Divalent ion trapping inside potassium channels of human T lymphocytes

Using the patch-clamp whole-cell recording technique, we investigated the influence of external Ca2+, Ba2+, K+, Rb+, and internal Ca2+ on the rate of K+ channel inactivation in the human T lymphocyte-derived cell line, Jurkat E6-1. Raising external Ca2+ or Ba2+, or reducing external K+, accelerated the rate of the K+ current decay during a depolarizing voltage pulse. External Ba2+ also produced a use-dependent block of the K+ channels by entering the open channel and becoming trapped inside. Raising internal Ca2+ accelerated inactivation at lower concentrations than external Ca2+, but increasing the Ca2+ buffering with BAPTA did not affect inactivation. Raising [K+]o or adding Rb+ slowed inactivation by competing with divalent ions. External Rb+ also produced a use-dependent removal of block of K+ channels loaded with Ba2+ or Ca2+. From the removal of this block we found that under normal conditions approximately 25% of the channels were loaded with Ca2+, whereas under conditions with 10 microM internal Ca2+ the proportion of channels loaded with Ca2+ increased to approximately 50%. Removing all the divalent cations from the external and internal solution resulted in the induction of a non-selective, voltage-independent conductance. We conclude that Ca2+ ions from the outside or the inside can bind to a site at the K+ channel and thereby block the channel or accelerate inactivation.     

The role of calcium ions in the closing of K channels

The effects of external Ca ion on K channel properties were studied in squid giant axons. Increasing the Ca concentration from 20 to 100 mM slowed K channel opening, and was kinetically equivalent to decreasing the depolarizing step by approximately 25 mV. The same Ca increase had a much smaller effect on closing kinetics, equivalent to making the membrane potential more negative by approximately mV. With regard to the conductance-voltage curve, this Ca increase was about equivalent to decreasing the depolarizing step by approximately 10 mV. The presence of K or Rb in the bath slowed closing kinetics and made the time course more complex: there were pronounced slow components in Rb and, to a lesser extent, in K. Increasing the Ca concentration strongly antagonized the slowing caused by Rb or K. Thus, Ca has a strong effect on closing kinetics only in the presence of these monovalent cations. Rb and K do not significantly alter opening kinetics, nor do they alter Ca's ability to slow opening kinetics. High Ca slightly affects the instantaneous I-V curve by selectively depressing inward current at negative voltages. The results imply that Ca has two actions on K channels, and in only one, the action on closing, does it compete with monovalent cations. We propose (a) that opening kinetics are slowed by binding of Ca to negatively charged parts of the gating apparatus that are at the external surface of the channel protein when the channel is closed; monovalent cations do not compete effectively in this action; (b) Ca (or possibly Mg) normally occupies closed channels and has a latching effect. External K or Rb competes with Ca for channel occupancy. Channels close sluggishly when occupied by a monovalent cation and tend to reopen. Thus, slow closing results from occupancy by K or Rb instead of Ca. The data are well fit by a model based on these ideas.     

