501—An electrochemical study of energy-dependent potassium accumulation in E. coli: Part IX. Reversal of the mechanism exchanging 2 H+ for K+ with the coupled synthesis of ATP

E. coli is able to exchange 2 H⁺ from the external medium for one K⁺ of a cell with the concurrent synthesis of ATP. The 2 H⁺/K⁺ exchange and the coupled ATP synthesis are in need of both the essential Δ$\text{}\text{?}$gm_H+ (around 24 kJ) and the high K⁺ gradient (10³) directed from a cell to the medium. The reverse pump cycle is actuated as well as the direct one [3] merely through an increase of osmolarity in the environmental medium. The reverse process can be blocked by the insignificant ncrease in external pH or in K⁺ concentration, as well as by DCCD or by protonophore. The stoichiometry of the entire pump cycle is ATP: 2 H⁺ :K⁺. These observations, as well as the previous findings [8,9] that 2 H⁺ from a cell and one external K⁺ are transported through F₁·F₀ and TrkA respectively, suggest that F₁·F₀ and TrkA form the structural association in bacterial membrane for the joint employment of phosphate bond energy, the supercomplex (F₁ ·F₀TrkA operating as an electrogenic proton-potassium pump with stable stoichiometry ATP:2 H⁺ :K⁺.     

EQCM Study of Ru and RuO2 Surface Electrochemistry

The present study represents comparative analysis of voltammetric and microgravimetric behavior of active ruthenium (Ru), electrochemically passivated ruthenium (Ru/RuO₂) and thermally formed RuO₂ electrodes in the solutions of 0.5 M H₂SO₄ and 0.1 M KOH. It has been found that cycling the potential of active Ru electrode within E ranges 0 V–0.8 V and 0 V–1.2 V in 0.5 M H₂SO₄ and 0.1 M KOH solutions, respectively, leads to continuous electrode mass increase, while mass changes observed in alkaline medium are considerably smaller than those in acidic one. Microgravimetric response of active Ru electrode in 0.5 M H₂SO₄ within 0.2 V–0.8 V has revealed reversible character of anodic and cathodic processes. The experimentally found anodic mass gain and cathodic mass loss within 0.2–0.8 V make 2.2–2.7 g F^?1, instead of 17 g F^?1, which is the theoretically predicted value for Ru(OH)₃ formation according to equation: Ru+3H₂O?Ru(OH)₃+3H⁺+3e^?. In the case of Ru/RuO₂ electrode relatively small changes in mass have been found to accompany the anodic and cathodic processes within E range between 0.4 V and 1.2 V in the solution of 0.5 M H₂SO₄. Meanwhile cycling the potential of thermally formed RuO₂ electrode under the same conditions has lead to continuous decrease in electrode mass, which has been attributed to irreversible dehydration of RuO₂ layer. On the basis of microgravimetric and voltammetric study as well as the coulometric analysis of the results conclusions are presented regarding the nature of surface processes taking place on Ru and RuO₂ electrodes.     

Bifunctional Ion‐Selective Electrode Based on C60‐Cryptand 22 for Silver and Iodine Ions

Fullerence C60‐cryptand 22 was prepared and successfully applied as the electric carrier in the PVC electrode membrane of a bifunctional ion‐selective electrode for cations, e.g., Ag⁺ ions as well as anions, e.g., I^? ions. The bifunctional ion‐selective electrode based on C60‐cryptand 22 can be applied as a Silver (Ag⁺) ion selective electrode with an internal electrode solution of 10^?3 M AgNO₃ in water (pH = 6.3), or as an Iodide (I^?) ion selective electrode with an acidic internal electrode solution of 10^?4 M KI_(aq) (pH = 2) in which the cryptand 22 is protonated, and the C60‐cryptand 22 is changed to C60‐Cryptand22–H⁺ and becomes an anionic electro‐carrier to absorb the I^? ion. The Ag⁺ ion selective electrode based on C60‐cryptand 22 gave a linear response with a near‐Nernstian slope (59.5 mV decade^?1) within the concentration range 10^?1‐10^?3 M Ag⁺_(aq). The Ag⁺ ion electrode exhibited comparatively good selectivity for silver ions, over other transition‐metal ions, alkali and alkaline earth metal ions. The Ag⁺ ion selective electrode with good stability and reproducibility was successfully used for the titration of Ag⁺_(aq) with Cl^? ions. The Iodide (I^?) Ion selective electrode based on protonated C60–cryptand22‐H⁺ also showed a linear response with a nearly Nernstian slope (58.5 mV decade^?1) within 10^?1 ‐ 10^?3 M I^? _(aq) and exhibited good selectivity for I^? ions and had small selectivity coefficients (10^?2–10^?3) for most of other anions, e.g., F^? , OH^?, CH₃COO^?, SO₄^2?, CO₃^2?, CrO₄^2?, Cr₂O₇^2? and PO₄^3? ions.     

