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.     

Structurally symmetrical,easily polarizable hydrogen bonds between side chains in proteins and proton-conducting mechanisms. III

(L -Cys)_n, (L -Lys)_n, and (L -Glu)_n were studied by ir spectroscopy in terms of their degree of deprotonation or protonation. It is shown that structurally symmetrical, easily polarizable SH ?S^? ? ^?S ?HS, N⁺H ?N ? N ?H⁺N, and OH ?O^? ? ^?O ?HO hydrogen bonds are formed between the side chains. The different wave number distributions of the ir continua caused by these hydrogen bonds show that the barrier in the double-minimum proton potential decreases in the series of these hydrogen bonds. The stability of these hydrogen bonds against hydration increases in this series. The OH ?O^? ? ^?O ?HO bonds are not broken by small amounts of water. With (L -Cys)_n the formation of easily polarizable hydrogen bonds and a β-structure–coil transition are strongly interdependent. As a result of this coupling effect, the β-structure–coil transition becomes cooperative. With (L -Glu)_n, the formation of the polarizable hydrogen bonds and the observed conformational change are independent processes. The (L -Glu)_n conformation changes from α-helix to coil only if more than 80% of the residues are deprotonated. Finally, on the basis of the various types of easily polarizable hydrogen bonds, charge shifts in active centers of enzymes and the proton-conducting mechanism through hydrophobic regions of biological membranes are discussed.     

Proton polarizability and proton transfer in histidine-phosphate hydrogen bonds as a function of cations present: ir investigations

(L -His)_n- dihydrogen phosphate systems are studied by ir spectroscopy in the presence of various cations and as a function of the degree of hydration. Ir continua indicate that (I) OH … N ? O^?…H⁺N (IIR) hydrogen bonds are formed and that these bonds show high proton polarizability, which increases from the Li⁺ to the K⁺ system. In the K⁺?system, His-P_i-P_i chains are formed, showing particularly high proton polarizability due to collective proton motion within both hydrogen bonds. The OH N ? O^?…H^?N equilibria are determined from ir bands. With the Li⁺ system, 55% of the protons are present at the histidine residues; this percentage is smaller with the Na⁺ system (41%), and amounts to only 32% with the K⁺ system. With the increasing degree of hydration the removal of the degeneracy of ν_as?PO^2?₃ vanishes, indicating loosening of the cations from the phosphates. Nevertheless, the hydrogen bond acceptor O atom becomes more negative; a shift of the equilibrium to the right is observed in the OH… N ? O^?…H⁺N bond. This is explained by the strong interaction of the dipole of the hydrogen bonds with the water molecules. All these results show that protons can be shifted easily in these hydrogen bonds due to their high proton polarizability. The transfer equilibria can be controlled easily by local electrical fields. In addition, these results may be of significance when phosphates interact with proteins.     

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.     

Easily polarizable N+H…N hydrogen bonds between histidine side chains and proton translocation in proteins

Histidinium perchlorate having protecting groups at the α-amino and α-carboxylate group is studied by IR spectroscopy as function of the addition of protected histidine molecules. An intense continuous absorption arises, indicating that the N⁺H…N ? N…H⁺N formed are easily polarizable hydrogen bonds. From the integral absorbance of a band the concentration of the histidine-histidinium complex, i.e. the concentration of the easily polarizable hydrogen bonds is determined. It is shown that the absorbance of the continuum increases in proportion to the concentration of the easily polarizable N⁺H…N ? N…H⁺N bonds. Finally, it is discussed that via such an easily polarizable histidine-histidinium hydrogen bond a proton translocation in the active center of ribonuclease A may occur.     

