Ionic mechanisms underlying spontaneous CA1 neuronal firing in Ca2+-free solution

Hippocampal CA1 neurons exposed to zero-[Ca(2+)] solutions can generate periodic spontaneous synchronized activity in the absence of synaptic function. Experiments using hippocampal slices showed that, after exposure to zero-[Ca(2+)](0) solution, CA1 pyramidal cells depolarized 5-10 mV and started firing spontaneous action potentials. Spontaneous single neuron activity appeared in singlets or was grouped into bursts of two or three action potentials. A 16-compartment, 23-variable cable model of a CA1 pyramidal neuron was developed to study mechanisms of spontaneous neuronal bursting in a calcium-free extracellular solution. In the model, five active currents (a fast sodium current, a persistent sodium current, an A-type transient potassium current, a delayed rectifier potassium current, and a muscarinic potassium current) are included in the somatic compartment. The model simulates the spontaneous bursting behavior of neurons in calcium-free solutions. The mechanisms underlying several aspects of bursting are studied, including the generation of triplet bursts, spike duration, burst termination, after-depolarization behavior, and the prolonged inactive period between bursts. We show that the small persistent sodium current can play a key role in spontaneous CA1 activity in zero-calcium solutions. In particular, it is necessary for the generation of an after-depolarizing potential and prolongs both individual bursts and the interburst interval.     

Sodium currents in toad cardiac pacemaker cells

Cells in the pacemaker region of toad (Bufo marinus) sinus venosus had spontaneous rhythmic action potentials. The rate of firing of action potentials, the rate of diastolic depolarization and the maximum rate of rise of action potentials were reduced by TTX (10 nm to 1 m). Currents were recorded with the whole cell, tight seal technique from cells enzymatically dissociated from this region. Cells studied were identified as pacemaker cells by their characteristic morphology, spontaneous rhythmic action potential activity that could be blocked by cobalt but not by TTX and lack of inward rectification. When calcium, potassium and nonselective cation currents (I_f) activated by hyperpolarization were blocked, depolarization was seen to generate transient and persistent inward currents. Both were sodium currents: they were abolished by tetrodotoxin (10 to 100 nm), their reversal potential was close to the sodium equilibrium potential and their amplitude and reversal potential were influenced as expected for sodium currents when extracellular sodium ions were replaced with choline ions. The transient sodium current was activated at potentials more positive than –40 mV while the persistent sodium current was obvious at more negative potentials. It was concluded that, in toad pacemaker cells, TTX-sensitive sodium currents contributing both to the upstroke of action potentials and to diastolic depolarization may play an important role in setting heart rate.We thank the Australian National Heart Foundation for their support. D.A.S. is an NHMRC Senior Research Officer.     

Ionic currents influencing spontaneous firing and pacemaker frequency in dopamine neurons of the ventrolateral periaqueductal gray and dorsal raphe nucleus (vlPAG/DRN): A voltage-clamp and computational modelling study

Dopamine (DA) neurons of the ventrolateral periaqueductal gray (vlPAG) and dorsal raphe nucleus (DRN) fire spontaneous action potentials (APs) at slow, regular patterns in vitro but a detailed account of their intrinsic membrane properties responsible for spontaneous firing is currently lacking. To resolve this, we performed a voltage-clamp electrophysiological study in brain slices to describe their major ionic currents and then constructed a computer model and used simulations to understand the mechanisms behind autorhythmicity in silico. We found that vlPAG/DRN DA neurons exhibit a number of voltage-dependent currents activating in the subthreshold range including, a hyperpolarization-activated cation current (I_H), a transient, A-type, potassium current (I_A), a background, ‘persistent’ (I_NaP) sodium current and a transient, low voltage activated (LVA) calcium current (I_CaLVA). Brain slice pharmacology, in good agreement with computer simulations, showed that spontaneous firing occurred independently of I_H, I_A or calcium currents. In contrast, when blocking sodium currents, spontaneous firing ceased and a stable, non-oscillating membrane potential below AP threshold was attained. Using the DA neuron model we further show that calcium currents exhibit little activation (compared to sodium) during the interspike interval (ISI) repolarization while, any individual potassium current alone, whose blockade positively modulated AP firing frequency, is not required for spontaneous firing. Instead, blockade of a number of potassium currents simultaneously is necessary to eliminate autorhythmicity. Repolarization during ISI is mediated initially via the deactivation of the delayed rectifier potassium current, while a sodium background ‘persistent’ current is essentially indispensable for autorhythmicity by driving repolarization towards AP threshold.     

