Electrophysiological study of frog eggs at different stages of development. III) Ionic currents activated by intense hyperpolarization and depolarization of the oocyte at the final stage of vitellogenesis

In addition to K-selective channels, two kinds of voltage-dependent channels are present in the membrane of full-grown frog oocytes: 1) non-selective channels, activated by hyperpolarizing steps to potentials more negative than -80, -90 mV; 2) cationic channels, activated by depolarizing steps to potentials more positive than +30, +40 mV. The former are related to the inward rectification; the latter could contribute to the outward rectification of the I/V relationship. Therefore the membrane potential in full-grown oocytes tends to be maintained at a constant value due to the changes of permeability that follow possible potential variations occurring in both directions.     

Spontaneous action potentials and resting potential shifts in fertilized eggs of the tunicate Clavelina

Electrical activity in the fertilized egg of the tunicate Clavelina was studied with microelectrode recording and voltage clamp techniques. The resting potential could assume either of two stable values (approximately ?70 or ?30 mV) and could be shifted between these values by direct current stimulation. Spontaneous shifts between two stable resting potentials were also seen. Egg cells produced action potentials spontaneously and in response to depolarizing stimuli. Inward currents were carried by both Na and Ca ions and a prominent outward potassium current was seen with depolarization to voltages above ?15 mV. The steady-state current-voltage relationship (I–V curve) of the membrane showed two voltages where the net membrane current equaled zero: approximately ?35 and ?70 mV. Between these two voltages, membrane current was inward and carried by noninactivating Na and Ca currents. Inward rectification, which was blocked by external Rb, occurred at voltages below ?70 mV. The voltage dependence of inward rectification is thought by the authors to be important for establishing the more negative resting potential; it is also thought the presence of inward current which does not inactivate completely at voltages more negative than about ?20 mV is an important determinant of the more depolarized resting potential.     

三叉神经中脑核神经元膜的电学特性

用大鼠脑干脑片,给三叉神经中脑核79个神经元作了细胞内记录,测算了20个神经元膜的电学特性:静息电位-60.3±5.6mV;输入阻抗为10.5±5.4MΩ;时间常数1.3±0.5ms。电刺激可诱发动作电位,测算32个神经元的有关参数:阈电位-50—-55mV;波幅69.5±6.1mV;超射11.9±3.6mV;波宽0.8±0.2ms。TTX(0.3μmol/L)或无钠使之消失。通以长时程矩形波电流可引起200—250Hz的2—15个重复放电,但在通电停止前终止,TEA或4-AP可延长放电。膜电位-60—-55mV时在动作电位之后可看到阈下电位波动,它不受TTX的影响,无钙时消失,TEA或4-AP使波幅增大。静息电位去极化可使45个神经元中的40个发生外向整流作用,并被TEA,4-AP或无钙抑制,超极化则发生内向整流作用,Cs或无钠抑制之。灌流液中加入各种钾通道阻断药时神经元的稳态I-V曲线发生相应变化,提示I_(DR),l_A,I_(K(Ca))及I_Q可能都与静息时的膜电导有关。     

Electrophysiological properties of isolated rat liver cells

The electrophysiological properties of isolated rat liver cells were studied using the patch clamp method in whole-cell configuration. The membrane potential in isolated hepatocytes was -42 +/- 7 mV (n = 20). The input resistance (Rin) and the time constant (tau m) were 51 +/- 17 M (the range of 34 to 180 M omega) (n = 20) and 4.2 +/- 1.0 msec (the range of 3 to 16.5 ms) (n = 20). Assuming that the specific membrane capacitance is 1 microF/cm2, the membrane resistance and membrane capacitance were 42. +/- 9.0 K omega cm2 and 87 +/- 27 pF. These values indicate that isolated rat hepatocytes are not abnormally permeable or leaky. The current-voltage relationship was linear with no rectification. The depolarizing pulse from the resting potential did not induce fast or slow inward currents even when norepinephrine or high Ca2 (3.6 mM) were applied. This indicates that there is no voltage-sensitive Ca2+ channel in the isolated hepatocytes.     