Selectivity and gating of the type L potassium channel in mouse lymphocytes

Type l voltage-gated K+ channels in murine lymphocytes were studied under voltage clamp in cell-attached patches and in the whole-cell configuration. The kinetics of activation of whole-cell currents during depolarizing pulses could be fit by a single exponential after an initial delay. Deactivation upon repolarization of both macroscopic and microscopic currents was mono-exponential, except in Rb-Ringer or Cs-Ringer solution in which tail currents often displayed "hooks," wherein the current first increased or remained constant before decaying. In some cells type l currents were contaminated by a small component due to type n K+ channels, which deactivate approximately 10 times slower than type l channels. Both macroscopic and single channel currents could be dissected either kinetically or pharmacologically into these two K+ channel types. The ionic selectivity and conductance of type l channels were studied by varying the internal and external permeant ion. With 160 mM K+ in the cell, the relative permeability calculated from the reversal potential with the Goldman-Hodgkin-Katz equation was K+ (identical to 1.0) greater than Rb+ (0.76) greater than NH4+ = Cs+ (0.12) much greater than Na+ (less than 0.004). Measured 30 mV negative to the reversal potential, the relative conductance sequence was quite different: NH4+ (1.5) greater than K+ (identical to 1.0) greater than Rb+ (0.5) greater than Cs+ (0.06) much greater than Na+, Li+, TMA+ (unmeasurable). Single channel current rectification resembled that of the whole-cell instantaneous I-V relation. Anomalous mole-fraction dependence of the relative permeability PNH4/PK was observed in NH4(+)-K+ mixtures, indicating that the type l K+ channel is a multi-ion pore. Compared with other K+ channels, lymphocyte type l K+ channels are most similar to "g12" channels in myelinated nerve.     

Potassium channel block by internal calcium and strontium

We show that intracellular Ca blocks current flow through open K channels in squid giant fiber lobe neurons. The block has similarities to internal Sr block of K channels in squid axons, which we have reexamined. Both ions must cross a high energy barrier to enter the blocking site from the inside, and block occurs only with millimolar concentrations and with strong depolarization. With Sr (axon) or Ca (neuron) inside, IK is normal in time course for voltages less than about +50 mV; but for large steps, above +90 mV, there is a rapid time-dependent block or "inactivation." From roughly +70 to +90 mV (depending on concentration) the current has a complex time course that may be related to K accumulation near the membrane's outer surface. Block can be deepened by either increasing the concentration or the voltage. Electrical distance measurements suggest that the blocking ion moves to a site deep in the channel, possibly near the outer end. Block by internal Ca can be prevented by putting 10 mM Rb in the external solution. Recovery from block after a strong depolarization occurs quickly at +30 mV, with a time course that is about the same as that of normal K channel activation at this voltage. 20 mM Mg in neurons had no discernible blocking effect. The experiments raise questions regarding the relation of block to normal channel gating. It is speculated that when the channel is normally closed, the "blocking" site is occupied by a Ca ion that comes from the external medium.     

Interaction of internal anions with potassium channels of the squid giant axon

The interaction of internal anions with the delayed rectifier potassium channel was studied in perfused squid axons. Changing the internal potassium salt from K+ glutamate- to KF produced a reversible decline of outward K currents and a marked slowing of the activation of K channels at all voltages. Fluoride ions exert a differential effect upon K channel gating kinetics whereby activation of IK during depolarizing steps is slowed dramatically, but the rate of closing after the step is not much altered. These effects develop with a slow time course (30-60 min) and are specific for K channels over Na channels. Both the amplitude and activation rate of IK were restored within seconds upon return to internal glutamate solutions. The fluoride effect is independent of the external K+ concentration and test membrane potential, and does not recover with repetitive application of depolarizing voltage steps. Of 11 different anions tested, all inorganic species induced similar decreases and slowing of IK, while K currents were maintained during extended perfusion with several organic anions. Anions do not alter the reversal potential or shape of the instantaneous current-voltage relation of open K channels. The effect of prolonged exposure to internal fluoride could be partially reversed by the addition of cationic K channel blocking agents such as TEA+, 4-AP+, and Cs+. The competitive antagonism between inorganic anions and internal cationic K channel blockers suggests that they may interact at a related site(s). These results indicate that inorganic anions modify part of the K channel gating mechanism (activation) at a locus near the inner channel surface.     

