Steady-state ion transport by nonactin and trinactin

The fluxes of K⁺ and NH₄⁺ carried by nonactin and trinactin across thin lipid membranes have been measured as functions of ion activity, electric potential and time. In agreement with the predictions of a version of the carrier model in common use, the shape of the initial current-voltage relation is independent of the activity of the electrolyte, a_i while the ratio of the initial conductance, G₀, to the steady-state conductance, G_∞, increases according to G₀/G_∞ = const₁ + const₂ × a_i. For trinactin the data presented allow the estimation of the rate constants of the carrier process (in the limit of zero potential) in a manner which does not assume any particular variation with potential for the constants. Using empirically determined functions of potential, a complete set of values is also available for nonactin. The curve fitting which is necessary is described in the following paper. The data presently available for valinomycin are sufficient neither to test the model nor to determine a complete set of constants.     

Alkali ion transport through lipid bilayer membranes mediated by enniatin A and B and beauvericin

Summary Stationary conductance measurements with lipid bilayer membranes in the presence of enniatin A and B and beauvericin were performed. For comparison, some valinomycin systems were investigated. It was found that the conductance in the case of enniatin A and B is caused by a carrier ion complex with a 11 stoichiometry, whereas for beauvericin, a 31 carrier ion complex has to be assumed to explain the dependence of the conductance on carrier and ion concentration in the aqueous phase. The current-voltage curves measured with dioleoyl phosphatidylcholine membranes show a superlinear behavior for the three carriers in the presence of potassium. On the other hand, supralinear current-voltage curves were observed with membranes from different monoglycerides, except for beauvericin. The results obtained with enniatin A and B are in a satisfactory agreement with an earlier proposed carrier model assuming a complexation between carrier and ion at the membrane water interface.The discrimination between potassium and sodium ions is much smaller for the enniatins than for valinomycin. This smaller selectivity as well as the fact that potassium ions cause the highest conductance with lipid bilayer membranes may be due to the smaller size of the cyclic enniatin molecules, which contain 6 residues in the ringvs. 12 in the case of valinomycin. Charge-pulse relaxation studies were performed with enniatin A and B, beauvericin, and valinomycin. For monoolein membranes only in the case of valinomycin, all three relaxations predicted by the model could be resolved. In the case of the probably more fluid membranes from monolinolein (^{9, 12}-C_{18: 2}) and monolinolenin (^{9, 12, 15}-C_{18: 3}) for all carrier systems except for beauvericin, three relaxations were observed.The association rate constantk _R , the dissociation rate constantk _D , and the two translocation rate constantsk _MS andk _s for complexed and free carrier, respectively, could be calculated from the relaxation data. The carrier concentration in the aqueous phase had no influence on the rate constants in all cases, whereas a strong saturation of the association rate constantk _R with increasing ion concentration was found for the enniatins. Because of the saturation,k _R did not exceed a value of 4×10⁵ m ^–1 sec^–1 with 1m salt irrespective of carrier, ion, or membrane-forming lipid.A similar but less pronounced saturation behavior was also observed for the translocation rate constantk _S of the free carrier. The other two rate constants were independent of the ion concentration in the aqueous phase. In the case of the enniatins, the translocation rate constantk _MS was not independent from the kind of the transported ion. In the series K⁺, Rb⁺ and Cs⁺,k _MS increases about threefold. The turnover numbers for the carriers as calculated from the rate constants range between 10⁴ sec^–1 and 10⁵ sec^–1 and do not show a strong difference between the individual carriers. The conductance difference in the systems investigated here is therefore mainly caused by the partition coefficients, which are smaller for the enniatins than for valinomycin.     