Échelle d'acidité dans l'hydrogénodifluorure de potassium (KHF2) fondu à 250°C: Détermination électrochimique

In molten potassium hydrogenodifluoride (KHF₂) fully ionized into K⁺ and HF₂^?, at 250°C, the HF₂^? ion is slightly dissociated according to the equilibrium: HF₂^?HF+F^?. This is a solvent acid base equilibrium, HF being the strongest acid and F^? the strongest base in this system. By means of a voltammetric study we showed that the hydrogen electrode may be used as an acidity indicator electrode in the whole acidity range of the melt. By analysis of the equilibrium potential variation in acidic and in basic media, the HF₂^? dissociation constant (melt autoprotolysis constant): K_D = {HF} {F^?} was determined The experimental value: K_D=10^?2.05 mol² kg^?2 is compared with a calculated one, issued from thermodynamic data. Results obtained with other electrodes (LaF₃ monocrystal electrode and copper electrode) were discussed and compared with those obtained with the hydrogen electrode.     

Oxygen electrodes in fused salts: Investigation and mechanistic remarks on the system (Ni)O2, H2O/OH− in the (Na,K)NO3 eutectic melt

A potentiometric investigation on the system (Ni)O₂, H₂O/OH^? was carried out within the temperature range 513?T?636 K in the (Na, K)NO₃ equimolar mixture containing OH^? ions in the concentration range 5×10^?6<[OH^?]<10^?1m and flushed with a mixture of O₂ and H₂O at variable partial pressures. The system has been found to behave reversibly in all hydroxide concentration and temperature intervals studied with respect to all the species involved in the over-all electrode reaction ½ O₂+H₂O+2e^?=2OH^? so that the following nernstian relationship could be written E=E_O2,H₂O/OH^?+RT/Fln{[O₂]^1/4[H₂O]^1/2/[OH^?]} This potentiometric behaviour was tentatively interpreted on the basis of mechanistic models involving, in some steps, solid nickel oxides formed on the electrode surface by contact with the melt. The actual formation and existence of these compounds on the electrode surface under the given experimental conditions was proved by a proper XPS investigation.     

Hydrogen bonding: VII. Low temperature infrared spectral studies of potassium dihydrogen trifluoride,trihydrogen tetrafluoride,and tetrahydrogen pentafluoride; structure of the H3F−4 ION

We have recorded the infrared spectra of crystalline K⁺H₂F₃^?, K⁺H₃F₄^?, and K⁺H₄F₅^? at room temperature and 12–18 K. The broad (4&#x0303;00 cm^?1) anion F-H stretching bands for these three salts are not resolved at low temperature; however, in each case the F-H-F bending region is resolved into the maximum number of bands predicted by theory. The complexity of the F-H-F bending mode region shows the H₄F₅^? ion to be of lower symmetry than predicted by X-ray studies. The H₃F₄^? ion has three hydrogen fluorides hydrogen bonded to a central fluoride ion, rather than a chain type structure. The F-H stretching bands for the three ions have very similar frequencies (1750–1800 cm^?1), which shows the hydrogen bonds in the three ions to be of about the same strength, and to be significantly weaker than the hydrogen bond in the HF₂^? ion.     

F3CCN5S3, A BICYCLIC MULTIFUNCTIONAL SULFUR-NITROGEN LIGAND

The bicyclic sulfur-nitrogen heterocycle F₃CCN₅S₃ (1) was investigated as a donor and acceptor toward H⁺, metal cations, and F^?. Whereas the protonated species F₃CCN₅S₃H⁺ AsF₆ ^? (2) can be isolated, the product of the reaction with F^? is unstable and decomposes among other products to TAS⁺ F₃CCN₅S₃NC(NH₂)CF₃ ^? (3), which is isolated from this reaction in small amounts.     

