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Electrostatic control of the substrate access channel in cytochrome P-450cam.

Camphor binding to ferric cytochrome P-450cam is a two-step process. The first step corresponds to the diffusion of camphor into the heme pocket, and the second one corresponds to an observable spin transition of the heme iron. In this paper, electrostatic interactions that may control the opening of the structure to allow substrate access to the buried and not solvent-exposed active site were examined. The electrostatic interactions occurring at the protein surface were weakened by increasing the ionic strength of the medium with sodium salts and strengthened by decreasing the dielectric constant of the medium with ethylene glycol as a cosolvent. The results obtained with the wild-type protein were compared to those obtained with the site-directed mutant of cytochrome P-450cam in which the Arg 186-Asp 251 and Lys 178-Asp 251 salt bridges, located at the entrance of the proposed access channel, were suppressed by replacing Asp 251 with an asparagine residue. Over a range of sodium chloride concentrations from 0 to 400 mM, camphor binding is favored, as seen in the variation in the first step dissociation equilibrium constant, K1d, which decreases from 49.5 to 24 microM, respectively. Addition of ethylene glycol favors the dissociation of the substrate-bound complex. The addition of sodium to the ethylene glycol-containing samples reverses the effect of the cosolvent. Removal of the Arg 186-Asp 251 and Lys 178-Asp 251 salt bridges results in an alteration in camphor binding in which K1d is equal to 34 microM without sodium.(ABSTRACT TRUNCATED AT 250 WORDS)

Binding Sites↗

Anion binding and pH-dependent electrostatic effects in ribonuclease.

The solvent-accessibility-modified, Tanford-Kirkwood, discrete charge model for electrostatic effects is applied to both ribonuclease A and ribonuclease S. The behavior of individual titratable sites and the pH-dependent free energy of denaturation are correctly predicted. The use of the solvent-accessibility factor in reducing charge-site interactions introduces a higher Coulombic shielding for solvent-exposed sites. This shielding is interpreted as a higher local strength or alternatively a higher effective dielectric constant. Specific anion binding sites are determined by locating areas of high positive electrostatic potential at the protein solvent interface. The potential and thus the anion affinity of a given site are calculated and shown to vary with the pH-dependent charge array. pH-dependent anion binding constants are calculated for the ribonuclease S active site. These binding constants and the predicted response of the active-site histidine pK1/2 values to anion binding are shown to agree with experimental determinations.

Anions↗

Electrostatic modification of protein surfaces: effect on hemoglobin ligation and solubility.

Protein amino groups can be carboxymethylated under mild conditions by the combined use of glyoxylate ion and cyanoborohydride. The amino group is converted to a zwitterionic residue where the pK of the secondary amine is only slightly altered and a carboxyl group has been added some 3 A from the nitrogen atom in the amine. Modification of hemoglobin to low levels of carboxymethylation yields derivatives specifically modified at the terminal alpha-amino groups. These modified hemoglobins are models for the interactions between the protein and small anions. When the extent of modification is increased by treating the protein with a higher concentration of the modifying agents, lysine residues become converted to N epsilon-(carboxymethyl)lysine. In excess of 90% of lysine residues in hemoglobin and myoglobin can be modified by this technique. The increased negative charge can be adjusted to any intermediate level of modification. The change in electrostatic free energy that results from the altered distribution of charge on the protein surface can be correlated with functional properties. Thus, the increased repulsion between the hemoglobin dimers leads to dimerlike oxygen binding properties at a high degree of modification. Similarly, changes in protein solubility secondary to modification reflect altered tetramer-tetramer interactions in the solid state. This method for achieving an altered distribution of charge on the protein surface, a method which can be carried out in a specific or nonspecific fashion to achieve varying degrees of modification, represents a powerful tool for the study of electrostatic interactions in protein chemistry.

Amino Acid Sequence↗

Electron-transfer reactions of photoreduced flavin analogues with c-type cytochromes: quantitation of steric and electrostatic factors.

