Conditioning prepulses and kinetics of potassium conductance in the frog node

Summary The kinetics of potassium conductance were analyzed in response to voltage-clamp steps with holding potential (–75 mV) as initial condition and after a positive prepulse to-wards +45 mV of 10-msec duration. As the potassium reversal potentialE _K altered during potassium current flow, a method to obtain the conductance independent ofE _K was used. Conductance kinetics at 15°C were analyzed according to the Hodgkin-Huxley (HH) model. The time constant of potassium activation, with holding potential as initial condition, is a monotonous decreasing function of membrane potential. Its value ofca. 9 msec at –50 mV decreases to 1 msec at +30 mV. Changes inE _K did not affect the voltage dependency of this time constant. The time constant of potassium deactivation, i.e. the off-response following a 10-msec prepulse towards +45 mV, shows a completely different voltage dependency. At a membrane potential of –90 mV it is approximately 2 msec and gradually increases for more positive voltages towards a maximum value of about 6 msec, that is reached between –5 and 0 mV. At still larger values of membrane voltage this time constant starts to fall again. It is concluded that a HH-model, as applied for a single population of potassium channels, has to be rejected. Computer simulations indicate that an extension to two populations of independent potassium channels, each with HH-kinetics, is also inconsistent with the observed results.     

Gating currents of sodium channels in neurons of the rat trigeminal ganglia

Using a voltage-clamp technique and intracellular dialysis, gating currents of sodium channels were first recorded and studied in neurons of the rat trigeminal ganglia. The rising phase of gating currents lasted 30 to 70 µsec; these currents decayed in a monoexponential manner with a time constant equal to that for activation of the sodium current. Voltage dependences for the gating charge and sodium conductance were also nearly identical. Analysis of the activation of sodium conductance demonstrated that the power n of the activation variable in the equation used changed from more than 6 to 3 at test potentials of –30 mV and 0 mV, respectively. It is hypothesized that, with a change in the test potential within this voltage range, the cooperativity of activation undergoes a twofold decrease. In the presence of 2 mM caffeine or theophylline in the external solution, curves of the voltage dependence of the gating charge and sodium conductance shifted toward more negative values of the test potential, by 5.4 ± 0.7 mV, the maximum gating charge increased by 8.4 ± 3.2%, and the slope factor for both curves decreased by 9.2 ± 3.4%. Since the above effects were identical for both xanthines and developed under conditions of constant intracellular dialysis, i.e., under conditions where the effect of a change in the intracellular calcium concentration was ruled out, the most probable reason for these effects is a direct action of the tested agents on sodium ion channels, which facilitates the movement of gating charges.Neirofiziologiya/Neurophysiology, Vol. 36, Nos. 5/6, pp. 370–376, September–December, 2004.This revised version was published online in April 2005 with a corrected cover date and copyright year.     

Voltage Gating of Shaker K+ Channels : The Effect of Temperature on Ionic and Gating Currents

Ionic (I_i) and gating currents (I_g) from noninactivating Shaker H4 K⁺ channels were recorded with the cut-open oocyte voltage clamp and macropatch techniques. Steady state and kinetic properties were studied in the temperature range 2–22°C. The time course of I_i elicited by large depolarizations consists of an initial delay followed by an exponential rise with two kinetic components. The main I_i component is highly temperature dependent (Q₁₀ > 4) and mildly voltage dependent, having a valence times the fraction of electric field (z) of 0.2–0.3 e_o. The I_g On response obtained between −60 and 20 mV consists of a rising phase followed by a decay with fast and slow kinetic components. The main I_g component of decay is highly temperature dependent (Q₁₀ > 4) and has a z between 1.6 and 2.8 e_o in the voltage range from −60 to −10 mV, and ∼0.45 e_o at more depolarized potentials. After a pulse to 0 mV, a variable recovery period at −50 mV reactivates the gating charge with a high temperature dependence (Q₁₀ > 4). In contrast, the reactivation occurring between −90 and −50 mV has a Q₁₀ = 1.2. Fluctuation analysis of ionic currents reveals that the open probability decreases 20% between 18 and 8°C and the unitary conductance has a low temperature dependence with a Q₁₀ of 1.44. Plots of conductance and gating charge displacement are displaced to the left along the voltage axis when the temperature is decreased. The temperature data suggests that activation consists of a series of early steps with low enthalpic and negative entropic changes, followed by at least one step with high enthalpic and positive entropic changes, leading to final transition to the open state, which has a negative entropic change.     

