Intramolecular dielectric screening in proteins

This paper investigates the microscopic mechanisms of charge screening by proteins. For this purpose, we introduce the generalized susceptibility of a protein in response to a point charge, which is a scalar quantity dependent on position within the protein. The contribution to the susceptibility from atomic polarizabilities, associated with electronic degrees of freedom, is found to be highly uniform. By contrast, that from dynamic dipolar relaxation, associated with nuclear degrees of freedom, varies greatly between different regions of the protein. We investigate the possible r?le of this variation in the activity of proteins that interact functionally with charged species, and we formulate and test the hypothesis that this variation is correlated to functional activity. Model calculations give encouraging support to this hypothesis. The protein's dielectric properties are represented by a standard model in which electronic relaxation is described by a set of atomic polarizabilities, and dipolar relaxation is treated as a perturbation to normal mode dynamics. The model yields the desired susceptibility in closed form. Its obvious limitations are discussed. It is applied to several test systems, and is compared to various continuum models. Four model alpha-helices are considered, three of which play a r?le in vivo in the binding of charged ligands. We show that the intramolecular screening, and its spatial variation, can indeed play a part in this binding. The electron transfer between ferri- and ferrocytochrome c is considered. The dielectric relaxation of each molecule, associated respectively with its oxidation or its reduction, is known to be directly related to the activation free energy for the electron transfer reaction. Our analysis of the dielectric susceptibility will thus permit an estimate of this activation free energy. We show that the relaxation of the atomic positions ("dipolar relaxation") contributes 1 kcal/mol to this activation free energy, and that the molecule achieves this low value by providing a low dipolar susceptibility throughout its central part. In this case, the spatial variation of the susceptibility has a clear functional r?le.     

Variations of electrostatic interactions in myoglobin probed by UVRR spectroscopy. Effect of iron ligand and pH on tryptophan and tyrosine vibrations.

The present work investigates the variations of electrostatic interactions within the myoglobin molecule associated with azide heme binding and pH variations. Far ultraviolet (223 nm) resonance Raman spectroscopy of the tryptophan and tyrosine residues, along with acid-base titration measurements, have been used to monitor variations in the protein matrix. With previously determined mode assignments, it is shown that the Trp and Tyr residues of the globin moiety are influenced by the charge spatial distribution. Upon ligand binding or under various pH conditions, the polar interactions inside the protein appear to be modulated by the electric field generated by the charge array. It is concluded that the binding site properties of myoglobin can be modulated by the charge spatial distribution within the protein, even in the absence of measurable conformational changes of the bulk.     

Protein matrix and dielectric effect in cytochrome c

The effect of the protein matrix on the standard potential of a buried redox center has been investigated by using a selection of mutants and chemical derivatives in Saccharomyces cerevisiae cytochrome c isoform 1. Assuming only local structural perturbation and no alteration of the iron-ligation chemistry, Delta E(m)(0)' can be regarded as a measure of the difference in polypeptide solvation of the heme charge, which reflects the dielectric properties of the protein. The evaluation of an apparent dielectric constant (U(exp)/U(theo)) yields variable, and sometimes even negative, values if U(exp) = Delta G(0)redox. However, some consistent result are observed if U(exp) = Delta H(0)redox, with a measured epsilon(Delta Delta)(H)(redox) = 19 +/- 6. The variability is thus attributed to an entropic factor (epsilon(Delta Delta)(S)(redox)) that is investigated using a series of substitutions of Asn(52) and/or Tyr(67). In double mutants Y67F/N52I Y67F/N52V, where most of the hydrogen bond network in the heme crevice is eliminated, Delta S(redox) compares to the wild type. This indicates that a fully consistent hydrogen bond network has a similar polarizability as an apolar matrix. We therefore argue that the variability in net dielectric susceptibility arises from conformational polarizability, a factor that is not a function of atomic properties and coordinates and is therefore hard to predict using conventional physical relationships.     