We have found correlations between rate constants and the difference in redox potential of the reactants for electron-transfer reactions between oxidized cytochromes and either photoproduced riboflavin or flavin mononucleotide (FMN) semiquinones (the latter rate constants extrapolated to infinite ionic strength). The riboflavin-cytochrome rate constants are about 70% of those for reduction by lumiflavin, probably because of steric interference by the ribityl side chain. Reduction of cytochromes by FMN semiquinone was ionic strength dependent in all cases, due to electrostatic interactions. Extrapolation of rate constants to infinite ionic strength shows that the phosphate exerts a significant steric effect as well (rate constants average about 27% of those for lumiflavin, although part of this decrease is due to a difference in the semiquinone pK value). Differences in the magnitude of the FMN steric effect correlate well with surface topology differences for those cytochromes whose three-dimensional structures are known. Mitochondrial cytochromes c and the cytochromes c2 all showed attractive (plus-minus) interaction with FMN in spite of the fact that some of these proteins have large net negative charges. Four small c-type cytochromes (including Pseudomonas cytochrome c-551) show a weak repulsive interaction with FMN semiquinone. We conclude that flavosemiquinones interact at a site on the cytochromes that is near the exposed heme edge. There is a large positive electrostatic field at this site in mitochondrial cytochrome c and the cytochromes c2, but this region is primarily hydrophobic in Pseudomonas cytochrome c-551 and in the other small bacterial cytochromes.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗

Diffusion-enhanced lanthanide energy-transfer study of DNA-bound cobalt(III) bleomycins: comparisons of accessibility and electrostatic potential with DNA complexes of ethidium and acridine orange.

Energy transfer in the "rapid-diffusion" limit reflects the equilibrium properties of a donor-acceptor system. Rates of energy transfer from freely diffusing terbium chelates to DNA-binding chromophores change dramatically when DNA is added; energy transfer from an electrically neutral chelate is reduced because the energy acceptor becomes partially buried in DNA, while energy transfer from a positive chelate is increased because of electrostatic attraction. The rate constants for energy transfer to DNA-bound chromophores from a positively charged terbium chelate, relative to those from a neutral chelate, were used to estimate the following values for the electrostatic potential near the surface of each DNA-bound acceptor at 298 K in the presence of 1.0 mM added salt (in units of -e/kT): acridine orange, 4.54 +/- 0.11; ethidium, 4.66 +/- 0.07; green Co(III) bleomycin A2, 4.06 +/- 0.11; orange Co(III) bleomycin A2, 3.11 +/- 0.10. Smaller numbers indicate less negative potentials; these can be due to a combination of (1) positive charge on the chromophore, (2) location of the chromophore [particularly Co(III) bleomycin] away from the DNA phosphates, and/or (3) separation of DNA phosphate negative charges by an intercalator. The magnitudes of the individual rate constants indicate that all the DNA-bound chromophores can be directly encountered by the terbium probes. Energy-transfer rate constants from a neutral terbium chelate to DNA-bound and free acceptors can provide a measure of the accessibility of the terbium probe to each bound chromophore. The ratios of these rate constants were as follows: acridine orange, 0.17 +/- 0.01; ethidium, 0.27 +/- 0.02; green form of Co(III) bleomycin A2, 0.48 +/- 0.06; orange form of Co(III) bleomycin A2, 0.71 +/- 0.06. These results are consistent with the probable differences in binding mechanisms for the intercalating chromophores (ethidium and acridine orange) as compared to the Co(III) bleomycins (in which the relevant chromophores are nonintercalating metal centers). In addition, all the results imply that the green Co(III) bleomycin chromophore binds closer to DNA than the orange; this provides a first step toward understanding the structural basis for the different biological properties of these metallobleomycins. Control experiments and theoretical considerations necessary to establish the validity of the results are also presented.

Acridine Orange↗

Electrostatic interaction between anions bound to site I and the retinal Schiff base of halorhodopsin.

