Na + -K + -dependent conformation change of proteins of excitable membranes

A model for self-sustained potential oscillation of lipid bilayer membranes induced by the gel-liquid crystal phase transitions

To clarify the mechanism of self-sustained oscillation of the electric potential between the two solutions divided by a lipid bilayer membrane, a microscopic model of the membrane system is presented. It is assumed, on the basis of the observed results (Yoshikawa, K., T. Omachi, T. Ishii, Y. Kuroda, and K. liyama. 1985. Biochem. Biophys. Res. Commun. 133:740-744; Ishii, T., Y. Kuroda, T. Omochi, and K. Yoshikawa. 1986. Langmuir. 2:319-321; Toko, K., N. Nagashima, S. liyama, K. Yamafuji, and T. Kunitake. Chem. Lett. 1986:1375-1378), that the gel-liquid crystal phase transition of the membrane drives the potential oscillation. It is studied, by using the model, how and under what condition the repetitive phase transition may occur and induce the potential oscillation. The transitions are driven by the repetitive adsorption and desorption of proton by the membrane surface, actions that are induced the periodic reversal of the direction of protonic current. The essential conditions for the periodic reversal are (a) at least one kind of cations such as Na+ or K+ are included in the system except for proton, and the variation of their permeability across the membrane due to the phase transition is noticeably larger than that of proton permeability; and (b) the phase transition has a hysteresis. When these conditions are fulfilled, the self-sustained potential oscillation may be brought about by adjusting temperature, pH, and the cation concentration in the solutions on both sides of the membrane. Application of electric current across the membrane also induces or modifies the potential oscillation. Periodic, quasiperiodic, and chaotic oscillations appear especially, depending on the value of frequency of the applied alternating current.

The effect of transmembrane potential on the dynamic behavior of cell membranes

The relationship between transmembrane potential and lipid dynamics in the cytoplasmic membrane of mouse thymus cells has been investigated. Changes of transmembrane potential was followed by measuring the fluorescence emission of the anionic dye, bis-(1,3-dibutylbarbiturate)trimethine oxonol (diBa-C4-(3)). Assessment of lipid fluidity was carried out applying three fluorescent lipid probes, 1-[4-(trimethylammonium)phenyl]-6-phenyl-1,3,5-hexatriene (TMA-DPH), 12-(9-anthroyloxy)stearic acid (12-AS) and 1,6-diphenyl-1,3,5-hexatriene (DPH) used to monitor different structural regions of the bilayer. The fluorescence anisotropy of these probes was measured as a function of temperature at two values of transmembrane potential. In the case of DPH it proved to depend on the membrane potential in the higher temperature range (above 28 degrees C), while no such a dependence could be observed for DPH below this temperature range and for TMA-DPH and 12-AS in between 20 and 37 degrees C. These data suggest that changes in transmembrane potential are accompanied with some local alteration in membrane lipid dynamics and/or structure.

An ion-site interaction model for sodium currents in the giant axon

The time and voltage dependence of sodium currents in the Myxicola giant axon were examined as functions of the external sodium concentration. The results were incompatible with a model of free diffusion through a gated channel, but lent themselves to analysis in terms of a model involving a positive cooperative homotropic reaction in which Na+ interacts with two allosteric sites - a regulatory site and a transfer site - at the 'sodium channel'. The time-dependent solution of the rate equations describing the kinetics of the transfer reaction was derived as an expression describing the sodium current as a function of time, membrane potential and external sodium concentration. This function was used to test the validity of the model by its ability to predict the nerve excitability properties. The predicted i-v and i-t curves fitted the experimental results (p less than 0.005 and p less than 0.05, respectively). The computed parameters of these functions are consistent with other experimental results. The possibility of a noncooperative reaction was rejected.

Effect of ionic strength on the membrane fluidity of rabbit intestinal brush-border membranes. A fluorescence probe study

The effect of ionic strength on the fluidity of rabbit intestinal brush-border membranes has been studied using two fluorescence probes, pyrene and 1-anilino-8-naphthalene sulfonate (ANS). The imposition of a potential gradient on the pyrene-probed membrane vesicles (out greater than in) with increasing NaCl concentration in the medium resulted in a marked enhancement of the excimer formation efficiency, accompanied by a decrease in the ratio of fluorescence intensities of the probe at 392 and 375 nm. Fluorescence polarization of the pyrene-membrane complex is independent of temperature in the absence of salts, while it is dependent on temperature from 10 to 47 degrees C in the presence of salts, as shown by the thermal Perrin plots of polarization. It has been demonstrated that there is a linear relationship between the changes in the pyrene excimer formation efficiency in the membranes and of the values of the binding parameters of ANS for the membranes. From these results, it is suggested that the lipid phase of the membranes becomes more fluid by shielding negatively charged groups of the membrane surface and that there is a fairly close correlation between the membrane organization and the membrane surface charge density.