Whole-cell and single-channel currents across the plasmalemma of corn shoot suspension cells

Summary Whole-cell sealed-on pipettes have been used to measure electrical properties of the plasmalemma surrounding protoplasts isolated from Black Mexican sweet corn shoot cells from suspension culture. In these protoplasts the membrane resting potential (V _m ) was found to be –59±23 mV (n=23) in 1mm K _o ^– . The meanV _m became more negative as [K^–] _o decreased, but was more positive than the K⁺ equilibrium potential. There was no evidence of electrogenic pump activity. We describe four features of the current-voltage characteristic of the plasmalemma of these protoplasts which show voltagegated channel activity. Depolarization of the whole-cell membrane from the resting potential activates time- and voltage-dependent outward current through K⁺-selective channels. A local minimum in the outward current-voltage curve nearV _m =150 mV suggests that these currents are mediated by two populations of K⁺-selective channels. The absence of this minimum in the presence of verapamil suggests that the activation of one channel population depends on the influx of Ca²⁺ into the cytoplasm. We identify unitary currents from two K⁺-selective channel populations (40 and 125 pS) which open when the membrane is depolarized; it is possible that these mediate the outward whole-cell current. Hyperpolarization of the membrane from the resting potential produces time- and voltage-dependent inward whole-cell current. Current activation is fast and follows an exponential time course. The current saturates and in some cases decreases at membrane potentials more negative than –175 mV. This current is conducted by poorly selective K⁺ channels, whereP _Cl/P _K=0.43±0.15. We describe a low conductance (20 pS) channel population of unknown selectivity which opens when the membrane is hyperpolarized. It is possible that these channels mediate inward whole-cell current. When the membrane is hyperpolarized to potentials more negative than –250 mV large, irregular inward current is activated. A third type of inward whole-cell current is briefly described. This activates slowly and with a U-shaped current-voltage curve over the range of membrane potentials –90<V _m <0 mV.     

Gating of Single N-type Calcium Channels Recorded from Bullfrog Sympathetic Neurons

For many neurons, N-type calcium channels provide the primary pathway for calcium influx during an action potential. We investigated the gating properties of single N-type calcium channels using the cell-attached patch technique. With 100 mM Ba²⁺ in the pipet, mean N-channel open probability (P _o, measured over 100 ms) increased with depolarization, but the range at a single voltage was large (e.g., P _o at +40 mV ranged from 0.1 to 0.8). The open dwell time histograms were generally well fit by a single exponential with mean open time (τ_o) increasing from 0.7 ms at +10 mV to 3.1 ms at +40 mV. Shut time histograms were well fit by two exponentials. The brief shut time component (τ_sh1 = 0.3 ms) did not vary with the test potential, while the longer shut time component (τ_sh2) decreased with voltage from 18.9 ms at +10 mV to 2.3 ms at +40 mV. Although N-channel P _o during individual sweeps at +40 mV was often high (∼0.8), mean P _o was reduced by null sweeps, low P _o gating, inactivation, and slow activation. The variability in mean P _o across patches resulted from differences in the frequency these different gating processes were expressed by the channels. Runs analysis showed that null sweeps tended to be clustered in most patches, but that inactivating and slowly activating sweeps were generally distributed randomly. Low P _o gating (P _o = 0.2, τ_o = 1 ms at +40 mV) could be sustained for ∼1 min in some patches. The clustering of null sweeps and sweeps with low P _o gating is consistent with the idea that they result from different modes of N-channel gating. While P _o of the main N-channel gating state is high, the net P _o is reduced to a maximum value of close to 0.5 by other gating processes.     

