Effects of N-alcohols on potassium conductance in squid giant axons

Effect of heptanol and ethanol on excitation wave propagation in a neonatal rat ventricular myocyte monolayer

In this work, the action of heptanol and ethanol was investigated in a two-dimensional (2D) model of cardiac tissue: the neonatal rat ventricular myocyte monolayer. Heptanol is known in electrophysiology as a gap junction uncoupler but may also inhibit voltage-gated ionic channels. Ethanol is often associated with the occurrence of arrhythmias. These substances influence sodium, calcium, and potassium channels, but the complete mechanism of action of heptanol and ethanol remains unknown. The optical mapping method was used to measure conduction velocities (CVs) in concentrations of 0.05-1.8 mM heptanol and 17-1342 mM ethanol. Heptanol was shown to slow the excitation wave significantly, and a mechanism that involves a simultaneous action on cell coupling and activation threshold was suggested. Whole-cell patch-clamp experiments showed inhibition of sodium and calcium currents at a concentration of 0.5 mM heptanol. Computer modeling was used to estimate the relative contribution of the cell uncoupling and activation threshold increase caused by heptanol. Unlike heptanol, ethanol slightly influenced the CV at clinically relevant concentrations. Additionally, the critical concentrations for re-entry formation in ethanol were determined.

Differential effects of methanol on rat aortic smooth muscle

The effects of methanol on isolated segments of rat aorta were investigated. In the absence of any vasoactive agent, methanol (5-675 mM) failed to alter basal tension. In rat aortic rings precontracted with high K+ (30 mM), methanol elicited a concentration-related relaxation at concentrations of from 5 to 675 mM. The K+-induced contraction in the presence of endothelium was more strongly inhibited by methanol than in the absence of endothelium. The effective concentration producing approximately 50% of the maximal relaxation response (ED50) to methanol was about 96 mM. Methanol-induced relaxations could not be abolished either by 5 x 10(-5) M N-nitro-L-arginine methyl ester (L-NAME) or NG-nitro-L-arginine (L-NNA), both selective inhibitors of nitric oxide (NO) formation; these relaxations were not potentiated by addition of excess L-arginine. An inhibitor of prostanoid synthesis, indomethacin (10(-5) M), had no effects on methanol-induced relaxation. Removal of extracellular Ca2+ ([Ca2+]o) resulted in almost complete inhibition of the relaxant effects of methanol on rat aortic ring segments. Marked attenuation of the relaxation responses of intact arteries to methanol was obtained after buffering intracellular Ca2+ ([Ca2+]i) with 10 microM BAPTA-AM. In 5-hydroxytryptamine (5-HT, 2.5 microM)- or phenylephrine (PE, 0.1 microM)-precontracted rat aortic rings, methanol amplified contractile responses to 5-HT and PE; these increased responses were concentration dependent. No significant differences in these methanol potentiated responses were found between aorta with or without endothelial cells. The amplified rat aortic smooth muscle responses induced by methanol after PE could be modified only by phentolamine, an antagonist of PE, while responses to 5-HT could be inhibited by methysergide (an antagonist of 5-HT) and by phentolamine, diphenhydramine, and haloperidol. Pretreatment with 50, 200, and 500 mM methanol increased rat aortic contractile responses induced by 5-HT and PE. Our results suggest that: (a) acute methanol exposure relaxes rat aortic smooth muscle contractile responses induced by high K+, leading to vessel relaxation. This relaxation effect of methanol is endothelium-dependent, clearly Ca2+ dependent, and independent of endogenous vasodilators such as acetylcholine, histamine, catecholamines, serotonin, or PG. (b) Methanol seems to increase potassium current by shifting the potential towards more negative values in depolarized vascular muscle cell membranes, probably inducing hyperpolarization of the cell membranes leading to a repolarization. (c) In contrast to the relaxant responses, methanol potentiates contractile response of rat aorta to 5-HT and PE.

Evidence for hemi-gap junctional channels in isolated horizontal cells of the skate retina

Prolonged depolarization of isolated, voltage-clamped skate retinal horizontal cells produces an outward current that exhibit a late onset and develops slowly with time. This current, which we refer to as the Q-current, is associated with an increase in membrane conductance, and is present when other voltage-gated conductances have been pharmacologically blocked. The reversal potential for the Q-current, obtained using tail current analysis, was close to 0 mV. The magnitude of the current was greatly reduced by superfusion with 25 mM acetate, and by 4 mM cobalt chloride, 2 mM 1-octanol, and a saturated solution of the general anesthetic halothane. In addition, the low-molecular weight fluorescent dye Lucifer yellow, applied extracellularly, entered the cells during activation of the Q-current, whereas a 3 kD dextran-fluorescein complex did not cross the cell membrane. The effects of divalent cations, the non-specific nature of the ionic current suggested by its reversal potential, the entry of Lucifer yellow, and the ability of acetate, halothane, cobalt, and octanol to block the current lead us to hypothesize that the Q-current results from the opening of hemi-gap junctional channels that mediate electrical coupling between skate horizontal cells.

Differential effects of alcohols on the spike threshold of an identified motor axon in a crab (Pachygrapsus crassipes)

Observations were made on the fast bender excitor (FBE) axon in autotomized crab limbs bathed in salines made up with different alcohols. It has been shown previously that the presence of ethanol at a certain level causes a single action potential to generate additional spikes in the peripheral axon branches. The present study examines the level of different alcohols required to induce peripheral spike generation. For primary alcohols, increasing the molecular weight decreased the level of alcohol required to produce peripheral spike generation. The threshold level of 2-butanol was greater than 1-butanol, but less than tertiary-butanol. These results are explained in terms of the partition coefficient, so that an alcohol with a higher partition coefficient enters the lipid bilayer more readily, thus a lower threshold level of that alcohol is required in the saline to generate additional spikes.

Biophysical properties of gap junctions between freshly dispersed pairs of mouse pancreatic beta cells

Coupling between beta cells through gap junctions has been postulated as a principal mechanism of electrical synchronization of glucose-induced activity throughout the islet of Langerhans. We characterized junctional conductance between isolated pairs of mouse pancreatic beta cells by whole-cell recording with two independent patch-clamp circuits. Most pairs were coupled (67%, n = 155), although the mean junctional conductance (gj) (215 +/- 110 pS) was lower than reported in other tissues. Coupling could be recorded for long periods, up to 40 min. Voltage imposed across the junctional or nonjunctional membranes had no effect on gj. Up to several hours of treatment to increase intracellular cAMP levels did not affect gj. Electrically coupled pairs did not show transfer of the dye Lucifer yellow. Octanol (2 mM) reversibly decreased gj. Lower concentrations of octanol (0.5 mM) and heptanol (0.5 mM) than required to uncouple beta cells decreased voltage-dependent K+ and Ca2+ currents in nonjunctional membranes. Although gj recorded in these experiments would be expected to be provided by current flowing through only a few channels of the unitary conductance previously reported for other gap junctions, no unitary junctional currents were observed even during reversible suppression of gj by octanol. This result suggests either that the single channel conductance of gap junction channels between beta cells is smaller than in other tissues (less than 20 pS) or that the small mean conductance is due to transitions between open and closed states that are too rapid or too slow to be resolved.