Proton translocation in hydrogen bonds with large proton polarizability formed between a Schiff base and phenols

OH…N ? O^?…H⁺N hydrogen bonds formed between N-all-transretinylidene butylamine (Schiff base) and phenols (1:1) are studied by IR spectroscopy. It is shown that both proton limiting structures of these hydrogen bonds have the same weight with Δ pK_a (50%) = (pK_a protonated Schiff base minus pK_a phenol) = 5.5. With the largely symmetrical systems, continua demonstrate that these hydrogen bonds show great proton polarizability. In the Schiff base + tyrosine system in a non-polar solvent the residence time of the proton at the tyrosine residue is much larger than that at the Schiff base. In CH₂CCl₂ these hydrogen bonds show, however, still proton polarizability, i.e., the position of the proton transfer equilibrium OH…N ? O^?…H⁺N is shifted to and fro as function of the nature of the environment of this hydrogen bond. Consequences regarding bacteriorhodopsin are discussed.     

Proton polarizability of poly(L-tyrosine)–hydrogen phosphate hydrogen bonds as a function of alkali cations

We studied films of poly(L -tyrosine) with hydrogen phosphate (residue/phosphate, 1:1) by ir spectroscopy. The influences of the alkali cations (Li⁺, Na⁺, K⁺) and of the degree of hydration were clarified. If Li⁺ ions are present, the OH ?^?OP hydrogen bonds formed in the dried films between the tyrosine OH groups and hydrogen phosphate are asymmetrical. The formation of hydrogen phosphate–hydrogen phosphate hydrogen bonds is prevented by the presence of the Li⁺ ions. With an increase in the degree of hydration, the tyrosine–phosphate bonds are not broken but become slightly stronger. Completely different behaviour is found if K⁺ ions are present. In dry films, the OH ?^?OP ? O^? ?HOP hydrogen bonds formed between tyrosine and hydrogen phosphate show large proton polarizability. The tyrosine proton has a noticeable residence time at the acceptor O atom of the phosphate. The difference in the behaviour of the system with K⁺ ions when compared to the system with Li⁺ ions can be explained, since the hydrogen acceptor O atom of phosphate ions is more negatively charged due to the weaker influence of the K⁺ ions. Furthermore, POH ?^?OP hydrogen bonds between hydrogen phosphate molecules are formed. With an increase in the degree of hydration, the tyrosine–hydrogen phosphate hydrogen bonds are broken, all tyrosine protons are found at the tyrosine residues, and the -PO₃^? groupings are in a symmetrical environment, indicating that the K⁺ ions are removed from these groupings. If the degree of hydration increases further, hydrogen-bonded systems such as hydrogen phosphate–water–hydrogen phosphate are formed that show large proton polarizability due to collective proton motion. When Na⁺ ions are present, the OH ?^?OP ? O^? ?HOP hydrogen bonds formed in dry films still show proton polarizability, but the residence time of the tyrosine proton at the phosphate is very short.     

Phosphate- N base hydrogen bonds involving proton transfer with reference to the non-enzymic hydrolysis of ATP

IR spectra of aqueous solutions of 1:1 mixtures of H₂PO₄^? and various N bases have been studied as models for (POH?N) → (P^?O?H⁺N) hydrogen bonds. 50% proton transfer is observed when the pKa of the protonated N base is 1.1 smaller than that of the phosphate group. The hydrogen bonds are easily polarizable near this equilibrium. These results strongly support the conclusion that such bonds contribute 1) to the self-association of ATP and ADP and 2) to the association of the hydrolysis products ADP and inorganic phosphate.     

Proton transfer and polarizability of hydrogen bonds formed between cysteine and lysine residues