Ionic permeability of K, Na, and Cl in potassium-depolarized nerve. Dependency on pH, cooperative effects, and action of tetrodotoxin.

The passive ionic membrane conductances (gj) and permeabilities (Pj) of K, Na, and Cl of crayfish (Procambarus clarkii) medial giant axons were determined in the potassium-depolarized axon and compared with that of the resting axon. Passive ionic conductances and permeabilities were found to be potassium dependent with a major conductance transition occurring around an external K concentration of 12-15 mM (Vm = -60 to -65 mV). The results showed that K, Na, and Cl conductances increased by 6.2, 6.9, and 27-fold, respectively, when external K was elevated from 5.4 to 40 mM. Permeability measurements indicated that K changed minimally with K depolarization while Na and Cl underwent an order increase in permeability. In the resting axon (K0 = 5.4 mM, pH = 7.0) PK = 1.33 X 10(-5), PCl = 1.99 X 10(-6), PNa = 1.92 X 10(-8) while in elevated potassium (K0 = 40 mM, pH 7.0), PK = 1.9 X 10(-5), PCl = 1.2 X 10(-5), and PNa = 2.7 X 10(-7) cm/s. When membrane potential is reduced to 40 mV by changes in internal ions, the conductance changes are initially small. This suggests that resting channel conductances depend also on ion environments seen by each membrane surface in addition to membrane potential. In elevated potassium, K, Na, and Cl conductances and permeabilities were measured from pH 3.8 to 11 in 0.2 pH increments. Here a cooperative transition in membrane conductance or permeability occurs when pH is altered through the imidazole pK (approximately pH 6.3) region. This cooperative conductance transition involves changes in Na and Cl but not K permeabilities. A Hill coefficient n of near 4 was found for the cooperative conductance transition of both the Na and Cl ionic channel which could be interpreted as resulting from 4 protein molecules forming each of the Na and Cl ionic channels. Tetrodotoxin reduces the Hill coefficient n to near 2 for the Na channel but does not affect the Cl channel. In the resting or depolarized axon, crosslinking membrane amino groups with DIDS reduces Cl and Na permeability. Following potassium depolarization, buried amino groups appear to be uncovered. The data here suggest that potassium depolarization produces a membrane conformation change in these ionic permeability regulatory components. A model is proposed where membrane protein, which forms the membrane ionic channels, is oriented with an accessible amino terminal group on the axon exterior. In this model the ionizable groups on protein and phospholipid have varied associations with the different ionic channel access sites for K, Na, and Cl, and these groups exert considerable control over ion permeation through their surface potentials.     

Properties of a tonically active, sodium-permeable current in mouse urinary bladder smooth muscle

Urinary bladder smooth muscle (UBSM) elicits depolarizing action potentials, which underlie contractile events of the urinary bladder. The resting membrane potential of UBSM is approximately -40 mV and is critical for action potential generation, with hyperpolarization reducing action potential frequency. We hypothesized that a tonic, depolarizing conductance was present in UBSM, functioning to maintain the membrane potential significantly positive to the equilibrium potential for K(+) (E(K); -85 mV) and thereby facilitate action potentials. Under conditions eliminating the contribution of K(+) and voltage-dependent Ca(2+) channels, and with a clear separation of cation- and Cl(-)-selective conductances, we identified a novel background conductance (I(cat)) in mouse UBSM cells. I(cat) was mediated predominantly by the influx of Na(+), although a small inward Ca(2+) current was detectable with Ca(2+) as the sole cation in the bathing solution. Extracellular Ca(2+), Mg(2+), and Gd(3+) blocked I(cat) in a voltage-dependent manner, with K(i) values at -40 mV of 115, 133, and 1.3 microM, respectively. Although UBSM I(cat) is extensively blocked by physiological extracellular Ca(2+) and Mg(2+), a tonic, depolarizing I(cat) was detected at -40 mV. In addition, inhibition of I(cat) demonstrated a hyperpolarization of the UBSM membrane potential and decreased the amplitude of phasic contractions of isolated UBSM strips. We suggest that I(cat) contributes tonically to the depolarization of the UBSM resting membrane potential, facilitating action potential generation and thereby a maintenance of urinary bladder tone.     