Control of the redox potential of cytochrome c and microscopic dielectric effects in proteins

X-ray structural information provides the opportunity to explore quantitatively the relation between the microenvironments of heme proteins and their redox potentials. This can be done by considering the protein as a "solvent" for its redox center and calculating the difference between the electrostatic energy of the reduced and oxidized heme. Such calculations are presented here, applying the protein dipoles-Langevin dipoles (PDLD) model to cytochrome c. The calculations focus on an evaluation of the difference between the redox potentials of cytochrome c and the octapeptide-methionine complex formed by hydrolysis of cytochrome c. The corresponding difference (approximately 7 kcal/mol) is accounted for by the PDLD calculations. It is found that the protein provides basically a low dielectric environment for the heme, which destabilizes the oxidized heme (relative to its energy in water). The effect of the charged propionic acids on the heme is examined in a preliminary way. It is found that the negative charges of these groups are in a hydrophilic rather than a hydrophobic environment and that the protein-water system provides an effective high dielectric constant for their interaction with the heme. The dual nature of the dielectric effect of the cytochrome (a low dielectric constant for the self-energy of the heme and a high dielectric constant for charge-charge interactions) is discussed. The findings of this work are consistent with the difference between the folding energies of the reduced and oxidized cytochrome c.     

Comparison of the binding sites for high-potential iron-sulfur protein and cytochrome c on the tetraheme cytochrome subunit bound to the bacterial photosynthetic reaction center

A tetraheme cytochrome subunit bound to the photosynthetic reaction center (RC) of purple bacterium, Rubrivivax gelatinosus, interacts with two types of soluble electron donors, cytochromes c and high-potential iron-sulfur protein (HiPIP), at a binding domain in the vicinity of low-potential heme 1, the fourth heme from the special pair of bacteriochlorophyll. To clarify the mechanism of the interaction, the domain around heme 1 was examined using site-directed mutants that changed the surface charge in the region within 20 A from the heme edge. In the case of the interaction with soluble cytochrome c, a strong dependence on the sign of the introduced charge was observed in all mutants: positive charge inhibited the reaction rate, whereas additional negative charge accelerated it. This confirmed the electrostatic nature of the binding. Interaction with HiPIP was inhibited by a limited number of mutations at the close vicinity of heme 1, and no acceleration was observed (the effects of some mutations were independent of the sign of the introduced charge). The acidic residues which were critically important for the binding of cytochrome c showed much less contribution to the binding of HiPIP. The binding site for HiPIP appears to be mostly formed by uncharged and hydrophobic residues, occupying a significantly smaller area than the cytochrome-c-binding site. It is proposed that the docking of HiPIP to the RC in Rvi. gelatinosus is primarily controlled by hydrophobic contacts between protein surfaces, thus differing from the electrostatic mode of the RC-cytochrome c interaction.     

Voltammetric probes of cytochrome electroreactivity: the effect of the protein matrix on outer-sphere reorganization energy and electronic coupling probed through comparisons with the behavior of porphyrin complexes

Using surface-modified electrodes composed of omega-hydroxyalkanethiols, an experimentally based value for the inner-sphere reorganization energy of the bis(imidazole)iron porphyrin system has been obtained by examining the solvent dependence of the reorganization energy of bis(N-methylimidazole)meso-tetraphenyl iron porphyrin. The value obtained (0.41 +/- 0.06 eV) is remarkably similar to values we have recently reported for the reorganization energy of cytochrome b(5) (0.43 +/- 0.02 eV) and cytochrome c (0.58 +/- 0.06 eV). This strongly suggests that the protein matrix mimics the behavior of a low dielectric solvent and effectively shields the heme from the solvent. The effect of the orientation of the heme relative to the electrode was also explored by sytematically varying the steric bulk of the axial ligands. On the basis of a good linear correlation between the electronic coupling and the cosine of the angle between the heme plane and the surface of the electrode, it is suggested that a parallel orientation of the heme yields a maximum in the electronic coupling. Relevance to interheme protein electron transfer is discussed.     