(L -Cys)_n + N-base systems and (L -Cys)_n + (L -Lys)_n systems were studied by ir spectroscopy. It is shown that in the water-free systems, SH ?N ? S^? ?H⁺N hydrogen bonds are formed. With the (L -Cys)_n + N-base systems, both proton-limiting structures in the SH ?N ? S^? ?H⁺N bonds have equal weight when the pK_a of the protonated N-base is 2 pK_a units larger than that of (L -Cys)_n. The same is true with the water-free (L -Cys)_n + (L -Lys)_n system. Thus, with regard to the type of proton potentials present, these hydrogen bonds are proton-transfer hydrogen bonds showing very large proton polarizabilities. This is confirmed by the occurrence of continua in the ir spectra. Small amounts of water open these hydrogen bonds and increase the transfer of the proton to (L -Lys)_n. In the (L -Lys)_n + N-base systems, with increasing proton transfer the backbone of (L -Cys)_n changes from antiparallel β-structure to coil. In (L -Cys)_n + (L -Lys)_n, the conformation is determined by the (L -Lys)_n conformation and changes depending on the chain length of (L -Lys)_n. Finally, the reactivity increase in the active center of fatty acid synthetase, which should be caused by the shift of a proton, is discussed on the basis of the great proton polarizability of the cysteine–lysine hydrogen bonds.     

Proton transfer in and polarizability of hydrogen bonds in proteins. Tyrosine-lysine and glutamic acid-lysine hydrogen bonds — IR investigations

The OH N O^– H⁺N hydrogen bonds formed between tyrosine and lysine, and between glutamic acid and lysine residues are studied by infrared spectroscopy considering the following systems: (l-lys)_n + phenol, copoly (l-lys, l-tyr)_n, (l-lys)_n + (l-tyr)_n and (l-lys)_n + (l-glu)_n. The phenol-lysine hydrogen bonds are largely symmetrical in the average if the pK_a of the protonated lysine is 2.2 units larger than that of the phenols. In the case of the hydrogen bonds between tyrosine and lysine residues in copoly (l-lys, l-tyr)_n and (l-lys)_n + (l-tyr)_n, the weight of the proton limiting structure OH N is 80–90%, and that of the polar O^– H⁺N structure 10–20%. Double minimum proton potentials occur but the proton is preferentially present at the tyrosine residues. In the (l-lys)_n + (l-glu)_n system, the protons are present at the lysine residues. Thus, these hydrogen bonds have very large dipole moments (about 10 D). With the lysine-phenole hydrogen bonds, hydration shifts the proton transfer equilibrium a little in favour of the polar proton limiting structure O^– H⁺N. These hydrogen bonds are broken to a large extent, however, when only about 3 water molecules are present per lysine residue. When less water is present, as in the copoly (l-lys, l-tyr)_n and (l-lys)_n + (l-tyr)_n systems, these hydrogen bonds are, however, formed quantitatively. Thus — as discussed in this paper — the tyrosine-lysine hydrogen bonds can participate in proton conducting hydrogen bonded systems — as, for instance, present in bacteriorhodopsin — performing the proton transport through hydrophobic regions of biological membranes.     

Infrared investigation of poly-L-histidine structure dependent on protonation

Poly-L -histidine (PLH) films at different degrees of protonation were produced mid subjected to infrared spectroscopic investigation (range 4000-650 cm^?1). In addition, the N-deuterated film spectra were plotted. The amide II and III bands show that the peptide group is present in the trans form. The amide I and II bands show that at 0% and 50% protonation the PLH occurs as an α-helix and at 100% protonation as a random coil with some ranges in β structure. At 0% and 50% protonation, no hydration water is bound to the backbone. At 0% protonation all NH groups are linked to each other or to water molecules via hydrogen bonds. At 50% protonation NH⁺?N bonds form between the imidazole rings. These protons are present in continuous energy level distribution. Such bonds with tunneling protons are extremely polarizable and between these bonds may act proton dispersion forces. The Cl^? ions are bonded to the NH groups of the imidazole groups. The hydration water is bonded to the Cl^?? ions and to the NH groups. At 100% protonation, hydration water is bonded also to the CO groups of the backbone. The NH groups of the backbone, like those of the rings, endeavor especially in the dry state to bond to the Cl^? ions. This leads to a strong steric constraint of the random coil.     