Efficiency,Na+/K+ selectivity and temperature dependence of ion transport through lipid membranes by (221)C10-Cryptand,an ionizable mobile carrier

Summary The kinetics of Na⁺ and K⁺ transport across the membrane of large unilamellar vesicles (LUV) were determined at two pH's when transport was induced by (221)C₁₀-cryptand (diaza-1,10-decyl-5-pentaoxa-4,7,13,16,21-bicyclo [8.8.5.] tricosane) at various temperatures, and by nonactin at 25°C and (222)C₁₀-cryptand at 20 and 25°C. The rate of Na⁺ and K⁺ transport by (221)C₁₀ saturated with the cation and carrier concentrations. Transport was noncooperative and exhibited selectivity for Na⁺ with respect to K⁺. The apparent affinity of (221)C₁₀ for Na⁺ was higher and less pH-dependent than that for K⁺, and seven times higher than that of (222)C₁₀ for K⁺ ions (20.5vs. 1.7 kcal·mole^–). The efficiency of (221)C₁₀ transport of Na⁺ was pH-and carrier concentration-dependent, and was similar to that of nonactin; its activation energy was similar to that for (222)C₁₀ transport of K⁺ (35.5 and 29.7 kcal · mole^–1, respectively). The reaction orders in cationn(S) and in carrierm(M), respectively, increased and decreased as the temperature rose, and were both independent of carrier or cation concentrations; in most cases they varied slightly with the pH.n(S) varied with the cation at pH 8.7 and with the carrier for Na⁺ transport only, whilem(M) always depended on the type of cation and carrier. Results are discussed in terms of the structural, physico-chemical and electrical characteristics of carriers and complexes.     

Nonactin,monactin, dinactin,trinactin, and tetranactin. A Raman spectroscopic study

Raman spectra are reported for crystalline nonactin, monactin, dinactin, trinactin, and tetranactin and their solutions in CCl₄, CHCl₃, CH₃OH, and 4:1 (v/v) CH₃OH:CHCl₃. The macrotetrolide nactins selectively bind a wide variety of cations, and are important model compounds for the study of ion complexation. The conformations of nonactin, monactin, and dinactin in solution are similar. Their conformations are found to be sufficiently open to permit the ester carbonyl groups to form hydrogen bonds with CH₃OH; this gives rise to characteristic changes in the vibration frequencies associated with the ester groups. Nonactin, which is the least soluble of the nactins in CH₃OH, is also the least effective at forming hydrogen bonds with CH₃OH. The greater ability of the higher nactins to form hydrogen bonds with CH₃OH may be due to the increased inductive effect of ethyl over methyl side chains, which may increase the dipole moment of the ester carbonyl groups. Spectra of crystalline nonactin, monactin, and tetranactin are fairly similar, while the spectra of dinactin and trinactin comprise a second, distinct family. This is consistent with X-ray crystallographic studies, which show that nonactin and tetranactin form monoclinic crystals, while trinactin is triclinic.     

Kinetic analysis of carrier-mediated ion transport by the charge-pulse technique

Summary The charge-pulse technique has been used previously for the study of quasistationary processes in membranes which required only a moderate time resolution. It is shown here that a time resolution of about 400 nsec may be achieved with this technique and that it may be applied to the kinetic analysis of carrier-mediated ion transport. By this method we have studied the transport of alkali ions through optically black monoolein membranes in the presence of the ion carrier valinomycin. All three relaxation processes that are predicted by theory have been resolved. From the relaxation times and the relaxation amplitudes the rate constants for the association (k _R ) and the dissociation (k _D ) of the ioncarrier complex, as well as the translocation rate constants of the complex (k _MS ) and the free carrier (k _S ) could be obtained. For 1m Rb⁺ at 25° C the values arek _R =3×10⁵ m ^–1 sec^–1,k _D =2×10⁵ sec^–1,k _MS =3×10⁵ sec^–1,k _S =4×10⁴ sec^–1. The activation energies of the single rate constants which have been estimated from experiments at two different temperatures range between 50 and 90 kJ/mol.     