Ionic permeability of K, Na, and Cl in potassium-depolarized nerve. Dependency on pH, cooperative effects, and action of tetrodotoxin

The passive ionic membrane conductances (gj) and permeabilities (Pj) of K, Na, and Cl of crayfish (Procambarus clarkii) medial giant axons were determined in the potassium-depolarized axon and compared with that of the resting axon. Passive ionic conductances and permeabilities were found to be potassium dependent with a major conductance transition occurring around an external K concentration of 12-15 mM (Vm = -60 to -65 mV). The results showed that K, Na, and Cl conductances increased by 6.2, 6.9, and 27-fold, respectively, when external K was elevated from 5.4 to 40 mM. Permeability measurements indicated that K changed minimally with K depolarization while Na and Cl underwent an order increase in permeability. In the resting axon (K0 = 5.4 mM, pH = 7.0) PK = 1.33 X 10(-5), PCl = 1.99 X 10(-6), PNa = 1.92 X 10(-8) while in elevated potassium (K0 = 40 mM, pH 7.0), PK = 1.9 X 10(-5), PCl = 1.2 X 10(-5), and PNa = 2.7 X 10(-7) cm/s. When membrane potential is reduced to 40 mV by changes in internal ions, the conductance changes are initially small. This suggests that resting channel conductances depend also on ion environments seen by each membrane surface in addition to membrane potential. In elevated potassium, K, Na, and Cl conductances and permeabilities were measured from pH 3.8 to 11 in 0.2 pH increments. Here a cooperative transition in membrane conductance or permeability occurs when pH is altered through the imidazole pK (approximately pH 6.3) region. This cooperative conductance transition involves changes in Na and Cl but not K permeabilities. A Hill coefficient n of near 4 was found for the cooperative conductance transition of both the Na and Cl ionic channel which could be interpreted as resulting from 4 protein molecules forming each of the Na and Cl ionic channels. Tetrodotoxin reduces the Hill coefficient n to near 2 for the Na channel but does not affect the Cl channel. In the resting or depolarized axon, crosslinking membrane amino groups with DIDS reduces Cl and Na permeability. Following potassium depolarization, buried amino groups appear to be uncovered. The data here suggest that potassium depolarization produces a membrane conformation change in these ionic permeability regulatory components. A model is proposed where membrane protein, which forms the membrane ionic channels, is oriented with an accessible amino terminal group on the axon exterior. In this model the ionizable groups on protein and phospholipid have varied associations with the different ionic channel access sites for K, Na, and Cl, and these groups exert considerable control over ion permeation through their surface potentials.

Control of ionic permeability by membrane charged groups: dependency on pH, depolarization, tetrodotoxin and procaine

The membrane permeabilities of K, Na, and Cl were determined in crayfish giant axons from pH 3.8 to 11.4. In general, cation permeability increases with pH while anion permeability decreases. In normal saline (Ko = 5.4 mM, pH = 7), P(K) = 1.33 X 10-5, P(Cl) - 1.49 X 10-6, and P(Na) = 1.92 X 10-8 cm/s. Increasing external potassium results in a dramatic membrane conductance change around Ko = 12 mM (Vm = -60 mV) which results primarily from changes in P(Na) and P(Cl). In elevated potassium (Ko = 40 mM, pH = 7), P(K), P(Cl), and P(Na) increase by 1.45, 8.1 and 14.2. In the potassium depolarized axon, P(Na) and P(Cl) show a cooperative change when pH is altered through the imidazole pK region (pK = 6.3). These changes are not seen in normal saline, or with P(K). A Hill coefficient n = 4 was found for the cooperative change of P(Na) and P(Cl). An interpretation here is the four protein molecules interact to form the Na and Cl ionic channels. Tetrodotoxin has minimal effects on passive permeabilities but reduce the Hill coefficient n for P(Na) but not P(Cl), while procaine reduces n for both P(Na) and P(Cl). The results show that membrane fixed charged groups have varied association and control over the different ion permeabilities. In addition, membrane conformational changes are also involved in permeability control.

Conformational studies on murein-lipoprotein from the outer membrane of Escherichia coli

Conformational studies on an isolated integral membrane protein are reported. Lipoprotein of Escherichia coli outer membrane was released from murein by treatment with either lysozyme or trypsin. The isolated lysozyme-released lipoprotein (lipoprotein I) contained 2 or 3 muropeptides covalently linked at the C-terminal end, while the trypsin-released lipoprotein (lipoprotein II) was free of muropeptides and lacked the C-terminal peptide Tyr-Arg-Lys. Circular dichroism spectra of the two preparations were essentially identical, and they show an alpha-helix content of about 80%. According to calculations based on the Chou-Fasman rules for proteins of known sequence, lipoprotein is 64% alpha-helix and 15% beta-structure. Infrared spectroscopy qualitatively supports these values. The conformation was stable in the pH range of 5 - 12. Danaturation of lipoprotein by heat, 8 M urea, or sodium dodecylsulphate was a fully reversible, cooperative process. The thermal denaturation of lipoprotein occurs in two steps with transition points at 79.4 degrees C for lipoprotein I and at 85.1 degrees C for lipoprotein II. Lioprotein markedly changes conformation at dodecylsulphate concentrations where micelle formation sets in. The unusual behaviour of the lipoprotein convormation in sodium dodecylsulphate is discussed in relation to the lipoprotein conformation and aggregation within the membrane.