Role of heme in structural organization of cytochrome c probed by semisynthesis

The heme prosthetic group of cytochrome c is covalently attached to the protein through thioether bonds to two cysteine side chains. The role of covalent heme attachment to cytochrome c is not understood, and most heme proteins bind the prosthetic group by iron ion ligation and tertiary interactions only. A two-armed attachment seems redundant if the role of covalent connection is to limit heme group orientation or to decouple heme affinity from redox potential. These considerations suggested that one role for covalent attachment of the rigid planar heme might be in organizing the cytochrome c protein structure. Indeed, porphyrin cytochrome c (in which the heme iron ion has been removed) is substantially more ordered than apocytochrome c, having characteristics consistent with a molten globule state. To assess the importance of planar rigidity in ordering this protein, semisynthesis was used to substitute porphyrin by two hydrophobic surrogates, one based on biphenyl and the other on phenanthrene, which have different degrees of planarity and rigidity. The expected two-armed covalent attachment of each surrogate was confirmed in the protein products by a variety of methods including mass spectrometry and NMR. Despite being only about half the size of the porphyrin macrocycle, and lacking any possibility for ligation or polar group interactions with the surrounding protein, the two surrogates confer helix contents that are comparable to that of the molten globule formed by porphyrin cytochrome c under similar solution conditions. The pH titrations of the derivatives monitored by circular dichroism exhibit reversible, bell-shaped folding and unfolding transitions, implying that charge group interactions in the protein are involved in stabilizing the helical structures formed. The thermal transitions of the two derivatives at neutral pH are cooperative, with similar midpoints. The similarity of helical content and structural stability in the two derivatives indicates that the increase in conformational freedom by the biphenyl surrogate does not substantially reduce protein structural stability. The similarity of the two derivatives to porphyrin cytochrome c suggests that the common feature among the three covalently attached groups-their hydrophobicity-is by far the dominant factor in organizing stable structures in the protein.     

The redox properties of cytochromes b imposed by the membrane electrostatic environment.

The effect of the dipole potential field of extended membrane spanning alpha-helices on the redox potentials of b cytochromes in energy transducing membranes has been calculated in the context of a three phase model for the membrane. In this model, the membrane contains three dielectric layers; (i) a 40-A hydrophobic membrane bilayer, with dielectric constant em = 3-4, (ii) 10-20-A interfacial layers of intermediate polarity, ein = 12-20, that consist of lipid polar head groups and peripheral protein segments, and (iii) an external infinite water medium, ew = 80. The unusually positive midpoint potential, Em = +0.4 V, of the "high potential" cytochrome b-559 of oxygenic photosynthetic membranes, a previously enigmatic property of this cytochrome, can be explained by (i) the position of the heme in the positive dipole potential region near the NH2 termini of the two parallel helices that provide its histidine ligands, and (ii) the loss of solvation energy of the heme ion due to the low dielectric constant of its surroundings, leading to an estimate of +0.31 to +0.37 V for the cytochrome Em. The known tendency of this cytochrome to undergo a large -delta Em shift upon exposure of thylakoid membranes to proteases or damaging treatments is explained by disruption of the intermediate polarity (ein) surface dielectric layer and the resulting contact of the heme with the external water medium. Application of this model to the two hemes (bn and bp) of cytochrome b of the cytochrome bc1 complex, with the two hemes placed symmetrically in the low dielectric (em) membrane bilayer, results in Em values of hemes bn and bp that are, respectively, somewhat too negative (approximately -0.1 V), and much too positive (approximately +0.3 V), leading to a potential difference, Em(bp) - Em(bn), with the wrong sign and magnitude, +0.25 V instead of -0.10 to -0.15 V. The heme potentials can only be approximately reconciled with experiment, if it is assumed that the two hemes are in different dielectric environments, with that of heme bp being more polar.     