Factors affecting the relative magnitudes of the ouabain-sensitive and the ouabian-insensitive fluxes of thallium ion in erythrocytes

A maximal rate of the ouabain-sensitive ²⁰⁴Tl influx in human erythrocytes can be attained at trace concentrations of Tl⁺ in Mg²⁺ isotonic media free of K⁺ and Na⁺. The maximal influx of Tl⁺ from isotonic Mg(NO₃)₂ at 20°C and pH 7.4 was $\text{0.45}\text{mM}\text{· 1}{}^{\mathrm{?1}}\text{· h}{}^{\mathrm{?1}}$ with a $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 0.025 mM. In contrast to the active influx of Tl⁺, the passive Tl⁺ fluxes were neither saturated nor influenced by external cations in the range of concentrations of Tl⁺ and K⁺ studied. The rate constants of Tl⁺ passive fluxes in human and cat erythrocytes can be related to pH by the equation $\text{log}\text{k}{}_{\mathrm{<mtext>in(out)</mtext>}}\text{= –A + B ·}\text{pH}$, where $\text{A}$ and $\text{B}$ are empirical constants for particular conditions. The apparent activation energy was 16 and 11 kcal/mol in sulphate and nitrate media, respectively. Tl⁺ and the alkali metal cations seem to overcome a common barrier in the erythrocyte membrane. Nevertheless, the rate of the passive penetration of Tl⁺ is about two orders of magnitude faster than those of K⁺ or Rb⁺. An extra non-Coulombic interaction between Tl⁺ and membrane ligands appears to be involved providing an accumulation of Tl⁺ somewhere in the vicinity of the membrane barrier and increasing the diffusion fluxes of Tl⁺ in both directions.     

Effects of Tl<Superscript>+</Superscript> on ion permeability,membrane potential and respiration of isolated rat liver mitochondria

It is known that permeability of the inner mitochondrial membrane is low to most univalent cations (K⁺, Na⁺, H⁺) but high to Tl⁺. Swelling, state 4, state 3, and 2,4-dinitrophenol (DNP)-stimulated respiration as well as the membrane potential (ΔΨ_mito) of rat liver mitochondria were studied in media containing 0–75 mM TlNO₃ either with 250 mM sucrose or with 125 mM nitrate salts of other monovalent cations (KNO₃, or NaNO₃, or NH₄NO₃). Tl⁺ increased permeability of the inner mitochondrial membrane to K⁺, Na⁺, and H⁺, that was manifested as stimulation of the swelling of nonenergized and energized mitochondria as well as via an increase of state 4 and dissipation of ΔΨ_mito. These effects of Tl⁺ increased in the order of sucrose <K⁺ <Na⁺ ≤ NH₄⁺. They were stimulated by inorganic phosphate and decreased by ADP, Mg²⁺, and cyclosporine A. Contraction of energized mitochondria, swollen in the nitrate media, was markedly inhibited by quinine. It suggests participation of the mitochondrial K⁺/H⁺ exchanger in extruding of Tl⁺-induced excess of univalent cations from the mitochondrial matrix. It is discussed that Tl⁺ (like Cd²⁺ and other heavy metals) increases the ion permeability of the inner membrane of mitochondria regardless of their energization and stimulates the mitochondrial permeability transition pore in low conductance state. The observed decrease of state 3 and DNP-stimulated respiration in the nitrate media resulted from the mitochondrial swelling rather than from an inhibition of respiratory enzymes as is the case with the bivalent heavy metals.     

Gating Properties of Inward-Rectifier Potassium Channels: Effects of Permeant Ions

Two inward-rectifier K⁺ channels, ROMK2 (Kir1.1b) and IRK1 (Kir2.1), were expressed in Xenopus oocytes and their gating properties were studied in cell-attached membrane patches. The gating properties depended strongly on the ion being conducted (K⁺, NH₄ ⁺, Rb⁺, or Tl⁺), suggesting tight coupling between permeation and gating. Mean open times were strongly dependent on the nature of the conducted ion. For ROMK2 the order from the longest to the shortest times was K⁺ > Rb⁺ > Tl⁺ > NH₄ ⁺. For IRK1 the sequence was K⁺ > NH₄ ⁺ > Tl⁺. In both cases the open times decreased monotonically as the membrane voltage was hyperpolarized. Both the absolute values and the voltage dependence of closed times were dependent on the conducted species. ROMK2 showed a single closed state whose mean lifetimes were biphasic functions of voltage. The maxima were at various voltages for different ions. IRK1 had at least two closed states whose lifetimes decreased monotonically with K⁺, increased monotonically with Tl⁺, and were relatively constant with NH₄ ⁺ as the conducted ion. We explain the ion-dependence of gating by assuming that the ions bind to a site within the permeation pathway, resulting in a stable, ion-dependent, closed state of the channel. The patterns of voltage-dependence of closed-state lifetimes, which are specific for different ions, can be explained by variations in the rate at which the bound ions leave the pore toward the inside or the outside of the cell. Received: 18 April 2001/Revised: 28 June 2001     

