Membrane phosphate headgroups' modulation of permeation of alkaline cations in gramicidin channels.

The function of membrane proteins is modulated by lipid bilayers. The permeation of ions in gramicidin A channels (gA) is markedly distinct in monoglyceride and phospholipid membranes. It was previously demonstrated that membrane phosphate headgroups accelerate the rate of proton transfer in gA. However, the permeation of alkalines in gA channels is considerably slower in phospholipid than in monoglyceride membranes. In this study, gA channels were reconstituted in various membranes of ceramides, monoglycerides, phospholipids, or sphingolipids. It is demonstrated that single channel conductances to alkalines are similar among bilayers consisting of phospholipids and sphingolipids, and ceramides and monoglycerides. The presence of phosphate headgroups in membranes (and not the double acyl chains in lipids) attenuates alkaline permeation and enhances the proton transfer permeation in gA channels. In ceramide membranes in low ionic strength (<250 mM) solutions, gA channels become dysfunctional. The experimental results are discussed in regard to membrane/solution and membrane/protein interfaces.

Enhancement of proton transfer in ion channels by membrane phosphate headgroups.

The transfer of protons (H+) in gramicidin (gA) channels is markedly distinct in monoglyceride and phospholipid membranes. In this study, the molecular groups that account for those differences were investigated using a new methodology. The rates of H+ transfer were measured in single gA channels reconstituted in membranes made of plain ceramides or sphingomyelins and compared to those in monoglyceride and phospholipid bilayers. Single-channel conductances to protons (gH) were significantly larger in sphingomyelin than in ceramide membranes. A novel and unsuspected finding was that H+ transfer was heavily attenuated or completely blocked in ceramide (but not in sphingomyelin) membranes in low-ionic-strength solutions. It is reasoned that H-bond dynamics at low ionic strengths between membrane ceramides and gA makes channels dysfunctional. The rate of H+ transfer in gA channels in ceramide membranes is significantly higher than that in monoglyceride bilayers. This suggests that solvation of the hydrophobic surface of gA channels by two acyl chains in ceramides stabilizes the gA channels and the water wire inside the pore, leading to an enhancement of H+ transfer in relation to that occurring in monoglyceride membranes. gH values in gA channels are similar in ceramide and monoglyceride bilayers and in sphingomyelin and phospholipid membranes. It is concluded that phospho headgroups in membranes have significant effects on the rate of H+ transfer at the membrane gA channel/solution interfaces, enhancing the entry and exit rates of protons in channels.

Proton transfer in water wires in proteins: modulation by local constraint and polarity in gramicidin a channels.

The transfer of protons in membrane proteins is an essential phenomenon in biology. However, the basic rules by which H(+) transfer occurs in water wires inside proteins are not well characterized. In particular, the effects of specific atoms and small groups of atoms on the rate of H(+) transfer in water wires are not known. In this study, new covalently linked gramicidin-A (gA) peptides were synthesized, and the effects of specific atoms and peptide constraints on the rate of H(+) transfer were measured in single molecules. The N-termini of two gA peptides were linked to various molecules: S,S-cyclopentane diacid, R,R-cyclopentane diacid, and succinic acid. Single-channel proton conductances (g(H)) were measured at various proton concentrations ([H(+)]) and compared to previous measurements obtained in the S,S- and R,R-dioxolane-linked as well as in native gA channels. Replacing the S,S-dioxolane by an S,S-cyclopentane had no effects on the g(H)-[H(+)] relationships, suggesting that the constrained and continuous transition between the two gA peptides via these S,S linkers is ultimately responsible for the two- to fourfold increase in g(H) relative to native gA channels. It is likely that constraining a continuous transition between the two gA peptides enhances the rate of H(+) transfer in water wires by decreasing the number of water wire configurations that do not transfer H(+) at higher rates as in native gA channels (a decrease in the activation entropy of the system). On the other hand, g(H) values in the R,R-cyclopentane are considerably larger than those in R,R-dioxolane-linked gA channels. One explanation would be that the electrostatic interactions between the oxygens in the dioxolane and adjacent carbonyls in the R,R-dioxolane-linked gA channel attenuate the rate of H(+) transfer in the middle of the pore. Interestingly, g(H)-[H(+)] relationships in the R,R-cyclopentane-linked gA channel are quite similar to those in native gA channels. g(H) values in succinyl-linked gA channels display a wide distribution of values that is well represented by a bigaussian. The larger peaks of these distributions are similar to g(H) values measured in native gA channel. This observation is also consistent with the notion that constraining the transition between the two beta-helical gA peptides enhances the rate of H(+) transfer in water wires by decreasing the activation entropy of the system.

