Solvent substitution as a probe of channel gating in Myxicola. Differential effects of D2O on some components of membrane conductance.

Careful examination of effects of solvent substitution on excitable membranes offers the theoretical possibility of identifying those aspects of the gating and translocation processes which are associated with significant changes in solvent order. Such information can then be used to develop or modify moire detailed models. We have examined the effects of heavy water substitution in Cs+-and K+-dialyzed Myxicola giant axons. At temperatures of 4-6 degrees C, the rates of Na+, K+, and Na+ inactivation during a maintained depolarization were all showed by approximately 50% in the presence of D2O. In contrast, the effects of solvent substitution on the time-course of prepulse inactivation and reactivation were much larger, with slowing averaging 160%. Studies at higher temperatures yielded Q10's for Na+ activation and K+ activation which were essentially comparable (0.72) and slightly but significantly smaller than that for inactivation during a maintained depolarization (0.84). In contrast, the Q10 for the D2O effect on prepulse inactivation was approximately 0.48. Heavy water substitution decrease Gk to a significantly greater extent than G(Na), while the decrease in the conductance of the Na+ channel caused by D2O was independent of whether the current-carrying species was Na+ or Li+. Sodium channel selectivity to the alkali metal cations and NH4+ was not changed by D2O substitution.     

Sodium channel activation mechanisms. Insights from deuterium oxide substitution.

Schauf and Bullock (1979. Biophys. J. 27:193-208; 1982. Biophys. J. 37:441-452), using Myxicola giant axons, demonstrated that solvent substitution with deuterium oxide (D2O) significantly affects both sodium channel activation and inactivation kinetics without corresponding changes in gating current or tail current rates. They concluded that (a) no significant component of gating current derives from the final channel opening step, and (b) channels must deactivate (during tail currents) by a different pathway from that used in channel opening. By contrast, Oxford (1981. J. Gen. Physiol. 77:1-22) found in squid axons that when a depolarizing pulse is interrupted by a brief (approximately 100 microseconds) return to holding potential, subsequent reactivation (secondary activation) is very rapid and shows almost monoexponential kinetics. Increasing the interpulse interval resulted in secondary activation rate returning towards control, sigmoid (primary activation) kinetics. He concluded that channels open and close (deactivate) via the same pathway. We have repeated both sets of observations in crayfish axons, confirming the results obtained in both previous studies, despite the apparently contradictory conclusions reached by these authors. On the other hand, we find that secondary activation after a brief interpulse interval (50 microseconds) is insensitive to D2O, although reactivation after longer interpulse intervals (approximately 400 microseconds) returns towards a D2O sensitivity similar to that of primary activation. We conclude that D2O-sensitive primary activation and D2O-insensitive tail current deactivation involve separate pathways. However, D2O-insensitive secondary activation involves reversal of the D2O-insensitive deactivation step. These conclusions are consistent with "parallel gate" models, provided that one gating particle has a substantially reduced effective valence.     

Properties of single Na+ channels in cut-open Myxicola giant axons

Time- and voltage-dependent behavior of the Na+ conductance in dialyzed intact Myxicola axons was compared with cut-open axons subjected to loose-patch clamp of the interior and to axons where Gigaseals were formed after brief enzyme digestion. Voltage and time dependence of activation, inactivation, and reactivation were identical in whole-axons and loose-patch preparations. Single channels observed in patch-clamp axons had a conductance of 18.3 +/- 2.3 pS and a mean open time of 0.84 +/- 0.12 ms. The time-dependence of Na+ currents found by averaging patch-clamp records was similar to intact axons, as was the voltage dependence of activation. Steady-state inactivation in patch-clamped axons was shifted by an average of 15 mV from that seen in loose-patch or intact axons. Substitution of D2O for H2O decreased single channel conductance by 24 +/- 6% in patch-clamped axons compared with 28 +/- 4% in intact axons, slowed inactivation by 58 +/- 8% compared with 49 +/- 6%, and increased mean open time by 52 +/- 7%. The results confirm observations on macroscopic channel behavior in Myxicola and resemble that seen in other excitable tissues.     

The gap junction channel. Its aqueous nature as indicated by deuterium oxide effects.

