Contributions of engineered surface salt bridges to the stability of T4 lysozyme determined by directed mutagenesis.

Six designed mutants of T4 lysozyme were created in an attempt to create putative salt bridges on the surface of the protein. The first three of the mutants, T115E (Thr 115 to Glu), Q123E, and N144E, were designed to introduce a new charged side chain close to one or more existing charged groups of the opposite sign on the surface of the protein. In each of these cases the putative electrostatic interactions introduced by the mutation include possible salt bridges between residues within consecutive turns of an alpha-helix. Effects of the mutations ranged from no change in stability to a 1.5 degrees C (0.5 kcal/mol) increase in melting temperature. In two cases, secondary (double) mutants were constructed as controls in which the charge partner was removed from the primary mutant structure. These controls proteins indicate that the contributions to stability from each of the engineered salt bridges is very small (about 0.1-0.25 kcal/mol in 0.15 M KCl). The structures of the three primary mutants were determined by X-ray crystallography and shown to be essentially the same as the wild-type structure except at the site of the mutation. Although the introduced charges in the T115E and Q123E structures are within 3-5 A of their intended partner, the introduced side chains and their intended partners were observed to be quite mobile. It has been shown that the salt bridge between His 31 and Asp 70 in T4 lysozyme stabilizes the protein by 3-5 kcal/mol [Anderson, D. E., Becktel, W. J., & Dahlquist, F. W. (1990) Biochemistry 29, 2403-2408]. To test the effectiveness of His...Asp interactions in general, three additional double mutants, K60H/L13D, K83H/A112D, and S90H/Q122D, were created in order to introduce histidine-aspartate charge pairs on the surface of the protein. Each of these mutants destabilizes the protein by 1-3 kcal/mol in 0.15 M KCl at pH values from 2 to 6.5. The X-ray crystallographic structure of the mutant K83H/A112D has been determined and shows that there are backbone conformational changes of 0.3-0.6 A extending over several residues. The introduction of the histidine and aspartate presumably introduces strain into the folded protein that destabilizes this variant. It is concluded that pairs of oppositely charged residues that are on the surface of a protein and have freedom to adopt different conformations do not tend to come together to form structurally localized salt bridges. Rather, such residues tend to remain mobile, interact weakly if at all, and do not contribute significantly to protein stability. It is argued that the entropic cost of localizing a pair of solvent-exposed charged groups on the surface of a protein largely offsets the interaction energy expected from the formation of a defined salt bridge. There are examples of strong salt bridges in proteins, but such interactions require that the folding of the protein provides the requisite driving energy to hold the interacting partners in the correct rigid alignment.     

Anticooperativity in a Glu-Lys-Glu salt bridge triplet in an isolated alpha-helical peptide

Salt bridges between oppositely charged side chains are well-known to stabilize protein structure, though their contributions vary considerably. Here we study Glu-Lys and Lys-Glu salt bridges, formed when the residues are spaced i, i + 4 surface of an isolated alpha-helix in aqueous solution. Both are stabilizing by -0.60 and -1.02 kcal/mol, respectively, when the interacting residues are fully charged. When the side chains are spaced i, i + 4, i + 8, forming a Glu-Lys-Glu triplet, the second salt bridge provides no additional stabilization to the helix. We attribute this to the inability of the central Lys to form two salt bridges simultaneously. Analysis of these salt bridges in protein structures shows that the Lys-Glu interaction is dominant, with the side chains of the Glu-Lys pair far apart.     

Comparison of the structural basis for thermal stability between archaeal and bacterial proteins

In this study, the structural basis for thermal stability in archaeal and bacterial proteins was investigated. There were many common factors that confer resistance to high temperature in both archaeal and bacterial proteins. These factors include increases in the Lys content, the bends and blanks of secondary structure, the Glu content of salt bridge; decreases in the number of main–side chain hydrogen bond and exposed surface area, and changes in the bends and blanks of amino acids. Certainly, the utilization of charged amino acids to form salt bridges is a primary factor. In both heat-resistant archaeal and bacterial proteins, most Glu and Asp participate in the formation of salt bridges. Other factors may influence either archaeal or bacterial protein thermostability, which includes the more frequent occurrence of shorter 3₁₀-helices and increased hydrophobicity in heat-resistant archaeal proteins. However, there were increases in average helix length, the Glu content in salt bridges, temperature factors and decreases in the number of main–side chain hydrogen bonds, uncharged–uncharged hydrogen bonds, hydrophobicity, and buried and exposed polar surface area in heat-resistant bacterial proteins. Evidently, there are few similarities and many disparities between the heat-resistant mechanisms of archaeal and bacterial proteins.     

