A competing salt-bridge suppresses helix formation by the isolated C-peptide carboxylate of ribonuclease A

The C-peptide of ribonuclease A (residues 1 to 13) is obtained by cyanogen bromide cleavage at Met13, which converts methionine to a mixture of homoserine lactone (giving C-peptide lactone) and homoserine carboxylate (giving C-peptide carboxylate). The helix-forming properties of C-peptide lactone have been reported. The helix is formed intramolecularly in aqueous solution, is stabilized at low temperatures (0 to 20 °C) and also by a pH-dependent interaction between sidechains. The C-peptide lactone helix is about 1000-fold more stable than expected from “host-guest” data for helix formation in synthetic polypeptides.Here we report the failure of C-peptide carboxylate to form an α-helix in comparable conditions. Formation of a salt-bridge between the α-COO^? group and the imidazolium ring of His12⁺ appears to be responsible for the suppression of helix formation. The presence of the Hse13-COO^? … His12⁺ salt-bridge in C-peptide carboxylate is shown by ¹H nuclear magnetic resonance titration of the amide proton resonances of His12 and Hse13, and is expected from model peptide studies. The most probable reason why C-peptide carboxylate does not form an α-helix is that the Hse13-COO^? … His12⁺ salt-bridge competes successfully with a helix stabilizing salt-bridge (Glu9^? … His12⁺).S-peptide (residues 1 to 20 of ribonuclease A) does form an α-helix with properties similar to those of the C-peptide (lactone) helix, which shows that the lactone ring of C-peptide lactone is not needed for helix formation.These results support the hypothesis that a Glu9^? … His12⁺ salt-bridge stabilizes the C-peptide (lactone) helix, and they show that specific interactions between side-chains can be important in preventing as well as in promoting α-helix formation.     

Thermodynamic parameters for the helix-coil thermal transition of ribonuclease-S-peptide and derivatives from 1H-NMR data

Values for the thermodynamic quantities, ΔH° = 11.8 ± 2.0 Kcal/mole and ΔS° = 43.6 ± 6.0 e.u., of the 3-13 helix–coil equilibrium of isolated S-peptide (19 residue N-terminal fragment of ribonuclease A) in aqueous solution (3 m M, 1M NaCl, pD 5.4) have been determined from a joint analysis of the Thr 3γ, Ala 6β, Phe 8meta, and Phe 8para ¹H chemical shift vs temperature curves (?7 to 80°C) in several aqueous–trifluorethanol mixtures. Chemical shifts in the coil and in the helix have been determined for up to 16 protons belonging to the 3-13 fragment. Thermodynamic parameters have also been determined for C-peptide (13 residue fragment) and a number of S-peptide derivatives. From the variation of the values of the thermodynamic parameters at pD 2.5, 5.4, and 8.0, a quantitation of the two helix-stabilizing side-chain interactions can be made: (1) Δ(ΔH°) ? 5 Kcal/mole and Δ(ΔS°) ? 18 e.u. for the salt bridge Glu 2^? … Arg 10⁺ and (2) Δ(ΔH°) ? 3 Kcal/mole and Δ(ΔS°) = 9 e.u. for the one in which the His 12⁺ imidazolium group is involved, presumably a partial stacking with the Phe 8 side chain.     

Deprotonation of Glu9 destabilizes the alpha-helix in C-peptide of RNase A

pK values of Glu2, Glu9, and His12 in the lactone and carboxylate forms of C-peptide at 4.5 and 21 degrees, 0.1 M NACl, have been determined from pH-tritration shifts of n.m.r. signals of the glutamate gamma and histidine ring protons. These have been used in an analysis of the well known pH-induced helix-coil transition in the C-peptide lactone. It has been shown that Glu12 deprotonation results in a twofold increase of the helix content, whereas deprotonation of Glu9 leads to a 28% drop. This latter effect is probably related to Glu-9-His+12 salt bridge formation. The transition within the pH range 5.5-7.5 follows exactly the deprotonation curve of His+12 residue.     