The effects of temperature and solvent substitution with deuterium oxide (D2O) on axoplasmic (ga) and gap junctional (gj) conductances were examined in the earthworm septate median giant axon (MGA). The temperature coefficients (Q10) for ga and gj were 1.4 and 1.5, respectively, between 5 and 15 degrees C. Substitution with D2O rapidly reduced both ga and gj by 20% and increased the Q10's to 1.5 and 1.8, respectively. The reduction in ga upon substitution with D2O and with cooling in either solvent reflects the changes that occur in solvent viscosity, which indicates that ion mobility in axoplasm, as in free solution, is primarily governed by viscous properties of the solvent. The similar initial reduction observed for gj suggests that solvent occupies the gap junction channel volume and influences transjunctional ion mobility. With time there was a further reduction in gj at 20 degrees C and a larger Q10 in D2O. The enhanced effects of D2O on gj cannot be accounted for by solvent viscosity alone and may be due to an increased hydration of the channels and/or the transport ions and by isotope effects of hydrogen-deuterium exchange on the channel protein that reduce gj.     

Gating currents in th intact crayfish giant axon.

Both single-sweep and signal-averaged asymmetry current are measured from intact crayfish axons after ionic currents are blocked with tetrodotoxin and 4-aminopyridine. The ON asymmetry charge saturates at about 0 mV and no ON charge movement is detectable at voltages negative to -140 mV. The areas of ON and OFF asymmetry charge are equal for short depolarizations but the ratio QOFF/QON decreases for longer depolarizing pulses. Sodium and asymmetry current magnitudes can be changed in parallel by lowering the hold potential or by imposing conditioning prepulses. Our results are consistent with the concept that asymmetry current in generated by movement of trapped charge in association with Na channel gating.     

Electrophysiological modifications induced by the fluorescent probe, pyrene, on Myxicola giant axons

Current- and voltage-clamp experiments on Myxicola giant axons labelled with pyrene showed decreased Na+ and K+ conductances. The low-frequency membrane capacity and the gating charge transfer were slightly reduced. It may be inferred that pyrene is incorporated in some hydrophobic membrane domains close to the ionic channels.     

Characteristics of sodium tail currents in Myxicola axons. Comparison with membrane asymmetry currents.

Sodium currents after repolarization to more negative potentials after initial activation were digitally recorded in voltage-clamped Myxicola axons compensated for series resistance. The results are inconsistent with a Hodgkin-Huxley-type kinetic scheme. At potentials more negative than -50 mV, the Na+ tails show two distinct time constants, while at more positive potentials only a single exponential process can be resolved. The time-course of the tail currents was totally unaffected when tetrodotoxin (TTX) was added to reduce gNa to low values, demonstrating the absence of any artifact dependent on membrane current. Tail currents were altered by [Ca++] in a manner consistent with a simple alteration in surface potential. Asymmetry current "off" responses are well described by a single exponential. The time constant for this response averaged 2.3 times larger than that for the rapid component of the Na+ repolarization current and was not sensitive to pulse amplitude or duration, although it did vary with holding potential. Other asymmetry current observations confirm previous reports on Myxicola.     

FPL 64176 modification of Ca(V)1.2 L-type calcium channels: dissociation of effects on ionic current and gating current

FPL 64176 (FPL) is a nondihydropyridine compound that dramatically increases macroscopic inward current through L-type calcium channels and slows activation and deactivation. To understand the mechanism by which channel behavior is altered, we compared the effects of the drug on the kinetics and voltage dependence of ionic currents and gating currents. Currents from a homogeneous population of channels were obtained using cloned rabbit Ca(V)1.2 (alpha1C, cardiac L-type) channels stably expressed in baby hamster kidney cells together with beta1a and alpha2delta1 subunits. We found a striking dissociation between effects of FPL on ionic currents, which were modified strongly, and on gating currents, which were not detectably altered. Inward ionic currents were enhanced approximately 5-fold for a voltage step from -90 mV to +10 mV. Kinetics of activation and deactivation were slowed dramatically at most voltages. Curiously, however, at very hyperpolarized voltages (< -250 mV), deactivation was actually faster in FPL than in control. Gating currents were measured using a variety of inorganic ions to block ionic current and also without blockers, by recording gating current at the reversal potential for ionic current (+50 mV). Despite the slowed kinetics of ionic currents, FPL had no discernible effect on the fundamental movements of gating charge that drive channel gating. Instead, FPL somehow affects the coupling of charge movement to opening and closing of the pore. An intriguing possibility is that the drug causes an inactivated state to become conducting without otherwise affecting gating transitions.     