Selectivity of interaction of univalent cations with mammalian ribosomes studied by equilibrium dialysis in the presence of the K+ analogue, 204Tl+

The interaction of K⁺ with mammalian ribosomes was studied by equilibrium dialysis and compared with that of other univalent cations. The heavy K⁺ analogue, Tl⁺, binds more firmly than K⁺ to ribosomes and, unlike K⁺, has a practically useful isotope. With ²⁰⁴Tl⁺ as a marker of K⁺-selective binding the ribosome-cation interaction could be followed down to levels below 0.1 average Tl⁺-occupied site per ribosome. The Tl⁺/ribosome ratio varied with the free Tl⁺ concentration in a multiple way. At high Tl⁺ saturation Tl⁺ was easily displaced by Mg²⁺. With decreasing Tl⁺ saturation the competitive activity of Mg⁺⁺ was strikingly reduced, indicating that Tl⁺ and Mg⁺⁺ compete with different efficiency for different classes of sites.The experiments on univalent cations were performed at 1.5 mM Mg²⁺ under two complementary conditions: (1) Ribosomes were pretreated with 5 × 10^?2, 5 × 10^?3, and 5 × 10^?4 M LiNO₃, NaNO₃, KNO₃, and CsNO₃, and then equilibrated with different concentrations of ²⁰⁴TlNO₃ in the same buffers. (2) Ribosomes were pretreated with 10^?2, 10^?4, and 10^?6 M ²⁰⁴TlNO₃, and then equilibrated with different concentrations of LiNO₃, NaNO₃, KNO₃, and CsNO₃ (displacement experiments). At high Tl⁺ saturation Na⁺ and Li⁺ were about as active as K⁺ and Cs⁺ in competing with ²⁰⁴Tl⁺. With decreasing Tl⁺ saturation a differentiation occurred in favor of K⁺ and Cs⁺, with some preference for K⁺. It is concluded that ribosomes contain a limited number of sites with pronounced ion specificity. Of physiological cations K⁺ is most firmly bound to these sites.     

Movement of thallous ion across the ascites cell membrane

Summary The movement of thallous ion (Tl⁺ across the ascites cell membrane has been characterized. Analogous to previous findings for⁸⁶Rb⁺ (used as a tracer for K⁺),²⁰⁴Tl⁺-influx could be resolved into three components: a ouabain-inhibitable pump flux, a passive flux, and a furosemide- or NO ₃ ^– -sensitive exchange flux. Although Tl⁺ moved approximately nine times faster across the membrane than K⁺, the pump/leak ratio was equal for the two ions. This suggests that the pump- and leak-pathways share a common rate-limiting step. The exchange mechanism was shown to provide close coupling between the Tl⁺- and K⁺-gradients.     