Local secondary structure in ribonuclease A denatured by guanidine · HCl near 1 °C

Recent work has shown that a short α-helix can be stable in water near 1 °C when stabilized by specific interactions between side-chains, while earlier “host-guest” results with random copolymers have shown that a short α-helix is unstable in water at all temperatures in the absence of stabilizing side-chain interactions. As regards the mechanism of protein folding, it is now reasonable on energetic grounds to consider isolated α-helices and β-sheets as the first intermediates on the pathway of protein folding. Proton nuclear magnetic resonance is used here to detect isolated secondary structures in ribonuclease A denatured by guanidine · HCl (GuHCl). Temperatures near 1 °C are used because the low-temperature stability of the C-peptide helix may be a general property of isolated secondary structures in water.Our procedure is to titrate with GuHCl the C2H resonance lines of the four histidine residues of denatured ribonuclease A. Studies of model peptides (C-peptide (lactone) and C-peptide carboxylate, residues 1 to 13 of ribonuclease A; S-peptide, residues 1 to 20) show linear titration curves for the C2H resonance of His12 above 0.5 M-GuHCl, once helix unfolding is complete. Deviations from this line are used to monitor helix formation. The GuHCl titration curves of the other three histidine residues are also linear, once unfolding is complete. The results show that the helix found in C-peptide and S-peptide is also found in denatured ribonuclease A, where it behaves as an isolated helix not stabilized significantly by interactions with other chain segments. Studies of denatured S-protein show that the remaining three His residues, His48, His105 and His119, are involved in structure only below 1 m-GuHCl at 9 °C, pH 1.9. The nature of this structure is not known. The main conclusion from this work is that the His12 helix can be observed as a stable, isolated helix in denatured ribonuclease A near 1 °C, and that none of the other three His residues is involved in a comparably stable local structure. In native ribonuclease A, His12 is within an α-helix and the other three His residues are involved in a 3-stranded β-sheet structure.The helix-coil transition of C-peptide has also been studied for other side-chain resonances by GuHCl titration. Typically, but not always, the titration curves are linear after helix unfolding takes place and resonance lines from different residues of the same amino acid type can be resolved in GuHCl solutions. This is true of the four histidine residues of ribonuclease A although their pK values in 5 m-GuHCl are nearly the same. In C-peptide, the βCH₃ resonance of Ala6 is affected strongly by GuHCl while the lines of Ala4 and Ala5 are shifted only weakly by GuHCl. Evidently the interactions between GuHCl and side-chains in an unfolded peptide depend upon neighboring groups.     

A pH-dependent variation in alpha-helix structure of the S-peptide of ribonuclease A studied by Monte Carlo simulated annealing.

Low-energy conformations of the S-peptide fragment (20 amino acid residues long) of ribonuclease A were studied by Monte Carlo simulated annealing. The obtained lowest-energy structures have alpha-helices with different size and location, depending distinctively on the ionizing states of acidic amino acid residues. The simulation started from completely random initial conformation and was performed without any bias toward a particular structure. The most conspicuous alpha-helices arose from the simulation when both Glu 9 and Asp 14 were assumed to be electrically neutral, whereas the resulting conformations became much less helical when Asp 14 rather than Glu 9 was allowed to have a negative charge. Together with experimental evidence that the alpha-helix in the S-peptide is most stable at pH 3.8, we consider the helix formation need the carboxyl group of Asp 14 to be electrically neutral in this weakly acidic condition. In contrast, a negative charge at Asp 14 appears to function in support of a view that this residue is crucial to helix termination owing to its possibility to form a salt bridge with His 12. These results indicate that the conformation of the S-peptide depends considerably on the ionizing state of Asp 14.     