Kinetics of interaction of scorpion toxin with sodium channels in the Ranvier node membrane

The kinetics of binding the toxin ofButhus eupeus venom with sodium channels with a holding potential of –120 mV and subsequent dissociation of the toxin-channel complex during a shift of membrane potential (V_M) to between –60 and +120 mV were investigated by the voltage clamping method on the Ranvier node membrane. The rate of dissociation was shown to increase if V_M was shifted toward more positive values, exponentially with an e-fold increase every 32.3 mV. The results are in agreement with the hypothesis that dissociation of the toxin-channel complex during depolarization is determined by the difference between electrical energies of the inactivated states of normal and toxin-modified channels.Institute of Cytology, Academy of Sciences of the USSR, Leningrad. Translated from Neirofiziologiya, Vol. 12, No. 6, pp. 619–626, November–December, 1980.     

Arachidonic acid inhibition of L-type calcium (CaV1.3b) channels varies with accessory CaVβ subunits

Arachidonic acid (AA) inhibits the activity of several different voltage-gated Ca²⁺ channels by an unknown mechanism at an unknown site. The Ca²⁺ channel pore-forming subunit (Ca_Vα₁) is a candidate for the site of AA inhibition because T-type Ca²⁺ channels, which do not require accessory subunits for expression, are inhibited by AA. Here, we report the unanticipated role of accessory Ca_Vβ subunits on the inhibition of Ca_V1.3b L-type (L-) current by AA. Whole cell Ba²⁺ currents were measured from recombinant channels expressed in human embryonic kidney 293 cells at a test potential of −10 mV from a holding potential of −90 mV. A one-minute exposure to 10 µM AA inhibited currents with β_1b, β₃, or β₄ 58, 51, or 44%, respectively, but with β_2a only 31%. At a more depolarized holding potential of −60 mV, currents were inhibited to a lesser degree. These data are best explained by a simple model where AA stabilizes Ca_V1.3b in a deep closed-channel conformation, resulting in current inhibition. Consistent with this hypothesis, inhibition by AA occurred in the absence of test pulses, indicating that channels do not need to open to become inhibited. AA had no effect on the voltage dependence of holding potential–dependent inactivation or on recovery from inactivation regardless of Ca_Vβ subunit. Unexpectedly, kinetic analysis revealed evidence for two populations of L-channels that exhibit willing and reluctant gating previously described for Ca_V2 channels. AA preferentially inhibited reluctant gating channels, revealing the accelerated kinetics of willing channels. Additionally, we discovered that the palmitoyl groups of β_2a interfere with inhibition by AA. Our novel findings that the Ca_Vβ subunit alters kinetic changes and magnitude of inhibition by AA suggest that Ca_Vβ expression may regulate how AA modulates Ca²⁺-dependent processes that rely on L-channels, such as gene expression, enzyme activation, secretion, and membrane excitability.     

High-conductance K+ channel in pancreatic islet cells can be activated and inactivated by internal calcium

Summary The Ca²⁺-activated K⁺ channel in rat pancreatic islet cells has been studied using patch-clamp single-channel current recording in excised inside-out and outside-out membrane patches. In membrane patches exposed to quasi-physiological cation gradients (Na⁺ outside, K⁺ inside) large outward current steps were observed when the membrane was depolarized. The single-channel current voltage (I/V) relationship showed outward rectification and the null potential was more negative than –40 mV. In symmetrical K⁺-rich solutions the single-channelI/V relationship was linear, the null potential was 0 mV and the singlechannel conductance was about 250 pS. Membrane depolarization evoked channel opening also when the inside of the membrane was exposed to a Ca²⁺-free solution containing 2mm EGTA, but large positive membrane potentials (70 to 80 mV) were required in order to obtain open-state probabilities (P) above 0.1. Raising the free Ca²⁺ concentration in contact with the membrane inside ([Ca²⁺]_i) to 1.5×10^–7 m had little effect on the relationship between membrane potential andP. When [Ca²⁺]_i was increased to 3×10^–7 m and 6×10^–7 m smaller potential changes were required to open the channels. Increasing [Ca²⁺]_i further to 8×10^–7 m again activated the channels, but the relationship between membrane potential andP was complex. Changing the membrane potential from –50 mV to +20 mV increasedP from near 0 to 0.6 but further polarization to +50 mV decreasedP to about 0.2. The pattern of voltage activation and inactivation was even more pronounced at [Ca²⁺]_i=1 and 2 m. In this situation a membrane potential change from –70 to +20 mV increasedP from near 0 to about 0.7 but further polarization to +80 mV reducedP to less than 0.1. The high-conductance K⁺ channel in rat pancreatic islet cells is remarkably sensitive to changes in [Ca²⁺]_i within the range 0.1 to 1 m which suggests a physiological role for this channel in regulating the membrane potential and Ca²⁺ influx through voltage-activated Ca²⁺ channels.     