The influence of different anions on the deprotonation of the retinal Schiff base of halorhodopsin in the dark was investigated. We find that a large number of anions cause a significant increase of the pKa of the Schiff base, an effect attributed to binding to "site I" on the protein. The concentration dependencies of the spectroscopic shifts associated with the changes of the pKa yielded dissociation constants (and thus binding energies) for the anions, which were related to the Stokes radii. The data fit the predictions of electrostatic interaction between the anions and the positive charge associated with site I, if the latter is located within a few angstroms from the surface of the protein. The specificity of site I toward various anions is quantitatively explained by the differences in the change of Born energy upon transfer of the anions from water to the binding site. The changes in the deprotonation energy of the Schiff base upon the binding of anions, delta delta Gdeprot, could be calculated from the delta pKa at infinite anion concentration. Unexpectedly, the delta delta Gdeprot values were remarkably close to the energies of binding to site I. Thus, site I and the Schiff base are strongly electrostatically coupled, either because of close proximity or because of the possibility of allosteric energy transfer between them.

Anions↗

Fluorescent probes of electrostatic potential 1 nm from the membrane surface.

We measured the electrostatic potential 1 nm from the surface of charged phospholipid bilayer membranes to test the predictions of the Gouy-Chapman theory. Fluorescent probes (anthraniloyl, 5-(dimethylamino)naphthalene-1-sulfonyl, Lucifer yellow) were attached covalently to the sialic acid residue of the ganglioside galactosyl-N-acetylgalactosaminyl(N-acetylneuraminyl)galactosylglucosylc eramide (GM1). These fluorescent gangliosides were incorporated into neutral [phosphatidylcholine (PC)] or charged [phosphatidylserine (PS)] phospholipid bilayers, and the fluorescence was quenched with the cations thallium and 4-amino-2,2,6,6-tetramethylpiperidine-1-oxyl (tempamine). We calculated the electrostatic potential at the chromophore from the quenching ratio using the Boltzmann relation: the average potential was -30 mV for PS bilayers in 0.1 M NaNO3. We assume the chromophore is 1 nm from the surface because X-ray diffraction measurements demonstrate that the sialic acid residue of GM1 is 1 nm from the surface of a PC/GM1 bilayer [McDaniel, R. V., & McIntosh, T. J. (1986) Biophys. J. 49, 94-96]. We also used thallium and tempamine to quench the fluorescence of chromophores located at the surface of the PS membranes; in 0.1 M NaNO3 the average surface potential was -80 mV, which agrees with other measurements. The Gouy-Chapman theory predicts that the potential 1 nm from a membrane with a surface potential of -80 mV is -24 mV; this prediction agrees qualitatively with the experimental results obtained with fluorescent gangliosides.

Electrochemistry↗

Reconstitution of transferrin receptor in mixed lipid vesicles. An example of the role of elastic and electrostatic forces for protein/lipid assembly.

We studied the interaction of transferrin receptors (of cell line Molt-4) with mixed model membranes as a function of lipid chain length (phospholipids with C14:0 and C18:1 hydrocarbon chains) and of the surface charge of the membrane using mixtures of C14:0 lecithin (DMPC) with C14:0 phosphatidylglycerol (DMPG) and C14:0 phosphatidylserine (DMPS). Spontaneous self-assembly of receptors and lipids was achieved by freeze-thaw cycles of a codispersion of mixed vesicles and receptors in buffer and subsequent separation of receptor-loaded and receptor-free vesicles by density gradient centrifugation. Information on specific lipid/protein interaction mechanisms was obtained by evaluation of protein-induced shifts of phase boundaries of lipid mixtures by calorimetry and by FTIR spectroscopy of partially deuterated lipid mixtures. The important role (1) of minimizing the elastic forces caused by the mismatch of the lengths of hydrophobic cores of the protein (lp) and the bilayer (lL) and (2) of the electrostatic coupling of protein head groups with the charged membrane/water interface for the lipid/protein self-assembly is established. The electrostatic interaction energy per receptor is about 10(3) kBT (by coupling to about 1000 charged lipids) which is sufficient to overcompensate the elastic energy associated with a mismatch of lp - lL approximately 1.0 nm. The maximum receptor concentration incorporated was measured as a function of membrane surface charge and lipid chain length. The maximum receptor molar fraction varied from xpmax = 5 x 10(-5) for DMPC to xpmax = 4 x 10(-4) for 1:1 DMPC/DMPG; moreover xpmax is higher for DMPS than for DMPG as charged component. For the long-chain lipids, xpmax is higher for a 9:1 DEPE/DEPC mixture [(4.2-9) x 10(-4)] than for pure DEPC (ca. 3.5 x 10(-4)). By decomposition of reconstituted receptors with proteases, we demonstrated the homogeneous orientation of the receptor with its extracellular head group pointing to the convex side of the vesicles.(ABSTRACT TRUNCATED AT 250 WORDS)