Infrared study of synthetic peptide analogues of the calcium‐binding site III of troponin C: The role of helix F of an EF‐hand motif

The EF‐hand motif (helix–loop–helix) is a Ca²⁺‐binding domain that is common among many intracellular Ca²⁺‐binding proteins. We applied Fourier‐transform infrared spectroscopy to study the synthetic peptide analogues of site III of rabbit skeletal muscle troponin C (helix E–loop–helix F). The 17‐residue peptides corresponding to loop–helix F (DRDADGYIDAEELAEIF), where one residue is substituted by the D ‐type amino acid, were investigated to disturb the α‐helical conformation of helix F systematically. These D ‐type‐substituted peptides showed no band at about 1555 cm^?1 even in the Ca²⁺‐loaded state although the native peptide (L ‐type only) showed a band at about 1555 cm^?1 in the Ca²⁺‐loaded state, which is assigned to the side‐chain COO^? group of Glu at the 12th position, serving as the ligand for Ca²⁺ in the bidentate coordination mode. Therefore, helix F is vital to the interaction between the Ca²⁺ and the side‐chain COO^? group of Glu at the 12th position. Implications of the COO^? antisymmetric stretch and the amide‐I′ of the synthetic peptide analogues of the Ca²⁺‐binding sites are discussed. © 2012 Wiley Periodicals, Inc. Biopolymers 99: 342–347, 2013.     

Diverse gating in K channels: Differential role of the pore-helix glutamate in stabilizing the channel pore

The selectivity filter and adjacent regions in the bacterial KcsA and inwardly rectifying K⁺ (Kir) channels reveal significant conformational changes that cause the channel pore to transition from an activated to inactive state (C-type inactivation) once the channel is open. The meshwork of residues stabilizing the pore of KcsA involves Glu71–Asp80 carboxyl–carboxylate interaction ‘behind’ the selectivity filter. Interestingly, the Kir channels do not have this exact interaction, but instead have a Glu–Arg salt bridge where the Glu is in the same position but the Arg is one position N-terminal compared to the Asp in KcsA. Also, the Kir channels lack the Trp that hydrogen bonds to Asp80 in KcsA. Here, the sequence and structural information are combined to understand the dissimilarity in the role of the pore-helix Glu in stabilizing the pore structure in KcsA and Kir channels. This review illustrates that although Glu is quite conserved among both types of channels, the network of interactions is not translatable from one channel to the other; thereby suggesting a unique phenomenon of diverse gating patterns in K⁺ channels.     

Effect of side chain length on intrahelical interactions between carboxylate- and guanidinium-containing amino acids

The charge-containing hydrophilic functionalities of encoded charged amino acids are linked to the backbone via different numbers of hydrophobic methylenes, despite the apparent electrostatic nature of protein ion pairing interactions. To investigate the effect of side chain length of guanidinium- and carboxylate-containing residues on ion pairing interactions, α-helical peptides containing Zbb–Xaa (i, i + 3), (i, i + 4) and (i, i + 5) (Zbb = carboxylate-containing residues Aad, Glu, Asp in decreasing length; Xaa = guanidinium residues Agh, Arg, Agb, Agp in decreasing length) sequence patterns were studied by circular dichroism spectroscopy (CD). The helicity of Aad- and Glu-containing peptides was similar and mostly pH independent, whereas the helicity of Asp-containing peptides was mostly pH dependent. Furthermore, the Arg-containing peptides consistently exhibited higher helicity compared to the corresponding Agp-, Agb-, and Agh-containing peptides. Side chain conformational analysis by molecular mechanics calculations showed that the Zbb–Xaa (i, i + 3) and (i, i + 4) interactions mainly involved the χ ₁ dihedral combinations (g+, g+) and (g?, g+), respectively. These low energy conformations were also observed in intrahelical Asp–Arg and Glu–Arg salt bridges of natural proteins. Accordingly, Asp and Glu provides variation in helix characteristics associated with Arg, but Aad does not provide features beyond those already delivered by Glu. Importantly, nature may have chosen the side chain length of Arg to support helical conformations through inherent high helix propensity coupled with stabilizing intrahelical ion pairing interactions with the carboxylate-containing residues.     