Dielectric constant dependence of biological oxidation-reduction. 1. A model of polarity-dependent ferrocytochrome c oxidation

A theoretical model for the effect of the dielectric constant (c) of the solvent medium on ferrocytochrome c oxidation by ferricyanide is developed to account for the observed variations of the rate constant (k) of reactions in aqueous binary mixtures with alcohols (less than 5-10 mol% ethanol and propranolol). A correlation between k and c is found if ln k is expressed as a function of the Kirkwood parameter (c-1)(2c+1). The results of calculations indicate that the use of the 'overall dipole moment' of cytochrome c in oxidoreduction studies is likely to be unreliable. Instead, the decrease in k in alcohol/water mixtures is best explained--in conformity with Onsager's theory of the reaction field--by a polarity effect on the dipole moment of the cytochrome c heme upon diffusion of the polar solvent molecules into the low dielectric constant heme crevice.     

The medium reorganization energy for the charge transfer reactions in proteins

A low static dielectric permittivity of proteins causes the low reorganization energies for the charge transfer reactions inside them. This reorganization energy does not depend on the pre-existing intraprotein electric field. The charge transferred inside the protein interacts with its aqueous surroundings; for many globular proteins, the effect of this surroundings on the reorganization energy is comparable with the effect of reorganization of the protein itself while for the charge transfer in the middle of membrane the aqueous phase plays a minor role. Reorganization energy depends strongly on the system considered, and hence there is no sense to speak on the "protein reorganization energy" as some permanent characteristic parameter. We employed a simple algorithm for calculation of the medium reorganization energy using the numerical solution of the Poisson-Boltzmann equation. Namely, the reaction field energy was computed in two versions - all media having optical dielectric permittivity, and all the media with the static one; the difference of these two quantities gives the reorganization energy. We have calculated reorganization energies for electron transfer in cytochrome c, various ammine-ruthenated cytochromes c, azurin, ferredoxin, cytochrome c oxidase, complex of methylamine dehydrogenase with amicyanin, and for proton transfer in α-chymotrypsin. It is shown that calculation of the medium reorganization energy can be a useful tool in analysis of the mechanisms of the charge transfer reactions in proteins.     

Cytochrome c and cytochrome c oxidase interactions: the effects of ionic strength and hydrostatic pressure studied with site-specific modifications of cytochrome c.

Seven cytochromes c, in which individual lysines have been modified to the propylthiobimane derivatives, have been prepared. These derivatives were also converted to the porphyrin cytochromes c by treatment with HF. The properties of both types of modified proteins were studied in their reactions with cytochrome c oxidase. The results show that lysines 25, 27, 60, 72, and 87 do not contribute a full charge to the binding interaction with the oxidase. These five residues, with the exception of the lysine-60 derivative, on the front surface of the protein and contain the solvent-accessible edge of the heme prosthetic group. By contrast, lysines 8 and 13 at the top of the front surface do contribute a full charge to the binding interaction with the oxidase. The removal of the positive charge on any one lysine weakens the binding to cytochrome c oxidase by at least 1 kcal (1 cal = 4.1868 J). The presence of bimane at lysines 13 and 87 clearly forces the separation of the cytochrome c and oxidase, but this does not occur with the other complexes. The bimane-modified lysine-13 protein, and to a lesser extent that modified at lysine 8, show the interesting effect of enhanced complex formation with cytochrome c oxidase when subjected to pressure, possibly because of entrapment of water at the newly created interface of the complex. Our observations indicate that the two proteins of the cytochrome c - cytochrome oxidase complex have preferred, but not obligatory, spatial orientations and that interaction occurs without either protein losing significant portions of its hydration shell.     

