ELECTRICAL EXCITABILITY OF ISOLATED FROG SKIN AND TOAD BLADDER

Determination of the driving force of the Na(+) pump in toad bladder by means of vasopressin

Vasopressin stimulates Na(+) transport across toad bladder largely or entirely by decreasing the resistance to Na(+) entry into the transporting epithelial cells. Therefore, the hormone should induce proportional changes in short circuit current (I S ) and tissue conductance; the ratio of these changes should equal the driving force (E Na) of the Na(+) pump.Administration of vasopressin provided a rapid, reversible and reproducible technique for the measurement ofE Na. Values calculated forE Na ranged from 74 to 186 mV, in agreement with previously published estimates. The results were not dependent on the vasopressin concentration over a wide range of concentrations.Ouabain, an agent thought to inhibit specifically the Na(+) pump, decreased bothI S andE Na. On the other hand, amiloride, a diuretic thought to block specifically Na(+) entry, markedly reducedI S , without reducingE Na.It is concluded that vasopressin constitutes a probe for the rapid reproducible determination ofE Na under a wide variety of physiological conditions.

Analysis of Spike Electrogenesis and Depolarizing K Inactivation in Electroplaques of Electrophorus electricus, L

Voltage clamp analyses, combined with pharmacological tools demonstrate the independence of reactive Na and K channels in electrically excitable membrane of eel electroplaques. Spike electrogenesis is due to Na activation and is eliminated by tetrodotoxin or mussel poison, or by substituting choline, K, Cs, or Rb for Na in the medium. The K channels remain reactive, but K activation is always absent, the electroplaques responding only with K inactivation. This is indicated by an increased resistance when the membrane is depolarized by more than about 30 mv. The resting resistance (1 to 5 ohm cm²) is dependent upon the ionic conditions, but when K inactivation occurs the resistance becomes about 10 ohm cm² in all conditions. K inactivation does not change the EMF significantly. The transition from low to high resistance may give rise to a negative-slope voltage current characteristic, and to regenerative inactivation responses under current clamp. The further demonstration that pharmacological K inactivation (by Cs or Rb) leaves Na activation and spike electrogenesis unaffected emphasizes the independence of the reactive processes and suggests different chemical compositions for the membrane structures through which they operate.

Tissue electroporation. Observation of reversible electrical breakdown in viable frog skin

Experiments by others have used isolated cell or bilayer membrane preparations to study the dramatic phenomena associated with electroporation. The present study observes electroporation behavior in an intact tissue. Viable samples of frog skin (Rana pipiens) were exposed to short electrical pulses of varying width and magnitude under "charge injection" conditions. After a pulse, the transtissue potential decayed with two distinct time constants, one short (tau approximately 0.3 ms) and the other longer (tau L approximately 2 ms). Above thresholds for the pulse magnitude and for the pulse width tau L decreased significantly, with progressively smaller tau L as the pulse magnitude and width increased. The postpulse potential, delta Utissue (t), and resistance, Rtissue, also decreased progressively. The tissue subsequently recovered to its original resistance and open circuit potential, delta U tissue,oc, within 2-3 min after a pulse. At that time another pulse experiment could be carried out, demonstrating repeatability and reversibility. No significant permanent changes in Rtissue and delta Utissue,oc were found. This is interpreted as avoidance of significant tissue damage. Taken together, these dramatic phenomena are characteristic of the reversible electrical breakdown previously observed in charge injection experiments with artificial planar bilayer membranes and with isolated cell membranes by similar very short pulses. The present experiments therefore demonstrate that electroporation can be repeatedly caused and observed in a viable tissue without apparent damage.

Electrophysiology of Necturus urinary bladder: II. Time-dependent current-voltage relations of the basolateral membranes