1H-n.m.r. study of the folding of ribonuclease 12-(beta-(3-pyridyl)-L-Ala) S-peptide (1-14)

The 1H-n.m.r. spectra (360 MHz) of 12-(beta-(3-pyridyl)-L-Ala) ribonuclease S-peptide (1-14), a tetradecapeptide incorporating (beta-3-pyridyl-L-Ala) instead of His at position 12, have been assigned. The shift vs. temperature dependence has been analyzed at three different pD's in terms of a two-state helix (3-13) in equilibrium coil equilibrium, and the corresponding values for the thermodynamic quantities delta H degrees and delta S degrees determined. Helix populations at 0 degrees C have been measured as a function of pD, showing their dependence on two apparent pKa's at approximately 3.3 and 5.5, with a maximum at pD approximately 4.2. All the obtained results show that the new peptide has very similar folding properties to those shown by S-peptide and particularly to those of C-peptide. The 3-13 helix formed is stabilized by two interactions: a salt-bridge Glu 2-...Arg 10+ and a partial stacking between the aromatic rings of residues Phe 8 and His 12. Calculations involving ring current shifts and potential energies validate the possible existence of this latter interaction, which must present a local geometry defined by chi 81 180 degrees, chi 82 100 degrees, chi 121-60 and chi 122 80.     

Proton transfer and polarizability of hydrogen bonds in proteins coupled with conformational changes. I. Infrared investigation of poly(glutamic acid) with various N Bases

The nature of hydrogen bonds formed between carboxylic acid residues and histidine residues in proteins is studied by ir spectroscopy. Poly(glutamic acid) [(Glu)_n] is investigated with various monomer N bases. The position of the proton transfer equilibrium OH…?N ? O^?…?H⁺N is determined considering the bands of the carboxylic group. It is shown that largely symmetrical double minimum energy surfaces are present in the OH…?N ? O^?…?H⁺N bonds when the pK_a of the protonated N base is two values larger than that of the carboxylic groups of (Glu)_n. Hence OH…?N ? O^?…?H⁺N bonds between glutamic and aspartic acid residues and histidine residues in proteins may be easily polarizable proton transfer hydrogen bonds. The polarizability of these bonds is one to two orders of magnitude larger than usual electron polarizabilities; therefore, these bonds strongly interact with their environment. It is demonstrated that water molecules shift these proton transfer equilibria in favor of the polar proton boundary structure. The access of water molecules to such bonds in proteins and therefore the position of this proton transfer equilibrium is dependent on conformation. The amide bands show that (Glu)_n is α-helical with all systems. The only exception is the (Glu)_n-n-propylamine system. When this system is hydrated (Glu)_n is α-helical, too. When it is dried, however, (Glu)_n forms antiparallel β-structure. This conformational transition, dependent on degree of hydration, is reversible. An excess of n-propylamine has the same effect on conformation as hydration.     

Positional dependence of the effects of negatively charged Glu side chains on the stability of two-stranded α-helical coiled-coils

The effects on protein stability of negatively charged Glu side chains at different positions along the length of the α-helix were investigated in the two-stranded α-helical coiled-coil. A native coiled-coil has been designed which consists of two identical 35 residue polypeptide chains with a heptad repeat Q_gV_aG_bA_cL_dQ_eK_f and a Cys residue at position 2 to allow the formation of an interchain 2-2′ disulphide bridge. This coiled-coil contains no intra- or interchain electrostatic interactions and served as a control for peptides in which Glu was substituted for Gln in the e or g heptad positions. The effect of the substitutions on stability was determined by urea denaturation at 20°C with the degree of unfolding monitored by circular dichroism spectroscopy. A Glu substituted for Gln near the N-terminus in each chain of the coiled-coil stabilizes the coiled-coil at pH 7, consistent with the charge–helix dipole interaction model. This stability increase is modulated by pH change and the addition of salt (KCl or guanidine hydrochloride), confirming the electrostatic nature of the effect. In contrast, Glu substitution in the middle of the helix destabilizes the coiled-coil because of the lower helical propensity and hydrophobicity of Glu compared with Gln at pH 7. Taking the intrinsic differences into account, the apparent charge–helix dipole interaction at the N-terminus is approximately 0.35 kcal/mol per Glu substitution. A Glu substitution at the C-terminus destabilizes the coiled-coil more than in the middle owing to the combined effects of intrinsic destabilization and unfavourable charge–helix dipole interaction with the negative pole of the helix dipole. The estimated destabilizing charge–helix dipole interaction of 0.08 kcal/mol is smaller than the stabilizing interaction at the N-terminus. The presence of a 2-2′disulphide bridge appears to have little influence on the magnitude of the charge–helix dipole interactions at either end of the coiled-coil. © 1997 European Peptide Society and John Wiley & Sons, Ltd.     