Effect of Mentha x piperita essential oil and monoterpenes on cucumber root membrane potential.

Peppermint (Mentha piperita L.) essential oil and its main components were assessed for their ability to interfere with plant plasma membrane potentials. Tests were conducted on root segments isolated from etiolated seedlings of cucumber (Cucumis sativus L.). Increasing the concentration of peppermint essential oil from 5 to 50 ppm caused a decrease in membrane potential (Vm) hyperpolarization of 10-3 mV, whereas concentrations from 100 up to 900 ppm caused an increasing depolarization of Vm (from 5 to 110 mV). When tested at 300 ppm, (+)-menthyl acetate, (-)-limonene and 1,8-cineole did not exert any significant effect on V(m), whereas (+)-menthofuran (73 mV), (+)-pulegone (85 mV), (+)-neomenthol (96 mV), (-)-menthol (105 mV) and (-)-menthone (111 mV) showed increased ability to depolarize V(m). A plot of log of octanol-water partition coefficient (K(ow)) against their depolarizing effect showed a significant negative correlation, suggesting that among all monoterpenoids increased membrane depolarization depends on lower K(ow). However, among monoterpene ketones, alcohols and furans, increased membrane depolarization is associated with a decline in water solubility. The possible effect of monoterpenoids on membrane ion fluxes is also discussed, since changes in the bioelectric potential of cells imply changes in the flux of ions across the plasma membrane     

Time-dependent actions of aluminates on membrane and action potentials of snail neurons

Aluminum (Al) is one of the elements, which is frequently subjected to experiments, however, the neurological observations with it are rather conflicting. The cause of this controversiality is not known but relates to some human disorders such as Alzheimer's disease and others as well. We studied the time-dependent actions of AlCl3 base solutions on resting membrane potential (Em), input resistance (Rin) and spike shape in giant neurons of the snail Helix pomatia L. at pH 7.7 and room temperature (22-24 degrees C) by use of intracellular technique. We reported significant differences in the effectiveness of the various Al solutions depending on the time of storage before use in the experiments (0, 2 and 6 days at room temperature). Freshly prepared and applied Al solutions caused a significant and dose-dependent depolarization with a concomitant decrease of Rin and the amplitude of the action potentials, but the 6 days solutions induced a hyperpolarization. Ouabain (0.1 mM) antagonized the hyperpolarization. The pH (7.1 or 7.7) and the time of the storage in combination also modified the direct membrane effects. Our experiments show that Al can induce differential membrane effects depending on the presence of various aluminum compounds. Namely, the predominate aluminum-monomer at pH 7.7 the Al(OH)4- might cause depolarization but the polynuclear aluminum complexes after polymerization of the monomers could hyperpolarize the neuronal membrane. We suppose, that the time-dependent equilibrium of various aluminum complexes plays a role in generating controversies in this field and emphasize again the importance of standardization of the experimental protocol.     

Electrophysiological control of ciliary motor responses in the ctenophorePleurobrachia