As reported previously (S.R. Thomas et al., J. Membrane Biol. 73:157-175, 1983) the current-voltage (I-V) relations of the Na-entry step across the apical membrane of short-circuited Necturus urinary bladder in the presence of varying mucosal Na concentrations are (i) time-independent between 20-90 msec and (ii) conform to the Goldman-Hodgkin-Katz constant field flux equation for a single cation over a wide range of voltages. In contrast, the I-V relations of the basolateral membrane under these conditions are (i) essentially linear between the steady-state, short-circuited condition and the reversal potential (Es); and (ii) are decidedly time-dependent with Es increasing and the slope conductance, gs, decreasing between 20 and 90 msec after displacing the transepithelial electrical potential difference. Evidence is presented that this time-dependence cannot be attributed entirely to the electrical capacitance of the tissue. The values of gs determined at 20 msec are linear functions of the short-circuit current, Isc, confirming the relations reported previously, which were obtained using a more indirect approach. The values of Es determined at 20 msec are significantly lower than any reasonable estimate of the electromotive force for K across the basolateral membrane, indicating that this barrier possesses a significant conductance to other ions which may exceed that to K. In addition, these values increase linearly with decreasing Isc and approach the value of the electrical potential difference across the basolateral membrane observed when Na entry across the apical membrane is blocked with amiloride or when Na is removed from the mucosal solution. A possible explanation for the time-dependence of Es and gs is offered and the implications of these findings regarding the interpretation of previous microelectrophysiologic studies of epithelia are discussed.

Metabolic regulation of apical sodium permeability in toad urinary bladder in the presence and absence of aldosterone

In the present study, further evidence was adduced for energy-dependent regulation of passive apical transport of Na in toad bladder epithelium. In potassium-depolarized preparations studied by current-voltage analysis, additions of pyruvate or glucose to the media of substrate-depleted bladders evoked proportionate increases in the transepithelial Na current and in apical Na permeability. These responses were large in aldosterone pretreated hemibladders and almost absent in the aldosterone-depleted preparations or when hormonal action was blocked by spironolactone or cycloheximide. The substrate-induced increases in apical Na permeability were fully reversed by appropriate metabolic inhibitors, i.e. 2-deoxyglucose and oxythiamine. Moreover, the inhibitory effect of 2-deoxyglucose was bypassed by the addition of pyruvate to the serosal medium. Thus apical Na permeability is clearly sensitive to the supply of cellular energy. The possibility that changes in intracellular free Na activity may mediate metabolic regulation of apical Na permeability was evaluated by prolonged exposure to Na-free mucosal and serosal media, with and without inhibition of the Na/K-pump by ouabain. The stimulatory and inhibitory effects of pyruvate, 2-deoxyglucose and oxythiamine on Na currents and Na conductances were preserved under these circumstances. Furthermore, reduction of serosal Ca to a minimal level of 3 microM, was without effect on the response to metabolic inhibition. These experiments demonstrate the existence of Na-independent metabolic regulation of apical Na transport and imply that neither basal-lateral nor mitochondrial Na/Ca exchange is required for this regulatory process under the imposed conditions. The possibility that a Na-independent, Ca transport mechanism in mitochondria or endoplasmic reticulum may be involved in metabolic regulation of apical Na transport, however, remains to be evaluated.

Voltage transients during ionic substitution in renal cortical tubules

A voltage transient is described which is found during proximal tubular perfusion with impermeant cation or anion salt solutions in the rat. It was shown that the magnitude of transepithelial diffusion potentials depended on luminal hydrostatic pressure, suggesting that the observed transients might be the consequence of the enlargement of ionic pathways by tubular dilatation. Thus, when reporting PD values, care should be taken to define the pressure levels at which measurements were performed.

Structural responses to voltage-clamping in the toad urinary bladder. I. The principal role of granular cells in the active transport of sodium

The structural consequences of clamping the transepithelial potential difference across the toad's urinary bladder have been examined. Reducing the potential to zero (short-circuiting) produced no apparent changes in the morphology of any of the four cell types which comprise the epithelium. Computer assisted, morphometric analysis of quick frozen specimens revealed no measurable difference in granular cell volume between open-and short-circuited preparations. However, when the open-circuit potential was quantitatively reversed (serosa negative with respect to mucosa), some of the preparations showed a marked increase in granular cell volume. To examine this more systematically twelve preparations were voltage-clamped at 50 mV (serosa negative); eight of the twelve revealed prominent granular cell swelling relative to control, short-circuited preparations. Only in this group of eight had the external circuit current fallen substantially during the clamping interval. Mitochondria-rich cells were not affected detectably. Application of the diuretic amiloride prior to clamping at reversed potential prevented granular cell swelling in every case. Goblet cells which were often affected by the - 50 mV clamp were not protected by the diuretic. Granular cell swelling thus appeared to be dependent on sodium entry at the mucosal surface. We also observed that, after voltage reversal, the apical "tight" junctions of the bladders were blistered as they are with hypertonic mucosal media. This blistering was associated with an increase in passive ionic permeability and was not prevented by application of amiloride. This finding is consistent with the evidence that the junction is a complex barrier with asymetric, and hence, rectifying properties for intrinsic ionic conductance as well as hydraulic permeability. These findings, together with others from the literature, lead to the conclusion that the granular cells constitute the principal, if not sole, elements for active sodium transport across toad urinary bladder and that they swell when sodium entry exceeds the transport capacity of the pump at the basal-lateral surface.