Proton Dispersion Forces: Secondary-Structure Stabilizing Forces between the Hydrogen Bonds of the Polynucleotides

In the double helix formed by the semiprotonated polycytidylic acid (poly C), both strands are linked via NH⁺...N hydrogen bonds. It is a known fact that such symmetrical hydrogen bonds with a double minimum potential well are extremely polarizable. This polarizability causes interaction effects, in particular the proton dispersion forces between such hydrogen bonds. These forces result in a shift of the energy levels and a continuum is observed in the infrared (IR) spectra of solutions in which such hydrogen bonds are present. The continuum occurs in the IR spectrum of the semiprotonated poly C, when the former is present in coiled state. If the double helix forms, an extremely broad band of the NH stretching vibration is observed instead of the continuum, since in the double helix all hydrogen bonds are oriented equally to one another and polarize each other mutually to a strong degree. The proton dispersion forces between the hydrogen bonds balance a considerable part of the electrostatic repulsion of the protons and hence enable the double helix to form. It is conceivable that an unsymmetrical double minimum potential well is present in the NH...N bonds in the DNA and RNA. Such bonds may likewise be considerably more polarizable than electron systems and thus, in this case too, proton dispersion forces would contribute to helix stabilization.     

Mechanism of Hydroxyl Radical Scavenging by Rebamipide: Identification of Mono-hydroxylated Rebamipide as a Major Reaction Product

Rebamipide, an antiulcer agent, is known as a potent hydroxyl radical (^?OH) scavenger. In the present study, we further characterized the scavenging effect of rebamipide against ^?OH generated by ultraviolet (UV) irradiation of hydrogen peroxide (H²O²), and identified the reaction products to elucidate the mechanism of the reaction. Scavenging effect of rebamipide was accessed by ESR using DMPO as a ^?OH-trapping agent after UVB exposure (305?nm) to H²O² for 1?min in the presence of rebamipide. The signal intensity of ^?OH adduct of DMPO (DMPO-OH) was markedly reduced by rebamipide in a concentration-dependent fashion as well as by dimethyl sulfoxide and glutathione as reference radical scavengers. Their second order rate constant values were 5.62?×?10¹⁰, 8.16?×?10⁹ and 1.65?×?10¹⁰?M^-1?s^-1, respectively. As the rebamipide absorption spectrum disappeared during the reaction, a new spectrum grew due to generation of rather specific reaction product. The reaction product was characterized by LC-MS/MS and NMR measurements. Finally, a hydroxylated rebamipide at the 3-position of the 2(1H)-quinolinone nucleus was newly identified as the major product exclusively formed in the reaction between rebamipide and the ^?OH generated by UVB/H²O². Specific formation of this product explained the molecular characteristics of rebamipide as a potential ^?OH scavenger.     

Congruence between PM H<Superscript>+</Superscript>-ATPase and NADPH oxidase during root growth: a necessary probability

Plasma membrane (PM) H⁺-ATPase and NADPH oxidase (NOX) are two key enzymes responsible for cell wall relaxation during elongation growth through apoplastic acidification and production of ˙OH radical via O₂˙^?, respectively. Our experiments revealed a putative feed-forward loop between these enzymes in growing roots of Vigna radiata (L.) Wilczek seedlings. Thus, NOX activity was found to be dependent on proton gradient generated across PM by H⁺-ATPase as evident from pharmacological experiments using carbonyl cyanide m-chlorophenylhydrazone (CCCP; protonophore) and sodium ortho-vanadate (PM H⁺-ATPase inhibitor). Conversely, H⁺-ATPase activity retarded in response to different ROS scavengers [CuCl₂, N, N’ –dimethylthiourea (DMTU) and catalase] and NOX inhibitors [ZnCl₂ and diphenyleneiodonium (DPI)], while H₂O₂ promoted PM H⁺-ATPase activity at lower concentrations. Repressing effects of Ca⁺² antagonists (La⁺³ and EGTA) on the activity of both the enzymes indicate its possible mediation. Since, unlike animal NOX, the plant versions do not possess proton channel activity, harmonized functioning of PM H⁺-ATPase and NOX appears to be justified. Plasma membrane NADPH oxidase and H⁺-ATPase are functionally synchronized and they work cooperatively to maintain the membrane electrical balance while mediating plant cell growth through wall relaxation.     