Rapid recovery from K current inactivation on membrane hyperpolarization in molluscan neurons

Recovery from K current inactivation was studied in molluscan neurons using two-microelectrode and internal perfusion voltage clamps. Experiments were designed to study the voltage-dependent delayed outward current (IK) without contamination from other K currents. The amount of recovery from inactivation and the rate of recovery increase dramatically when the membrane potential is made more negative. The time course of recovery at the resting potential, -40 mV, is well fit by a single exponential with a time constant of 24.5 s (n = 7). At more negative voltages, the time course is best fit by the sum of two exponentials with time constants at -90 mV of 1.7 and 9.8 s (n = 7). In unclamped cells, a short hyperpolarization can cause rapid recovery from inactivation that results in a shortening of the action potential duration. We conclude that there are two inactivated states of the channel and that the time constants for recovery from both states are voltage dependent. The results are discussed in terms of the multistate model for K channel gating that was developed by R. N. Aldrich (1981, Biophys. J., 36:519-532).     

Differences in calcium homeostasis between retinal rod and cone photoreceptors revealed by the effects of voltage on the cGMP-gated conductance in intact cells

We measured currents under voltage clamp in intact retinal rod photoreceptors with tight seal electrodes in the perforated patch mode. In the dark, membrane depolarization to voltages > or = +20 mV activates a time- and voltage-dependent outward current in the outer segment. This dark voltage-activated current (DVAC) increases in amplitude with a sigmoidal time course that is voltage dependent. DVAC reaches its maximum enhancement of approximately 30% in 4-6 s at +60 mV. DVAC is entirely suppressed by light and its current-voltage curve and reversal potential are the same as those of the photocurrent. Therefore, DVAC arises from the opening in darkness of the cGMP-gated channels of the outer segment. DVAC is blocked by BAPTA loaded into the cell's cytoplasm and is enhanced by lowering extracellular Ca2+ concentration. Because the cGMP-gated channels are not directly gated by voltage and because BAPTA blocks DVAC, we suggest this signal arises from a voltage-dependent decrease in cytoplasmic Ca2+ concentration that, in turn, activates guanylyl cyclase and causes cGMP synthesis. In rods loaded with high cytoplasmic Na+, membrane depolarization in darkness to voltages > or = +20 mV inactivates the outward current in the outer segment with an exponential time course. We call this DVIC (dark, voltage-inactivated current). DVIC reflects voltage-dependent closing of the cGMP-gated channel in the dark. DVIC, too, is blocked by cytoplasmic BAPTA, and it arises from a voltage-dependent rise in cytoplasmic Ca2+ in darkness, which occurs only if cytoplasmic Na is high. We develop a quantitative model to calculate the rate and extent of the voltage-dependent change in cytoplasmic Ca2+ concentration in a normal rod. We assume that this concentration is controlled by the balance between Ca2+ influx through the cGMP-gated channels and its efflux through a Na+/Ca2+, K+ exchanger. Lowered cytoplasmic Ca2+ is linked to guanylyl cyclase activation with characteristics determined from biochemical studies. The model considers the cytoplasmic buffering of both Ca2+ and cGMP. Simulated data generated by the model fit well DVAC measured in rods and also DVAC previously measured in cones. DVAC in cones is larger in magnitude and faster in time course than that in rods. The successful fit of DVAC by the model leads us to suggest that the activity and Ca2+ dependence of the enzymes of transduction are not different in rods and cones, but the quantitative features of Ca2+ homeostasis in the outer segment of the two receptor types differ profoundly.(ABSTRACT TRUNCATED AT 400 WORDS)     

Effects of abscisic acid on K+ channels in Vicia faba guard cell protoplasts

Potassium channels were resolved in Vicia faba guard cell protoplasts by patch voltage-clamp. Whole-cell currents and single K+ channels had linear instantaneous current-voltage relations, reversing at the calculated Nernst potential for K+. Whole cell K+ currents activated exponentially during step depolarizations, with half-activation times of 400-450 msec at +80 mV and 90-110 msec at +150 mV. Single K+ channel conductance was 65 +/- 5 pS with a mean open time of 1.25 +/- 0.30 msec at 150 mV. Potassium channels were blocked by internal Cs+ and by external TEA+, but they were insensitive to external 4-aminopyridine. Application of 10 microM abscisic acid increased mean open time and caused long-lasting bursts of channel openings. Since internal and external composition can be controlled, patch-clamped protoplasts are ideal systems for studying the role of ion channels in plant physiology.     