Occluding junctions in a cultured transporting epithelium: structural and functional heterogeneity

MDCK cells (epithelioid of renal origin) form monolayers which are structurally and functionally similar to transporting epithelia. One of these similarities is the ability to form occluding junctions and act as permeability barriers. This article studies the junctions of MDCK monolayers formed on a permeable and transparent support (a disk of nylon cloth coated with collagen) by combining two different approaches: (i) Scanning of the electric field: the disk is mounted as a flat sheet between two Lucite chambers and pulses of 20--50 microA cm-2 are passed across. The apical surface of the monolayer is then scanned with a microelectrode to detect those points where the current is flowing. This shows that the occluding junctions of this preparation are not homogeneous, but contain long segments of high resistance, intercalated with sites of high conductance. (ii) Freeze fracture electron microscopy: the junctions are composed of regions of eight to ten strands intercalated with others where the strands are reduced to one or two ridges. The sites of high conductance may correspond to those segments where the number of junctional strands is reduced to 1 or 2. It is concluded that the occluding junctions of MDCK monolayers are functionally and morphologically heterogeneous, with "tight" regions intermixed with "leaky" ones.

Relationship of transient electrical properties to active sodium transport by toad urinary bladder

Application of voltage pulses of 10 mV for periods of 9 sec across toad urinary bladder elicits a rapid deflection in transepithelial current. Frequently, the current decays back towards its baseline value during the course of the polarizing pulse. This transient phenomenon can be induced, or its magnitude increased, by raising the mucosal or serosal Na+ concentration. The transient can be abolished by sufficiently hyperpolarizing the tissue (rendering serosa positive to mucosa), by inhibiting transcellular Na+ transport with amiloride or ouabain, and by increasing the serosal K+ concentration. Vasopressin increases net Na+ movement across toad bladder but does not elicit these transients. It is proposed as a working hypothesis for further study that the transient behavior characterized in this study reflects: (1) the partition of Na+ between the apical plasma membrane and contiguous fluid layers, (2) the partition of K+ between the basolateral plasma membrane and adjacent submucosal fluid layer, and (3) the negative feedback interaction between intracellular Na+ activity and Na+ permeability of the apical plasma membrane of the transporting cells.

Precipitation membrane effects in biologic membranes: the role of calcium

Biologic membranes display rectification of electrical current, as well as other properties, in many respects similar to precipitation membranes. The experiments reported here, performed in frog skin, show that these characteristics are dependent upon the presence of calcium. Upon elimination of calcium from the bathing solution, the property of electrical rectification is lost, the current-voltage relation assuming a linear form. Readministration of calcium brings about complete recovery of the rectification pattern. This behavior is analogous to chemical deconditioning of precipitation membranes. Our findings support the assumption that the binding of calcium in biologic membranes produces electrical effects characteristic of precipitation membranes.

Power density spectra of frog skin potential, current and admittance functions during patch clamp

Clamp current fluctuations in frog skin of areas down to 0.07 cm2 are dominated by low frequency components (less than 100 Hz). Patch clamp of 0.001 cm2 under high density fluorosilicone oil exhibits components up to 5000 Hz, often including a peak in the current power density spectrum. The admittance spectrum also exhibits a peak at the same frequency. In some skins no peak was observed, but the break in the curve was too sharp to be Lorentzian. In all instances the final limiting slope approached 1/f2. The resonance peak was observed in either Cl- or SO = 4 Ringer's but disappeared when Na+ was replaced with K+. Resonance frequency varied from 100 to 700 Hz.