Prey capture by a tentacle of the ctenophore Pleurobrachia elicits a reversal of beat direction and increase in beat frequency of comb plates in rows adjacent to the catching tentacle (Tamm and Moss 1985). These ciliary motor responses were elicited in intact animals by repetitive electrical stimulation of a tentacle or the midsubtentacular body surface with a suction electrode. An isolated split-comb row preparation allowed stable intracellular recording from comb plate cells during electrically stimulated motor responses of the comb plates, which were imaged by high-speed video microscopy. During normal beating in the absence of electrical stimulation, comb plate cells showed no changes in the resting membrane potential, which was typically about -60 mV. Trains of electrical impulses (5/s, 5 ms duration, at 5-15 V) delivered by an extracellular suction electrode elicited summing facilitating synaptic potentials which gave rise to graded regenerative responses. High K+ artificial seawater caused progressive depolarization of the polster cells which led to volleys of action potentials. Current injection (depolarizing or release from hyperpolarizing current) also elicited regenerative responses; the rate of rise and the peak amplitude were graded with intensity of stimulus current beyond a threshold value of about -40 mV. Increasing levels of subthreshold depolarization were correlated with increasing rates of beating in the normal direction. Action potentials were accompanied by laydown (upward curvature of nonbeating plates), reversed beating at high frequency, and intermediate beat patterns. TEA increased the summed depolarization elicited by pulse train stimulation, as well as the size and duration of the action potentials. TEA-enhanced single action potentials evoked a sudden arrest, laydown and brief bout of reversed beating. Dual electrode impalements showed that cells in the same comb plate ridge experienced similar but not identical electrical activity, even though all of their cilia beat synchronously. The large number of cells making up a comb plate, their highly asymmetric shape, and their complex innervation and electrical characteristics present interesting features of bioelectric control not found in other cilia.     

Electrophysiological responses of crayfish oocytes to biogenic amines

Intracellular recordings were made from immature, growing oocytes of the crayfish Pacifastacus leniusciulus. Oocytes had a relatively negative resting potential of -74.7+/-2.2 mV (n=26; range -53 to -90) and a mean input resistance of 0.86+/-0.19 MOmega (n=22; range 0.17-3.3). Octopamine induced a long-lasting response involving biphasic changes in input resistance, together with bi- or multiphasic changes in membrane potential. The resistance-decreasing phase involved (in different oocytes) membrane hyperpolarization, depolarization or both. The resistance-increasing phase was usually a depolarization. The hyperpolarizing form of the resistance-decreasing response, and the depolarizing resistance-increasing response reversed in polarity at membrane potentials of (respectively) -90 and -92 mV, suggesting increases and decreases in K(+) conductance underly the biphasic changes in input resistance. The threshold concentration for the response was remarkably low (>10(-12) M) and showed little or no dose-dependence over the concentration range 10(-12)-10(-6) M. Similar responses were evoked by dopamine and serotonin (at 10(-9) M), although a higher proportion of oocytes responded to octopamine and/or dopamine than to serotonin.     

TEA-Sensitive Currents Contribute to Membrane Potential of Organ Surface Primo-node Cells in Rats

The primo-vascular (Bonghan) tissue has been identified in most tissues in the body, but its structure and functions are not yet well understood. We characterized electrophysiological properties of the cells of the primo-nodes (PN) on the surface of abdominal organs using a slice patch clamp technique. The most abundant were small round cells (~10 μm) without processes. These PN cells exhibited low resting membrane potential (−36 mV) and did not fire action potentials. On the basis of the current–voltage (I–V) relationships and kinetics of outward currents, the PN cells can be grouped into four types. Among these, type I cells were the majority (69%); they showed strong outward rectification in I–V relations. The outward current was activated rapidly and sustained without decay. Tetraethylammonium (TEA) dose-dependently blocked both outward and inward current (IC₅₀, 4.3 mM at ±60 mV). In current clamp conditions, TEA dose-dependently depolarized the membrane potential (18.5 mV at 30 mM) with increase in input resistance. The tail current following a depolarizing voltage step was reversed at −27 mV, and transient outward current like A-type K⁺ current was not expressed at holding potential of −80 mV. Taken together, the results demonstrate for the first time that the small round PN cells are heterogenous, and that, in type I cells, TEA-sensitive current with limited selectivity to K⁺ contributed to resting membrane potential of these cells.     

Acetylcholine receptors in monkey and rabbit oocytes

Membrane potential responses to acetylcholine (ACh, 10(-7)-10(-3 M) were investigated in monkey and rabbit ovarian oocytes. In monkey oocytes ACh most commonly elicited a short-latency hyperpolarization concomitant with a decreased membrane input resistance (Rin). Under voltage-clamp short-latency ACh currents had an equilibrium potential of approximately -40 mV. In rabbit oocytes responses to ACh consisted of an increase in Rin or of a depolarization with an equilibrium potential of approximately -15 mV. Curare, hexamethonium, and atropine (10(-5)-10(-3) M) did not block these ACh responses. Thus, the oocyte membrane in the rabbit contains ACh receptors that cannot be classified as either muscarinic or nicotinic.     