The multi-ion nature of the pore in Shaker K+ channels.

We have investigated some of the permeation properties of the pore in Shaker K channels. We determined the apparent permeability ratio of K+, Rb+, and NH4+ ions and block of the pore by external Cs+ ions. Shaker channels were expressed with the baculovirus/Sf9 expression system and the channel currents measured with the whole-cell variant of the patch clamp technique. The apparent permeability ratio, PRb/PK, determined in biionic conditions with internal K+, was a function of external Rb+ concentration. A large change in PRb/PK occurred with reversed ionic conditions (internal Rb+ and external K+). These changes in apparent permeability were not due to differences in membrane potential. With internal K+, PNH4/PK was not a function of external NH4+ concentration (at least over the range 50-120 mM). We also investigated block of the pore by external Cs+ ions. At a concentration of 20 mM, Cs+ block had a voltage dependence equivalent to that of an ion with a valence of 0.91; this increased to 1.3 at 40 mM Cs+. We show that a 4-barrier, 3-site permeation model can simulate these and many of the other known properties of ion permeation in Shaker channels.     

Barium modulates the gating of batrachotoxin-treated Na+ channels in high ionic strength solutions.

Batrachotoxin-activated rat brain Na+ channels were reconstituted in neutral planar phospholipid bilayers in high ionic strength solutions (3 M NaCl). Under these conditions, diffuse surface charges present on the channel protein are screened. Nevertheless, the addition of extracellular and/or intracellular Ba2+ caused the following alterations in the gating of Na+ channels: (a) external (or internal) Ba2+ caused a depolarizing (or hyperpolarizing) voltage shift in the gating curve (open probability versus membrane potential curve) of the channels; (b) In the concentration range of 10-120 mM, extracellular Ba2+ caused a larger voltage shift in the gating curve of Na+ channels than intracellular Ba2+; (c) voltage shifts of the gating curve of Na+ channels as a function of external or internal Ba2+ were fitted with a simple binding isotherm with the following parameters: for internal Ba2+, delta V0.5,max (maximum voltage shift) = -11.5 mV, KD = 64.7 mM; for external Ba2+, delta V0.5,max = 13.5 mV, KD = 25.8 mM; (d) the change in the open probability of the channel caused by extracellular or intracellular Ba2+ is a consequence of alterations in both the opening and closing rate constants. Extracellular and intracellular divalent cations can modify the gating kinetics of Na+ channels by a specific modulatory effect that is independent of diffuse surface potentials. External or internal divalent cations probably bind to specific charges on the Na+ channel glycoprotein that modulate channel gating.     

Block of squid axon K channels by internally and externally applied barium ions

We have studied the interactions of Ba ion with K channels. Ba2+ blocks these channels when applied either internally or externally in millimolar concentrations. Periodic depolarizations enhance block with internal Ba2+, but diminish the block caused by external Ba2+. At rest, dissociation of Ba2+ from blocked channels is very slow, as ascertained by infrequent test pulses applied after washing Ba2+ form either inside or outside. The time constant for recovery from internal and external Ba2+ is the same. Frequent pulsing greatly shortens recovery time constant after washing away both Ba2+in and Ba2+out. Block by Ba2+ applied internally or externally is voltage dependent. Internal Ba2+ block behaves like a one-step reaction governed by a dissociation constant (Kd) that decreases e-fold/12 mV increase of pulse voltage: block deepens with more positive pulse voltage. For external Ba2+, Kd decreases e-fold/18 mV as holding potential is made more negative: block deepens with increasing negativity. Millimolar external concentrations of some cations can either lessen (K+) or enhance (NH+4, Cs+) block by external Ba2+. NH+4 apparently enhances block by slowing exist of Ba ions from the channels. Rb+ and Cs+ also slow clearing of Ba ions from channels. We think that (a) internally applied Ba2+ moves all the way through the channels, entering only when activation gates are open; (b) externally applied Ba2+ moves two-thirds of the way in, entering predominantly when activation gates are closed; (c) at a given voltage, Ba2+ occupies the same position in the channels whether it entered from inside or outside.     