Electrostatic interaction of cytochrome c with cytochrome c1 and cytochrome oxidase

The reactions of horse heart cytochrome c with succinate-cytochrome c reductase and cytochrome oxidase were studied as a function of ionic strength using both spectrophotometric and oxygen electrode assay techniques. The kinetic parameter Vmax/Km for both reactions decreased very rapidly as the ionic strength was increased, indicating that electrostatic interactions were important to the reactions. A new semiempirical relationship for the electrostatic energy of interaction between cytochrome c and its oxidation-reduction partners was developed, in which specific complementary charge-pair interactions between lysine amino groups on cytochrome c and negatively charged carboxylate groups on the other protein are assumed to dominate the interaction. The contribution of individual cytochrome c lysine amino groups to the electrostatic interaction was estimated from the decrease in reaction rate caused by specific modification of the lysine amino groups by reagents that change the charge to 0 or -1. These estimates range from -0.9 kcal/mol for lysines immediately surrounding the heme crevice of cytochrome c to 0 kcal/mol for lysines well removed from the heme crevice region. The semiempirical relationship for the total electrostatic energy of interaction was in quantitative agreement with the experimental ionic strength dependence of the reaction rates when the parameters were based on the specific lysine modification results. The electrostatic energies of interaction between cytochrome c and its reductase and oxidase were nearly the same, providing additional evidence that the two reactions take place at similar sites on cytochrome c.     

Import of apocytochrome c into the mitochondrial intermembrane space along a cytochrome c1 sorting pathway

The question of whether cytochrome c could be functionally sorted to the mitochondrial intermembrane space along a "conservative sorting" pathway was investigated using a fusion protein termed pLc1-c. pLc1-c contains 3-fold targeting information, namely, the complete bipartite presequence of the cytochrome c1 precursor joined to the amino terminus of apocytochrome c. pLc1-c could be selectively imported into the intermembrane space either directly across the outer membrane along a cytochrome c import route or along a cytochrome c1 route via the matrix. Thus, apocytochrome c could be sorted along a conservative sorting pathway; however, following reexport from the matrix, apo-Lc1-c could not be converted to its holo counterpart. Despite the apparent similarity of structure and functional location of the heme lyases and similarity of the heme binding regions in their respective apoproteins, cytochrome c heme lyase and cytochrome c1 heme lyase apparently have different and nonoverlapping substrate specificities.     

Electronic and vibrational spectroscopy of the cytochrome c:cytochrome c oxidase complexes from bovine and Paracoccus denitrificans.

The 1:1 complex between horse heart cytochrome c and bovine cytochrome c oxidase, and between yeast cytochrome c and Paracoccus denitrificans cytochrome c oxidase have been studied by a combination of second derivative absorption, circular dichroism (CD), and resonance Raman spectroscopy. The second derivative absorption and CD spectra reveal changes in the electronic transitions of cytochrome a upon complex formation. These results could reflect changes in ground state heme structure or changes in the protein environment surrounding the chromophore that affect either the ground or excited electronic states. The resonance Raman spectrum, on the other hand, reflects the heme structure in the ground electronic state only and shows no significant difference between cytochrome a vibrations in the complex or free enzyme. The only major difference between the Raman spectra of the free enzyme and complex is a broadening of the cytochrome a3 formyl band of the complex that is relieved upon complex dissociation at high ionic strength. These data suggest that the differences observed in the second derivative and CD spectra are the result of changes in the protein environment around cytochrome a that affect the electronic excited state. By analogy to other protein-chromophore systems, we suggest that the energy of the Soret pi* state of cytochrome a may be affected by (1) changes in the local dielectric, possibly brought about by movement of a charged amino acid side chain in proximity to the heme group, or (2) pi-pi interactions between the heme and aromatic amino acid residues.     

Crystal structure of oxidized Bacillus pasteurii cytochrome c553 at 0.97-A resolution