Influence of membrane structure on ion transport through lipid bilayer membranes

Summary Charge-pulse relaxation studies with the positively charged PV-K⁺ complex (cyclo-(d-Val-l-Pro-l-Val-d-Pro)₃) and the negatively charged lipophilic ion dipicrylamine (DPA^–) have been performed in order to study the influence of structural properties on ion transport through lipid bilayer membranes. First, the thickness of monoolein membranes was varied over a wide range using differentn-alkanes and slovent-free membranes. The thickness (d) of the hydrocarbon core of these membranes varied between 4.9 and 2.5 nm. For both transport systems the partition coefficient was found to be rather insensitive to variations ind. The same was valid for the translocation rate constantk _MS of PV-K⁺, whereas a strong increase of the translocation rate constantk _i of DPA-with decreasingd was observed. In a further set of experimental conditions the structure of the lipids, such as number and position of the double bonds in the hydrocarbon chain and its chain length as well as the nature of the polar head group, was varied. The translocation constantk _MS of PV-K⁺ transport was found to be much more sensitive to these variations thank _i of DPA-.Much larger variations ink _i andk _MS were observed in membranes made from lipids with ether instead of ester linkages between glycerol backbone and hydrocarbon chain. The results are in qualitative agreement with the surface potentials of monolayers made from corresponding lipids. Increasing amounts of cholesterol in membranes of dioleoylphosphatidylcholine caused a strong decrease ofk _MS (PV-K⁺), whereask _i was found to be rather insensitive to this variation.In monoolein membranes cholesterol causes a decrease ofk _MS up to sixfold and a increase ofk _i up to eightfold. The partition coefficient of DPA^– was insensitive to cholesterol, whereas of PV-K⁺ was found to decrease about eightfold in these membranes. The influence of cholesterol onk _MS is discussed on the basis of viscosity changes in the membrane and the change ink _i of DPA^– and of PV-K⁺ on the basis of a possible change of the dipole potential of the membranes. The other sterols, epicholesterol and ergosterol cause no change in the kinetics of the two probes.The different influence of membrane properties like thickness, viscosity, and dipole potential on the two transport systems is discussed under the assumption that the adsorption planes of the two probes have different positions in a membrane. Possibly because of a larger hydrophobic interaction, the adsorption plane of PV-K⁺ is located more towards the hydrocarbon side and that of DPA^– more towards the aqueous side of the dipole layer.     

Ion complexation in nonactin,monactin, and dinactin: A Raman spectroscopic study

The ability of the macrotetrolide nactins to complex selectivity with a wide variety of cations makes these ionophorous antibiotics important model systems for the study of biologic ionic transport. We report a Raman spectroscopic investigation of the Na⁺, K⁺, Rb⁺, Cs⁺, Tl⁺, NH₄⁺, NH₃OH⁺, C(NH₂)₃⁺, and Ba⁺⁺ complexes of nonactin, monactin, and dinactin in 4:1 (v/v) CH₃OH/CHCl₃ and in the solid state. The nactins display characteristic spectral changes upon complexation, some of which are specific for a given cation. In the K⁺, Rb⁺, Cs⁺, NH₃OH⁺, and C(NH₂)₃⁺ complexes, which are apparently isosteric, the ester carbonyl stretch frequency is found to be linearly proportional to the cation–carbonyl electrostatic interaction energy, as calculated from a simplified model. Deviations for the Na⁺, NH₄⁺, Tl⁺, and Ba⁺⁺ complexes are interpreted as arising from additional nonelectrostatic interactions. Additional information is obtained from other spectral regions and from measurements of depolarization ratios. Spectra of the nactin complexes differ from each other more in the solid state than in solution, reflecting the effects of crystalline contact forces.     

A laser-T-jump study of the adsorption of dipolar molecules to planar lipid membranes

The adsorption of the herbicide 2,4-dichlorophenoxyacetic acid (2,4-D) as well as of other dipolar molecules to the interface of artificial lipid membranes gives rise to a change of the dipole potential between the membrane interior and water. As a consequence of the adsorption of the neutral species, the conductance of planar membranes, observed in the presence of the macrocyclic ion carriers nonactin or valinomycin, may change by many orders of magnitude. Using this effect in combination with a laser-T-jump technique, the kinetics of the adsorption process were measured and were interpreted on the basis of a Langmuir-isotherm. A partition coefficient (at small concentrations) of _HA =4.7·10^–4 cm, a rate constant of desorption k _HA100 s^-1 and a maximum surface density N _D=7.7·10¹³/cm² were found. The concentration at half saturation is K _HA=2.7·10^-4 M.Using these values the membrane conductance induced by the ion carrier nonactin and the shape of the current-voltage relationship as a function of the ligand concentration in water was analyzed. A maxiumum dipole potential of V _D ^max =-239 m V and a contribution of b=3.1·10^-15V cm² per single adsorbed 2,4-D molecule was found. 74% of the dipole potential acts on the inner membrane barrier separating the two interfacial adsorption planes of nonactin. The remainder (26%) favours interfacial complex formation between nonactin and K⁺ from the aqueous phase. The data hold for membranes formed from dioleoyllecithin in n-decane.     