Proton transfer in gramicidin water wires in phospholipid bilayers: attenuation by phosphoethanolamine.

The transfer of protons in water wires was studied in native gramicidin A (gA), and in the SS- and RR-diastereoisomers of dioxolane-linked gA channels (SS and RR channels). These peptides were incorporated into membranes comprised of distinct combinations of phospholipid headgroups and acyl chains. Quantitative relationships between single channel conductances to H+ (g(H)) and [H+] were determined in distinct phospholipid membranes, and are in remarkable contrast with results previously obtained in monoglyceride membranes. In particular: 1), g(H)-[H+] relationships for the various gA channels in distinct phospholipid membranes are well fitted by single adsorption isotherms. A simple kinetic model assuming mono-occupancy of channels by protons fits said relationships. This does not occur with monoglyceride membranes. 2), Under nonsaturating [H+], g(H) is approximately 1 order of magnitude larger in phospholipid than in monoglyceride membranes. 3), Differences between rates of H+ transfer in various gA channels are still present but considerably attenuated in phospholipid relative to monoglyceride membranes. 4), Charged phospholipid headgroups affect g(H) via changes in [H+] at the membrane/solution interfaces. 5), Phosphoethanolamine groups caused a marked attenuation of g(H) relative to membranes with other phospholipid headgroups. This attenuation is voltage-dependent and tends to saturate H+ currents at voltages larger than 250 mV. This effect is likely to occur by limiting the access and exit of H+ in and out of the channel due to relatively strong oriented H-bonds between waters and phosphoethanolamine groups at channel interfaces. The differential effects of phospholipids on proton transfer could be reasoned by considering solvation effects of side chain residues of gramicidin channels by double acyl chains and by the presence of polar headgroups facilitating the entrance/exit of protons through the channel mouths.

Et tu, Grotthuss! and other unfinished stories.

This review article is divided into three sections. In Section 1, a short biographical note on Freiherr von Grotthuss is followed by a detailed summary of the main findings and ideas present in his 1806 paper. Attempts to place Grotthuss contribution in the context of the science done at his time were also made. In Section 2, the modern version of the Grotthuss mechanism is reviewed. The classical Grotthuss model has been recently questioned and new mechanisms and ideas regarding proton transfer are briefly discussed. The last section discusses the significance of a classical Grotthuss mechanism for proton transfer in water chains inside protein cavities. This has been an interesting new twist in the ongoing history of the Grotthuss mechanism. A summary and discussion of what was learned from probably the simplest currently available experimental models of proton transfer in water wires in semi-synthetic ion channels are critically presented. This review ends discussing some of the questions that need to be addressed in the near future.

The transfer of protons in water wires inside proteins.

The translocation of protons across membrane proteins is an essential phenomenon in biology. Only in recent years however, have we started to study in detail some of the basic features of proton transfer in water molecules inside proteins at the single molecule level. Due to their truly unique features, gramicidin-based ion channels have been used to probe proton transfer in both experimental and computational fronts. In this article, some of the new experimental findings on proton transfer in water molecules inside proteins will be reviewed. The results, their interpretations, and the perspectives toward the understanding of structure-function illations of proton transfer in proteins are discussed.

Kinetic isotope effects of proton transfer in aqueous and methanol containing solutions, and in gramicidin A channels.

The electrochemical conductivities of HCL and DCI were measured in: H(2)O and D(2)O; in methanol and fully deuterated methanol; and in water-methanol solutions. The single channel conductances to H(+) (g(H)) and D(+) (g(D)) in various gramicidin A (gA) ion channels incorporated in glycerylmonooleate planar bilayers were also measured. Kinetic isotope effects (KIE) were estimated from the ratio of conductivity measurements. In 1 and 5 M HCl aqueous solutions and in 1 M HCl+3.7 M methanol, the KIE ( approximately 1.35) is not different from values previously determined in dilute acid solutions. This suggests that the mobility of protons in those solutions is largely determined by proton transfer. In 10 M HCl, however, where the mobility of protons is likely to be determined by hydrodynamic diffusion, the measured KIE is considerably larger (1.47). Possible causes for this effect are discussed. The KIE of proton conductivities in 5 and 50 mM HCl in methanol and d-methanol is approximately 1.15. This is considerably smaller than the ratio between conductivities of 5 mM KCl in methanol and d-methanol (1.24). The KIE values (1.22-1.37) for g(H) in gA channels in 1 M HCl are significantly larger than for other monovalent cations and consistent with H(+) transfer. Methanol reduces g(H) in gA channels. The KIE of this effect is not different from the one measured in the absence of methanol. Possible mechanisms for the methanol-induced block of H(+) conductivities in solution and gA channels are discussed.