The steady-state distribution of gating charge in crayfish giant axons.

Progressive shifts of holding potential (Vh) in crayfish giant axons, from -140 to -70 mV, reduce gating currents seen in depolarizing steps (to 0 mV test potential) while proportionately increasing gating currents in hyperpolarizing steps (to -240 mV). The resulting sigmoid equilibrium charge distribution (Q-Vh curve) shows an effective valence of 1.9e and a midpoint of -100 mV. By contrast, Q-V curves obtained using hyperpolarizing and/or depolarizing steps from a single holding potential, change their "shape" depending on the chosen holding potential. For holding potentials at the negative end of the Q-Vh distribution (e.g., -140 mV), negligible charge moves in hyperpolarizing pulses and the Q-V curve can be characterized entirely from depolarizing voltage steps. The slope of the resulting simple sigmoid Q-V curve also indicates an effective valence of 1.9e. When the axon is held at less negative potentials significant charge moves in hyperpolarizing voltage steps. The component of the Q-V curve collected using hyperpolarizing pulses shows a significantly reduced slope (approximately 0.75e) by comparison with the 1.9e slope found using depolarizing pulses or from the Q-Vh curve. As holding potential is shifted in the depolarizing direction along the Q-Vh curve, an increasing fraction of total charge movement must be assessed in hyperpolarizing voltage steps. Thus charge moving in the low slope component of the Q-V curve increases as holding potential is depolarized, while charge moving with high apparent valence decreases proportionately. Additional results, together with simulations based on a simple kinetic model, suggest that the reduced apparent valence of the low slope component of the Q-V curve results from gating charge immobilization occurring at holding potential. Immobilization selectively retards that fraction of total charge moving in hyperpolarizing pulses. Misleading conclusions, as to the number and valence of the gating particles, may therefore be derived from Q-V curves obtained by other than depolarizing pulses from negative saturated holding potentials.     

Sodium currents in the giant axon of the crab Carcinus maenas

Measurements were made of the kinetics and steady-state properties of the sodium conductance changes in the giant axon of the crab Carcinus maenas. The conductance measurements were made in the presence of small concentrations of tetrodotoxin and as much electrical compensation as possible in order to minimize errors caused by the series resistance. After an initial delay of 10-150 microsec, the conductance increase during depolarizing voltage clamp pulses followed the Hodgkin-Huxley kinetics. Values of the time constant for the activation of the sodium conductance lay on a bell-shaped curve with a maximum under 180 microsec at -40 mV (at 18 degrees C). Values of the time constant for the inactivation of the sodium conductance were also fitted using a bell-shaped curve with a maximum under 7 msec at -70 mV. The effects of membrane potential on the fraction of Na channels available for activation studied using double pulse protocols suggest that hyperpolarizing potentials more negative than -100 mV lock a fraction of the Na channels in a closed conformation.     

Ionic mechanisms underlying the responses of off-center bipolar cells in the carp retina. I. Studies on responses evoked by light

Off-center bipolar cells show hyperpolarizing responses to spot illumination in the receptive field center and depolarization responses to an annulus in the surround. To understand the ionic mechanisms underlying these responses, we examined the current-voltage relationship of these bipolar cells, input resistance changes during their light-evoked responses, and the reversal potentials of these responses. Off-center bipolar cells generally showed inward rectification when they were hyperpolarized and outward rectification when they were strongly depolarized. The membrane potential at which the I-V relationship deviated from linearity varied in individual cells. Hyperpolarizing center responses were generally accompanied by a resistance increase, irrespective of signal inputs either from red- sensitive cones or from rods, and the response polarities reversed at greater than +50 mV. Depolarizing surround responses were accompanied by a resistance decrease with a reversal potential at about +28 mV (one case). From the above observations, it is suggested that the center responses are generated by a decrease in sodium conductance (gNa) and the surround response is generated by an increase in gNa.     