This article reports the first X-ray structure of the soluble form of a c-type cytochrome isolated from a Gram-positive bacterium. Bacillus pasteurii cytochrome c(553), characterized by a low reduction potential and by a low sequence homology with cytochromes from Gram-negative bacteria or eukaryotes, is a useful case study for understanding the structure-function relationships for this class of electron-transfer proteins. Diffraction data on a single crystal of cytochrome c(553) were obtained using synchrotron radiation at 100 K. The structure was determined at 0.97-A resolution using ab initio phasing and independently at 1.70 A in an MAD experiment. In both experiments, the structure solution exploited the presence of a single Fe atom as anomalous scatterer in the protein. For the 0.97-A data, the phasing was based on a single data set. This is the most precise structure of a heme protein to date. The crystallized cytochrome c(553) contains only 71 of the 92 residues expected from the intact protein sequence, lacking the first 21 amino acids at the N-terminus. This feature is consistent with previous evidence that this tail, responsible for anchoring the protein to the cytoplasm membrane, is easily cleaved off during the purification procedure. The heme prosthetic group in B. pasteurii cytochrome c(553) is surrounded by three alpha-helices in a compact arrangement. The largely exposed c-type heme group features a His-Met axial coordination of the Fe(III) ion. The protein is characterized by a very asymmetric charge distribution, with the exposed heme edge located on a surface patch devoid of net charges. A structural search of a representative set of protein structures reveals that B. pasteurii cytochrome c(553) is most similar to Pseudomonas cytochromes c(551), followed by cytochromes c(6), Desulfovibrio cytochrome c(553), cytochromes c(552) from thermophiles, and cytochromes c from eukaryotes. Notwithstanding a low sequence homology, a structure-based alignment of these cytochromes shows conservation of three helical regions, with different additional secondary structure motifs characterizing each protein. In B. pasteurii cytochrome c(553), these motifs are represented by the shortest interhelix connecting fragments observed for this group of proteins. The possible relationships between heme solvent accessibility and the electrochemical reduction potential are discussed.     

Redox-dependent structure change and hyperfine nuclear magnetic resonance shifts in cytochrome c

Proton nuclear magnetic resonance assignments for reduced and oxidized equine cytochrome c show that many individual protons exhibit different chemical shifts in the two protein forms, reflecting diamagnetic shift effects due to structure change, and in addition contact and pseudocontact shifts that occur only in the paramagnetic oxidized form. To evaluate the chemical shift differences (delta delta) for structure change, we removed the pseudocontact shift contribution by a calculation based on knowledge of the electron spin g tensor. The g-tensor parameters were determined from the delta delta values of a large set (64) of C alpha H protons at well-defined spatial positions in the oxidized horse protein. The g-tensor calculation, when repeated using only 12 available C alpha H proton resonances for cytochrome c from tuna, proved to be remarkably stable. The largest principal value of the g tensor (gz) falls precisely along the ligand bond between the heme iron and methionine-80 sulfur, while gx and gy closely match the natural heme axes defined by the pyrrole nitrogens. The derived g tensor was then used together with spatial coordinates for the oxidized form to calculate the pseudocontact shift contribution (delta pc) to proton resonances at 400 identifiable sites throughout the protein, so that the redox-dependent chemical shift discrepancy, delta delta-delta pc, could be evaluated. Large residual changes in chemical shift define the Fermi contact shifts, which are found as expected to be limited to the immediate covalent structure of the heme and its ligands and to be asymmetrically distributed over the heme. Smaller chemical shift discrepancies point to a concerted change, involving residues 39-43 and 50-60 (bottom of the protein), and to other changes in the immediate vicinity of the heme ligands. Also, the three internal water molecules are implicated in redox sensitivity. The residues found to change are in good but not perfect agreement with prior X-ray diffraction observations of subangstrom redox-related displacements in the tuna protein. The chemical shift discrepancies observed appear in the main to reflect structure-dependent diamagnetic shifts rather than hyperfine effects due to displacements in the pseudocontact shift field. Although 51 protons in 29 different residues exhibit significant chemical shift changes, the general impression is one of small structural adjustments to redox-dependent strain rather than sizeable structural displacements or rearrangements.     