Access to the complement factor B scissile bond is facilitated by association of factor B with C3b protein

Factor B is a zymogen that carries the catalytic site of the complement alternative pathway C3 convertase. During convertase assembly, factor B associates with C3b and Mg(2+) forming a pro-convertase C3bB(Mg(2+)) that is cleaved at a single factor B site by factor D. In free factor B, a pair of salt bridges binds the Arg(234) side chain to Glu(446) and to Glu(207), forming a double latch structure that sequesters the scissile bond (between Arg(234) and Lys(235)) and minimizes its unproductive cleavage. It is unknown how the double latch is released in the pro-convertase. Here, we introduce single amino acid substitutions into factor B that preclude one or both of the Arg(234) salt bridges, and we examine their impact on several different pro-convertase complexes. Our results indicate that loss of the Arg(234)-Glu(446) salt bridge partially stabilizes C3bB(Mg(2+)). Loss of the Arg(234)-Glu(207) salt bridge has lesser effects. We propose that when factor B first associates with C3b, it bears two intact Arg(234) salt bridges. The complex rapidly dissociates unless the Arg(234)-Glu(446) salt bridge is released whereupon conformational changes occur that activate the metal ion-dependent adhesion site and partially stabilize the complex. The remaining salt bridge is then released, exposing the scissile bond and permitting factor D cleavage.     

Contribution of salt bridges near the surface of a protein to the conformational stability

Salt bridges play important roles in the conformational stability of proteins. However, the effect of a surface salt bridge on the stability remains controversial even today; some reports have shown little contribution of a surface salt bridge to stability, whereas others have shown a favorable contribution. In this study, to elucidate the net contribution of a surface salt bridge to the conformational stability of a protein, systematic mutant human lysozymes, containing one Glu to Gln (E7Q) and five Asp to Asn mutations (D18N, D49N, D67N, D102N, and D120N) at residues where a salt bridge is formed near the surface in the wild-type structure, were examined. The thermodynamic parameters for denaturation between pH 2.0 and 4.8 were determined by use of a differential scanning calorimeter, and the crystal structures were analyzed by X-ray crystallography. The denaturation Gibbs energy (DeltaG) of all mutant proteins was lower than that of the wild-type protein at pH 4, whereas there was little difference between them near pH 2. This is caused by the fact that the Glu and Asp residues are ionized at pH 4 but protonated at pH 2, indicating a favorable contribution of salt bridges to the wild-type structure at pH 4. Each contribution was not equivalent, but we found that the contributions correlate with the solvent inaccessibility of the salt bridges; the salt bridge contribution was small when 100% accessible, while it was about 9 kJ/mol if 100% inaccessible. This conclusion indicates how to reconcile a number of conflicting reports about role of surface salt bridges in protein stability. Furthermore, the effect of salts on surface salt bridges was also examined. In the presence of 0.2 M KCl, the stability at pH 4 decreased, and the differences in stability between the wild-type and mutant proteins were smaller than those in the absence of salts, indicating the compensation to the contribution of salt bridges with salts. Salt bridges with more than 50% accessibility did not contribute to the stability in the presence of 0.2 M KCl.     