Saturation transfer electron paramagnetic resonance detection of sickle hemoglobin aggregation during deoxygenation.

In Myxicola axons, substitution of tetramethylammonium (TMA+) for Cs+ alters intramembrane charge movements (gating currents). Although the total charge moved during and following a depolarizing step remains constant, with TMA+ the ON response has additional slower component(s), and the OFF response is retarded. Concommitantly, TMA+ produces the same voltage-dependent block of Na+ inactivation in Myxicola as has been observed in other preparations. At large positive potentials as many as 70% of the Na+ channels fail to inactivate in the steady state. In addition, TMA+ slows Na+ activation, retards the inactivation of those Na+ channels that remain able to inactivate, and decreases the maximum Na+ conductance. The steady-state Na+ conductance induced by internal TMA+ or Na+ is consistent with a scheme in which these internal cations simply modify Na+ channels in an all-or-none fashion so that a fraction become incapable of inactivating.     

Sensitivity of the sodium and potassium channels of Myxicola giant axons to changes in external pH

Myxicola giant axons were studied using standard voltage-clamp techniques in solutions whose pH values ranged from 3.9 to 10.2. Buffer concentrations of 50 mM or greater were necessary to demonstrate the full effect of pH. In acidic solutions the axon underwent a variable depolarization, and both the sodium and potassium conductances were reversibly depressed with approximate pKa's of 4.8 and 4.4, respectively. The voltage dependence of GNa was only slightly altered by acidic conditions, whereas there occurred large shifts in GK along the voltage axis consistent with a substantial decrease in net negative surface charge in the vicinity of the K+ channels. The sodium and potassium activation rate constants were decreased by acidic conditions, but the results could not be described as a simple translation along the voltage axis.     

Magnitude and location of surface charges on Myxicola giant axons

The effects of changes in the concentration of calcium in solutions bathing Myxicola giant axons on the voltage dependence of sodium and potassium conductance and on the instantaneous sodium and potassium current-voltage relations have been measured. The sodium conductance-voltage relation is shifted along the voltage axis by 13 mV in the hyperpolarizing direction for a fourfold decrease in calcium concentration. The potassium conductance-voltage relation is shifted only half as much as that for sodium. There is no effect on the shape of the sodium and potassium instantaneous current-voltage curves: the normal constant-field rectification of potassium currents is maintained and the normal linear relationship of sodium currents is maintained. Considering that shifts in conductances would reflect the presence of surface charges near the gating machinery and that shape changes of instantaneous current-voltage curves would reflect the presence of surface charges near the ionic pores, these results indicate a negative surface charge density of about 1 electronic charge per 120 A2 near the sodium gating machinery, about 1 e/300 A2 for the potassium gating machinery, and much less surface charge near the sodium or potassium pores. There may be some specific binding of calcium to these surface charges with an upper limit on the binding constant of about 0.2 M-1. The differences in surface charge density suggest a spatial separation for these four membrane components.     

Interactions between quaternary lidocaine, the sodium channel gates, and tetrodotoxin.

A voltage clamp technique was used to study sodium currents and gating currents in squid axons internally perfused with the membrane impermeant sodium channel blocker, QX-314. Block by QX-314 is strongly and reversibly enhanced if a train of depolarizing pulses precedes the measurement. The depolarization-induced block is antagonized by external sodium. This antagonism provides evidence that the blocking site for the drug lies inside the channel. Depolarization-induced block of sodium current by QX-314 is accompanied by nearly twofold reduction in gating charge movement. This reduction does not add to a depolarization-induced immobilization of gating charge normally present and believed to be associated with inactivation of sodium channels. Failure to act additively suggests that both, inactivation and QX-314, affect the same component of gating charge movement. Judged from gating current measurement, a drug-blocked channel is an inactivated channel. In the presence of external tetrodotoxin and internal QX-314, gating charge movement is always half its normal size regardless of conditioning, as it QX-314 is then permanently present in the channel.     