The formation of flouride complexes of titanium(IV)

The complex formation equilibria between titanium(IV) and fluoride ions have been studied at 25°C in 3 M(Na)Cl ionic medium by measuring, with an ion selective electrode for F^?, the free HF concentration in acid Ti(IV) solutions. The [H⁺] was kept within 0.25 and I M where the predominant form of uncomplexed metal is the dihydroxotitanium(IV) ion, Ti(OH)²⁺₂. The potentiometric data have been explained by assuming Ti(OH)₂F⁺, TiF₄ and HTiF^?₆, with equilibrium constants given in Table 3. Within the accuracy of the present e.m.f. study, ±0.2 mV, no evidence for intermediate complexes bearing 2, 3 and 5 F^? was found.From a special series of measurements, carried out by replacing a large part of the Cl^? with ClO^?₄, it is concluded that no appreciable amount of Ti(IV)Cl complexes is formed at the 3 M level employed as ionic medium.     

On the existence of H2F+ in dilute hydrofluoric acid solutions

The existence of H₂F⁺, which has been long postulated in dilute aqueous HF solutions, was investigated by fluoride ion-selective electrode potentiometry. Even under conditions conducive to its formation precise measurements yielded only equivocal evidence for its occurrence. It is thought that H₂F⁺ will exist only in very concentrated HF solutions with low water activities.     

Electrochemical reactions with protonations at equilibrium: Part X. The kinetics of the p-benzoquinone/hydroquinone couple on a platinum electrode

The kinetics of the p-benzoquinone/hydroquinone Q/QH₂ couple on a platinum electrode are analysed on the basis of the theory presented earlier (E. Laviron, J. Electroanal. Chem., 146 (1983) 15) for the nine-member square scheme when the protonations are assumed to be at equilibrium, using experimental data from the literature. The square scheme is of the NN type. The Tafel plots and the variations of the experimental apparent rate constants between pH 0 and 7 are in good agreement with the theoretical predictions. The heterogeneous rate constants found for the elemental electrochemical steps are as follow: Q Q^?, k_h3=1/6×10^?3 cm s^?1; QH^.QH^?, k_h5=0.11 cm s^?1; QH⁺QH^., k_h2?160 cm s^?1; k_h4 for the reaction QH₂^+.QH₂ is in the range 0.5–4 cm s^?1. Between pH 0 and 7, the reaction sequence during the reduction is, for the most part, successively H⁺e^?H⁺e^?, e^?H⁺H⁺e^?, and e^?H⁺e^?H⁺ (reverse sequence during the oxidation).     

Optisch aktive übergangsmetall-komplexe XX. Optisch aktive cyclopentadienyl-perfluoropropyl-kobalt-komplexe mit zweizähnigen schiff-basen

In the reaction of C₅H₅ Co(C₃F₇)(CO)I with the Schiff base NN′, derived from S-(-)-?-phenylethylamine and pyridine carbaldehyde-2, the salt [C₅H₅Co(C₃F₇)NN′]⁺ I^? (Ia,b) is formed, which can be transformed to [C₅H₅ Co(C₃F₇)NN′]⁺ PF₆^? (IIa,b). The sodium salt Na⁺ [NN″]^? of the Schiff base, derived from S-(-)-α-phenylethylamine and pyrrol carbaldehyde-2, in the reaction with C₅H₅ C0(C₃F₇)(CO)I yields the neutral complex C₅H₅ Co(C₃F₇)NN″ (IIIa,b). The diastereoisomeric pairs IIa,b and IIIa,b are separated by fractional crystallisation and chromatography respectively into the optically pure components which differ in their ¹H NMR spectra. The IR, UV, CD, mass spectra and optical rotations of the new compounds IIa, IIb, IIIa and IIIb are compared.     

Oxygen evolution on SrFeO3 electrode

Oxygen evolution reactions on SrFeO₃ were investigated in alkaline and acidic solutions. It was found that the catalytic activity for the oxygen evolution reaction in the alkaline solution is high. The following reaction steps (V)+Fe+2H₂O→(O)+FeOH₂+2H⁺+2e^? in acidic solution and FeOH+OH^?→FeO^?+H₂O in alkaline solution are presumed to be rate-controlling in the anodic evolution of oxygen on SrFeO₃ electrode, where (V) denotes oxygen vacancy on the electrode surface. The reaction mechanism and the catalytic property are discussed in connection to the band structure of the oxide.     