Voltage dependence of the effects of (±)-kavain on the rate of inactivation of Na+ channels

The dependence of the efficacy of the influence of a kava-pyrone (±)-kavain (330 µM) on the frequency of activation of Na⁺ channels and voltage dependence of the effects of (±)-kavain on the rate of inactivation of these channels were studied in experiments on isolated neurons from the rat hippocampus. In all series of experiments, the holding potential equalled –100 mV. The efficacy of (±)-kavain-induced blockade of Na⁺ channels was independent of the frequency of stimulation within the range up to 10/sec. In the control experiments, the rate of inactivation increased with the rise of depolarization from –40 mV to +30 mV, and then the saturation effect was observed. At the membrane potential of –40 mV, the rate of (±)-kavain-evoked inactivation increased approximately by a factor of 2.5. At the more positive shifts of the membrane potential, the efficacy of the effects of (±)-kavain on the rate of inactivation became noticeably reduced, and at +30 mV (±)-kavain exerted no distinct influence on this parameter.Neirofiziologiya/Neurophysiology, Vol. 28, No. 6, pp. 312–315, November–December, 1996.     

Sodium currents in the giant axon of the crabCarcinus maenas

Summary Measurements were made of the kinetics and steady-state properties of the sodium conductance changes in the giant axon of the crabCarcinus 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 sec, 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 sec at –40 mV (at 18°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.     

Fast Inactivation in Shaker K+ Channels : Properties of Ionic and Gating Currents

Fast inactivating Shaker H4 potassium channels and nonconducting pore mutant Shaker H4 W434F channels have been used to correlate the installation and recovery of the fast inactivation of ionic current with changes in the kinetics of gating current known as “charge immobilization” (Armstrong, C.M., and F. Bezanilla. 1977. J. Gen. Physiol. 70:567–590.). Shaker H4 W434F gating currents are very similar to those of the conducting clone recorded in potassium-free solutions. This mutant channel allows the recording of the total gating charge return, even when returning from potentials that would largely inactivate conducting channels. As the depolarizing potential increased, the OFF gating currents decay phase at −90 mV return potential changed from a single fast component to at least two components, the slower requiring ∼200 ms for a full charge return. The charge immobilization onset and the ionic current decay have an identical time course. The recoveries of gating current (Shaker H4 W434F) and ionic current (Shaker H4) in 2 mM external potassium have at least two components. Both recoveries are similar at −120 and −90 mV. In contrast, at higher potentials (−70 and −50 mV), the gating charge recovers significantly more slowly than the ionic current. A model with a single inactivated state cannot account for all our data, which strongly support the existence of “parallel” inactivated states. In this model, a fraction of the charge can be recovered upon repolarization while the channel pore is occupied by the NH₂-terminus region.     

Components of gating charge movement and S4 voltage-sensor exposure during activation of hERG channels

The human ether-á-go-go–related gene (hERG) K⁺ channel encodes the pore-forming α subunit of the rapid delayed rectifier current, I_Kr, and has unique activation gating kinetics, in that the α subunit of the channel activates and deactivates very slowly, which focuses the role of I_Kr current to a critical period during action potential repolarization in the heart. Despite its physiological importance, fundamental mechanistic properties of hERG channel activation gating remain unclear, including how voltage-sensor movement rate limits pore opening. Here, we study this directly by recording voltage-sensor domain currents in mammalian cells for the first time and measuring the rates of voltage-sensor modification by [2-(trimethylammonium)ethyl] methanethiosulfonate chloride (MTSET). Gating currents recorded from hERG channels expressed in mammalian tsA201 cells using low resistance pipettes show two charge systems, defined as Q₁ and Q₂, with V_1/2’s of −55.7 (equivalent charge, z = 1.60) and −54.2 mV (z = 1.30), respectively, with the Q₂ charge system carrying approximately two thirds of the overall gating charge. The time constants for charge movement at 0 mV were 2.5 and 36.2 ms for Q₁ and Q₂, decreasing to 4.3 ms for Q₂ at +60 mV, an order of magnitude faster than the time constants of ionic current appearance at these potentials. The voltage and time dependence of Q₂ movement closely correlated with the rate of MTSET modification of I521C in the outermost region of the S4 segment, which had a V_1/2 of −64 mV and time constants of 36 ± 8.5 ms and 11.6 ± 6.3 ms at 0 and +60 mV, respectively. Modeling of Q₁ and Q₂ charge systems showed that a minimal scheme of three transitions is sufficient to account for the experimental findings. These data point to activation steps further downstream of voltage-sensor movement that provide the major delays to pore opening in hERG channels.     