Effects of unstirred layers or transport number discontinuities on the transient and steady-state current-voltage relationships of membranes

The effects of current-induced electrolyte accumulation and depletion on the electrical properties of a two-layered membrane system have been examined. The membrane consisted of a charged, ion permselective layer and an uncharged, non-selective layer. The model was designed to reveal the properties of membranes possessing long pores with ionic charges at one end or of ion-selective membranes bounded by highly unstirred aqueous layers. Electrolyte concentration profiles in the inert layer and their time-dependent changes were obtained from solutions of the diffusion equation under the condition of constant current. The profiles were then used to calculate the voltage developed across the membrane at various times after the current is switched on. The theoretical results are presented in the form of i-V curves with reduced coordinates that can be used to obtain time-current-voltage relationships for membranes of the type considered having any thickness of the non-selective layer and bathed in any concentration of any 1:1 electrolyte. Experimental results on a model composite membrane were in good agreement with calculations that assume that ion transport occurs only under the influence of electrical potential and concentration gradients, suggesting that in such systems, the combined effects of convection, osmosis, electro-osmosis, and concentration-dependence of diffusion coefficients, activity coefficients, and transference numbers are small. Voltage fluctuations in the form of periodic spikes were observed experimentally at the limiting current density (the current density at which the electrolyte concentration at one surface of the selective layer goes to 0). These phenomena were not seen when the current was in the direction leading to accumulation of electrolyte in the non-selective (unstirred) layer. Such composite membranes can exhibit S-shaped and N-shaped i-V curves under ramp-voltage and ramp-current clamps, respectively.

"Action potentials" in Neurospora crassa, a mycelial fungus

Occasional spontaneous "action potentials" are found in mature hyphae of the fungus Neurospora crassa. They can arise either from low-level sinusoidal oscillations of the membrane potential or from a linear slow depolarization which accelerates into a rapid upstroke at a voltage 5-20 mV depolarized from the normal resting potential (near-180 mV). The "action potentials" are long-lasting, 1-2 min and at the peak reach a membrane potential near-40 mV. A 2-to 8-fold increase of membrane conductance accompanies the main depolarization, but a slight decrease of membrane conductance occurs during the slow depolarization. Two plausible mechanisms for the phenomenon are (a) periodic increases of membrane permeability to inorganic ions, particularly H+ or Cl- and (b) periodic decreases in activity of the major electrogenic pump (H+) or the Neurospora membrane, coupled with a nonlinear (inverse signoid) current-boltage relationship. Identification of action potential-like disturbances in fungi means that such behavior has now been found in all major biologic taxa which have been probed with suitable electrodes. As yet there is no obvious function for the events in fungi.

Effect of calcium and vasopressin on the response of frog skin to prostaglandin E1

1. Prostaglandin E(1) increases sodium transport as measured by short circuit current (SCC) across isolated frog skin whereas calcium, added to the external Ringer fluid, decreases sodium transport. To help establish the site of action of prostaglandin the possible interaction of these two agents on sodium transport has been examined.2. The effect of a standard dose of prostaglandin (0.5 x 10(-6)M) on the short circuit current was tested on paired skins with either zero or high calcium (22.4 mM) in the external Ringer fluid. In ten experiments the responses to prostaglandin (expressed in muA/cm(2)) were not significantly affected by external calcium.3. In another series of experiments the chelating agent, EGTA, was included in calcium-free external Ringer in order to promote greater depletion of skin calcium. The response of these skins to the standard dose of prostaglandin was of the same order of magnitude as that of control skins. The response was not sustained in contrast to that of normal skins and skins in high-calcium fluids.4. In a further series of experiments the reverse procedure was adopted whereby the response of the skin to low and high doses of calcium in the external Ringer was recorded in control conditions and when the skin had responded fully to twice the standard dose of prostaglandin. In addition, the calcium-sensitive current was calculated for each skin in both circumstances. The latter was unchanged on addition of prostaglandin, and graded doses of calcium caused the same degree of inhibition of the short circuit current.5. The results show no interaction between external calcium and prostaglandin and also no need for external calcium in prostaglandin stimulation of sodium transport.6. The findings do not support the concept of chelation by prostaglandin of calcium from critical sites on the skin as the primary mechanism of its action on sodium transport. The results closely parallel those of a similar type of study into the relationship between vasopressin and external calcium on frog skin also.7. When frog skin has responded fully to either prostaglandin E(1) or vasopressin, it shows no response to the other, although removal of calcium from the external Ringer fluid causes a further increase in short circuit current.8. Vasopressin causes a further increase in short circuit current in skins treated with prostaglandin F(1alpha). Prostaglandin F(1alpha) may be a weaker agonist on frog skin than either vasopressin or prostaglandin E(1).

