Asymmetric displacement currents, Ig, were measured in squid axons at different hydrostatic pressures, P, up to 60 MPa. Potassium and sodium currents were abolished by intracellular Cs+ and TEA+, by extracellular Tetrodotoxin (TTX), and by Na+ substitution with Tris+. The time course of Ig became progressively slower with increasing pressure, and the amplitude decreased. With appropriate scaling in time and amplitude, Ig records at any given P could be made to superimpose very well with those obtained at atmospheric pressure. The same scaling factors yielded a good superposition of all records obtained for voltage steps to membrane potentials in the range -30 to +42 mV. The ratio between the amplitude and time factors was larger than unity and increased with P, indicating a progressive decrease (up to 35% at 60 MPa) of the total charge displaced, Q, with no significant change in its voltage dependence. The time-scaling factor increased exponentially with P, as expected if all the steps involved in the opening of a sodium channel, and producing a major charge redistribution, have the same activation volume, delta V not equal to g approximately 17 cm3/mol. This value is roughly one-half of that characterizing the pressure dependence of sodium current activation, suggesting that some late, rate-limiting step in the opening of sodium channels has a large activation volume without being accompanied by an easily detected charge movement. Part of the decrease of Q with pressure could be attributed to an increase in sodium inactivation. However, we cannot exclude the possibility that there is a reversible reduction in the number of fast activating sodium channels, similar to the phenomenon that has been reported to occur at low temperatures (Matteson and Armstrong 1982).

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1. The time course of sodium currents (INa) in squid giant axon was analysed using viscous non-electrolyte solutions on both sides of the axolemma. It slowed reversibly as the nonelectrolyte concentration increased. The activation, deactivation (closing) and inactivation processes were slowed in a similar manner. showing that the basic gating mechanism did not change in these solutions and only a slight increase in the activation free energy was one of the main causes of slowing. 4. Eight non-electrolytes, formamide, ethylene glycol, glycerol, erythritol, glucose, sorbitol, sucrose and polyethylene glycol (mean molecular weight 600) were used. The amount of slowing was correlated with the gram concentration (g Fl) of non-electrolytes, but not with molar concentration (M) and solution osmolarity (osmol Fl). 6. Values of a and y deviated frequently from those in an ideal case, i.e. 100% for a and 1 for y, and they scattered, having a tendency to decrease as a function of molecular weight. 7. The slowing was also expressed as an exponential function of the solution osmolarity.A predicted solute-inaccessible volume V. ranged (in nm3 per molecule) between 0 09 and 1 45. The value of Va increased as a logarithmic function of the molecular weight of the nonelectrolyte. 8. This solute-inaccessible volume should be distributed in all hydrophilic parts of the sodium channel protein, but is not located in the channel conducting pore itself. The slowing of gating could be explained by a model in which a rate-limiting step is a hydration process that occurs after local small structural changes have exposed new, unhydrated faces (transient hydrated-states model).9. Considering the opposite dependencies of parameters a (or y) and fi on the molecular weight, sodium channel gating is likely to reflect a combination of these two models, which are coupled in microscopic segment movements. We emphasize with this combination of models that fluctuating hydrophilic structures play an important role in determining time constants in the gating process.

The time course of excitation of intracellularly perfused squid giant axons was slowed as the solution viscosity was raised by adding neutral molecules, i.e., glucose and glycerol. By twofold increase of the solution viscosity, the duration of action potential was prolonged to 2.7-fold and the maximum rate of rise decreased to one-half. At the same time, the membrane resistance at resting state increased by 60%. These effects were reversible. The time course of inward and outward currents was slowed also. When the solution viscosity increased to twofold, the time to peak inward current increased by 80%, and the amplitudes of peak inward and steady outward currents decreased by 60% and by 70%, respectively. These effects were not specific for the sodium or the potassium channel. Effects of solution viscosity occurred in both hypotonic and hypertonic solutions. Q10 values of temperature dependence of the time course of the action potential were equal in any viscous solutions. These effects in viscous solutions were explained by the change in solution viscosity but not by the change in solution osmolarities, ionic activities, or solution resistivity.

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The structural stability of bacteriorhodopsin was studied by denaturation experiments, using aliphatic alcohol as denaturants. The disappearance of a positive peak at 285 nm of the circular dichroism spectra, the change in the intrinsic fluorescence decay time, and the decrease of the regeneration activity bacteriorhodopsin indicated the denaturation of the tertiary structure of this protein at a methanol concentration of about 3 M. The circular dichroism band at 222 nm was unchanged by the denaturation. It was concluded that the alcohol-denatured state in water was similar to the molten globule state of soluble proteins, in which only the tertiary structure was destroyed. Solvent substitution from water to hexane did not cause denaturation of bacteriorhodopsin. However, further addition of alcohol destroyed the secondary as well as the tertiary structures. Comparing the alcohol effects of bacteriorhodopsin in water to that in hexane, the dominant interactions for the structure formation of this protein could be revealed: the hydrophobic interaction that arose from the structure of water is essential for the stability of membrane spanning helices, while the interaction which binds the helices is polar in nature.

Squid giant axon could be excited in concentrated glycerol solutions containing normal concentrations of electrolytes, when osmolalities of solutions inside and outside the axon were matched. These glycerol solutions did not freeze at the temperature as low as -19 degrees C. The nerve excitation in these solutions were observed at this low temperature. The excitation process at this low temperature was slowed down and time constants of the excitation kinetics were several hundredfold larger than those in normal seawater at 10 degrees C, under which temperature the squid habituated. The temperature coefficients for the electrophysiological membrane parameters under this condition were larger than those in normal seawater above 0 degrees C. The Q10 value for the conduction velocity was 2.0 and that of the duration of the action potential was around 8.5. The time course of the membrane currents was also slowed with the Q10 value of around 5 and the magnitude decreased with the Q10 value of around 2 as the temperature was lowered. The Q10 values for the kinetics of the on process of the Na-channel were around 4.5 and were almost the same as those of the off process of the Na-channel in the wide range of the temperature below 0 degrees C. The Q10 value of the on process of K-channel was around 6.5 and was larger than those for Na-channel. The Q10 values increased gradually as the temperature was lowered.