Theoretical study of the structure and dynamic fluctuations of dioxolane-linked gramicidin channels.

Gramicidin is a hydrophobic peptide that assembles as a head-to-head dimer in lipid membranes to form water-filled channels selective to small monovalent cations. Two diastereoisomeric forms, respectively SS and RR, of chemically modified channels in which a dioxolane ring links the formylated N-termini of two gramicidin monomers, were shown to form ion channels. To investigate the structural basis underlying experimentally measured differences in proton conductance in the RR and SS channels, we construct atomic-resolution models of dioxolane-linked gramicidin dimers by analogy with the native dimer. A parametric description of the linker compatible with the CHARMM force field used for the peptide is derived by fitting geometry, vibrational frequencies, and energy to the results of ab initio calculations. The linker region of the modified gramicidin dimers is subjected to an extensive conformational search using high-temperature simulated annealing, and free-energy surfaces underlying the structural fluctuations of the channel backbone at 298K are computed from molecular dynamics simulations. The overall secondary structure of the beta-helical gramicidin pore is retained in both linked channels. The SS channel is found in a single conformation resembling that of the native dimer, with its peptide bonds undergoing rapid librations with respect to the channel axis. By contrast, its RR counterpart is characterized by local backbone distortions in which the two peptide bonds flanking the linker are markedly tilted in order to satisfy the pitch of the helix. In these distorted structures, each of the two carbonyl groups points either in or out of the lumen. Flipping these two peptides in and out involves thermally activated transitions, which results in four distinct conformational states at equilibrium with one another on a nanosecond time scale. This work opens the way to detailed comparative studies of structure-function relationships in biological proton ducts.

Proton transfer in gramicidin channels is modulated by the thickness of monoglyceride bilayers.

The thickness of monoglyceride planar bilayers has significant effects on the transfer of protons in both native gramicidin A (gA) and in covalently linked SS- and RR-dioxolane-linked gA proteins. Planar bilayers with various thicknesses were formed from an appropriate combination of monoglyceride with various fatty acid lengths and solvent. Bilayer thicknesses ranged from 25 A (monoolein in squalene) to 54 A (monoeicosenoin in decane). Single-channel conductances to protons (g(H)) were measured in the concentration range of 10-5000 mM HCl. In native gA as well as in RR channels, the shape of the log(g(H))-log([H(+)]) relationships was nonlinear and remained basically unaltered in monoglyceride bilayers with various thicknesses. For both native gA and RR channels, g(H) values were systematically and significantly larger in thin than in thick bilayers. By contrast, the shape of the log(g(H))-log([H(+)]) relationships in the SS channel was linear (with a slope considerably smaller than 1) in thick (>37 A) bilayers. However, in thin (<37 A) bilayers these plots became nonlinear and g(H) values approached those obtained in native gA channels. The linearization of the log-log plots in the SS channel in thick bilayers is a consequence of a dramatic increase (instead of a decrease as in native gA and RR channels) of g(H) in these bilayers in [H(+)] <1 M. The gating characteristics of the various gA channels as a function of bilayer thickness followed the same pattern as described previously. It was noticed, however, that in the thickest monoglyceride bilayer used in this study, both the SS- and RR-dioxolane-linked channels opened in a mode of bursting activity instead of remaining in the open state as in thin bilayers. It is proposed that the thickness of monoglyceride bilayers modulates proton transfer in native gA channels by a combination of factors including the access resistances of channels to H(+), and fluctuations in both the structure of the lipid bilayer and in the distance between gA monomers. The differential effects of relatively thick monoglyceride bilayers on proton transfer in both dioxolane-linked gA channels must relate to distinct interactions between the bilayers and the SS and RR dioxolanes.

On the origin of closing flickers in gramicidin channels: a new hypothesis.