Responsiveness of cardiac Na+ channels to a site-directed antiserum against the cytosolic linker between domains III and IV and their sensitivity to other modifying agents

Elementary Na⁺ currents were recorded in inside-out patches from neonatal rat heart cardiocytes to analyze the influence of a site-directed polyclonal anti-serum against the linker region between the domains III and IV (amino acids 1489–1507 of the cardiac Na⁺ channel protein) on Na⁺ channel gating and to test whether this part of the -subunit may be considered as a target for modifying agents such as the (–)-enantiomer of DPI 201-106.Anti-SLP 1 serum (directed against amino acids 1490–1507) evoked, usually within 10–15 min after cytosolic administration, modified Na⁺ channel activity. Antiserum-modified Na⁺ channels retain a single open state but leave, at –60 mV for example, their conducting configuration consistently with an about threefold lower rate than normal Na⁺ channels. Another outstanding property of noninactivating Na⁺ channels, enhanced burst activity, may be quite individually pronounced, a surprising result which is difficult to interpret in terms of structure function relations. Removal of inactivation led to an increase of reconstructed peak I _Na (indicating a rise in NP _o) and changed I _Na decay to obey second-order kinetics, i.e., open probability declined slowly but progressively during membrane depolarization. The underlying deactivation process is voltage dependent and responds to a positive voltage shift with a deceleration but may operate even at the same membrane potential with different rates. Iodatemodified Na⁺ channels exhibit very similar properties including a conserved conductance. They are likewise controlled by an efficient, voltage-dependent deactivation process. Modification by (–)-DPI 201-106 fundamentally contrasts to the influence of anti-SLP 1 serum and the protein reagent iodate since (–)-DPI-modified Na⁺ channels maintain their open probability for at least 120 msec, i.e., a deactivation process seems lacking. This functional difference suggests that the linker region between the domains III and IV of the -subunit may not be the only target for (–)-DPI 201-106 and related compounds, if at all.This work was supported by a grant of the Deutsche Forschungs-gemeinschaft (Ko 778/2–4), Bonn.     

Mechanism of Maxi-K Channel Activation by Dehydrosoyasaponin-I

Dehydrosoyasaponin-I (DHS-I) is a potent activator of high-conductance, calcium-activated potassium (maxi-K) channels. Interaction of DHS-I with maxi-K channels from bovine aortic smooth muscle was studied after incorporating single channels into planar lipid bilayers. Nanomolar amounts of intracellular DHS-I caused the appearance of discrete episodes of high channel open probability interrupted by periods of apparently normal activity. Statistical analysis of these periods revealed two clearly separable gating modes that likely reflect binding and unbinding of DHS-I. Kinetic analysis of durations of DHS-I-modified modes suggested DHS-I activates maxi-K channels through a high-order reaction. Average durations of DHS-I-modified modes increased with DHS-I concentration, and distributions of these mode durations contained two or more exponential components. In addition, dose-dependent increases in channel open probability from low initial values were high order with average Hill slopes of 2.4–2.9 under different conditions, suggesting at least three to four DHS-I molecules bind to maximally activate the channel. Changes in membrane potential over a 60-mV range appeared to have little effect on DHS-I binding. DHS-I modified calcium- and voltage-dependent channel gating. 100 nM DHS-I caused a threefold decrease in concentration of calcium required to half maximally open channels. DHS-I shifted the midpoint voltage for channel opening to more hyperpolarized potentials with a maximum shift of −105 mV. 100 nM DHS-I had a larger effect on voltage-dependent compared with calcium-dependent channel gating, suggesting DHS-I may differentiate these gating mechanisms. A model specifying four identical, noninteracting binding sites, where DHS-I binds to open conformations with 10–20-fold higher affinity than to closed conformations, explained changes in voltage-dependent gating and DHS-I-induced modes. This model of channel activation by DHS-I may provide a framework for understanding protein structures underlying maxi-K channel gating, and may provide a basis for understanding ligand activation of other ion channels.     