Surface salt bridges modulate DNA wrapping by the type II DNA-binding protein TF1

The histone-like protein HU is involved in compaction of the bacterial genome. Up to 37 bp of DNA may be wrapped about some HU homologues in a process that has been proposed to depend on a linked disruption of surface salt bridges that liberates cationic side chains for interaction with the DNA. Despite significant sequence conservation between HU homologues, binding sites from 9 to 37 bp have been reported. TF1, an HU homologue that is encoded by Bacillus subtilis bacteriophage SPO1, has nM affinity for 37 bp preferred sites in DNA with 5-hydroxymethyluracil (hmU) in place of thymine. On the basis of electrophoretic mobility shift assays, we show that TF1-DNA complex formation is associated with a net release of only approximately 0.5 cations. The structure of TF1 suggests that Asp13 can form a dehydrated surface salt bridge with Lys23; substitution of Asp13 with Ala increases the net release of cations to approximately 1. These data are consistent with complex formation linked to disruption of surface salt bridges. Substitution of Glu90 with Ala, which would expose Lys87 predicted to contact DNA immediately distal to a proline-mediated DNA kink, causes an increase in affinity and an abrogation of the preference for hmU-containing DNA. We propose that hmU preference is due to finely tuned interactions at the sites of kinking that expose a differential flexibility of hmU- and T-containing DNA. Our data further suggest that the difference in binding site size for HU homologues is based on a differential ability to stabilize the DNA kinks.     

Cooperative helix stabilization by complex Arg-Glu salt bridges

Among the interactions that stabilize the native state of proteins, the role of electrostatic interactions has been difficult to quantify precisely. Surface salt bridges or ion pairs between acidic and basic side chains have only a modest stabilizing effect on the stability of helical peptides or proteins: estimates are roughly 0.5 kcal/mol or less. On the other hand, theoretical arguments and the occurrence of salt bridge networks in thermophilic proteins suggest that multiple salt bridges may exert a stronger stabilizing effect. We show here that triads of charged side chains, Arg(+)-Glu(-)-Arg(+) spaced at i,i+4 or i,i+3 intervals in a helical peptide stabilize alpha helix by more than the additive contribution of two single salt bridges. The free energy of the triad is more than 1 kcal/mol in excess of the sum of the individual pairs, measured in low salt concentration (10 mM). The effect of spacing the three groups is severe; placing the charges at i,i+4 or i,i+3 sites has a strong effect on stability relative to single bridges; other combinations are weaker. A conservative calculation suggests that interactions of this kind between salt bridges can account for much of the stabilization of certain thermophilic proteins.     

Salt bridges: geometrically specific, designable interactions

Salt bridges occur frequently in proteins, providing conformational specificity and contributing to molecular recognition and catalysis. We present a comprehensive analysis of these interactions in protein structures by surveying a large database of protein structures. Salt bridges between Asp or Glu and His, Arg, or Lys display extremely well-defined geometric preferences. Several previously observed preferences are confirmed, and others that were previously unrecognized are discovered. Salt bridges are explored for their preferences for different separations in sequence and in space, geometric preferences within proteins and at protein-protein interfaces, co-operativity in networked salt bridges, inclusion within metal-binding sites, preference for acidic electrons, apparent conformational side chain entropy reduction on formation, and degree of burial. Salt bridges occur far more frequently between residues at close than distant sequence separations, but, at close distances, there remain strong preferences for salt bridges at specific separations. Specific types of complex salt bridges, involving three or more members, are also discovered. As we observe a strong relationship between the propensity to form a salt bridge and the placement of salt-bridging residues in protein sequences, we discuss the role that salt bridges might play in kinetically influencing protein folding and thermodynamically stabilizing the native conformation. We also develop a quantitative method to select appropriate crystal structure resolution and B-factor cutoffs. Detailed knowledge of these geometric and sequence dependences should aid de novo design and prediction algorithms.     

Crystal structure of activated CheY. Comparison with other activated receiver domains