EPR determination of interaction redox potentials in a multiheme cytochrome: cytochrome c3 from Desulfovibrio desulfuricans Norway

In cytochromes c3 which contain four hemes per molecule, the redox properties of each heme may depend upon the redox state of the others. This effect can be described in terms of interaction redox potentials between the hemes and must be taken into account in the characterization of the redox properties of the molecule. We present here a method of measurement of these interactions based on the EPR study of the redox equilibria of the protein. The microscopic and macroscopic midpoint potentials and the interaction potentials are deduced from the analysis of the redox titration curves of the intensity and the amplitude of the EPR spectrum. This analysis includes a precise simulation of the spectrum of the protein in the oxidized state in order to determine the relative contribution of each heme to the spectral amplitude. Using our method on cytochrome c3 from D. desulfuricans Norway, we found evidence for the existence of weak interaction potentials between the hemes. The three interaction potentials which have been measured are characterized by absolute values lower than 20 mV in contrast with the values larger than 40-50 mV which have been reported for cytochrome c3 from D. gigas. Simulations of the spectra of samples poised at different potentials indicate a structural modification of the heme with the most negative potential during the first step of reduction. The correspondence between the redox sites as characterized by the EPR potentiometric titration and the hemes in the tridimensional structure is discussed.     

Redox protein electron-transfer mechanisms: electrostatic interactions as a determinant of reaction site in c-type cytochromes

The effect of ionic strength on the rate constant for electron transfer has been used to determine the magnitude and charge sign of the net electrostatic potential which exists in close proximity to the sites of electron transfer on various c-type cytochromes. The negatively charged ferricyanide ion preferentially reacts at the positively charged exposed heme edge region on the front side of horse cytochrome c and Paracoccus cytochrome c2. In contrast, at low ionic strength, the positively charged cobalt phenanthroline ion interacts with the negatively charged back side of cytochrome c2, and at high ionic strength at a positively charged site on the front side of the cytochrome. With horse cytochrome c, over the ionic strength range studied, cobalt phenanthroline reacts only at a positively charged site which is probably not at the heme edge. These inorganic oxidants do not react at the relatively uncharged exposed heme edge sites on Azotobacter cytochrome c5 and Pseudomonas cytochrome c-551, but rather at a negatively charged site which is away from the heme edge. The results demonstrate that at least two electron-transferring sites on a single cytochrome can be functional, depending on the redox reactant used and the ionic strength. Electrostatic interactions between charge distributions on the cytochrome surface and the other reactant, or interactions involving uncharged regions on the protein(s), are critical in determining the preferred sites of electron transfer and reaction rate constants. When unfavorable electrostatic effects occur at a site near the redox center, less optimal sites at a greater distance can become kinetically important.     

Amino acid sequence of subunit V of bovine heart cytochrome oxidase, the heme alpha-containing subunit.

The complete amino acid sequence of the heme alpha-containing subunit V of bovine heart cytochrome oxidase was determined to be: H2N-Ser-His-Gly-Ser-His-Glu-Thr-Asp-Glu-Glu-Phe-Asp-Ala-Arg-Trp-Val-Thr-Tyr-Phe-Asn-Lys-Pro-Asp-Ile-Asp-Ala-Trp-Glu-Leu-Arg-Lys-Gly-Met-Asn-Thr-Leu-Val-Gly-Tyr-Asp-Leu-Val-Pro-Glu-Pro-Lys-Ile-Ile-Asp-Ala-Ala-Leu-Arg-Ala-Cys-Arg-Arg-Leu-Asn-Asp-Phe-Ala-Ser-Ala-Val-Arg-Ile-Leu-Glu-Val-Val-Lys-Asp-Lys-Ala-Gly-Pro-His-Lys-Glu-Ile-Tyr-Pro-Tyr-Val-Ile-Gln-Glu-Leu-Arg-Pro-Thr-Leu-Asn-Glu-Leu-Gly-Ile-Ser-Thr-Pro-Glu-Glu-Leu-Gly-Leu-Asp-Lys-Val-COOH. The subunit V is a single polypeptide which consists of 109 amino acid residues. The protein contains 48.6% hydrophobic residues and 34.0% hydrophilic residues and it is an acidic protein having a net charge of -3 at neutral pH. The molecular weight of subunit V was calculated to be 12,436 and that for the heme alpha-containing polypeptide was 13,295.