Electrogenic and diffusive components of the membrane ofHydrodictyon africanum

Summary In cells of the freshwater algaHydrodictyon africanum, in solutions where [K⁺]₀=0.1mm and pH₀>7.0, the membrane in the light is hyperpolarized. The membrane potential difference {ie179-1} has values from –180 to –275 mV, more negative than any ion diffusion potential difference, and is predominantly a function of pH₀, and independent of [K⁺]₀. The hyperpolarization of the membrane appears to arise from an electrogenic efflux of H⁺, estimated from voltage-clamp data to be about 8 nmol m^–2 sec^–1 when pH₀=8.5. In the light the membrane conductanceg _m is about 0.084 S m^–2. At light-off, {ie179-2} becomes less negative, with a halftime for change of 15 to 30 sec andg _m decreases by about 0.052 S m^–2. After dark periods of up to 300 sec, {ie179-3} is largely independent of pH₀ for values greater than 6.0 and usually behaves as a combined K⁺ and Na⁺ diffusion potential with permeability ratioP _Na/P _K=0.05 to 0.2. The membrane potassium conductanceg _K has either a low value of 2–6×10^–2 Sm^–2, or a high value of up to 18×10^–2 S m^–2 depending on [K⁺]₀, the transition from low to high values occurring when {ie179-4} moves over a threshold value that is more negative than {ie179-5}, the electrochemical equilibrium potential for K⁺. The time for half-change of the transition is about 30 sec. The results are consistent with a model of the membrane in which the pump electromotive force and conductance are in parallel with diffusive electromotive forces and conductances. When the pump is operating its properties determine membrane properties, and when it is inoperative, or running at a diminished rate, the membrane properties are determined more by the diffusive pathways. Changes in both pump rate andg _K can account for a variety of characteristic changes in membrane PD and conductance occurring in response to ligh-dark changes, changes in light intensity, pasage of externally applied electric current across the membrane and changes in ionic constituents of the external medium.     

Conformation of tetranactin in solution.

The conformation of tetranactin, an ionophore, in chloroform was investigated by infrared and Raman spectra and by proton and ¹³C magnetic resonances. The infrared spectra show that the structure of its K⁺ complex in the solution is quite similar to that in crystals. The proton spin–spin coupling constants are explained well by assuming that the crystalline structure is retained in solution. The spin–lattice relaxation times of the ¹³C nuclei of the K⁺ complex indicate that its framework is rigid. The correlation time of the overall reorientation of the molecule was calculated to be 9 X 10^?11 sec. On the other hand, the conformation of the complexed form in chloroform differs from that in crystals. Despite the geometrical nonequivalence of the four subunits in the crystalline state, the nuclear magnetic resonance spectra show their magnetic equivalence in the solution. The proton spin–spin coupling constants have values that are averaged by rapid internal rotation. The spin–lattice relaxation times of the ¹³C nuclei in its framework are unexplained by the overall reorientation of the molecule, and reveal the existence of internal motion in the framework. The rate of the local motion of the framework is between 10²–10¹⁰ sec^?1. By comparison of the infrared spectra, it can be said that the mean conformation of the fluctuated framework of the uncomplexed tetranactin in the solution is similar to that of nonactin in the crystalline form, which has an S₄ symmetry axis through the center of the macrocyclic ring.     