Chemical Phenomena↗

Estimating the contribution of engineered surface electrostatic interactions to protein stability by using double-mutant cycles.

Coulombic interactions between charges on the surface of proteins contribute to stability. It is difficult, however, to estimate their importance by protein engineering methods because mutation of one residue in an ion pair alters the energetics of many interactions in addition to the coulombic energy between the two components. We have estimated the interaction energy between two charged residues, Asp-12 and Arg-16, in an alpha-helix on the surface of a barnase mutant by invoking a double-mutant cycle involving wild-type enzyme (Asp-12, Thr-16), the single mutants Thr----Arg-16 and Asp----Ala-12, and the double mutant Asp----Ala-12, Thr----Arg-16. The changes in free energy of unfolding of the single mutants are not additive because of the coulombic interaction energy. Additivity is restored at high concentrations of salt that shield electrostatic interactions. The geometry of the ion pair in the mutant was assumed to be the same as that in the highly homologous ribonuclease from Bacillus intermedius, binase, which has Asp-12 and Arg-16 in the native enzyme. The ion pair does not form a hydrogen-bonded salt bridge, but the charges are separated by 5-6 A. The mutant barnase containing the ion pair Asp-12/Arg-16 is more stable than wild type by 0.5 kcal/mol, but only a part of the increased stability is attributable to the electrostatic interaction. We present a formal analysis of how double-mutant cycles can be used to measure the energetics of pairwise interactions.

Amino Acid Sequence↗

Electrostatic effects in hemoglobin: hydrogen ion equilibria in human deoxy- and oxyhemoglobin A.

The modified Tanford-Kirkwood theory of Shire et al. [Shire, S. J., Hanania, G.I.H., & Gurd, F.R.N. (1974) Biochemistry 13, 2967] for electrostatic interactions was applied to the hydrogen ion equilibria of human deoxyhemoglobin and oxyhemoglobin. Atomic coordinates for oxyhemoglobin were generated by the application of the appropriate rigid rotation function to alpha and beta chains of the deoxyhemoglobin structure [Fermi, G. (1975) J. Mol. Biol. 97, 237]. The model employs two sets of parameters derived from the crystalline protein structures, the atomic coordinates of charged amino acid residues and static solvent accessibility factors to reflect their individual degrees of exposure to solvent. Theoretical titration curves based on a consistent set of pKint values compared closely with experimental potentiometric curves. Theoretical pK values at half-titration for individual protein sites corresponded to available observed values for both quaternary states. The results bring out the cumulative effects of numerous electrostatic interactions in the tetrameric structures and the major effects of the quaternary transition that result from changes in static solvent accessibility of certain ionizable groups.

Amino Acids↗

Duplex formation of a nonionic oligo(deoxythymidylate) analogue (heptadeoxythymidylyl-(3'-5')-deoxythymidine heptaethyl ester (d-(Tp(Et))7T)) with poly(deoxyadenylate). Evaluation of the electrostatic interaction.