Calcium- and voltage-dependent ion channels in Saccharomyces cerevisiae.

Ion channels in both the tonoplast and the plasma membrane of Saccharomyces cerevisiae have been characterized at the single channel level by patch-clamp techniques. The predominant tonoplast channel is cation selective, has an open-channel conductance of 120 pS in 100 mM KCl, and conducts Na+ or K+ equally well, and Ca2+ to a lesser extent. Its open probability (Po) is voltage-dependent, peaking at about -80 mV (cytoplasm negative), and falling to near zero at +80 mV. Elevated cytoplasmic Ca2+, alkaline cytoplasmic pH, and reducing agents activate the channel. The predominant plasma membrane channel is highly selective for K+ over anions and other cations, and shows strong outward rectification of the time-averaged current-voltage curves in cell-attached experiments. In isolated inside-out patches with micromolar cytoplasmic Ca2+, this channel is activated by positive going membrane voltages: mean Po is zero at negative membrane voltages and near unity at 100 mV. At moderate positive membrane voltages (20-40 mV), elevating cytoplasmic Ca2+ activates the channel to open in bursts of several hundred milliseconds duration. At higher positive membrane voltages, however, elevating cytoplasmic Ca2+ blocks the channel in a voltage-dependent fashion for periods of 2-3 ms. The frequency of these blocking events depends on cytoplasmic Ca2+ and membrane voltage according to second-order kinetics. Alternative cations, such as Mg2+ or Na+, block the yeast plasma-membrane K+ channel in a similar but less pronounced manner.     

Batrachotoxin-modified sodium channels from squid optic nerve in planar bilayers. Ion conduction and gating properties

Squid optic nerve sodium channels were characterized in planar bilayers in the presence of batrachotoxin (BTX). The channel exhibits a conductance of 20 pS in symmetrical 200 mM NaCl and behaves as a sodium electrode. The single-channel conductance saturates with increasing the concentration of sodium and the channel conductance vs. sodium concentration relation is well described by a simple rectangular hyperbola. The apparent dissociation constant of the channel for sodium is 11 mM and the maximal conductance is 23 pS. The selectivity determined from reversal potentials obtained in mixed ionic conditions is Na+ approximately Li+ greater than K+ greater than Rb+ greater than Cs+. Calcium blocks the channel in a voltage-dependent manner. Analysis of single-channel membranes showed that the probability of being open (Po) vs. voltage relation is sigmoidal with a value of 0.5 between -90 and -100 mV. The fitting of Po requires at least two closed and one open state. The apparent gating charge required to move through the whole transmembrane voltage during the closed-open transition is four to five electronic charges per channel. Distribution of open and closed times are well described by single exponentials in most of the voltage range tested and mean open and mean closed times are voltage dependent. The number of charges associated with channel closing is 1.6 electronic charges per channel. Tetrodotoxin blocked the BTX-modified channel being the blockade favored by negative voltages. The apparent dissociation constant at zero potential is 16 nM. We concluded that sodium channels from the squid optic nerve are similar to other BTX-modified channels reconstituted in bilayers and to the BTX-modified sodium channel detected in the squid giant axon.     