Continuum electrostatics of the C-peptide: anatomy of the problem.

A computational study of the role of all ionizable groups of the C-peptide in its helix-coil transition is performed within the framework of continuum electrostatics. The method employed in our computations involves a numeric solution of the Poisson equation with the Boundary Element Method. Our calculations correctly predict the experimentally observed trends in the helix-coil equilibrium of the C-peptide, and suggest that the mechanisms involved are more complex than usually presumed in the literature. Our results suggest that electrostatic interactions in the unfolded conformation are often more important than in the helix, total electrostatic contribution to the helix-coil transition due to the side chains of the C-peptide destabilizes the helix, changes in the helix stability produced by the changes in the ionization state of the side chains are dominated by side chain effects, the effect of the helix dipole on the energetics of the helix-coil transition of the C-peptide is either minor or similar to other contributions in magnitude; while the formation of a salt bridge is electrostatically favorable, formation of the hydrogen bond between a charged and a polar side chains is not. Factors limiting the accuracy of the computations are discussed.     

Helicity of short E-R/K peptides

Understanding the secondary structure of peptides is important in protein folding, enzyme function, and peptide‐based drug design. Previous studies of synthetic Ala‐based peptides (>12 a.a.) have demonstrated the role for charged side chain interactions involving Glu/Lys or Glu/Arg spaced three (i, i + 3) or four (i, i + 4) residues apart. The secondary structure of short peptides (<9 a.a.), however, has not been investigated. In this study, the effect of repetitive Glu/Lys or Glu/Arg side chain interactions, giving rise to E‐R/K helices, on the helicity of short peptides was examined using circular dichroism. Short E‐R/K–based peptides show significant helix content. Peptides containing one or more E‐R interactions display greater helicity than those with similar E‐K interactions. Significant helicity is achieved in Arg‐based E‐R/K peptides eight, six, and five amino acids long. In these short peptides, each additional i + 3 and i + 4 salt bridge has substantial contribution to fractional helix content. The E‐R/K peptides exhibit a strongly linear melt curve indicative of noncooperative folding. The significant helicity of these short peptides with predictable dependence on number, position, and type of side chain interactions makes them an important consideration in peptide design.     

On the Permeation by Dioxygen of the Cofactor‐Independent Unusual Oxygenase RhCC,in Complex with Substrate 4‐Hydroxyphenylenolpyruvate. A Molecular Dynamics Investigation

This work deals with a trimeric bacterial protein, RhCC, which, although belonging to the tautomerase superfamily, shows oxygenase activity. A model of the complex from RhCC and substrate 4‐hydroxyphenylenolpyruvate (4HPP), fitting the observation of extra electron densities from X‐ray diffraction of the crystal, could be built by autodocking. When subjected to molecular dynamics (MD) aided by an external random force applied to a O₂ molecule placed above 4HPP, this model evolved with O₂ egressing toward the bulk solvent from two nearly opposite gates. These were located between the nearly parallel helices 75 – 91 and 15 – 33 of either chain C (gate SE) or chain B (gate FL). Alternatively, with four O₂ molecules in the bulk solvent, unbiased MD led to O₂ entering the protein from gate SE and getting to 4HPP, while forming a stabilizing salt bridge between the 4HPP carboxylate and P1.C ⁺NH₂, thus providing scientific ground for a refined model of the complex.     