The heptaethyl ester of heptadeoxythymidylyl-(3'-5')-deoxythymidine (d-[Tp(Et)]7T or d-T8-Et) has been prepared by chemical methods. The material, consisting of a mixture of diastereoisomers, forms a 1:1 complex with (dA)n in neutral aqueous buffer; this interaction is virtually independent of ionic strength. The octamer triester does not bind to (dA)n-(dT)n, and it interacts with (rA)n only at low temperatures. By cochromatography with (dA)n on Sephadex G-50, d-T8-Et fractions with different binding affinities for the polyadenylates were obtained. This heterogeneity in binding affinity is ascribed to the diastereoisomerism of d-T8-Et. Enthalpies of dupoex formation were determined by the concentration variation method. At 0.1 M sodium ion concentration, the enthalpy of binding of the various d-T8-Et fractions to (dA)n is essentially invariant (-8.1 kcal/mol of base pairs at 0 degrees C to -8.6 kcal at 25 degrees C) and 1.6 kcal/mol of base pairs more negative than the enthalpy of binding of the phosphodiester analogue, d-(Tp)7T, to (dA)n (-6.8 kcal/mol of base pairs at 11 degrees C). This difference is the electrostatic contribution to the enthalpy of duplex formation, arising from the interstrand electrostatic repulsion and the intrastrand repulsion in d-(Tp)7T. The entropy of binding to (dA)n is more negative for the octamer triesters than for the diester analogue, and is different for the various d-T8-Et fractions. This is interpreted in terms of varying degrees of restriction of rotational freedom for the ethyl substituents upon double helix formation.

Chromatography, Gel↗

The magnitude of electrostatic interactions in inhibitor binding and during catalysis by ribonuclease A.

It is demonstrated that a model of nucleotide binding to ribonuclease A similar to that proposed by Hammes and coworkers (G. G. Hammes (1968), Adv. Protein Chem. 23, 1) is at least, approximately applicable for both cyclic nucleotide substrates and mononucleotide inhibitors at pH values less than or equal to 6.5 and as a function of ionic strength. Calorimetric data on various inhibitors show that the binding reaction can be thermodynamically dissected into a contribution arising from van der Waal's interaction of the nucleoside moiety, characterized by a large negative enthalpy change, and a contribution arising from electrostatic interactions between the negatively charged phosphate group of the inhibitor and the positively charged protein fabric, characterized by a large positive unitary entropy change. Assuming a catalytic mechanism involving the formation of a dianionic pentacoordinated phosphate transition state intermediate, the magnitude of the effect of electrostatic interactions on the overall rate enhancement by the enzyme is estimated to be 2 times 10(2) to 10(6). It is suggested that this effect, along with substrate approximation effects, is sufficient to "explain" the catalytic behavior of the enzyme.

Binding Sites↗

Nucleotide Binding to Na,K-ATPase: The Role of Electrostatic Interactions.

The contribution of electrostatic forces to the interaction of Na,K-ATPase with adenine nucleotides was investigated by studying the effect of ionic strength on nucleotide binding. At pH 7.0 and 20 degrees C, there was a qualitative correlation between the equilibrium dissociation constant (K(d)) values for ATP, ADP, and MgADP and their total charges. All K(d) values increased with increasing ionic strength. According to the Debye-Hückel theory, this suggests that the nucleotide binding site and its ligands have "effective" charges of opposite signs. However, quantitative analysis of the dependence on ionic strength shows that the product of the effective electrostatic charges on the ligand and the binding site is the same for all nucleotides, and is therefore independent of the total charge of the nucleotide. The data suggest that association of nucleotides with Na,K-ATPase is governed by a partial charge rather than the total charge of the nucleotide. This charge, interacting with positive charges on the protein, is probably the one corresponding to the alpha-phosphate of the nucleotide. Dissociation rate constants measured in complementary transient kinetic experiments were 13 s(-1) for ATP and 27 s(-1) for ADP, independent of the ionic strength in the range 0.1-0.5 M. This implies similar association rate constants for the two nucleotides (about 40 x 10(6) M(-1) s(-1) at I = 0.1 M). The results suggest that long-range Coulombic forces, affecting association rates, are not the main contributors to the observed differences in affinities, and that local interactions, affecting dissociation rates, may play an even greater role.