The submillisecond closing events (flickers) and the single channel conductances to protons (g(H)) were studied in native gramicidin A (gA) and in the SS and RR diastereoisomers of dioxolane-linked gA channels in planar bilayers. Bilayers were formed from glycerylmonooleate (GMO) in various solvents. In GMO/decane (thick) bilayers, the largest flicker frequency occurred in the SS channel (39 s(-1)), followed by the RR (4 s(-1)) and native gA channels (3 s(-1)). These frequencies were attenuated in GMO/squalene (thin) bilayers by 100-, 30-, and 70-fold in the SS, RR, and native gA channels, respectively. In thin bilayers, the average burst duration of native gA channels was 30-fold longer than in thick bilayers. The RR dioxolane-linked gA dimer "inactivated" in GMO/decane but not in squalene-containing bilayers. The mean closed time of flickers (approximately 0.12 ms) was essentially the same in various gA channels. In thin bilayers, g(H) values were larger by approximately 10% (SS), 30% (RR), and 20% (native gA) in relation to thick bilayers. It is concluded that flickers are not related to pre-dissociation or dissociation states of gA monomers, and do not seem to be caused by intrinsic conformational changes of channel proteins. It is proposed that flickers are caused by undulations of the bilayer that obliterate the openings of gA channels. Differences between flicker frequencies in various gA channels are likely to result from variations in channel geometries at the bilayer/channel interface. The smaller g(H) in thick bilayers suggests that the deformation of these bilayers around the gA channel creates a diffusional pathway next to the mouths of the channel that is longer and more restrictive than in thin GMO bilayers. A possible molecular interpretation for these effects is attempted.

Thermodynamic view of activation energies of proton transfer in various gramicidin A channels.

The temperature dependencies (range: 5-45 degrees C) of single-channel proton conductances (g(H)) in native gramicidin A (gA) and in two diastereoisomers (SS and RR) of the dioxolane-linked gA channels were measured in glycerylmonooleate/decane (GMO) and diphytanoylphosphatidylcholine/decane (DiPhPC) bilayers. Linear Arrhenius plots (ln (g(H)) versus K(-1)) were obtained for the native gA and RR channels in both types of bilayers, and for the SS channel in GMO bilayers only. The Arrhenius plot for proton transfer in the SS channel in DiPhPC bilayers had a break in linearity around 20 degrees C. This break seems to occur only when protons are the permeating cations in the SS channel. The activation energies (E(a)) for proton transfer in various gA channels (approximately 15 kJ/mol) are consistent with the rate-limiting step being in the channel and/or at the membrane-channel/solution interface, and not in bulk solution. E(a) values for proton transfer in gA channels are considerably smaller than for the permeation of nonproton currents in gA as well as in various other ion channels. The E(a) values for proton transfer in native gA channels are nearly the same in both GMO and DiPhPC bilayers. In contrast, for the dioxolane linked gA dimers, E(a) values were strongly modulated by the lipid environment. The Gibbs activation free energies (Delta G(#)(o)) for protons in various gA channels are within the range of 27-29 kJ/mol in GMO bilayers and of 20-22 kJ/mol in DiPhPC bilayers. The largest difference between Delta G(#)(o) for proton currents occurs between native gA (or SS channels) and the RR channel. In general, the activation entropy (Delta S) is mostly responsible for the differences between g(H) values in various gA channels, and also in distinct bilayers. However, significant differences between the activation enthalpies (Delta H(#)(o)) for proton transfer in the SS and RR channels occur in distinct membranes.

Diagnóstico da ambliopia / Diagnostic of amblyopia

O diagnóstico da ambliopia na fase pré-verbal é de crucial importância para o tratamento e prógóstico. O potencial visual evocado, o nistagmo óptico-cinético e a oclusäo, säo instrumentos que podem ser utilizados antes dos 2 anos de idade. O diagnóstico se completa com exames refratométrico e fundoscópico, se necessário, sob narcose

Ambliopia näo estrábica / Non strabismic amblyopia

O modelo animal desenvolvido por Von Noorden serve de entendimento para o problema da ambliopia näo estrabíca. Os casos de ambliopia obscuracional ocorrida após um período de sensitizaçäo näo säo mais capazes de recuperaçäo visual. Se a ambliopia obscuracional for interrompida antes de passado o período crítico, a acuidade visual pode normalizar, porém, a binocularidade está definitivamente perdida e a ambliopia recidiva. Nos casos de ambliopia obscuracional binocular, o processo tem um prognóstico melhor porque mesmo com acuidade visual baixa, exite binocularidade e näo ocorre a recidiva