The design and production of semisynthetic ribonucleases with increased thermostability by incorporation of S-peptide analogues with enhanced helical stability

Recent work has shown that, with synthetic analogues of C-peptide (residues 1-13 of ribonuclease A), the stability of the peptide helix in H2O depends strongly on the charge on the N-terminal residue. We have asked whether, in semisynthetic ribonuclease S reconstituted from S-protein plus an analogue of S-peptide (1-15), the stability of the peptide helix is correlated with the Tm of the reconstituted ribonuclease S. Six peptides have been made, which contain Glu9----Leu, a blocked alpha-COO- group (-CONH2), and either Gln11 or Glu11. The N-terminal residue has been varied; its charge varies from +2 (Lys) to -1 (succinyl-Ala). We have measured the stability of the peptide helix, the affinity of the peptide for S-protein (by C.D. titration), and the thermal stability of the reconstituted ribonuclease S. All six peptide analogues show strongly enhanced helix formation compared to either S-peptide (1-15) or (1-19), and the helix content increases as the charge on the N-terminal residue changes from +2 to -1. All six peptides show increased affinity for S-protein compared to S-peptide (1-19), and all six reconstituted ribonucleases S show an increase in Tm compared to the protein with S-peptide (1-19). The Tm increases as the charge on residue 1 changes from +2 to -1. The largest increment in Tm is 6 degrees. The results suggest that the stability of a protein can be increased by enhancing the stability of its secondary structure.     

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.     

Laser-excited raman spectroscopy of biomolecules. XII. Thermally induced conformational changes in poly(L-glutamic acid)

The α-helical from of poly(L -glutamic acid) [α-poly(Glu)] gives rise to the same amide I and III lines as α-poly(γ-benzyl-L -glutamate) at 1652 and 1296 cm^?1, respectively. The latter is a superposition of the amide III line near 1290 cm^?1 and a line deu to vibrational made of CH₂ groups of the side chain near 1300 cm^?1. A line at 924 cm^?1 is tentatively identified as characteristics of α-poly(Glu). Both the β₁- and β₂- forms of poly(Glu) give rise to characteristic of β-amide. III frequencies that are similar because of their similar backbone structures. Differences in the conformations of their side chains and in the environments of the backbone are reflected in the region 800–1200 cm^?1 and in the amide I. A line at 1042 cm^?1 and a pair at 1021 and 1059 cm^?1 are tentatively assigned as characteristic of β₁-poly(Glu) and β₂-poly(Glu), respectively. The α-β₂ transition in poly(L -Glu⁷⁸L -Val²²) is shown by the appearance of all the β₂-characteristic lines in the thermally transformed sample. The same features observed in poly(L -Glu⁹⁵L -Val⁵) also indicate that the α-β₂ transition of poly(Glu) is facilitated by the presence of L -valine and that the content of L -valine is not critical for this purpose. Investigation of the Raman spectra of the calcium, strontium, barium and sodium slats of poly(Glu) shows that these salts, under the conditions of preparation used, all the have random-coil conformations.     

Structure of hydrated Na+ ions around a region of A- or B-DNA helix

A molecular-dynamics simulation was used to carry out an introductory study of the hydration of a section of a rigid single A- or B-DNA helix with one Na⁺ counterion per nucleotide. Four Na⁺ ions and four nucleotides and periodic boundary conditions were used to mimic an infinite helix. The atoms of the helix and the Na⁺ ions were assumed to be Lennard-Jones spheres that also carried charges. Stillinger four-point charge model water molecules were used. We carried out five calculations, for 26 and 46 water molecules in B-DNA and 20, 32, and 46 in A-DNA fragments. The arrangements of the Na⁺ ions are found to have some similarities to those obtained by Clementi and Corongiu. In the calculations with 46 water molecules, we found that two Na⁺ ions can be bridged by about two water molecules and form a hydrated bound pair, which in turn forms a bridge between the guanine N7 and a near phosphate group. These bound pairs may be important in stabilizing the helix structure of DNA molecules.     