The crystal structure of BeF(3)(-)-activated CheY, with manganese in the magnesium binding site, was determined at 2.4-A resolution. BeF(3)(-) bonds to Asp(57), the normal site of phosphorylation, forming a hydrogen bond and salt bridge with Thr(87) and Lys(109), respectively. The six coordination sites for manganese are satisfied by a fluorine of BeF(3)(-), the side chain oxygens of Asp(13) and Asp(57), the carbonyl oxygen of Asn(59), and two water molecules. All of the active site interactions seen for BeF(3)(-)-CheY are also observed in P-Spo0A(r). Thus, BeF(3)(-) activates CheY as well as other receiver domains by mimicking both the tetrahedral geometry and electrostatic potential of a phosphoryl group. The aromatic ring of Tyr(106) is found buried within a hydrophobic pocket formed by beta-strand beta4 and helix H4. The tyrosine side chain is stabilized in this conformation by a hydrogen bond between the hydroxyl group and the backbone carbonyl oxygen of Glu(89). This hydrogen bond appears to stabilize the active conformation of the beta4/H4 loop. Comparison of the backbone coordinates for the active and inactive states of CheY reveals that only modest changes occur upon activation, except in the loops, with the largest changes occurring in the beta4/H4 loop. This region is known to be conformationally flexible in inactive CheY and is part of the surface used by activated CheY for binding its target, FliM. The pattern of activation-induced backbone coordinate changes is similar to that seen in FixJ(r). A common feature in the active sites of BeF(3)(-)-CheY, P-Spo0A(r), P-FixJ(r), and phosphono-CheY is a salt bridge between Lys(109) Nzeta and the phosphate or its equivalent, beryllofluoride. This suggests that, in addition to the concerted movements of Thr(87) and Tyr(106) (Thr-Tyr coupling), formation of the Lys(109)-PO(3)(-) salt bridge is directly involved in the activation of receiver domains generally.     

Peptide Binding to a PDZ Domain by Electrostatic Steering via Nonnative Salt Bridges

We have captured the binding of a peptide to a PDZ domain by unbiased molecular dynamics simulations. Analysis of the trajectories reveals on-pathway encounter complex formation, which is driven by electrostatic interactions between negatively charged carboxylate groups in the peptide and positively charged side chains surrounding the binding site. In contrast, the final stereospecific complex, which matches the crystal structure, features completely different interactions, namely the burial of the hydrophobic side chain of the peptide C-terminal residue and backbone hydrogen bonds. The simulations show that nonnative salt bridges stabilize kinetically the encounter complex during binding. Unbinding follows the inverse sequence of events with the same nonnative salt bridges in the encounter complex. Thus, in contrast to protein folding, which is driven by native interactions, the binding of charged peptides can be steered by nonnative interactions, which might be a general mechanism, e.g., in the recognition of histone tails by bromodomains.     

Surface salt bridges stabilize the GCN4 leucine zipper.

We present a study of the role of salt bridges in stabilizing a simplified tertiary structural motif, the coiled-coil. Changes in GCN4 sequence have been engineered that introduce trial patterns of single and multiple salt bridges at solvent exposed sites. At the same sites, a set of alanine mutants was generated to provide a reference for thermodynamic analysis of the salt bridges. Introduction of three alanines stabilizes the dimer by 1.1 kcal/mol relative to the wild-type. An arrangement corresponding to a complex type of salt bridge involving three groups stabilizes the dimer by 1.7 kcal/ mol, an apparent elevation of the melting temperature relative to wild type of about 22 degrees C. While identifying local from nonlocal contributions to protein stability is difficult, stabilizing interactions can be identified by use of cycles. Introduction of alanines for side chains of lower helix propensity and complex salt bridges both stabilize the coiled-coil, so that combining the two should yield melting temperatures substantially higher than the starting species, approaching those of thermophilic sequences.     

Molecular Dynamics Simulations of Peptides from the Central Domain of Smooth Muscle Caldesmon

Abstract

The central domain of smooth muscle caldesmon contains a highly charged region consisting of ten 13-residue repeats. Experimental evidence obtained from the intact protein and fragments thereof suggests that this entire region forms a single stretch of stable α-helix. We have carried out molecular dynamics simulations on peptides consisting of one, two and three repeats to examine the mechanism of α-helical stability of the central domain at the atomic level. All three peptides show high helical stability on the timescale of the MD simulations. Deviations from α-helical structure in all the simulations arise mainly from the formation of long stretches of π-helix. Interconversion between α-helical and π-helical conformations occurs through insertion of water molecules into α-helical hydrogen bonds and subsequent formation of reverse turns. The α-helical structure is stabilized by electrostatic interactions (salt bridges) between oppositely charged sidechains with i,i+4 spacings, while the π-helix is stabilized by i,i+5 salt bridge interactions. Possible i,i+3 salt bridges are of minor importance. There is a strong preference for salt bridges with a Glu residue N-terminal to a basic sidechain as compared to the opposite orientation. In the double and triple repeat peptides, strong i,i+4 salt bridges exist between the last Glu residue of one repeat and the first Lys residue of the next. This demonstrates a relationship between the repetitive nature of the central domain sequence and its ability to form very long stretches of α-helical structure.     