Adenosine Diphosphate↗

Electrostatic effects in highly charged proteins: salt sensitivity of pKa values of histidines in staphylococcal nuclease.

The pK(a) values of most histidines in small peptides and in myoglobin increase on average by 0.30 unit between 0.02 and 1.5 M NaCl [Kao et al. (2000) Biophys. J. 79, 1637]. The DeltapK(a) values reflect primarily the ionic strength dependence of the solvation energy; screening of Coulombic interactions contributes only in a minor way. This implies that Coulombic interactions are weak, or that attractive and repulsive contributions to the pK(a) values are balanced. To distinguish experimentally between these two possibilities, and to further characterize the magnitude and salt sensitivity of surface electrostatic interactions in proteins, the salt dependence of pK(a) values of histidines in staphylococcal nuclease was measured by (1)H NMR spectroscopy. Three of the four histidines titrated with significantly depressed pK(a) values, and the salt sensitivity of all histidine pK(a) values was substantial. In three cases, the pK(a) values increased by a full unit between 0.01 and 1.5 M KCl. Anion-specific effects were found; the pK(a) values measured under equivalent ionic strengths in SCN(-) and SO(4)(2-) were higher than in Cl(-); the order of the sensitivity of pK(a) values to anions was SCN(-) > Cl(-) > SO(4)(2-). Structure-based pK(a) calculations with continuum methods were performed to interpret the measured effects structurally and to test their ability to capture the experimental behavior. Calculations in which the protein interior was treated empirically with a dielectric constant of 20 reproduced the pK(a) values and their dependence on the concentration of Cl(-). According to the calculations, the pK(a) values are depressed because of unfavorable self-energies and repulsive Coulombic interactions. Their striking salt sensitivity reflects screening of weak, repulsive, Coulombic interactions among charges separated by more than 10 A. Long-range Coulombic interactions on the surfaces of proteins are weak, but they can add up to produce substantial electrostatic effects when positive and negative charges are not balanced.

Animals↗

Double mutant studies identify electrostatic interactions that are important for docking cytochrome c2 onto the bacterial reaction center.

Cytochrome c2 (cyt) is the mobile electron donor to the reaction center (RC) in photosynthetic bacteria. The electrostatic interactions involved in the dynamics of docking of cyt onto the RC were examined by double mutant studies of the rates of electron transfer between six modified Rhodobacter sphaeroides RCs in which negatively charged acid residues were replaced with Lys and five modified Rhodobacter capsulatus Cyt c2 molecules in which positively charged Lys residues were replaced with Glu. We measured the second-order rate constant, k2, for electron transfer from the reduced cyt to the oxidized primary donor on the RC, which reflects the energy of the transition state for the formation of the active electron transfer complex. Strong interactions were found between Lys C99 and Asp M184/Glu M95, and between Lys C54 and Asp L261/Asp L257. The interacting residues were found to be located close to each other in the recently determined crystal structure of the cyt-RC complex [Axelrod, H., et al. (2002) J. Mol. Biol. (in press)]. The interaction energies were approximately inversely proportional to the distances between charges. These results support earlier suggestions [Tetreault, M., et al. (2001) Biochemistry 40, 8452-8462] that the structure of the transition state in solution resembles the structure of the cyt-RC complex in the cocrystal and indicate that specific electrostatic interactions facilitate docking of the cyt onto the RC in a configuration optimized for both binding and electron transfer. The specific interaction between Asp M184 and Lys C99 may help to nucleate short-range hydrophobic contacts.

Cytochrome c Group↗

Residual electrostatic effects in the unfolded state of the N-terminal domain of L9 can be attributed to nonspecific nonlocal charge-charge interactions.