Inactivation of batrachotoxin-modified Na+ channels in GH3 cells. Characterization and pharmacological modification

Batrachotoxin (BTX)-modified Na+ currents were characterized in GH3 cells with a reversed Na+ gradient under whole-cell voltage clamp conditions. BTX shifts the threshold of Na+ channel activation by approximately 40 mV in the hyperpolarizing direction and nearly eliminates the declining phase of Na+ currents at all voltages, suggesting that Na+ channel inactivation is removed. Paradoxically, the steady-state inactivation (h infinity) of BTX-modified Na+ channels as determined by a two-pulse protocol shows that inactivation is still present and occurs maximally near -70 mV. About 45% of BTX-modified Na+ channels are inactivated at this voltage. The development of inactivation follows a sum of two exponential functions with tau d(fast) = 10 ms and tau d(slow) = 125 ms at -70 mV. Recovery from inactivation can be achieved after hyperpolarizing the membrane to voltages more negative than -120 mV. The time course of recovery is best described by a sum of two exponentials with tau r(fast) = 6.0 ms and tau r(slow) = 240 ms at -170 mV. After reaching a minimum at -70 mV, the h infinity curve of BTX-modified Na+ channels turns upward to reach a constant plateau value of approximately 0.9 at voltages above 0 mV. Evidently, the inactivated, BTX-modified Na+ channels can be forced open at more positive potentials. The reopening kinetics of the inactivated channels follows a single exponential with a time constant of 160 ms at +50 mV. Both chloramine-T (at 0.5 mM) and alpha-scorpion toxin (at 200 nM) diminish the inactivation of BTX-modified Na+ channels. In contrast, benzocaine at 1 mM drastically enhances the inactivation of BTX-modified Na+ channels. The h infinity curve reaches minimum of less than 0.1 at -70 mV, indicating that benzocaine binds preferentially with inactivated, BTX-modified Na+ channels. Together, these results imply that BTX-modified Na+ channels are governed by an inactivation process.     

Voltage-gated transient currents in bovine adrenal fasciculata cells. I. T-type Ca2+ current

The whole cell version of the patch clamp technique was used to identify and characterize voltage-gated Ca2+ channels in enzymatically dissociated bovine adrenal zona fasciculata (AZF) cells. The great majority of cells (84 of 86) expressed only low voltage-activated, rapidly inactivating Ca2+ current with properties of T-type Ca2+ current described in other cells. Voltage-dependent activation of this current was fit by a Boltzmann function raised to an integer power of 4 with a midpoint at -17 mV. Independent estimates of the single channel gating charge obtained from the activation curve and using the "limiting logarithmic potential sensitivity" were 8.1 and 6.8 elementary charges, respectively. Inactivation was a steep function of voltage with a v1/2 of -49.9 mV and a slope factor K of 3.73 mV. The expression of a single Ca2+ channel subtype by AZF cells allowed the voltage-dependent gating and kinetic properties of T current to be studied over a wide range of potentials. Analysis of the gating kinetics of this Ca2+ current indicate that T channel activation, inactivation, deactivation (closing), and reactivation (recovery from inactivation) each include voltage-independent transitions that become rate limiting at extreme voltages. Ca2+ current activated with voltage- dependent sigmoidal kinetics that were described by an m4 model. The activation time constant varied exponentially at test potentials between -30 and +10 mV, approaching a voltage-independent minimum of 1.6 ms. The inactivation time constant (tau i) also decreased exponentially to a minimum of 18.3 ms at potentials positive to 0 mV. T channel closing (deactivation) was faster at more negative voltages; the deactivation time constant (tau d) decreased from 8.14 +/- 0.7 to 0.48 +/- 0.1 ms at potentials between -40 and -150 mV. T channels inactivated by depolarization returned to the closed state along pathways that included two voltage-dependent time constants. tau rec-s ranged from 8.11 to 4.80 s when the recovery potential was varied from - 50 to -90 mV, while tau rec-f decreased from 1.01 to 0.372 s. At potentials negative to -70 mV, both time constants approached minimum values. The low voltage-activated Ca2+ current in AZF cells was blocked by the T channel selective antagonist Ni2+ with an IC50 of 20 microM. At similar concentrations, Ni2+ also blocked cortisol secretion stimulated by adrenocorticotropic hormone. Our results indicate that bovine AZF cells are distinctive among secretory cells in expressing primarily or exclusively T-type Ca2+ channels.(ABSTRACT TRUNCATED AT 400 WORDS)     