Strength and co-operativity of contributions of surface salt bridges to protein stability

Many of the interactions that stabilize proteins are co-operative and cannot be reduced to a sum of pairwise interactions. Such interactions may be analysed by protein engineering methods using multiple thermodynamic cycles comprising wild-type protein and all combinations of mutants in the interacting residues. There is a triad of charged residues on the surface of barnase, comprising residues Asp8, Asp12 and Arg110, that interact by forming two exposed salt bridges. The three residues have been mutated to alanine to give all the single, double and triple mutants. The free energies of unfolding of wild-type and the seven mutant proteins have been determined and the results analysed to give the contributions of the residues in the two salt bridges to protein stability. It is possible to isolate the energies of forming the salt bridges relative to the solvation of the separated ions by water. In the intact triad, the apparent contribution to the stabilization energy of the protein of the salt bridge between Asp12 and Arg110 is -1.25 kcal mol-1, whereas that of the salt bridge between Asp8 with Arg110 is -0.98 kcal mol-1. The strengths of the two salt bridges are coupled: the energy of each is reduced by 0.77 kcal mol-1 when the other is absent. The salt-linked triad, relative to alanine residues at the same positions, does not contribute to the stability of the protein since the favourable interactions of the salt bridges are more than offset by other electrostatic and non-electrostatic energy terms. Salt-linked triads occur in other proteins, for example, haemoglobin, where the energy of only the salt-bridge term is important and so the coupling of salt bridges could be of general importance to the stability and function of proteins.     

A Comprehensive Alanine-Scanning Mutagenesis Study Reveals Roles for Salt Bridges in the Structure and Activity of Pseudomonas aeruginosa Elastase

The relationship between salt bridges and stability/enzymatic activity is unclear. We studied this relationship by systematic alanine-scanning mutation analysis using the typical M4 family metalloprotease Pseudomonas aeruginosa elastase (PAE, also known as pseudolysin) as a model. Structural analysis revealed seven salt bridges in the PAE structure. We constructed ten mutants for six salt bridges. Among these mutants, six (Asp189Ala, Arg179Ala, Asp201Ala, Arg205Ala, Arg245Ala and Glu249Ala) were active and four (Asp168Ala, Arg198Ala, Arg253Ala, and Arg279Ala) were inactive. Five mutants were purified, and their catalytic efficiencies (k _cat/K _m), half-lives (t _1/2) and thermal unfolding curves were compared with those of PAE. Mutants Asp189Ala and Arg179Ala both showed decreased thermal stabilities and increased activities, suggesting that the salt bridge Asp189-Arg179 stabilizes the protein at the expense of catalytic efficiency. In contrast, mutants Asp201Ala and Arg205Ala both showed slightly increased thermal stability and slightly decreased activity, suggesting that the salt bridge Asp201-Arg205 destabilizes the protein. Mutant Glu249Ala is related to a C-terminal salt bridge network and showed both decreased thermal stability and decreased activity. Furthermore, Glu249Ala showed a thermal unfolding curve with three discernable states [the native state (N), the partially unfolded state (I) and the unfolded state (U)]. In comparison, there were only two discernable states (N and U) in the thermal unfolding curve of PAE. These results suggest that Glu249 is important for catalytic efficiency, stability and unfolding cooperativity. This study represents a systematic mutational analyses of salt bridges in the model metalloprotease PAE and provides important insights into the structure-function relationship of enzymes.     