A voltage-dependent persistent sodium current in mammalian hippocampal neurons

Currents generated by depolarizing voltage pulses were recorded in neurons from the pyramidal cell layer of the CA1 region of rat or guinea pig hippocampus with single electrode voltage-clamp or tight-seal whole-cell voltage-clamp techniques. In neurons in situ in slices, and in dissociated neurons, subtraction of currents generated by identical depolarizing voltage pulses before and after exposure to tetrodotoxin revealed a small, persistent current after the transient current. These currents could also be recorded directly in dissociated neurons in which other ionic currents were effectively suppressed. It was concluded that the persistent current was carried by sodium ions because it was blocked by TTX, decreased in amplitude when extracellular sodium concentration was reduced, and was not blocked by cadmium. The amplitude of the persistent sodium current varied with clamp potential, being detectable at potentials as negative as -70 mV and reaching a maximum at approximately -40 mV. The maximum amplitude at -40 mV in 21 cells in slices was -0.34 +/- 0.05 nA (mean +/- 1 SEM) and -0.21 +/- 0.05 nA in 10 dissociated neurons. Persistent sodium conductance increased sigmoidally with a potential between -70 and -30 mV and could be fitted with the Boltzmann equation, g = gmax/(1 + exp[(V' - V)/k)]). The average gmax was 7.8 +/- 1.1 nS in the 21 neurons in slices and 4.4 +/- 1.6 nS in the 10 dissociated cells that had lost their processes indicating that the channels responsible are probably most densely aggregated on or close to the soma. The half-maximum conductance occurred close to -50 mV, both in neurons in slices and in dissociated neurons, and the slope factor (k) was 5-9 mV. The persistent sodium current was much more resistant to inactivation by depolarization than the transient current and could be recorded at greater than 50% of its normal amplitude when the transient current was completely inactivated. Because the persistent sodium current activates at potentials close to the resting membrane potential and is very resistant to inactivation, it probably plays an important role in the repetitive firing of action potentials caused by prolonged depolarizations such as those that occur during barrages of synaptic inputs into these cells.     

A new scorpion toxin with a very high affinity for sodium channels. An electrophysiological study

The neurotoxic action of toxin gamma from the venom of the Brazilian scorpion Tityus serrulatus (TiTx gamma) has been investigated in cultured mouse neuroblastoma cells (N1E115) using the suction pipette technique. Addition of 14 to 53 nM TiTx gamma to the external solution causes nerve cell membrane depolarization, membrane potential oscillations and spontaneous action potentials within 10 min. None of these effects were observed within 15 min after application of 1 microM toxin IV from Centruroides sculpturatus venom. Under voltage clamp the amplitude of the sodium current evoked by test pulses to potentials more positive than -30 mV is reversibly reduced by 50% after 17 to 105 nM TiTx gamma. On the other hand, a sodium current component appears after TiTx gamma at test pulse potentials between -70 and -40 mV, for which no sodium current is observed in the control experiment. The outward potassium current is not significantly affected by the highest TiTx gamma concentrations used. The potential-dependence of inactivation of the sodium current component that is induced by TiTx gamma is shifted by -30 mV with respect to control values. The local anaesthetic procain at 1 mM discriminates between the two populations of sodium channels observed in the presence of TiTx gamma.     