Ion permeation and block of the gating pore in the voltage sensor of NaV1.4 channels with hypokalemic periodic paralysis mutations

Hypokalemic periodic paralysis and normokalemic periodic paralysis are caused by mutations of the gating charge–carrying arginine residues in skeletal muscle Na_V1.4 channels, which induce gating pore current through the mutant voltage sensor domains. Inward sodium currents through the gating pore of mutant R666G are only ∼1% of central pore current, but substitution of guanidine for sodium in the extracellular solution increases their size by 13- ± 2-fold. Ethylguanidine is permeant through the R666G gating pore at physiological membrane potentials but blocks the gating pore at hyperpolarized potentials. Guanidine is also highly permeant through the proton-selective gating pore formed by the mutant R666H. Gating pore current conducted by the R666G mutant is blocked by divalent cations such as Ba²⁺ and Zn²⁺ in a voltage-dependent manner. The affinity for voltage-dependent block of gating pore current by Ba²⁺ and Zn²⁺ is increased at more negative holding potentials. The apparent dissociation constant (K_d) values for Zn²⁺ block for test pulses to −160 mV are 650 ± 150 µM, 360 ± 70 µM, and 95.6 ± 11 µM at holding potentials of 0 mV, −80 mV, and −120 mV, respectively. Gating pore current is blocked by trivalent cations, but in a nearly voltage-independent manner, with an apparent K_d for Gd³⁺ of 238 ± 14 µM at −80 mV. To test whether these periodic paralyses might be treated by blocking gating pore current, we screened several aromatic and aliphatic guanidine derivatives and found that 1-(2,4-xylyl)guanidinium can block gating pore current in the millimolar concentration range without affecting normal Na_V1.4 channel function. Together, our results demonstrate unique permeability of guanidine through Na_V1.4 gating pores, define voltage-dependent and voltage-independent block by divalent and trivalent cations, respectively, and provide initial support for the concept that guanidine-based gating pore blockers could be therapeutically useful.     

Mechanisms of tubocurarine action on nicotinic cholinoreceptors of rat sympathetic ganglia neurons

The effects of tubocurarine (TC) on current induced by acetylcholine (ACh) in neurons of rat upper cervical ganglia were investigated using techniques for voltage-clamping at the membrane. Reinforcement of TC-induced blockade was achieved by paired application of ACh following prior activation of nicotinic cholinoreceptors, indicating that TC blocked the channels opened by ACh. On average, the TC-open channel complex persisted for 9.8±0.5 sec (n=7) at –50 mV and 20–24°C. It was found that increases exponentially with hyperpolarization at the membrane (a shift in membrane potential of 61 mV corresponds to an e-fold change). Suppression of ACh-induced current (ACh current) was eliminated completely under the effects of 3–30 M with depolarization of up to 80–100 mV at the membrane. Suppression of ACh current produced by membrane potential at negative levels is intensified with increasing doses of ACh. Findings would indicate that blockade of ionic channels opened by ACh is the only mechanism of TC action on nicotinic cholinoreceptors in rat sympathetic ganglia.A. A. Bogomolets Institute of Physiology, Academy of Sciences of the Ukrainian SSR, Kiev. Translated from Neirofiziologiya, Vol. 20, No. 5, pp. 672–680, September–October, 1988.     