Complexation of lithium(I), sodium(I), silver(I) and thallium(I) by 4,7,13,16-tetraoxa-1,10-diazabicyclo[8.5.5]eicosane and 4, 7, 13-trioxa-1,10-diazabicyclo[8.5.5]eicosane in trimethyl phosphate. A potentiometric titration and Li and Na nuclear magnetic resonance study

Complexation of M⁺=Li⁺, Na⁺, Ag⁺ and TI⁺ by the cryptands 4, 7, 13, 18-tetraoxa-l, 10-diazabicyclo[8.5.5]eicosane (C211) and 4,7,13-trioxa-1,10-diazabicyclo[8.5.5]eicosane (C21C₅) to form the cryptates [M.C211]⁺ and [M.C21C₅]⁺ has been studied in trimethyl phosphate by potentiometric titration and ⁷Li and ²³Na NMR spectroscopy. For [M.C211]⁺ the logarithm of the apparent stability constants, log K (dm³ mol^-1)=6.98±0.05, 5.38±0.05, 9.82±0.02 and 3.95±0.02 for M⁺ =Li⁺, Na⁺, Ag⁺ and TI⁺, respectively; and for [M.C21C₅]⁺ log K (dm³ mol^-1)=2.40±0.10, 1.90±0.05, 6.04±0.02 and 2.42±0.10 for M⁺=Li⁺, Na⁺, Ag⁺ and Tl⁺, respectively. The decomplexation kinetic parameters for [Na.C211]⁺ are: k_d (298.2 K)=6.924±0.50 s^-l, ΔH_d≠=62.2±0.9 kJ mol^-1, and ΔS_d≠= -20.3±2.7 J K^-1 mol^-1; and those for [Li.C21C₅]⁺ are: k_d (298.2 K)=23.3±0.4 s^-1, ΔH_d≠ =61.2±1.1 kJ mol^-1, and ΔS_d≠= -13.6±3.6 J K^-1 mol^-1. Metal ion exchange on [Li.C211]⁺ is in the very slow extreme of the NMR timescale up to 390 K and k_d « 4 s^-1 at 298.2 K, while in contrast exchange on [Na.C21C₅]⁺ is in the fast extreme of the NMR timescale at 298.2 K (k_d≈ 10⁴ s^-1). These data are compared with those obtained in other solvents.     

Inorganic ion compositions in the Ulvophyceae and the Rhodophyceae, with special reference to sulfuric acid ion accumulations

Cellular pH estimated from cell extract pH, and the ion compositions of major inorganic ions (Na⁺, NH₄⁺, K⁺, Mg²⁺, Ca²⁺, Cl^?, Br^?, NO₃^?, S0₄²‐) were studied by ion chromatography in 15 species of 4 orders (Cladophorales, Codiales, Siphonocladales and Ulvales) of Ulvophyceae and 49 species of 8 orders (Bangiales, Ceramiales, Corallinales, Cryptonemiales, Gelidiales, Gigartinales, Nemaliales and Rhodymeniales) of Rhodophyceae. Among the Rhodophyceae, relatively low intracellular pH (approximately 2.0 within cells) and high concentration of S0₄^2‐ was demonstrated in Plocamium telfairiae(Harvey) Harvey. Furthermore, five species of Hypnea Lamouroux were shown to contain high concentrations of S0₄^2‐ balanced by relatively high concentrations of Na⁺. Among the Ulvophyceae, Codium cylindricum Holmes and Ulva pertusa Kjellman contained high concentrations of S0₄^2‐ balanced by relatively high concentrations of Mg²⁺.     