Residual electrostatic interactions in the unfolded state of the N-terminal domain of L9 (NTL9) were found by Kuhlman et al. [(1999) Biochemistry 38, 4896-4903]. These residual interactions are analyzed here by the Gaussian-chain model [Zhou, H.-X. (2002) Proc. Natl. Acad. Sci. U.S.A. 99, 3569-3574]. The original model is made more realistic by replacing "standard" model-compound pK(a) values for ionizable groups by those measured by Kuhlman et al. in peptide fragments of NTL9. The predicted pH dependence of the unfolding free energy is in agreement with experiment over the pH range of 1-7 at ionic strengths of 100 and 750 mM. This indicates that the residual electrostatic effects in the unfolded state of NTL9 can be attributed to nonspecific nonlocal charge-charge interactions.

Amino Acid Sequence↗

The stable assembly of newly synthesized PsaE into the photosystem I complex occurring via the exchange mechanism is facilitated by electrostatic interactions.

Photosystem I (PSI) is a photochemically active membrane protein complex that functions at the reducing site of the photosynthetic electron-transfer chain as plastocyanin-ferredoxin oxidoreductase. PsaE, a peripheral subunit of the PSI complex, plays an important role in the function of PSI. PsaE is involved in the docking of ferredoxin/flavodoxin to the PSI complex and also participates in the cyclic electron transfer around PSI. The molecular characterization of the assembly of newly synthesized PsaE in the thylakoid membranes or in isolated PSI complexes is the subject of the present study. For this purpose the Mastigocladus laminosus psaE gene was cloned and overexpressed in Escherichia coli, and the resulting PsaE protein was purified to homogeneity by affinity chromatography. The purified PsaE was then introduced into thylakoids isolated from M. laminosus, and the newly introduced PsaE subunit saturates the membrane. The solubilization and separation of the different thylakoid protein complexes indicated that PsaE accumulates specifically in its functional location, the PSI complex. A similar stable assembly was detected when PsaE was introduced into purified PSI complexes, i.e., in the absence of other thylakoid components. This strongly indicates that the information for the stable assembly of PsaE into PSI lies within the polypeptide itself and within other subunits of the PSI complex that interact with it. To determine the nature of these interactions, the assembly reaction was performed in conditions affecting the ionic/osmotic strength. We found that altering the ionic strength significantly affects the capability of PsaE to assemble into isolated thylakoids or PSI complexes, strongly supporting the fact that electrostatic interactions are formed between PsaE and other PSI subunits. Moreover, the data suggest that the formation of electrostatic interactions occurs concomitantly with an exchange step in which newly introduced PsaE replaces the subunit present in situ.

Cyanobacteria↗

Investigations of Sso7d catalytic residues by NMR titration shifts and electrostatic calculations.

Sso7d is a small basic protein consisting of 62 amino acids isolated from the thermoacidophilic archeobacterium Sulfolobus solfataricus. The protein is endowed with DNA binding properties, RNase activity, and the capability of rescuing aggregated proteins in the presence of ATP. In this study, the electrostatic properties of Sso7d are investigated by using the Poisson-Boltzmann calculation of the surface potential distribution and following by NMR spectroscopy the proton chemical shift pH titration of acidic residues. Although the details of the catalytic mechanism still have to be defined, the results from NMR experiments confirm the possible involvement of Glu35 as the proton acceptor in the catalytic reaction, as seen by its abnormally high pK(a) value. Poisson-Boltzmann calculations and NMR titration shifts suggest the presence of a possible hydrogen bond between Glu35 and Tyr33, with a consequent rather rigid arrangement at these positions. Comparison with RNase T1 suggests that Tyr7 may be a good candidate for acting as a proton donor in the active site of Sso7d as shown by its low phenolic pK(a) of approximately 9.3. Titration experiments performed with the UpA, a RNA dinucleotide model, showed that the protein residues affected by the interaction are mainly located in a different region with respect to the surface affected by DNA recognition, in good agreement with the surface potential distribution found with electrostatic calculations.

Archaeal Proteins↗