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.     

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.     

Proton transfer in and polarizability of hydrogen bonds coupled with conformational changes in proteins. II. IR investigation of polyhistidine with various carboxylic acids

Polyhistidine-carboxylic acid systems are studied by ir spectroscopy. It is shown that OH ?N ? O^?…H⁺N bonds formed between carboxylic groups and histidine residues are easily polarizable proton-transfer hydrogen bonds when the pK_a of the protonated histidine residues is about 2.8 units larger than that of the carboxylic groups. From these results it bis concluded that OH ?N ? O^? ?H⁺N bonds between glutamic or aspartic acid histidine residues in proteins may be easily polarizable proton-transfer bonds. Furthermore, it is demonstrated that water molecules shift the proton-transfer equilibria in these hydrogen bonds in favor of the polar structure, i.e., due to water or polar environments OH ?N ? O^? ?H⁺N bonds with smaller ΔpK_a values become easily polarizable proton-transfer hydrogen bonds. A consideration of the amide bands of polyhistidine shows that it can be present in five different conformations. It is shown that these conformational changes are strongly related to the degree of proton transfer. Hence, the degree of proton transfer, the degree of hydration, and conformation are not independent of each other, but are strongly coupled. Further proof for the interdependence of proton transfer and conformational changes are hysteresis effects, which are observed with studies of polyhistidine dependent on carboxylic acid, adsorption and desorption. OH ?N ? O^? ?H⁺N bonds between aspartic and glutamic acid and histidine residues are present in hemoglobin, in ribonucleases, and in proteases, whereby this type of bond is preferentially found in the active centers of these enzymes. It is pointed out that hydrogen bonds with such interaction properties should be of great significance for structure and especially functions of proteins in which they are present.     

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.     

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.     

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.     

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.     

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.     

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.     

Crystal Structure of 2′-Deoxycytidine Hemidihydrogenphosphate Reveals C+·C Base Pairs and Tight,Hydrogen-Bonded (H2PO4 −)∞ Columns (1)

Abstract

2′-Deoxycytidine hemidihydrogenphosphate has been crystallized in the hexagonal space group P6₂ with α=25.839(3), c = 12.529(1) Å. The structure has been solved using the Patterson search method. The asymmetric unit contains two protonated, base-paired 2′-deoxycytidine dimers and two H₂PO₄ ^? anions. The C⁺·C base pairs are composed of a protonated and a neutral species each and are triple H-bonded, the central N(3)…N(3) bonds being 2.850(7) and 2.884(5) Å. The conformations of the four nucleosides fall in the same category (sugar puckers 2·-endo, glycosidic links anti) but in one of them the glycosidic torsion angle is quite low with consequences in other geometrical parameters. The H₂PO₄ ^? anions are located on twofold axes and form two types of tight columns with P…P separations about 4.18 Å The neighboring units along a column are linked via two very short O…H…O hydrogen bonds (O…O about 2.49 Å) leading to effective equalization of the P-O bonds. The base pairs of the two dC⁺·dC cations are coplanar and form layers perpendicular to the phosphate columns repeating every c/3. Within the layers, the dimers form a network through 0(5′)…O(2) hydrogen bonds but their primary intermolecular interactions have the form of H-bond anchors [N(4)-H…O-P and 0(3′)-H…O-P] to the phosphate groups.     

Gloeobacter Rhodopsin,Limitation of Proton Pumping at High Electrochemical Load

We studied the photocurrents of a cyanobacterial rhodopsin Gloeobacter violaceus (GR) in Xenopus laevis oocytes and HEK-293 cells. This protein is a light-driven proton pump with striking similarities to marine proteorhodopsins, including the D121-H87 cluster of the retinal Schiff base counterion and a glutamate at position 132 that acts as a proton donor for chromophore reprotonation during the photocycle. Interestingly, at low extracellular pH_o and negative voltage, the proton flux inverted and directed inward. Using electrophysiological measurements of wild-type and mutant GR, we demonstrate that the electrochemical gradient limits outward-directed proton pumping and converts it into a purely passive proton influx. This conclusion contradicts the contemporary paradigm that at low pH, proteorhodopsins actively transport H⁺ into cells. We identified E132 and S77 as key residues that allow inward directed diffusion. Substitution of E132 with aspartate or S77 with either alanine or cysteine abolished the inward-directed current almost completely. The proton influx is likely caused by the pK_a of E132 in GR, which is lower than that of other microbial ion pumping rhodopsins. The advantage of such a low pK_a is an acceleration of the photocycle and high pump turnover at high light intensities.     

Gloeobacter Rhodopsin,Limitation of Proton Pumping at High Electrochemical Load

We studied the photocurrents of a cyanobacterial rhodopsin Gloeobacter violaceus (GR) in Xenopus laevis oocytes and HEK-293 cells. This protein is a light-driven proton pump with striking similarities to marine proteorhodopsins, including the D121-H87 cluster of the retinal Schiff base counterion and a glutamate at position 132 that acts as a proton donor for chromophore reprotonation during the photocycle. Interestingly, at low extracellular pH_o and negative voltage, the proton flux inverted and directed inward. Using electrophysiological measurements of wild-type and mutant GR, we demonstrate that the electrochemical gradient limits outward-directed proton pumping and converts it into a purely passive proton influx. This conclusion contradicts the contemporary paradigm that at low pH, proteorhodopsins actively transport H⁺ into cells. We identified E132 and S77 as key residues that allow inward directed diffusion. Substitution of E132 with aspartate or S77 with either alanine or cysteine abolished the inward-directed current almost completely. The proton influx is likely caused by the pK_a of E132 in GR, which is lower than that of other microbial ion pumping rhodopsins. The advantage of such a low pK_a is an acceleration of the photocycle and high pump turnover at high light intensities.     