A transient voltage-dependent outward current in cultured cerebellar granules

Granule cells were dissociated from rat cerebella with a procedure that yields a 98% pure cell population. Potassium currents in these cells were studied using the patch-clamp technique. Depolarizing pulses of 10 mV step and 100 ms duration from a holding potential of –80 mV elicited two different potassium outward currents: a transient, low-voltage activated component and a long lasting, high-voltage activated component. At +30 mV, the total current reached an amplitude of 2 nA (mean value of 15 experiments). The reversal potential of the transient current, estimated by measuring tail currents, was –77 mV, close to that predicted by the Nernst equation. The transient current was half inactivated with a holding potential of –78 mV and completely inactivated with –50 mV or more positive holding potentials. Finally, the current decay could be fitted by the sum of two exponentials with time constants of about 20 and 250 ms.     

Voltage gated ionic channels in rat cultured astrocytes, reactive astrocytes and an astrocyte-oligodendrocyte progenitor cell

Astrocytes (both type 1 and type 2), cultured from the central nervous system of newborn or 7 day old rats show voltage gated sodium and potassium channels that are activated when the membrane is depolarized to greater than -40 mV. The sodium channels in these cells have an h-infinity curve similar to that of nodal membranes but the activation (peak current-voltage) curves are shifted along the voltage axis by about +30 mV. These sodium currents are blocked only by high concentrations of tetrodotoxin. The voltage activated potassium currents in both types of astrocyte show at least two components; an inactivating component that is suppressed at holding potentials of greater than -40 mV and a persistent, non-inactivating current. Several types of single channel currents were observed in outside-out membrane patches from type 2 astrocytes. One type of potassium channel showed inactivation on depolarization and may contribute to the whole-cell inactivating current. In contrast, oligodendrocytes showed no obvious voltage gated membrane channels. The properties of the type 2 astrocyte-oligodendrocyte progenitor cell were investigated in two ways: 1) by examination of cells just beginning to differentiate along the "electrically silent" oligodendrocyte pathway or 2) by recording from progenitor cells cultured for 24 hours in the presence of cycloheximide to block the appearance of new membrane channels. In both cases, voltage gated inward (sodium) and outward (potassium) currents were noted. The outward current response showed both an inactivating and a non-inactivating component. Similar voltage activated inward and outward membrane currents were noted in reactive astrocytes freshly isolated (3-6 hours) from lesioned areas of adult rat brains.(ABSTRACT TRUNCATED AT 250 WORDS)     

The effect of temperature on the outward currents in the soma of molluscan neurones in voltage-clamp conditions.

The delayed outward current in snail neurones was separated into two components with different temperature sensitivity: (i) a persistent component and (ii) a transient (inactivating) component. The effect of cooling on the value of the transient current is strongly dependent upon the value of the conditioning potential. It was supposed that cooling causes a decrease in the negative surface potential in the vicinity of the potassium pathways and removes their inactivation. Simultaneously cooling depresses the potassium conductance. The effect on surface potential is more distinct with conditioning potentials at which a significant fraction of the transient outward current is inactivated. The effect of cooling on the transient component of the fast outward current was similar to that on the transient component of the delayed outward current.     

