We examined the development of K+ secretion after removing Cl- from the basolateral surface of isolated skins of Rana temporaria using noise analysis. K+ secretion was defined by the appearance of a Lorentzian component in the power density spectrum (PDS) when Ba2+ was present in the apical bath (0.5 mM). No Lorentzians were observed when tissues were bathed in control, NaCl Ringer solution. Replacement of basolateral Cl- by gluconate, nitrate, or SO4- (0-Clb) yielded Lorentzians with corner frequencies near 25 Hz, and plateau values (So) that were used to estimate the magnitude of K+ secretion through channels in the apical cell membranes of the principal cells. The response was reversible and reproducible. In contrast, removing apical Cl- did not alter the PDS. Reduction of basolateral Cl- to 11.5 mM induced Lorentzians, but with lower values of So. Inhibition of Na+ transport with amiloride or by omitting apical Na+ depressed K+ secretion but did not prevent its appearance in response to 0-Clb. Using microelectrodes, we observed depolarization of the intracellular voltage concomitant with increased resistance of the basolateral membrane after 0-Clb. Basolateral application of Ba2+ to depolarize cells also induced K+ secretion. Because apical conductance and channel density are unchanged after 0-Clb, we conclude that K+ secretion is "induced" simply by an increase of the electrical driving force for K+ exit across this membrane. Repolarization of the apical membrane after 0-Clb eliminated K+ secretion, while further depolarization increased the magnitude of the secretory current. The cell depolarization after 0-Clb is most likely caused directly by a decrease of the basolateral membrane K+ conductance. Ba2(+)-induced Lorentzians also were elicited by basolateral hypertonic solutions but with lower values of So, indicating that cell shrinkage per se could not entirely account for the response to 0-Clb and that the effects of 0-Clb may be partly related to a fall of intracellular Cl-.

Isolated epithelia of frog skin were prepared with collagenase, and the cells were punctured with intracellular microelectrodes across their apical (outer) and basolateral (inner) surfaces. Regardless of the route of cell puncture, the intracellular voltage (Vosc) in short-circuited isolated epithelia was markedly negative, averaging -70.4 mV for apical punctures and -91.6 mV for basolateral punctures. As in intact epithelia, amiloride outside caused the Vosc to become more negative (means of -96.7 and -101.8 mV), with a concomitant increase in the resistance of the apical barrier. Increasing the [K)i of the basolateral solution from 2.4 to 8.0 or 14.4 mM caused rapid step depolarization (5-10 s) of the Vosc under transepithelial Na transporting and amiloride-inhibited conditions of Na transport, with the delta Vosc ranging between 23.9 and 68.3 mV per decade change of [K]i. The finding that the Vosc of isolated epithelia of frog skin is independent of the route of cell penetration is consistent with the notion that the cells of the stratified epithelium are electrically coupled (functional syncitium). Moreover, the isolated epithelium can serve as a useful preparation, especially in studies designed to investigate the properties of the basolateral surfaces of cells.

Studies were done with isolated frog skin to determine the effects of 10(-4) M ouabain on the electrophysiological parameters of outer and inner barriers of the Na-transporting cells. Microelectrodes were used to impale the skins from the outer surface to determine the intracellular voltages (Vsco) under conditions of short-circuiting and under conditions where a voltage clamp was used to vary the transepithelial voltage, VT. From this, the electrical resistances of outer (Rfo) and inner (RI) barriers were estimated. In addition, the driving force for active transepithelial Na transport (ENa = E'1) was estimated from the values of VT when the Vo = 0 mV (Helman and Fisher. 1977. J. Gen. Physiol. 69: 571-604). Studies were done with skins bathed with the usual 2.4 meq/liter [K]i in the inner solution as well as with reduced [K]i of 0.5 and 0 meq/liter. Characteristically, the responses to ouabain could be described by an initial rapid phase (5-10 min) during which time the Ri was increased markedly and the E'1 was decreased from control values. Thereafter, during the slow phases of the response, the resistances of both outer and inner barriers increased continuously and markedly with time leading ultimately to essentially complete inhibition of the short-circuit current. Similar studies were done with skins exposed to 10(-4) M amiloride in the outer solution. Although estimates of Ri could not be obtained under these conditions, the effects on the Vsco and E'1 were similar to those observed for the Na-transporting skins. However, the magnitudes of the effects were less and relatively slower than observed for the Na-transporting skins. The results of these studies were analyzed within the context of a proposed electrical model that takes into account the observation that the magnitude of the voltage at the inner barrier appears to exceed the equilibrium potential for K especially when transepithelial Na transport is inhibited at the apical barrier of the cells.