Salt bridges destabilize a leucine zipper designed for maximized ion pairing between helices

Interhelical salt bridges are common in leucine zippers and are thought to stabilize the coiled coil conformation. Here we present a detailed thermodynamic investigation of the designed, disulfide-linked leucine zipper AB(SS) whose high-resolution NMR structure shows six interhelical ion pairs between heptad positions g of one helix and e' of the other helix but no ion pairing within single helices. The average pK(a) value of the Glu side chain carboxyl groups of AB(SS) is slightly higher than the pK(a) of a freely accessible Glu in an unfolded peptide [Marti, D. N., Jelesarov, I., and Bosshard, H. R. (2000) Biochemistry 39, 12804-12818]. This indicates that the salt bridges are destabilizing, a prediction we now have confirmed by determining the pH +/- stability profile of AB(SS). Circular dichroism-monitored unfolding by urea and by heating and differential scanning calorimetry show that the coiled coil conformation is approximately 5 kJ/mol more stable when salt bridges are broken by protonation of the carboxyl side chains. Using guanidinium chloride as the denaturant, the increase in the free energy of unfolding on protonation of the carboxyl side chains is larger, approximately 17 kJ/mol. The discrepancy between urea and guanidinium chloride unfolding can be ascribed to the ionic nature of guanidinium chloride, which screens charge-charge interactions. This work demonstrates the difficulty of predicting the energetic contribution of salt bridges from structural data alone even in a case where the ion pairs are seen in high-resolution NMR structures. The reason is that the contribution to stability results from a fine balance between energetically favorable Coulombic attractions and unfavorable desolvation of charges and conformational constraints of the residues involved in ion pairing. The apparent discrepancy between the results presented here and mutational studies indicating stabilization by salt bridges is discussed and resolved. An explanation is proposed for why interhelical salt bridges are frequently found in natural coiled coils despite evidence that they do not directly contribute to stability.     

The role of helix 1 aspartates and salt bridges in the stability and conversion of prion protein

A key event in the pathogenesis of transmissible spongiform encephalopathies is the conversion of PrP-sen to PrP-res. Morrissey and Shakhnovich (Morrissey, M. P., and Shakhnovich, E. I. (1999) Proc. Natl. Acad. Sci. U. S. A. 96, 11293-11298) proposed that the conversion mechanism involves critical interactions at helix 1 (residues 144-153) and that the helix is stabilized on PrP-sen by intra-helix salt bridges between two aspartic acid-arginine ion pairs at positions 144 and 148 and at 147 and 151, respectively. Mutants of the hamster prion protein were constructed by replacing the aspartic acids with either asparagines or alanines to destabilize the proposed helix 1 salt bridges. Thermal and chemical denaturation experiments using circular dichroism spectroscopy indicated the overall structures of the mutants are not substantially destabilized but appear to unfold differently. Cell-free conversion reactions performed using ionic denaturants, detergents, and salts (conditions unfavorable to salt bridge formation) showed no significant differences between conversion efficiencies of mutant and wild type proteins. Using conditions more favorable to salt bridge formation, the mutant proteins converted with up to 4-fold higher efficiency than the wild type protein. Thus, although spectroscopic data indicate the salt bridges do not substantially stabilize PrP-sen, the cell-free conversion data suggest that Asp-144 and Asp-147 and their respective salt bridges stabilize PrP-sen from converting to PrP-res.     

Phosphoenolpyruvate: sugar phosphotransferase system from the hyperthermophilic Thermoanaerobacter tengcongensis

Thermoanaerobacter tengcongensis is a thermophilic eubacterium that has a phosphoenolpyruvate (PEP) sugar phosphotransferase system (PTS) of 22 proteins. The general PTS proteins, enzyme I and HPr, and the transporters for N-acetylglucosamine (EIICB(GlcNAc)) and fructose (EIIBC(Fru)) have thermal unfolding transitions at ～90 °C and a temperature optimum for in vitro sugar phosphotransferase activity of 65 °C. The phosphocysteine of a EIICB(GlcNAc) mutant is unusually stable at room temperature with a t(1/2) of 60 h. The PEP binding C-terminal domain of enzyme I (EIC) forms a metastable covalent adduct with PEP at 65 °C. Crystallization of this adduct afforded the 1.68 ? resolution structure of EIC with a molecule of pyruvate in the active site. We also report the 1.83 ? crystal structure of the EIC-PEP complex. The comparison of the two structures with the apo form and with full-length EI shows differences between the active site side chain conformations of the PEP and pyruvate states but not between the pyruvate and apo states. In the presence of PEP, Arg465 forms a salt bridge with the phosphate moiety while Glu504 forms salt bridges with Arg186 and Arg195 of the N-terminal domain of enzyme I (EIN), which stabilizes a conformation appropriate for the in-line transfer of the phosphoryl moiety from PEP to His191. After transfer, Arg465 swings 4.8 ? away to form an alternative salt bridge with the carboxylate of Glu504. Glu504 loses the grip of Arg186 and Arg195, and the EIN domain can swing away to hand on the phosphoryl group to the phosphoryl carrier protein HPr.     

