, and myoglobin is complexed with these sites. The dependence of K _m on ionic strength proves the important role of coulombic interactions in the formation of the quenching complex. Since the overall charge of myoglobin is shown not to influence the K _m values, the ionic strength dependence must be due to local electrostatic interactions in which polar groups of some part of the myoglobin molecule participate. The most likely candidates to interact with anionic groups of mitochondrial phospholipids are invariant lysine and arginine residues in the environment of the myoglobin heme cavity, which do not change their ionization state in the pH range investigated.     

Immunological measurements of conformational motility in regions of the myoglobin molecule.

The conformational motilities of three regions of the sperm whale myoglobin molecule and of an isolated peptide of myoglobin have been examined by measuring the equilibrium constant for the native equilibrium nonnative transition. The immunological approach of Furie et al. (Furie, B., Schechter, A.N., Sachs D., and Anfinsen, C.B. (1975), J. Mol. Biol.92, 497-506) was used with convenient modifications. Antibodies specific to the nonnative conformations were used in assaying for competition between the radioactively labeled peptide and native myoglobin. Labeling was by 125I iodination of the peptide or its 3-(4-hydroxyphenyl)propionyl derivative, and separation of the immune complex from the free peptide was either by ammonium sulfate precipitation or by centrifugation of the antibodies immobilized on Agarose beads. For the antigenic regions of the sequence (1-55), the measured conformational equilibrium constant was 840 +/- 200 at 22 degrees C; the value for the C-terminal region (132-153) was 280 +/- 120 at 25 degrees C, while that for the region (66-76) adjacent to the heme group was greater than 2.5 x 10(6). Measurements on the isolated peptide (132-153) indicated that 1% of the molecules adopt native-type folding in aqueous solution at 36 degrees C.     

Applying the stochastic difference equation to DNA conformational transitions: a study of B-Z and B-A DNA transitions

Despite the existence of numerous models to account for the B-Z DNA transition, experimenters have not yet arrived at a conclusive answer to the structural and dynamical features of the B-Z transition. By applying the stochastic difference equation to simulate the B-Z DNA transition, we have shown that the stretched intermediate model of the B-Z transition is more probable than other B-Z transition models such as the Harvey model. This is accomplished by comparing potential energy profiles of various B-Z DNA transition models and calculating relative probabilities based on the stochastic difference equation with respect to length (SDEL) formalism. The results garnered in this article allow for new approaches in determining the structural transition of B-DNA to Z-DNA experimentally. We have also simulated the B-A DNA transition using the stochastic difference equation. Unlike the B-Z DNA transition, the mechanism for the B-A DNA transition is well established. The variation in the pseudorotation angle during the transition is in good agreement with experimental results. Qualitative features of the simulated B-A transition also agree well with experimental data. The SDEL approach is thus a suitable numerical technique to compute long-time molecular dynamics trajectory for DNA molecules.