A differential molecualr topography of the Pr and Pfr forms of native oat phytochrome as probed by fluoresence quenching

Tryptophan (Trp) surface topography of the red- and far-red-absorbing forms of phytochrome (Pr, Pfr) ofAvena sativa L. has been investigated by analyzing quenching of the two components of Trp fluorescence decay, in order to understand the differences in the two forms at the molecular level. Stern-Volmer kinetic analysis of the quenching data for two cationic surface quenchers, Cs⁺ and Tl⁺, showed strong quenching of the short component of the Pr fluorescence (Stern-Volmer constants,K _sv , 27.2 and 21.4 M⁻¹, respectively) relative to that of Pfr fluorescenceK _sv , 10.4 and 12.3 M⁻¹, respectively). The long component of the Trp fluorescence was quenched differentially by Cs⁺ and Tl⁺, withK _sv of 9.0 and 19.8 M⁻¹, respectively, for the Pr fluorescence andK _sv of 13.7 and 8.7 M⁻¹, respectively, for the Pfr fluorescence. The results indicate that the phytochrome Trp residues with short fluorescence lifetime are more accessible to the cationic surface quenchers than those with long fluorescence lifetime. The data, taken together with our earlier study (Singh et al. 1988, Biochim, Biophys. Acta936, 395–405), indicate that most, if not all the ten Trp residues of phytochrome, are fluorescent and exist in distinct groups differing in their topography and microenvironment, and the peptide segment containing Trp-774 and Trp-778 within the 55-kilodalton C-terminal domain of phytochrome also undergoes a subtle alteration in its surface topography during Pr→Pfr phototransformation. This paper is dedicated to Professor Hans Mohr in commemoration of his 60th birthday     

Influence of Tl+ activator ions on the luminescence characteristics of KCl0.5Br0.5:Eu2+ powder phosphors

Photoluminescence (PL) of thallium co‐doped with KCl_0.5Br_0.5:Eu²⁺ powder phosphors display emission bands at 320 and 370 nm attributable to centres involving Tl⁺ ions in addition to characteristic Eu²⁺ emission around 420 nm. Additional PL excitation and emission bandS observed around 260 and 380 nm, respectively, were observed in the double‐doped KCl_0.5Br_0.5:Eu²⁺, Tl⁺ powder phosphors and are attributed to complex centres involving Tl⁺ and Eu²⁺ ions. The enhancement observed in the intensity of Eu²⁺ emission around 420 nm with the addition of TlBr in KCl_0.5Br_0.5:Eu²⁺ powder phosphors is attributed to the energy transfer from Tl⁺ → Eu²⁺ ions. Photostimulated luminescence (PSL) studies of γ‐irradiated KCl_0.5Br_0.5:Eu²⁺, Tl⁺ mixed phosphors are reported and a tentative PSL mechanism in the phosphors has been suggested. Copyright © 2009 John Wiley & Sons, Ltd.     

Specific potassium ion interactions facilitate homocysteine binding to betaine‐homocysteine S‐methyltransferase

Betaine‐homocysteine S‐methyltransferase (BHMT) is a zinc‐dependent methyltransferase that uses betaine as the methyl donor for the remethylation of homocysteine to form methionine. This reaction supports S‐adenosylmethionine biosynthesis, which is required for hundreds of methylation reactions in humans. Herein we report that BHMT is activated by potassium ions with an apparent K_M for K⁺ of about 100 µM. The presence of potassium ions lowers the apparent K_M of the enzyme for homocysteine, but it does not affect the apparent K_M for betaine or the apparent k_cat for either substrate. We employed molecular dynamics (MD) simulations to theoretically predict and protein crystallography to experimentally localize the binding site(s) for potassium ion(s). Simulations predicted that K⁺ ion would interact with residues Asp26 and/or Glu159. Our crystal structure of BHMT bound to homocysteine confirms these sites of interaction and reveals further contacts between K⁺ ion and BHMT residues Gly27, Gln72, Gln247, and Gly298. The potassium binding residues in BHMT partially overlap with the previously identified DGG (Asp26‐Gly27‐Gly28) fingerprint in the Pfam 02574 group of methyltransferases. Subsequent biochemical characterization of several site‐specific BHMT mutants confirmed the results obtained by the MD simulations and crystallographic data. Together, the data herein indicate that the role of potassium ions in BHMT is structural and that potassium ion facilitates the specific binding of homocysteine to the active site of the enzyme. Proteins 2014; 82:2552–2564. © 2014 Wiley Periodicals, Inc.