成年蜜蜂脑神经细胞的培养和电生理特征

为了研究杀虫剂等对蜜蜂毒性作用的神经机制,需在体外建立成年蜜蜂脑神经细胞的分离培养和电生理记录技术并研究其正常电生理特征,而对成年蜜蜂脑神经细胞的分离培养和电生理特性的研究报道甚少。我们采用酶解和机械吹打相结合的方法获得了数量较多且活力较好的成年意大利蜜蜂Apis mellifera脑神经细胞,并用全细胞膜片钳技术研究了成年意大利蜜蜂脑神经细胞对电流和电压刺激的反应,获得了成年意蜂脑神经细胞的基本电生理特征以及钠电流和钾电流的特性。全细胞电流钳的记录结果表明,在体外培养条件下,细胞无自发放电发生,注射电流后仅引起细胞单次放电,引起细胞放电的阈电流平均为60.8±63 pA; 细胞动作电位产生的阈电位平均为−27.4±2.3 mV。用全细胞电压钳记录了神经细胞的钠电流和钾电流。钠电流的分离是在电压刺激下通过阻断钾通道和钙通道实现。细胞的内向钠电流在指令电压为−40～−30 mV左右激活,−10 mV达峰值,钠通道的稳态失活电压V_1/2为−58.4 mV; 外向钾电流成份至少包括较小的快速失活钾电流和和较大的缓慢失活钾电流（占总钾电流的80%）,其半激活膜电位V_1/2为3.86 mV,无明显的稳态失活。结果提示缓慢失活钾电流的特征可能是细胞单次放电的机制之一。     

Voltage-sensitive calcium flux promoted by vesicles in an isolated cardiac sarcolemma preparation

Summary The effect of membrane potential on the vesicular uptake of calcium in an isolated cardiac sarcolemma preparation from canine ventricle was evaluated. Membrane potentials were developed by the establishment of potassium gradients across the vesicular membranes. In the presence of valinomycin, the fluorescence changes of the voltage sensitive dye, diS-C₃-(5) were consistent with the development of potassium equilibrium potentials. Using EGTA to remove endogenous calcium from the preparation and to maintain a low intravesicular calcium concentration over time, the uptake of calcium was linear from 5 to 100 sec, in the absence of sodium, at both –98 and –1 mV. The rate of calcium uptake (calcium influx) was approximately twofold greater at –1 mV than at –98 mV, and prepolarization of the membrane potential to –98 mV did not enhance calcium influx upon subsequent depolarization to –1 mV. Hence, calcium influx was voltage-sensitive but not depolarization-induced and did not inactivate with time. Furthermore, the calcium influx was not inhibited by the organic calcium antagonists, which suggests that this flux did not occur via the transient calcium channel. Evaluation of calcium influx over a wide range of membrane potentials produced a profile consistent with the hypothesis that calcium entered the vesicles through the pathway responsible for the persistent inward current observed in voltage-clamped isolated myocytes. A model was proposed to account for these results.     

Ionic currents in dispersed chemoreceptor cells of the mammalian carotid body

Ionic currents of enzymatically dispersed type I and type II cells of the carotid body have been studied using the whole cell variant of the patch-clamp technique. Type II cells only have a tiny, slowly activating outward potassium current. By contrast, in every type I chemoreceptor cell studied we found (a) sodium, (b) calcium, and (c) potassium currents. (a) The sodium current has a fast activation time course and an activation threshold at approximately -40 mV. At all voltages inactivation follows a single exponential time course. The time constant of inactivation is 0.67 ms at 0 mV. Half steady state inactivation occurs at a membrane potential of approximately -50 mV. (b) The calcium current is almost totally abolished when most of the external calcium is replaced by magnesium. The activation threshold of this current is at approximately -40 mV and at 0 mV it reaches a peak amplitude in 6-8 ms. The calcium current inactivates very slowly and only decreases to 27% of the maximal value at the end of 300-ms pulses to 40 mV. The calcium current was about two times larger when barium ions were used as charge carriers instead of calcium ions. Barium ions also shifted 15-20 mV toward negative voltages the conductance vs. voltage curve. Deactivation kinetics of the calcium current follows a biphasic time course well fitted by the sum of two exponentials. At -80 mV the slow component has a time constant of 1.3 +/- 0.4 ms whereas the fast component, with an amplitude about 20 times larger than the slow component, has a time constant of 0.16 +/- 0.03 ms. These results suggest that type I cells have predominantly fast deactivating calcium channels. The slow component of the tails may represent the activity of a small population of slowly deactivating calcium channels, although other possibilities are considered. (c) Potassium current seems to be mainly due to the activity of voltage-dependent potassium channels, but a small percentage of calcium-activated channels may also exist. This current activates slowly, reaches a peak amplitude in 5-10 ms, and thereafter slowly inactivates. Inactivation is almost complete in 250-300 ms. The potassium current is reversibly blocked by tetraethylammonium. Under current-clamp conditions type I cells can spontaneously fire large action potentials. These results indicate that type I cells are excitable and have a variety of ionic conductances. We suggest a possible participation of these conductances in chemoreception.     