Die Kristallstruktur des Hydrazinium-monofluorids

The hydrazinium monofluoride N₂H₅F crystallizes with orthorhombic symmetry, space group P2₁2₁2₁,a=4.592 Å,b=8.217 Å,c=12.341 Å, and 8 formula units. The structure was determined by the permutation method in projection, and by the three-dimensionalPatterson function, refined by Full-Matrix-Least-Squares (R=0.056). The structure consists of N₂H₅ ⁺- and F^?-ions, bonded with hydrogen bonds N?H ... N and N?H ... F. Each N₂H₅ ⁺ ion is surrounded by four F^?-ions and two nitrogen atoms of two different N₂H₅ ⁺ ions. Each F^? ion is connected with four different N₂H₅ ⁺ ions.     

A simple model of solvation within the molecular orbital theory

A simple model of solvation within the molecular orbital method is proposed whereby the effect of solvent molecules is simulated by the inclusion of fractional point charges at the solvent atomic centers. The method is applied to three solvation problems: the hydration of Li⁺ and F^? and the solvation effect on the interaction between NH₃ and HF. The results of the first two calculations indicate that the point charge model is capable of reliably predicting solvation energies. The calculations for H₃N···HF demonstrate that the hydration has a profound effect on the potential energy surface favoring a proton transfer structure H₃NH⁺···F^?.     

An electrochemical study of energy-dependent potassium accumulation in E. coli Part 15. K+-uptaking activity on glycolysing Trk mutants

The characteristics of two-step K⁺ uptake and H⁺-K⁺ exchange, the K⁺ dependence of growth and the K⁺ gradient between the cytoplasm and the medium in glycolysing Escherichia coli Trk mutants with defects in the TrkH and the TrkG systems, forming a K⁺-uptaking TrkA activity, were studied.It is concluded that K⁺ uptake with a low affinity and DCCD-sensitive H⁺-K⁺ exchange with a fixed ratio of 2H⁺ to K⁺ in glycolysing bacteria take place through the TrkH system formed by the TrkA, TrkE and TrkH gene products. This system can interact directly with F₀F₁ and form a united supercomplex functioning as a H⁺-K⁺ pump. A system of K⁺ uptake with a low affinity involving in H⁺-K⁺ exchange with variable stoichiometry contains at least the TrkA protein, which can interact with the separate F₀.     

“Best Match” Model and Effect of Na+/H+ Exchange on Anion Attachment to Peptides and Stability of Formed Adducts in Negative Ion Electrospray Mass Spectrometry

The “Best Match” model has been extended to account for the role that Na⁺/H⁺ exchange plays on anion attachment in negative ion electrospray. Without any Na⁺/H⁺ exchange on (Glu) fibrinopeptide B, the higher basicity anions F^? and CH₃COO^? can hardly form observable adducts; however, after multiple Na⁺/H⁺ exchanges, adduct formation is enabled. Moreover, dissociation pathways of CF₃COO^? adducts with singly deprotonated peptides that have undergone 0 to 3 Na⁺/H⁺ exchanges exhibit a shift in CID product ions from losing predominately CF₃COOH (case of 0 Na⁺/H⁺ exchanges) to losing predominately CF₃COO^? (case of 3 Na⁺/H⁺ exchanges). These phenomena can be rationalized by considering that Na⁺ cations exchange at, and serve to “block”, the most acidic sites, thereby forcing implicated anions to attach to lower acidity protons. In addition to forming ion pairs with carboxylate groups, Na⁺ also participates in formation of tri-atomic ions of the form ANaA^? during adduct dissociation. The fact that low gas-phase basicity (GB) anions preferentially form ANaA^? species, even though high GB anions form more stable tri-atomic species, indicates that the monatomic ions were not in close contact in the initial adduct. The propensity for formation of stable anionic adducts is dependent on the degree of matching between anion GBs and GB_app of deprotonated sites on the peptide. The GB_app is raised dramatically as the charge state of the peptide increases via a through-space effect. The presence of Na⁺ on carboxylate sites substantially decreases the GB_app by neutralizing these sites, while slightly increasing the intrinsic GBs by an inductive effect.