Response of the frog skin to steady-state voltage clamping. II. The active pathway

Active Na transport across frog skin was separated from passive Na movement utilizing urea influx as a measure of passive (shunt) permeability. In this manner, the response of the overall active Na transport system to an applied potential was determined over a range from +200 mV to -100 mV. Active Na transport displays saturation as a function of applied potential, and both the level of saturation and the potential at which it is achieved are functions of the Na concentration in the external solution. The saturation with potential appears to involve a different step in the transport process than the saturation of Na flux as a function of external Na concentration. The observations can be qualitatively described by either a one-barrier or two-barrier model of the Na transport system.

Mode of operation of ampullae of Lorenzini of the skate, Raja

Ampullae of Lorenzini are sensitive electroreceptors. Applied potentials affect receptor cells which transmit synaptically to afferent fibers. Cathodal stimuli in the ampullary lumen sometimes evoke all-or-none "receptor spikes," which are negative-going recorded in the lumen, but more frequently they evoke graded damped oscillations. Cathodal stimuli evoke nerve discharge, usually at stimulus strengths subthreshold for obvious receptor oscillations or spikes. Anodal stimuli decrease any ongoing spontaneous nerve activity. Cathodal stimuli evoke long-lasting depolarizations (generator or postsynaptic potentials) in afferent fibers. Superimposed antidromic spikes are reduced in amplitude, suggesting that the postsynaptic potentials are generated similarly to other excitatory postsynaptic potentials. Anodal stimuli evoke hyperpolarizations of nerves in preparations with tonic activity and in occasional silent preparations; presumably tonic release of excitatory transmitter is decreased. These data are explicable as follows: lumenal faces of receptor cells are tonically (but asynchronously) active generating depolarizing responses. Cathodal stimuli increase this activity, thereby leading to increased depolarization of and increased release of transmitter from serosal faces, which are inexcitable. Anodal stimuli act oppositely. Receptor spikes result from synchronized receptor cell activity. Since cathodal stimuli act directly to hyperpolarize serosal faces, strong cathodal stimuli overcome depolarizing effects of lumenal face activity and are inhibitory. Conversely, strong anodal stimuli depolarize serosal faces, thereby causing release of transmitter, and are excitatory. These properties explain several anomalous features of responses of ampullae of Lorenzini.

In vitro techniques for avoiding edge damage in studies of frog skin

Frog skins mounted between chambers without compression, with a liquid insulator and a tissue adhesive, were studied in vitro. Since voltage and electrical resistance per unit area were unchanged by a tenfold decrease in area of skin studied, it is concluded that these mounting techniques do not produce edge damage and consequently provide a means for study of the skin in its absence.

The hyperpolarizing region of the current-voltage curve in frog skin

Excitability (action potential and refractory period) has been described by A. Finkelstein in the depolarizing region of the current-voltage (I-V) curve of the isolated frog skin. Recently Fishman and Macey interpreted this phenomenon as a consequence of a region with negative resistance that confers to the I-V curve an N shape. We have studied the I-V relation of the isolated frog skin in the hyperpolarizing region with a current-ramp system. It was found that in Na(2)SO(4) Ringer's, the resistance continuously increases in the hyperpolarizing direction. When hyperpolarization reaches 300 mv an electrical breakdown occurs, occasionally followed by a region of negative resistance. In NaCl Ringer's the breakdown was also found although the I-V relation was reasonably linear. Unidirectional Na(+) outflux was measured at different levels of voltage clamping across the skin and with different Na(+) concentrations in the solutions. The Na(+) outflux was found to be relatively independent of these parameters. Based on these results a Na(+) rectifying structure is postulated. An electrical model for active Na(+) transport including a diode and an oscillator is proposed. The effects of CO(2), nitrogen, amiloride, and ouabain on the I-V relation are described.