Analysis of spontaneous electrical activity in cerebellar Purkinje cells acutely isolated from postnatal rats

Whole-cell patch recording techniques were used to analyze spontaneous electrical activity in cerebellar Purkinje cells acutely isolated from postnatal rats. Spontaneous activity was present in 65% of the cells examined, and it included simple and complex firing patterns which persisted under conditions that eliminated residual or reformed synaptic contacts. Under voltage clamp, both spontaneous and quiescent cells displayed similar voltage-dependent conductances. Inward current was carried by Na⁺ through tetrodotoxin (TTX)-sensitive channels and by Ca²⁺ through P-type and T-type Ca channels. P-type current was present in all cells examined. T-type current was found in <50%, and it did not correlate with spontaneous activity. We found no evidence of a transient (A-type) potassium current or hyperpolarization-activated cationic current in either spontaneous or quiescent cells. Spontaneous activity did correlate with a lower activation threshold of the Na current, resulting in substantial overlap of the activation and inactivation curves. TTX reduced the holding current of spontaneous cells clamped between −50 and −30 mV, consistent with the presence of a Na "window" current. We were unable, however, to measure a persistent component of the Na current using voltage steps, a result which may reflect the complex gating properties of Na channels. An Na window current could provide the driving force underlying spontaneous activity, as well as plateau potentials, in Purkinje cells. © 1997 John Wiley & Sons, Inc. J Neurobiol 33: 18–32, 1997     

Automaticity in cardiac cells.

Automaticity is the result of dynamic changes in transmembrane currents during electrical diastole. It is readily demonstrated in most cardiac cell types. In all four cardiac cell types studied by the voltage clamp technique (Purkinje, ventricular, atrial, and sino-atrial node fibers), the major change detected during diastolic depolarization is a decrease in outward current. This decrease in a repolarizing current (largely potassium mediated) permits an inward current (sodium and/or calcium mediated) to depolarize the cell.All four cardiac cell types appear to possesess a time-dependent potassium conductance which controls the decrease in outward current over the ?70 to ?30 mV potential range. Purkinje fibers manifest an additional conductance which is responsible for automaticity in this type of cell at potentials between ?100 and ?70 mV.     

A delayed rectifier current is modulated by the circadian pacemaker in Bulla

Basal retinal neurons of the marine mollusc Bulla gouldiana continue to express a circadian modulation of their membrane conductance for at least two cycles in cell culture. Voltage-dependent currents of these pacemaker cells were recorded using the whole-cell perforated patch-clamp technique to characterize outward currents and investigate their putative circadian modulation. Three components of the outward potassium current were identified. A transient outward current (IA) was activated after depolarization from holding potentials greater than -30 mV, inactivated with a time constant of 50 ms, and partially blocked by 4-aminopyridine (1-5 mM). A Ca(2+)-dependent potassium current (IK(Ca)) was activated by depolarization to potentials more positive than -10 mV and was blocked by removing Ca2+ from the bath or by applying the Ca2+ channel blockers Cd2+ (0.1-0.2 mM) and Ni2+ (1-5 mM). A sustained Ca(2+)-independent current component including the delayed rectifier current (IK) was recorded at potentials positive to -20 mV in the absence of extracellular Na+ and Ca2+ and was partially blocked by tetraethylammonium chloride (TEA, 30mM). Whole-cell currents recorded before and after the projected dawn and normalized to the cell capacitance revealed a circadian modulation of the delayed rectifier current (IK). However, the IA and IK(Ca) currents were not affected by the circadian pacemaker.     