Theoretical insight into the conversion of xylose to furfural in the gas phase and water

The antioxidant properties of some phenolic Schiff bases in the presence of different reactive particles such as ^•OH, ^•OOH, (CH₂=CH−O−O^•), and ^-•O₂ were investigated. The thermodynamic values, ΔH _BDE, ΔH _IP, and ΔH _PA, were used for this purpose. Three possible mechanisms for transfer of hydrogen atom, concerted proton−electron transfer (CPET), single electron transfer followed by proton transfer (SET-PT), and sequential proton loss electron transfer (SPLET) were considered. These mechanisms were tested in solvents of different polarity. On the basis of the obtained results it was shown that SET-PT antioxidant mechanism can be the dominant mechanism when Schiff bases react with radical cation, while SPLET and CPET are competitive mechanisms for radical scavenging of hydroxy radical in all solvents under investigation. Examined Schiff bases react with the peroxy radicals via SPLET mechanism in polar and nonpolar solvents. The superoxide radical anion reacts with these Schiff bases very slowly.

     

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.     

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.     

Concerted involvement of cooperative proton–electron linkage and water production in the proton pump of cytochrome c oxidase

In cytochrome c oxidase, oxido-reductions of heme a/Cu_A and heme a₃/Cu_B are cooperatively linked to proton transfer at acid/base groups in the enzyme. H⁺/e⁻ cooperative linkage at Fe_a3/Cu_B is envisaged to be involved in proton pump mechanisms confined to the binuclear center. Models have also been proposed which involve a role in proton pumping of cooperative H⁺/e⁻ linkage at heme a (and Cu_A). Observations will be presented on: (i) proton consumption in the reduction of molecular oxygen to H₂O in soluble bovine heart cytochrome c oxidase; (ii) proton release/uptake associated with anaerobic oxidation/reduction of heme a/Cu_A and heme a₃/Cu_B in the soluble oxidase; (iii) H⁺ release in the external phase (i.e. H⁺ pumping) associated with the oxidative (R → O transition), reductive (O → R transition) and a full catalytic cycle (R → O → R transition) of membrane-reconstituted cytochrome c oxidase. A model is presented in which cooperative H⁺/e⁻ linkage at heme a/Cu_A and heme a₃/Cu_B with acid/base clusters, C₁ and C₂ respectively, and protonmotive steps of the reduction of O₂ to water are involved in proton pumping.     

Hydration effect on proton transfer in melamine−cyanuric acid complex

Self-assembly of melamine-cyanuric acid (MC) leads to urinary tract calculi and renal failure. The hydration effects on molecular geometry, the IR spectra, the frontier molecular orbital, the energy barrier of proton transfer (PT), as well as the stability of MC were explored by density functional theory (DFT) calculations. The intramolecular PT breaks the big π-conjugated ring of melamine or converts the p-π conjugation (:N-C'=O) to π-π conjugation (O=C-N=C') of cyanuric acid. The intermolecular PT varies the coupling between melamine and cyanuric acid from pure hydrogen bonds (N_a…HN_d and NH…O) to the cooperation of cation…anion electrostatic interaction (N_aH⁺…N_d ^-) and two NH…O hydrogen bonds. Distinct IR spectra shifts occur for N_a…HN_d stretching mode upon PT, i.e., blue-shift upon intramolecular PT and red-shift upon intermolecular PT. It is expected that the PT would inhibit the generation of rosette-like structure or one-dimensional tape conformer for the MC complexes. Hydration obviously effects the local geometric structure around the water binding site, as well as the IR spectra of NH…O and N…HN hydrogen bonds. Hydration decreases the intramolecular PT barrier from ~45 kcal mol^-1 in anhydrous complex to ~11.5 kcal mol^-1 in trihydrated clusters. While, the hydration effects on intermolecular PT barrier is slight. The relative stability of MC varies slightly by hydration due to the strong hydrogen bond interaction between melamine and cyanuric acid fragments.

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Graphical Abstract Hydration effect on proton transfer in melamine?cyanuric acid complex

     

Perturbation of Hydrogen Bonds in the Adenine…Thymine Base Pair by Na+, Mg2+, Ca2+ and NH4 + Cations

Abstract

Perturbation of the hydrogen bonds in the adenine…thymine base pair by Na⁺, Mg²⁺, Ca²⁺ and NH₄ ⁺ cations has been investigated by means of ab initio SCF calculations with the STO-3G basis set. The geometry of adenine…thymine, as well as those of the perturbed pairs were optimized. Approach of any cation to thymine at 06 leads to destabilization of the adenine…thy mine pair; divalent cations (Mg²⁺, Ca²⁺) have a profound effect on the structure of the base pair. The approach of a cation to other available sites (thymine: O2, adenine N1 and N3) leads, on the other hand, to stabilization of the base pair. If a water molecule is placed between the cation and the base pair, the structure and stability of the base pair are changed only negligibly.     

An aluminoborate cluster [AlB12O14(OH)12]: Synthesis and structure of [C5H6N][AlB12O14(OH)12]

A new aluminoborate, [C₅H₆N][AlB₁₂O₁₄(OH)₁₂], has been hydrothermally synthesized at 200 °C. The single-crystal diffraction study reveals that it crystallizes in space group C2/c. It consists of aluminoborate clusters [AlB₁₂O₁₄(OH)₁₂]⁻ and counterions [C₅H₆N]⁺. The aluminoborate cluster contains an Al(OH)₆ octahedron as a core that is capped by two raft-like polyborate units [B₆O₇(OH)₆]. These clusters are further interlinked by extensive hydrogen bonding to form a three-dimensional (3D) network, containing large channels along the b-axis, in which the [C₅H₆N]⁺ cations are located.