SCF-CI studies of correlation effects on hydrogen bonding and ion hydration

Previous single-determinant Hartree-Fock studies on the equilibrium structures and stabilities of H₂ O, H₃ O⁺ as well as of the monohydrated ionic systems Li⁺ · H₂O, F^? · H₂O and the hydrogen bonded water dimer, H₂ O · HOH, are extended by large scale configuration interaction calculations including all the possible single and double excitations arising from the canonical set of Hartree-Fock molecular orbitals. The correlation energy effects on the equilibrium geometrical parameters of the systems under consideration are found to be quite small. The contributions of the correlation energy to the total binding energies of the weakly interacting composed systems are obtained to be of the order of 1 kcal/mole, leading to a considerable increase of the hydrogen bond strength in F^? · H₂O and H₂O · HOH and to a small decrease of the binding energy in Li⁺ · H₂ O. The observed strengthening of the hydrogen bonding interaction due to correlation is shown to be partly compensated by the change in the vibrational zero-point energy of the composed systems compared to the non-interacting subsystems. Approximate force constants corresponding to the intersystem vibrations in Li⁺ · H₂O, F^? · H₂ O, and H₂O · HOH are deduced from the calculated potential curve data on the SCF and the CI level of accuracy.     

Anion Receptors Containing ‐NH Binding Sites: Hydrogen‐Bond Formation or Neat Proton Transfer?

When the amide‐containing receptor 1 ⁺ is in a solution of dimethyl sulfoxide (DMSO) in the presence of basic anions (CH₃COO^?, F^?, H₂PO₄^?), it undergoes deprotonation of the ‐NH fragment to give the corresponding zwitterion, which can be isolated as a crystalline solid. In the presence of less basic anions (Cl^?, Br^?, NO₃^?), 1 ⁺ establishes true hydrogen‐bond interactions of decreasing intensity. The less acidic receptor 2 ⁺ undergoes neat proton transfer with only the more basic anions CH₃COO^? and F^?, and establishes hydrogen‐bond interactions with H₂PO₄^?. An empirical criterion for discerning neutralisation and hydrogen bonding, based on UV/Vis and ¹H NMR spectra, is proposed.     

Liquid-membrane type 8-quinolinol-5-sulfonate ion selective electrode and its application to potentiometric titration

A nitrobenzene extract of the ion-pair consisting of 8-quinolinol-5-sulfonate (Hqs^?) and the cation of zephiramine (Z⁺Cl^?, benzyldimethyltetradecylammonium chloride) was used as an ion-exchanging liquid membrane for the electrode responding to Hqs^? ion. The potential response showed the Nernstian slope with the Hqs^? activities varying from 10^?2 to 10^?4.5 mol l^?1. The break points in the potential-pH plot with the constant analytical concentration of H₂qs correspond to the values of the negative logarithm of the acid dissociation constant of H₂qs. The present electrode was successfully applied to the potentiometric titration of copper(II) with H₂qs.     

Structure and Composition of the 200 K‐Superconducting Phase of H2S at Ultrahigh Pressure: The Perovskite (SH−)(H3S+)

At ultrahigh pressure (>110 GPa), H₂S is converted into a metallic phase that becomes superconducting with a record T_c of approximately 200 K. It has been proposed that the superconducting phase is body‐centered cubic H₃S (Im m, a=3.089 Å) resulting from the decomposition reaction 3 H₂S→2 H₃S+S. The analogy between H₂S and H₂O led us to a very different conclusion. The well‐known dissociation of water into H₃O⁺ and OH^? increases by orders of magnitude under pressure. H₂S is anticipated to behave similarly under pressure, with the dissociation process 2 H₂S→H₃S⁺+SH^? leading to the perovskite structure (SH^?)(H₃S⁺). This phase consists of corner‐sharing SH₆ octahedra with SH^? ions at each A site (the centers of the S₈ cubes). DFT calculations show that the perovskite (SH^?)(H₃S⁺) is thermodynamically more stable than the Im m structure of H₃S, and suggest that the A site hydrogen atoms are most likely fluxional even at T_c .