Subthreshold sodium current from rapidly inactivating sodium channels drives spontaneous firing of tuberomammillary neurons

A role for "persistent," subthreshold, TTX-sensitive sodium current in driving the pacemaking of many central neurons has been proposed, but this has been impossible to test pharmacologically. Using isolated tuberomammillary neurons, we assessed the role of subthreshold sodium current in pacemaking by performing voltage-clamp experiments using a cell's own pacemaking cycle as voltage command. TTX-sensitive sodium current flows throughout the pacemaking cycle, even at voltages as negative as -70 mV, and this current is sufficient to drive spontaneous firing. When sodium channels underlying transient current were driven into slow inactivation by rapid stimulation, persistent current decreased in parallel, suggesting that persistent sodium current originates from subthreshold gating of the same sodium channels that underlie the phasic sodium current. This behavior of sodium channels may endow all neurons with an intrinsic propensity for rhythmic, spontaneous firing.     

Ion Levels and Membrane Potential in Chick Heart Tissue and Cultured Cells

Intracellular concentrations of sodium and potassium as well as resting potentials and overshoots have been determined in heart tissue from chick embryos aged 2–18 days. Intracellular potassium declined from 167 mM at day 2 to 117–119 mM at days 14–18. Intracellular sodium remained nearly constant at 30–35 mM during the same period. The mean resting potential increased from -61.8 mV at day 3 to about -80 mV at days 14–18. The mean overshoot during the same period increased from 12 to 30 mV. P_Na/P_K calculated from the ion data and resting potentials declined from 0.08 at day 3 to 0.01 at days 14–18. Thus, the development of embryonic chick heart during days 2–14 is characterized by a declining intracellular potassium concentration and an increasing resting potential and overshoot. Heart cells from 7- to 8-day embryos, cultured either in monolayer or reassociated into aggregates, were compared with intact tissue of the same age. The intracellular concentrations of sodium and potassium were similar in the three preparations and cultured cells responded to incubation in low potassium medium or treatment with ouabain in a manner similar to that of intact tissue. Resting potentials and overshoots were also similar in the three preparations.     

Ionic currents in cardiac myocytes of squid, Alloteuthis subulata

This paper provides the first study of voltage-sensitive membrane currents present in heart myocytes from cephalopods. Whole cell patch clamp recordings have revealed six different ionic currents in myocytes freshly dissociated from squid cardiac tissues (branchial and systemic hearts). Three types of outward potassium currents were identified: first, a transient outward voltage-activated A-current (I_A), blocked by 4-aminopyridine, and inactivated by holding the cells at a potential of −40 mV; second, an outward, voltage-activated, delayed rectifier current with a sustained time course (I_K); and third, an outward, calcium-dependent, potassium current (I_K(Ca)) sensitive to Co²⁺ and apamin, and with the characteristic N-shaped current voltage relationship. Three inward voltage-activated currents were also identified. First, a rapidly activating and inactivating, sodium current (I_Na), blocked by tetrodotoxin, inactivated at holding potentials more positive than −40 mV, and abolished when external sodium was replaced by choline. Second, an L-type calcium current (I_Ca,L) with a sustained time course, suppressed by nifedipine or Co²⁺, and enhanced by substituting Ca²⁺ for Ba²⁺ in the external medium. The third inward current was also carried by calcium ions, but could be distinguished from the L-type current by differences in its voltage dependence. It also had a more transient time course, was activated at more negative potentials, and resembled the previously described low-voltage-activated, T-type calcium current. Accepted: 24 September 1999     