Contribution of arginine-glutamate salt bridges to helix stability

Peptide side chain interactions were studied by molecular dynamics simulation using explicit solvent on a peptide with the sequence AAARAAAAEAAEAAAARA. Three different protonation states of the glutamic acid side chains were simulated for four 20 ns runs each, a total simulation time of 240 ns. Two different salt bridge geometries were observed and the preferred geometry was found to depend on Glu — Arg residue spacing. Stable charge clusters were also observed, particularly in the fully charged peptide. Salt bridges were selectively interrupted upon protonation, with concomitant changes in secondary structure. The fully charged peptide was highly helical between residues 9 and 13, although protonation increased helicity near the N-terminus. The contribution of salt bridges to helix stability therefore depends on both position and relative position of charged residues within a sequence.     

Electrostatic couplings in OmpA ion-channel gating suggest a mechanism for pore opening

The molecular forces that drive structural transitions between the open and closed states of channels and transporters are not well understood. The gate of the OmpA channel is formed by the central Glu52-Arg138 salt bridge, which can open to form alternate ion pairs with Lys82 and Glu128. To gain deeper insight into the channel-opening mechanism, we measured interaction energies between the relevant side chains by double-mutant cycle analysis and correlated these with the channel activities of corresponding point mutants. The closed central salt bridge has a strong interaction energy of -5.6 kcal mol(-1), which can be broken by forming the open-state salt bridge Glu52-Lys82 (DeltaDeltaG(Inter) = -3.5 kcal mol(-1)) and a weak interaction between Arg138 and Glu128 (DeltaDeltaG(Inter) = -0.6 kcal mol(-1)). A covalent disulfide bond in place of the central salt bridge completely blocks the channel. Growth assays indicate that this gating mechanism could physiologically contribute to the osmoprotection of Escherichia coli cells from environmental stress.     

Peptide models of electrostatic interactions in proteins: NMR studies on two beta-turn tetrapeptides containing Asp-His and Asp-Lys salt bridges

Two model peptides Boc-Asp-Pro-Aib-X-NHMe [X = His (1) and X = Lys (2)] were synthesized to simulate intramolecular electrostatic interactions between ionizable side chains. Conformational analysis by 270-MHz 1H NMR in (CD3)2SO reveals that the backbone secondary structures of these two peptides are stabilized by two strong intramolecular hydrogen bonds, involving the consecutive carboxy-terminal NH groups. 1H NMR chemical shifts were measured in 1, 2, and a protected derivative, Boc-Asp(OBzl)-Pro-Aib-His-NHMe (3). These shifts were also measured for the model compounds Ac-Lys-NHMe, Boc-Asp-NHMe, and Boc-His-NHMe in their different states of ionization. An analysis of the chemical shifts of the ionization-sensitive reporter resonances suggests the formation of a strong intramolecular salt bridge in the lysyl peptide 2 and a bridge of moderate strength in the histidyl peptide 1. A comparison of the temperature dependence of chemical shifts in peptides 1-3 suggests that intramolecular salt bridge formation results in diminished backbone flexibility. The results establish that proximity effects confer far greater stability to intramolecular ion pair interactions vis-a-vis their intermolecular counterparts. The salt bridge interaction in peptide 1 displays a remarkable sensitivity to the dielectric constant of the solvent medium. The results suggest that these peptides are good simulators of the role of salt bridges in the structural dynamics of proteins.