An activation gating switch in Kv1.2 is localized to a threonine residue in the S2-S3 linker

The activation properties of Kv1.2 channels are highly variable, with reported half-activation (V_1/2) values ranging from ∼−40 mV to ∼+30 mV. Here we show that this arises because Kv1.2 channels occupy two distinct gating modes (“fast” and “slow”). “Slow” gating (τ_act = 90 ± 6 ms at +35 mV) was associated with a V_1/2 of activation of +16.6 ± 1.1 mV, whereas “fast” gating (τ_act = 4.5 ± 1.7 ms at +35 mV) was associated with a V_1/2 of activation of −18.8 ± 2.3 mV. It was possible to switch between gating modes by applying a prepulse, which suggested that channels activate to a single open state along separate “fast” and “slow” activation pathways. Using chimeras and point mutants between Kv1.2 and Kv1.5 channels, we determined that introduction of a positive charge at or around threonine 252 in the S2-S3 linker of Kv1.2 abolished “slow” activation gating. Furthermore, dialysis of the cytoplasm or excision of cell-attached patches from cells expressing Kv1.2 channels switched gating from “slow” to “fast”, suggesting involvement of cytoplasmic regulators. Collectively, these results demonstrate two modes of activation gating in Kv1.2 and specific residues in the S2-S3 linker that act as a switch between these modes.     

Voltage-dependent calcium and potassium conductances in striated muscle fibers from the scorpion,Centruroides sculpturatus

Ionic currents responsible for the action potential in scorpion muscle fibers were characterized using a three-intracellular microelectrode voltage clamp applied at the fiber ends (8–12°C). Large calcium currents (I _Ca) trigger contractile activation in physiological saline (5 mm Ca) but can be studied in the absence of contractile activation in a low Ca saline (2.5 mm). Barium (Ba) ions (1.5–3 mm) support inward current but not contractile activation.Ca conductance kinetics are fast (time constant of 3 msec at 0 mV) and very voltage dependent, with steady-state conductance increasing e-fold in approximately 4 mV. Half-activation occurs at –25 mV. Neither I _Ca nor I _Ba show rapid inactivation, but a slow, voltage-dependent inactivation eliminates I _Ca at voltages positive to –40 mV. Kinetically, scorpion channels are more similar to L-type Ca channels in vertebrate cardiac muscle than to those in skeletal muscle.Outward K currents turn on more slowly and with a longer delay than do Ca currents, and K conductance rises less steeply with voltage (e-fold change in 10 mV; half-maximal level at 0 mV). K channels are blocked by externally applied tetraethylammonium and 3,4 diaminopyridine.This work was supported by a grant from the NIH (NS-17510) to W.F.G. and a NRSA award to T.S. (GM-09921).     

A gating charge interaction required for late slow inactivation of the bacterial sodium channel NavAb

Voltage-gated sodium channels undergo slow inactivation during repetitive depolarizations, which controls the frequency and duration of bursts of action potentials and prevents excitotoxic cell death. Although homotetrameric bacterial sodium channels lack the intracellular linker-connecting homologous domains III and IV that causes fast inactivation of eukaryotic sodium channels, they retain the molecular mechanism for slow inactivation. Here, we examine the functional properties and slow inactivation of the bacterial sodium channel NavAb expressed in insect cells under conditions used for structural studies. NavAb activates at very negative membrane potentials (V_1/2 of approximately −98 mV), and it has both an early phase of slow inactivation that arises during single depolarizations and reverses rapidly, and a late use-dependent phase of slow inactivation that reverses very slowly. Mutation of Asn49 to Lys in the S2 segment in the extracellular negative cluster of the voltage sensor shifts the activation curve ∼75 mV to more positive potentials and abolishes the late phase of slow inactivation. The gating charge R3 interacts with Asn49 in the crystal structure of NavAb, and mutation of this residue to Cys causes a similar positive shift in the voltage dependence of activation and block of the late phase of slow inactivation as mutation N49K. Prolonged depolarizations that induce slow inactivation also cause hysteresis of gating charge movement, which results in a requirement for very negative membrane potentials to return gating charges to their resting state. Unexpectedly, the mutation N49K does not alter hysteresis of gating charge movement, even though it prevents the late phase of slow inactivation. Our results reveal an important molecular interaction between R3 in S4 and Asn49 in S2 that is crucial for voltage-dependent activation and for late slow inactivation of NavAb, and they introduce a NavAb mutant that enables detailed functional studies in parallel with structural analysis.