Properties of the calcium-activated chloride current in heart

We used the whole cell patch clamp technique to study transient outward currents of single rabbit atrial cells. A large transient current, IA, was blocked by 4-aminopyridine (4AP) and/or by depolarized holding potentials. After block of IA, a smaller transient current remained. It was completely blocked by nisoldipine, cadmium, ryanodine, or caffeine, which indicates that all of the 4AP-resistant current is activated by the calcium transient that causes contraction. Neither calcium-activated potassium current nor calcium-activated nonspecific cation current appeared to contribute to the 4AP-resistant transient current. The transient current disappeared when ECl was made equal to the pulse potential; it was present in potassium-free internal and external solutions. It was blocked by the anion transport blockers SITS and DIDS, and the reversal potential of instantaneous current-voltage relations varied with extracellular chloride as predicted for a chloride-selective conductance. We concluded that the 4AP-resistant transient outward current of atrial cells is produced by a calcium-activated chloride current like the current ICl(Ca) of ventricular cells (1991. Circulation Research. 68:424-437). ICl(Ca) in atrial cells demonstrated outward rectification, even when intracellular chloride concentration was higher than extracellular. When ICa was inactivated or allowed to recover from inactivation, amplitudes of ICl(Ca) and ICa were closely correlated. The results were consistent with the view that ICl(Ca) does not undergo independent inactivation. Tentatively, we propose that ICl(Ca) is transient because it is activated by an intracellular calcium transient. Lowering extracellular sodium increased the peak outward transient current. The current was insensitive to the choice of sodium substitute. Because a recently identified time-independent, adrenergically activated chloride current in heart is reduced in low sodium, these data suggest that the two chloride currents are produced by different populations of channels.     

The membrane potential of Ehrlich ascites tumor cells microelectrode measurements and their critical evaluation

Summary Intracellular potentials were measured, using a piezoelectric electromechanical transducer to impale Ehrlich ascites tumor cells with capillary microelectrodes. In sodium Ringer's, the potential immediately after the penetration was –24±7 mV, and decayed to a stable value of about –8 mV within a few msec. The peak potentials disappeared in potassium Ringer's and reappeared immediately after resuspension in sodium. Ringer's, whereas the stable potentials were only slightly influenced by the change of medium. The peak potential is in good agreement with the Nernst potential for chloride. This is also the case when cell sodium and potassium have been changed by addition of ouabain. It is concluded that the peak potentials represent the membrane potential of the unperturbed cell, and that chloride is in electrochemical equilibrium across the cell membrane.The membrane potential of about –11 mV previously reported corresponds to the stable potential in this study, and is considered as a junction potential between damaged cells and their environment. Similar potential differences were recorded between a homogenate of cells and Ringer's.The apparent membrane resistance of Ehrlich cells was about 70 cm². This is two orders of magnitude less than the value calculated from³⁶Cl fluxes, and may, in part, represent a leak in the cell membrane.For comparison, the influence of an eventual leak on measurements in red cells and mitochondria is discussed.     

A slow voltage-activated potassium current in rat vagal neurons.

Potassium currents play a key role in controlling the excitability of neurons. In this paper we describe the properties of a novel voltage-activated potassium current in neurons of the rat dorsal motor nucleus of the vagus (DMV). Intracellular recordings were made from DMV neurons in transverse slices of the medulla. Under voltage clamp, depolarization of these neurons from hyperpolarized membrane potentials (more negative than -80 mV) activated two transient outward currents. One had fast kinetics and had properties similar to A-currents. The other current had an activation threshold of around -95 mV (from a holding potential -110 mV) and inactivated with a time constant of about 3s. It had a reversal potential close to the potassium equilibrium potential. This current was not calcium dependent and was not blocked by 4-aminopyridine (5 mM), catechol (5 mM) or tetraethylammonium (20 mM). It was completely inactivated at the resting membrane potential. This current therefore represents a new type of voltage-activated potassium current. It is suggested that this current might act as a brake to repetitive firing when the neuron is depolarized from membrane potentials negative to the resting potential.