The N-shaped current-potential characteristic in frog skin. II. Kinetic behavior during ramp voltage clamp

Previous step voltage-clamp measurements on frog skin showed the presence of an N-shaped current-potential (I-V) relation in excitable skin. However, the collection and reconstruction of I-V data using discrete step changes of skin potential was tedious because of the long refractory period (up to 1 min) in frog skin. A direct and rapid (5 msec) method for recording the N-shaped I-V characteristic in real time is presented. Ramp functions are used as the command to the clamp system instead of a step function. Consequently the skin potential is forced to change in a linear manner (as commanded) and the skin current can be recorded as a continuous function of the controlled change of skin potential. With the ramp clamp, a low-resistance membrane state ( 10 Omega . cm(2)) resembling a breakdown phenomenon was observed at high skin potential ( 300 mv). Entry into the low resistance state resulted in a collapse of the N-shaped I-V relation to a nearly linear function. The utility of the ramp measurement is demonstrated by predicting (1) that the maximum rate of rise of the spike occurs at a voltage corresponding to the valley (local minimum) in the N-shaped I-V curve, (2) that the rate of rise of the spike increases with increasing clamp currents, (3) the voltage peak of the spike, and (4) the time course of the rising phase of the spike.

The N-shaped current-potential characteristic in frog skin. 3. Ionic dependence

A ramp voltage clamp measurement described previously is used to detect alterations in the frog skin current-potential (I-V) characteristic following removal or replacement of various ions in the solutions bathing the skin. The ionic requirements for the maintenance of a negative-slope I-V property are the following: Ca(++), Na(+), and Cl(-) must be in the outside solution; K(+) and Cl(-) must be in the inside solution. Removal of any one of these ions from its respective solution results in the decay and eventual disappearance of the negative slope.The similarity between the I-V characteristic following Ca(++) removal with EDTA from the outside solution and the I-V relation in a refractory skin suggests that the loss (refractory state) and recovery of the negative slope is a consequence of unbinding and subsequent rebinding of Ca(++) to membrane sites. The role of the univalent ions is not clear-presumably some or all of these ions constitute the current through the skin; however, some of these ions may also be involved in maintaining a membrane condition necessary for the existence of a negative slope I-V relation. Further, excitation does not appear to be a direct consequence of the Na(+) pump.

The N-shaped current-potential characteristic in frog skin. I. Time development during step voltage clamp

A fast (10 musec) voltage-clamp system similar to that used on nerve axons was applied across the frog skin. An electrical analog is used to obtain the electrical parameters and to estimate the time (300 musec) required to voltage clamp the excitable membrane layer in the skin. The speed of the clamp allows observation of the early development in time of an N-shaped current-potential (I-V) relation. The isochronal I-V curves constructed from step clamp data show the beginning of a negative slope in about 250 musec after successively applied step changes in skin potential (> 200 mv). Subsequently, the negative slope reaches a quasi-steady state interval (0.4-1.5 msec) and then decays and disappears in the next 20 msec. The negative slope I-V characteristic is only found in skins which exhibit spike generation under current clamp.

The flash-triggering action potential of the luminescent dinoflagellate Noctiluca

The action potential which elicits luminescence in Noctiluca is recorded from the flotation vacuole as a transient all-or-none hyperpolarization in response to either local or general application of inward (bath to vacuole) current. Experiments were performed to determine whether the unorthodox polarities of both the stimulus current and the potential response resulted from uncommon bioelectric mechanisms or from special morphological features of this species. The findings all indicate that the action potential belongs to the familiar class of responses which have their origin in voltage- and time-dependent selective increases in membrane permeability, and that morphological factors account for the observed deviations from normal behavior. Both the stimulus and the response have orthodox polarities provided the vacuole is designated as an "external" extracytoplasmic compartment. Differential recording between vacuole and cytoplasm showed that the action potential occurs across the vacuolar membrane, with the cytoplasmic potential, which at rest is negative with respect to the vacuole, overshooting zero and reversing sign to become transiently electropositive. The rising phase of the action potential therefore depends on active current flow through the vacuolar membrane from the vacuole into the cytoplasm. Propagation of the action potential over the subspherical cell from the locus of stimulation is thought to depend largely on the core conductor properties of the thin perivacuolar shell of cytoplasm which is bounded on its inner surface by the excitable membrane and on its outer surface by inexcitable membranes.