Maintained depolarization of synaptic terminals facilitates nerve-evoked transmitter release at a crayfish neuromuscular junction

Presynaptic and postsynaptic potentials were examined by intracellular recording at a crayfish neuromuscular junction. During normal synaptic transmission, the action potentials were recorded in the terminal region of the excitatory axon and postsynaptic responses were obtained in the muscle fibers. We found that it was possible to modify the synaptic transmission by applying depolarizing or hyperpolarizing currents through the presynaptic intracellular electrode. Typically, a 7-15 mV depolarization lasting longer than 50 msec leads to a large (500%) enhancement of transmitter release, even though the preterminal action potential is reduced in amplitude. Hyperpolarization increases the amplitude of the action potential, but slightly reduces the transmitter release. These results are different from those reported for other neuromuscular synapses and the squid giant synapse, but are similar in many respects to the results reported for several invertebrate central synapses. We conclude, first, that different synapses may have markedly different responses to conditioning by membrane polarization and, secondly, that maintained low-level depolarization may induce a potentiated state in the nerve terminal, perhaps brought about by slow entry of calcium.     

Isoform-specific lidocaine block of sodium channels explained by differences in gating

When depolarized from typical resting membrane potentials (V(rest) approximately -90 mV), cardiac sodium (Na) currents are more sensitive to local anesthetics than brain or skeletal muscle Na currents. When expressed in Xenopus oocytes, lidocaine block of hH1 (human cardiac) Na current greatly exceeded that of mu1 (rat skeletal muscle) at membrane potentials near V(rest), whereas hyperpolarization to -140 mV equalized block of the two isoforms. Because the isoform-specific tonic block roughly parallels the drug-free voltage dependence of channel availability, isoform differences in the voltage dependence of fast inactivation could underlie the differences in block. However, after a brief (50 ms) depolarizing pulse, recovery from lidocaine block is similar for the two isoforms despite marked kinetic differences in drug-free recovery, suggesting that differences in fast inactivation cannot entirely explain the isoform difference in lidocaine action. Given the strong coupling between fast inactivation and other gating processes linked to depolarization (activation, slow inactivation), we considered the possibility that isoform differences in lidocaine block are explained by differences in these other gating processes. In whole-cell recordings from HEK-293 cells, the voltage dependence of hH1 current activation was approximately 20 mV more negative than that of mu1. Because activation and closed-state inactivation are positively coupled, these differences in activation were sufficient to shift hH1 availability to more negative membrane potentials. A mutant channel with enhanced closed-state inactivation gating (mu1-R1441C) exhibited increased lidocaine sensitivity, emphasizing the importance of closed-state inactivation in lidocaine action. Moreover, when the depolarization was prolonged to 1 s, recovery from a "slow" inactivated state with intermediate kinetics (I(M)) was fourfold longer in hH1 than in mu1, and recovery from lidocaine block in hH1 was similarly delayed relative to mu1. We propose that gating processes coupled to fast inactivation (activation and slow inactivation) are the key determinants of isoform-specific local anesthetic action.     

Electrophysiological study of frog eggs at different stages of development. II) Outward rectification in oocytes at the final stage of vitellogenesis

Voltage-clamp experiments in full-grown frog oocytes, in a range of membrane potentials from 90 mV negative to 30 mV positive, have revealed the presence of voltage-dependent channels selective for K+, blocked by extracellular TEA. The percentage of open K+-channels increases with membrane depolarizations over a range from -40 mV to +10 mV, thus supporting the outward rectification in the I/V relationship. The current transport through the K+-channels open at different potential levels and in various [K+]o takes place in accordance with the constant-field assumptions. The leakage current of the oocyte membrane was found to be considerable large.     

Biophysical properties and slow voltage-dependent inactivation of a sustained sodium current in entorhinal cortex layer-II principal neurons: a whole-cell and single-channel study.