Inactivation viewed through single sodium channels

Recordings of the sodium current in tissue-cultured GH3 cells show that the rate of inactivation in whole cell and averaged single channel records is voltage dependent: tau h varied e-fold/approximately 26 mV. The source of this voltage dependence was investigated by examining the voltage dependence of individual rate constants, estimated by maximum likelihood analysis of single channel records, in a five-state kinetic model. The rate constant for inactivating from the open state, rather than closing, increased with depolarization, as did the probability that an open channel inactivates. The rate constant for closing from the open state had the opposite voltage dependence. Both rate constants contributed to the mean open time, which was not very voltage dependent. Both open time and burst duration were less than tau h for voltages up to -20 mV. The slowest time constant of activation, tau m, was measured from whole cell records, by fitting a single exponential either to tail currents or to activating currents in trypsin-treated cells, in which the inactivation was abolished. tau m was a bell-shaped function of voltage and had a voltage dependence similar to tau h at voltages more positive than -35 mV, but was smaller than tau h. At potentials more negative than about -10 mV, individual channels may open and close several times before inactivating. Therefore, averaged single channel records, which correspond with macroscopic current elicited by a depolarization, are best described by a convolution of the first latency density with the autocorrelation function rather than with 1 - (channel open time distribution). The voltage dependence of inactivation from the open state, in addition to that of the activation process, is a significant factor in determining the voltage dependence of macroscopic inactivation. Although the rates of activation and inactivation overlapped greatly, independent and coupled inactivation could not be statistically distinguished for two models examined. Although rates of activation affect the observed rate of inactivation at intermediate voltages, extrapolation of our estimates of rate constants suggests that at very depolarized voltages the activation process is so fast that it is an insignificant factor in the time course of inactivation. Prediction of gating currents shows that an inherently voltage-dependent inactivation process need not produce a conspicuous component in the gating current.     

A Fast Transient Outward Monovalent Current in Rat Saphenous Myocytes Passing Through Ca2+ Channels

Transient outward currents in rat saphenous arterial myocytes were studied using the perforated configuration of the patch-clamp method. When myocytes were bathed in a Na-gluconate solution containing TEA to block large-conductance Ca2+-activated K+ (BK) currents, depolarizing pulses positive to +20 mV from a holding potential of -100 mV induced fast transient outward currents. The activation and inactivation time constants of the current were voltage dependent, and at +40 mV were 3.6 +/- 0.8 ms and 23.9 +/- 6.4 ms (n = 4), respectively. The steady-state inactivation of the transient outward current was steeply voltage dependent (z = 1.7), with 50% of the current inactivated at -55 mV. The current was insensitive to the A-type K+ channel blocker 4-AP (1-5 mM), and was modulated by external Ca, decreasing to approximately 0.85 of control values upon raising Ca2+ from 1 to 10 mM, and increasing approximately 3-fold upon lowering it to 0.1 mM. Transient outward currents were also recorded following replacement of internal K+ with either Na+ or Cs+, raising the possibility that the current was carried by monovalent ions passing through voltage-gated Ca2+ channels. This hypothesis was supported by the finding that the transient outward current had the same inactivation rate as the inward Ba2+ current, and that both currents were effectively blocked by the L-type Ca2+ channel blocker, nifedipine and enhanced by the agonist BAYK8644.     