Induced pacemaker activity on toad skin

The electrical transients produced on the isolated abdominal skin obtained from Bufo arenarum Hensel, under the influence of inward current pulses of constant intensity have been studied. When both faces of the skin are bathed with Ringer's solution, short pulses of inward current give rise to transient variations of the potential difference between both faces of the skin with "all-or-nothing" characteristics (action potentials, AP). When the outer face is bathed with a modified Ringer solution with low sodium content (2.4 mM), the transients are longer and they are only evident when the pulse is several hundred milliseconds long. With even longer pulses (several seconds) a repetitive activity can be elicited, with the electrical characteristics of a "pacemaker" activity. In all these "excitability" phenomena Na(+) may be replaced by Li(+) in the outer solution. The logarithm of the duration of AP's is inversely related to the logarithm of the increase in concentration of Na(+) or Li(+) in the solution bathing the external face of the skin. The duration of AP's is increased when the Ca(++) concentration in the outer solution is raised. This effect is more evident with low sodium concentration on the outside. The evolution of the slope conductance during repetitive activity has been determined. The site and mechanisms of the "excitable" behavior of the skin and the induced repetitive activity are discussed. Under the experimental conditions employed the behavior of the skin is compared with that of normally excitable plasma membranes.

The site of the stimulatory action of vasopressin on sodium transport in toad bladder

Vasopressin increases the net transport of sodium across the isolated urinary bladder of the toad by increasing the mobility of sodium ion within the tissue. This change is reflected in a decreased DC resistance of the bladder; identification of the permeability barrier which is affected localizes the site of action of vasopressin on sodium transport. Cells of the epithelial layer were impaled from the mucosal side with glass micropipettes while current pulses were passed through the bladder. The resulting voltage deflections across the bladder and between the micropipette and mucosal reference solution were proportional to the resistance across the entire bladder and across the mucosal or apical permeability barrier, respectively. The position of the exploring micropipette was not changed and vasopressin was added to the serosal medium. In 10 successful impalements, the apical permeability barrier contributed 54% of the initial total transbladder resistance, but 98% of the total resistance change following vasopressin occurred at this site. This finding provides direct evidence that vasopressin acts to increase ionic mobility selectively across the apical permeability barrier of the transporting cells of the toad bladder.

Fast potential spike of frog skin generated at the outer surface of the epithelium

Experiments were performed to test which structure of frog skin epithelium is responsible for the electrical excitation (fast, all-or-none potential spike) displayed by this tissue during stimulation with a current pulse. Preselected cells of the outer epithelial surface were punctured by microelectrodes under microscopical observation. The major part of the transepithelia resting resistance and the major part of the spike were recorded between microelectrode tip and outside bathing solution. A leak between microelectrode and punctured membrane is made responsible for the attenuation of spike amplitude observed under these recording conditions. It is shown that if the spike is generated at but one of the series membranes of the epithelium, this membrane must be at the outermost border of the tissue.

Transepithelial potentials in Hydra

There is a maintained electrical potential of 15 to 40 millivolts across the two epithelial layers forming the body wall of Hydra, the inside of the animal being positive. Negativegoing (depolarizing) spikes are recorded spontaneously and sometimes in response to depolarizing current pulses. These spikes usually overshoot the zero potential level. The large size of the spikes and the orientation of the potential difference across the body wall indicate that this electrical activity is epithelial rather than nervous in origin.

Analysis of depolarizing and hyperpolarizing inactivation responses in gymnotid electroplaques

In electroplaques of several gymnotid fishes hyperpolarizing or depolarizing currents can evoke all-or-none responses that are due to increase in membrane resistance as much as 10- to 12-fold. During a response the emf of the membrane shifts little, if at all, when the cell either is at its normal resting potential, or is depolarized by increasing external K, and in the case of depolarizing responses when either Cl or an impermeant anion is present. Thus, the increase in resistance is due mainly, or perhaps entirely, to decrease in K permeability, termed depolarizing or hyperpolarizing K inactivation, respectively. In voltage clamp measurements the current-voltage relation shows a negative resistance region. This characteristic accounts for the all-or-none initiation and termination of the responses demonstrable in current clamp experiments. Depolarizing inactivation is initiated and reversed too rapidly to measure with present techniques in cells in high K. Both time courses are slowed in cells studied in normal Ringer's. Once established, the high resistance state is maintained as long as an outward current is applied. Hyperpolarizing inactivation occurs in normal Ringer's or with moderate excess K. Its onset is more rapid with stronger stimuli. During prolonged currents it is not maintained; i.e., there is a secondary increase in conductance. Hyperpolarizing inactivation responses exhibit a long refractory period, presumably because of persistence of this secondary increase in conductance.