Easily polarizable proton transfer hydrogen bonds between the side chains of histidine and the carboxylic acid groups of glutamic and aspartic acid residues in proteins

The nature of the hydrogen bonds formed between glutamic acid and histidine residues between aspartic acid and histidine residues is studied by i.r. spectroscopy. These studies were performed with $\text{(}\text{l}\text{-Glu}\text{)}{}_{\mathrm{n}}\text{+(}\text{l}\text{-His}\text{)}{}_{\mathrm{n}}$ and with associates of monomeric Glu + His and Asp + His systems in solutions whereby these amino acids had protected α-amino and α-carboxylic groups. It is shown that the OH …N?^?O?H⁺N bonds are easily polarizable proton transfer hydrogen bonds. The residence time of the proton at the His is a little larger in the case of the Asp + His than in the case of the Glu + His systems. Polar environments shift this proton transfer equilibrium in favour of the proton limiting structure ^?O?H⁺N, and less polar ones in favour of the structure OH?N. These results demonstrate that the large proton polarizability of the hydrogen bonded system in the active centre of chymotrypsin is responsible for the charge shift caused by the substrate, and thus for the increase in reactivity of the serine residue and the catalytic activity of the enzyme.     

Prototropic tautomerism and basic molecular principles of hypoxanthine mutagenicity: an exhaustive quantum-chemical analysis

The molecular structures, relative stability order, and dipole moments of a complete family of 21 planar hypoxanthine (Hyp) prototropic molecular–zwitterionic tautomers including ylidic forms were computationally investigated at the MP2/6–311++G(2df,pd)//B3LYP/6–311++G(d,p) level of theory in vacuum and in three different surrounding environments: continuum with a low dielectric constant (??=?4) corresponding to a hydrophobic interface of protein–nucleic acid interactions, dimethylsulfoxide (DMSO), and water. The keto-N1HN7H tautomer was established to be the global minimum in vacuum and in continuum with ??=?4, while Hyp molecule exists as a mixture of the keto-N1HN9H and keto-N1HN7H tautomers in approximately equal amounts in DMSO and in water at T?=?298.15?K. We found out that neither intramolecular tautomerization by single proton transfer in the Hyp base, nor intermolecular tautomerization by double proton transfer in the most energetically favorable Hyp·Hyp homodimer (symmetry C _2h ), stabilized by two equivalent N1H…O6 H-bonds, induces the formation of the enol tautomer (marked with an asterisk) of Hyp with cis-oriented O6H hydroxyl group relative to neighboring N1C6 bond. We first discovered a new scenario of the keto–enol tautomerization of Hyp?·?Hyp homodimer (C _2h ) via zwitterionic near-orthogonal transition state (TS), stabilized by N1⁺H…N1^? and O6⁺H…N1^? H-bonds, to heterodimer Hyp^??·?Hyp (C _s ), stabilized by O6H…O6 and N1H…N1 H-bonds. We first showed that Hyp^??·?Thy mispair (C _s ), stabilized by O6H…O4, N3H…N1, and C2H…O2 H-bonds, mimicking Watson–Crick base pairing, converts to the wobble Hyp?·?Thy base pair (C _s ), stabilized by N3H…O6 and N1H…O2 H-bonds, via high- and low-energy TSs and intermediate Hyp?·?Thy^?, stabilized by O4H…O6, N1H…N3, and C2H…O2 H-bonds. The most energetically favorable TS is the zwitterionic pair Hyp⁺?·?Thy^? (C _s ), stabilized by O6⁺H…O4^?, O6⁺H…N3^?, N1⁺H…N3^?, and N1⁺H…O2^? H-bonds. The authors expressed and substantiated the hypothesis, that the keto tautomer of Hyp is a mutagenic compound, while enol tautomer Hyp^? does not possess mutagenic properties. The lifetime of the nonmutagenic tautomer Hyp^? exceeds by many orders the time needed to complete a round of DNA replication in the cell. For the first time purine–purine planar H-bonded mispairs containing Hyp in the anti-orientation with respect to the sugar moiety – Hyp?·?Ade _syn , Hyp?·?Gua^? _syn , and Hyp?·?Gua _syn , that closely resembles the geometry of the Watson–Crick base pairs, have been suggested as the source of transversions. An influence of the surrounding environment (??=?4) on the stability of studied complexes and corresponding TSs was estimated by means of the conductor-like polarizable continuum model. Electron-topological, structural, vibrational, and energetic characterictics of all conventional and nonconventional H-bonds in the investigated structures are presented. Presented data are key to understanding elementary molecular mechanisms of mutagenic action of Hyp as a product of the adenine deamination in DNA.