The functional and biophysical properties of a sustained, or "persistent," Na(+) current (I(NaP)) responsible for the generation of subthreshold oscillatory activity in entorhinal cortex layer-II principal neurons (the "stellate cells") were investigated with whole-cell, patch-clamp experiments. Both acutely dissociated cells and slices derived from adult rat entorhinal cortex were used. I(NaP), activated by either slow voltage ramps or long-lasting depolarizing pulses, was prominent in both isolated and, especially, in situ neurons. The analysis of the gating properties of the transient Na(+) current (I(NaT)) in the same neurons revealed that the resulting time-independent "window" current (I(NaTW)) had both amplitude and voltage dependence not compatible with those of the observed I(NaP), thus implying the existence of an alternative mechanism of persistent Na(+)-current generation. The tetrodotoxin-sensitive Na(+) currents evoked by slow voltage ramps decreased in amplitude with decreasing ramp slopes, thus suggesting that a time-dependent inactivation was taking place during ramp depolarizations. When ramps were preceded by increasingly positive, long-lasting voltage prepulses, I(NaP) was progressively, and eventually completely, inactivated. The V(1/2) of I(NaP) steady state inactivation was approximately -49 mV. The time dependence of the development of the inactivation was also studied by varying the duration of the inactivating prepulse: time constants ranging from approximately 6.8 to approximately 2.6 s, depending on the voltage level, were revealed. Moreover, the activation and inactivation properties of I(NaP) were such as to generate, within a relatively broad membrane-voltage range, a really persistent window current (I(NaPW)). Significantly, I(NaPW) was maximal at about the same voltage level at which subthreshold oscillations are expressed by the stellate cells. Indeed, at -50 mV, the I(NaPW) was shown to contribute to >80% of the persistent Na(+) current that sustains the subthreshold oscillations, whereas only the remaining part can be attributed to a classical Hodgkin-Huxley I(NaTW). Finally, the single-channel bases of I(NaP) slow inactivation and I(NaPW) generation were investigated in cell-attached experiments. Both phenomena were found to be underlain by repetitive, relatively prolonged late channel openings that appeared to undergo inactivation in a nearly irreversible manner at high depolarization levels (-10 mV), but not at more negative potentials (-40 mV).     

The calcium-independent transient outward potassium current in isolated ferret right ventricular myocytes. I. Basic characterization and kinetic analysis

Enzymatically isolated myocytes from ferret right ventricles (12-16 wk, male) were studied using the whole cell patch clamp technique. The macroscopic properties of a transient outward K+ current I(to) were quantified. I(to) is selective for K+, with a PNa/PK of 0.082. Activation of I(to) is a voltage-dependent process, with both activation and inactivation being independent of Na+ or Ca2+ influx. Steady-state inactivation is well described by a single Boltzmann relationship (V1/2 = -13.5 mV; k = 5.6 mV). Substantial inactivation can occur during a subthreshold depolarization without any measurable macroscopic current. Both development of and recovery from inactivation are well described by single exponential processes. Ensemble averages of single I(to) channel currents recorded in cell-attached patches reproduce macroscopic I(to) and indicate that inactivation is complete at depolarized potentials. The overall inactivation/recovery time constant curve has a bell-shaped potential dependence that peaks between -10 and -20 mV, with time constants (22 degrees C) ranging from 23 ms (-90 mV) to 304 ms (-10 mV). Steady-state activation displays a sigmoidal dependence on membrane potential, with a net aggregate half- activation potential of +22.5 mV. Activation kinetics (0 to +70 mV, 22 degrees C) are rapid, with I(to) peaking in approximately 5-15 ms at +50 mV. Experiments conducted at reduced temperatures (12 degrees C) demonstrate that activation occurs with a time delay. A nonlinear least- squares analysis indicates that three closed kinetic states are necessary and sufficient to model activation. Derived time constants of activation (22 degrees C) ranged from 10 ms (+10 mV) to 2 ms (+70 mV). Within the framework of Hodgkin-Huxley formalism, Ito gating can be described using an a3i formulation.