Characterization of K+ currents in rat malignant lymphocytes (Nb2 Cells)

Membrane K+ currents of malignant lymphocytes (Nb2 cells) were studied with the whole-cell patch-clamp method. Upon depolarization, K+ currents activate with a delay and follow a sigmoid time course, resembling other delayed rectifier K+ currents present in nerve and muscle cells. The activation time constant of these currents is voltage dependent, increasing from 1 msec at +90 mV to approximately 37 msec at -30 mV. The fractional number of open channels has a sigmoid voltage dependence with a midpoint near -25 mV. Deactivation of K+ currents in Nb2 cells is voltage dependent and follows a simple exponential time course. Time constant of this process increases from 5 msec at -115 mV to almost 80 msec at -40 mV. The relative permeability of K+ channels to different monovalent cations follows the sequence: K+ (1) greater than Rb+ (0.75) greater than NH4+ (0.11) greater than Cs+ (0.07) greater than Na+ (0.05). Inactivation of K+ currents is a biexponential process with time constants of approximately 600 and 7,000 msec. Inactivation of K+ currents in Nb2 cells is not a voltage-dependent process. The steady-state inactivation curve of K+ currents has a midpoint near -40 mV. Following a 500-msec voltage pulse, inactivation of K+ currents recovers with a simple exponential process with a time constant of 9 sec. Short duration (approximately 50 msec) voltage-clamp pulses do not induce significant inactivation of these currents. K+ currents in malignant lymphocytes do not display the phenomenon of cumulative inactivation as described for other delayed rectifier-type K+ channels. Application of a train of voltage pulses to positive potentials at different frequencies induces a moderate decrease in peak outward currents. The use of substances (N-bromoacetamide, trypsin, chloramine-T, and papain) that remove the inactivation of Na+ and K+ currents in other cells are not effective in removing the inactivation of K+ currents present in this lymphoma cell line. Significant differences were found between the characteristics of K+ currents in this malignant cell line and those present in normal lymphocytes. Possible physiological implications for these differences and for the role of K+ currents in the proliferation of normal and malignant lymphocytes are discussed.     

Permeation of Na+ through a delayed rectifier K+ channel in chick dorsal root ganglion neurons

In whole-cell patch clamp recordings from chick dorsal root ganglion neurons, removal of intracellular K+ resulted in the appearance of a large, voltage-dependent inward tail current (Icat). Icat was not Ca2+ dependent and was not blocked by Cd2+, but was blocked by Ba2+. The reversal potential for Icat shifted with the Nernst potential for [Na+]. The channel responsible for Icat had a cation permeability sequence of Na+ >> Li+ >> TMA+ > NMG+ (PX/PNa = 1:0.33:0.1:0) and was impermeable to Cl-. Addition of high intracellular concentrations of K+, Cs+, or Rb+ prevented the occurrence of Icat. Inhibition of Icat by intracellular K+ was voltage dependent, with an IC50 that ranged from 3.0-8.9 mM at membrane potentials between -50 and -110 mV. This voltage- dependent shift in IC50 (e-fold per 52 mV) is consistent with a single cation binding site approximately 50% of the distance into the membrane field. Icat displayed anomolous mole fraction behavior with respect to Na+ and K+; Icat was inhibited by 5 mM extracellular K+ in the presence of 160 mM Na+ and potentiated by equimolar substitution of 80 mM K+ for Na+. The percent inhibition produced by both extracellular and intracellular K+ at 5 mM was identical. Reversal potential measurements revealed that K+ was 65-105 times more permeant than Na+ through the Icat channel. Icat exhibited the same voltage and time dependence of inactivation, the same voltage dependence of activation, and the same macroscopic conductance as the delayed rectifier K+ current in these neurons. We conclude that Icat is a Na+ current that passes through a delayed rectifier K+ channel when intracellular K+ is reduced to below 30 mM. At intracellular K+ concentrations between 1 and 30 mM, PK/PNa remained constant while the conductance at -50 mV varied from 80 to 0% of maximum. These data suggest that the high selectivity of these channels for K+ over Na+ is due to the inability of Na+ to compete with K+ for an intracellular binding site, rather than a barrier that excludes Na+ from entry into the channel or a barrier such as a selectivity filter that prevents Na+ ions from passing through the channel.