Diethylpyrocarbonate inhibition of vacuolar H+-pyrophosphatase possibly involves a histidine residue

Vacuolar proton pumping pyrophosphatase (H⁺-PPase; EC 3.6.1.1) plays a pivotal role in electrogenic translocation of protons from cytosol to the vacuolar lumen at the expense of PP_i hydrolysis. A histidine-specific modifier, diethylpyrocarbonate (DEPC), could substantially inhibit enzymic activity and H⁺-translocation of vacuolar H⁺-PPase in a concentration-dependent manner. Absorbance of vacuolar H⁺-PPase at 240 nm was increased upon incubation with DEPC, demonstrating that an N-carbethoxyhistidine moiety was probably formed. On the other hand, hydroxylamine, a reagent that can deacylate N-carbethoxyhistidine, could reverse the absorption change at 240 nm and partially restore PP_i hydrolysis activity as well. The pK _a of modified residues of the enzyme was determined to be 6.4, a value close to that of histidine. Thus, we speculate that inhibition of vacuolar H⁺-PPase by DEPC possibly could be attributed to the modification of histidyl residues on the enzyme. Furthermore, inhibition of vacuolar H⁺-PPase by DEPC follows pseudo-first-order rate kinetics. A reaction order of 0.85 was calculated from a double logarithmic plot of the apparent reaction constant against DEPC concentration, suggesting that the modification of one single histidine residue on the enzyme suffices to inhibit vacuolar H⁺-PPase. Inhibition of vacuolar H⁺-PPase by DEPC changes V _max but not K _m values. Moreover, DEPC inhibition of vacuolar H⁺-PPase could be substantially protected against by its physiological substrate, Mg²⁺-PP_i. These results indicated that DEPC specifically competes with the substrate at the active site and the DEPC-labeled histidine residue might locate in or near the catalytic domain of the enzyme. Besides, pretreatment of the enzyme with N-ethylmaleimide decreased the degree of subsequent labeling of H⁺-PPase by DEPC. Taken together, we suggest that vacuolar H⁺-PPase likely contains a substrate-protectable histidine residue contributing to the inhibition of its activity by DEPC, and this histidine residue may located in a domain sensitive to the modification of Cys-629 by NEM.     

N-Cyclo-N'-(4-Dimethylamino-alpha-Naphthyl)Carbodiimide Inhibits Membrane-Bound and Partially Purified Tonoplast ATPase from Maize Roots

Certain carboxylic acid groups within the primary structure of proton translocating proteins are thought to be involved in the proton pathway. In this report, the effects of a lipophilic carboxylic acid reactive reagent, N-cyclo-N′(4-dimethylamino-α-naphthyl)carbodiimide (NCD-4), on the two types of proton pumps in maize (Zea mays L.) root microsomes were investigated. NCD-4 was found to inhibit the vacuolar-type H⁺-ATPase in microsomal preparations; however, the plasma membrane-type H⁺-ATPase was unaffected. The H⁺-ATPase in highly purified tonoplast vesicles was also inhibited by NCD-4. Inhibition was dependent on the concentration and length of exposure to the reagent. However, there was little, if any, increase in the fluorescence of treated vesicles, indicating few carboxylic acid residues were reacting. Inhibition of the tonoplast H⁺-ATPase by NCD-4 was examined further with a partially purified preparation. The partially purified H⁺-ATPase also showed sensitivity to the NCD-4, supporting the hypothesis that this carboxylic acid reagent is an inhibitor of the tonoplast ATPase from maize roots.     

Theoretical studies on protein-nucleic acid interactions. II. Hydrogen bonding of amino acid side chains with bases and base pairs of nucleic acids

With a view to understanding the role of hydrogen bonds in the recognition of nucleic acids by proteins, hydrogen bonding between the bases and base pairs of nucleic acids and the amino acids (Asn, Gln, Asp and Glu, and charged residues Arg⁺, Glu^?, and Asp^?) has been studied by a second-order perturbation theory. Binding energies have been calculated for all possible configurations involving a pair of hydrogen bonds between the base (or base pair) and the amino acid residue. Our results show that the hydrogen bonding in these cases has a large contribution from electrostatic interaction. In general, the charged amino acids, compared to the uncharged ones, form more stable complexes with bases or base pairs. The hydrogen-bond energies are an order of magnitude smaller than the Coulombic interaction energies between basic amino acids (Lys⁺, Arg⁺, and His⁺) and the phosphate groups of nucleic acids. The stabilities of the complexes of amino acids Asn, Gln, Asp, and Glu with bases are in the order: G–X > C–X > A–X U–X or T–X, and G · C–X > A · T(U)–X, where X is one of these amino acid residues. It has been shown that Glu^? and Asp^? can recognize guanine in single-stranded nucleic acids; Arg⁺ can recognize G · C base pairs from A · T base pairs in double-stranded structures.     

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.     

The influences of water solvent on the structures and stabilities of Na+–AD conformers

The influences of water solvent on the structures and stabilities of the complex ion conformers formed by the coordination of alanine dipeptide (AD) and Na⁺ have been investigated using supramolecular and polarizable continuum solvation models at the level of B3LYP/6-311++G**, respectively; 12 monohydrated and 12 dihydrated structures of Na⁺–AD complex ion were obtained after full geometrical optimization. The results showed that H₂O molecules easily bind with Na⁺ of Na⁺–AD complex ion, forming an ion-lone pair interaction with the Na–O bond length of 2.1–2.3 Å. Besides, H₂O molecules also can form hydrogen bonds O_W–H_W···O(1), O_W–H_W···O(2), N(1)–H(1)···O_W or N(2)–H(2)···O_W with O or N groups of the Na⁺–AD backbone. The most stable gaseous bidentate conformer C7AB of Na⁺–AD is still the most stable one in the solvent of water. However, the structure of the most unstable gaseous conformer α′B of Na⁺–AD collapses under the attack of H₂O molecules and changes into C7AB conformation. Computations with IEFPCM solvation model of self-consistent reaction field theory give that aqueous C5A is more stable than C7_eqB and that the stabilization energies of water solvent on monodentate conformers of Na⁺–AD complex ion (about 272–294 kJ/mol) are more than those on bidentate ones (about 243 kJ/mol).     

Single‐Atom to Single‐Atom Grafting of Pt1 onto FeN4 Center: Pt1@FeNC Multifunctional Electrocatalyst with Significantly Enhanced Properties

Nonprecious metal catalysts (NPMCs) Fe?N?C are promising alternatives to noble metal Pt as the oxygen reduction reaction (ORR) catalysts for proton‐exchange‐membrane fuel cells. Herein, a new modulation strategy is reported to the active moiety Fe?N₄ via a precise “single‐atom to single‐atom” grafting of a Pt atom onto the Fe center through a bridging oxygen molecule, creating a new active moiety of Pt₁?O₂?Fe₁?N₄. The modulated Fe?N?C exhibits remarkably improved ORR stabilities in acidic media. Moreover, it shows unexpectedly high catalytic activities toward oxygen evolution reaction (OER) and hydrogen evolution reaction (HER), with overpotentials of 310 mV for OER in alkaline solution and 60 mV for HER in acidic media at a current density of 10 mA cm^?2, outperforming the benchmark RuO₂ and comparable with Pt/C(20%), respectively. The enhanced multifunctional electrocatalytic properties are associated with the newly constructed active moiety Pt₁?O₂?Fe₁?N₄, which protects Fe sites from harmful species. Density functional theory calculations reveal the synergy in the new active moiety, which promotes the proton adsorption and reduction kinetics. In addition, the grafted Pt₁?O₂? dangling bonds may boost the OER activity. This study paves a new way to improve and extend NPMCs electrocatalytic properties through a precisely single‐atom to single‐atom grafting strategy.