Modification of potassium channel kinetics by amino group reagents.

We have examined the actions of several amino group reagents on delayed rectifier potassium channels in squid giant axons. Three general classes of reagents were used: (1) those that preserved the positive charge of amino groups; (2) those that neutralize the charge; and (3) those that replace the positive with a negative charge. All three types of reagents produced qualitatively similar effects on K channel properties. Trinitrobenzene sulfonic acid (TNBS) neutralizes the peptide terminal amino groups and the epsilon-amino group of lysine groups. TNBS (a) slowed the kinetics of macroscopic ionic currents; (b) increased the size of ionic currents at large positive voltages; (c) shifted the voltage-dependent probability of channel opening to more positive potentials but had no effect on the voltage sensitivity; and (d) altered several properties of K channel gating currents. The actions of TNBS on gating currents suggest the presence of multiple gating current components. These effects are not all coupled, suggesting that several amino groups on the external surface of K channels are important for channel gating. A simple kinetic model that considers the channel to be composed of independent heterologous subunits is consistent with most of the modifications produced by amino group reagents.     

Asymmetry currents in intracellularly perfused squid giant axons.

Asymmetry currents were recorded from intracellularly perfused squid axons subjected to exactly equal positive and negative voltage clamp pulses at a temperature close to 0 degrees C. The voltage and time dependence of the asymmetry currents was studied at a holding potential of minus 80 to minus 100 mV. The effect of varying the holding potential was investigated. The latter experiments showed that the voltage dependence of the asymmetrical charge movement is different from the voltage dependence of the m system.     

Gating of the bacterial sodium channel, NaChBac: voltage-dependent charge movement and gating currents

The bacterial sodium channel, NaChBac, from Bacillus halodurans provides an excellent model to study structure-function relationships of voltage-gated ion channels. It can be expressed in mammalian cells for functional studies as well as in bacterial cultures as starting material for protein purification for fine biochemical and biophysical studies. Macroscopic functional properties of NaChBac have been described previously (Ren, D., B. Navarro, H. Xu, L. Yue, Q. Shi, and D.E. Clapham. 2001. Science. 294:2372-2375). In this study, we report gating current properties of NaChBac expressed in COS-1 cells. Upon depolarization of the membrane, gating currents appeared as upward inflections preceding the ionic currents. Gating currents were detectable at -90 mV while holding at -150 mV. Charge-voltage (Q-V) curves showed sigmoidal dependence on voltage with gating charge saturating at -10 mV. Charge movement was shifted by -22 mV relative to the conductance-voltage curve, indicating the presence of more than one closed state. Consistent with this was the Cole-Moore shift of 533 micros observed for a change in preconditioning voltage from -160 to -80 mV. The total gating charge was estimated to be 16 elementary charges per channel. Charge immobilization caused by prolonged depolarization was also observed; Q-V curves were shifted by approximately -60 mV to hyperpolarized potentials when cells were held at 0 mV. The kinetic properties of NaChBac were simulated by simultaneous fit of sodium currents at various voltages to a sequential kinetic model. Gating current kinetics predicted from ionic current experiments resembled the experimental data, indicating that gating currents are coupled to activation of NaChBac and confirming the assertion that this channel undergoes several transitions between closed states before channel opening. The results indicate that NaChBac has several closed states with voltage-dependent transitions between them realized by translocation of gating charge that causes activation of the channel.     

Multiple-state model of ionic channel in reproducing the time course of electrophysiological events.

BACKGROUND: The predictions of the Hodgkin-Huxley model do not accurately fit all the measurements of voltage-clamp currents, gating charge and single-channel currents. There are many quantitative differences between the predicted and measured characteristics of the sodium and potassium channels. For example, the two-state gate model has exponential onset kinetics, whereas the sodium and potassium conductances show S-shaped activation and the sodium conductance shows an exponential inactivation. In this paper we shall examine a more general channel model that can more faithfully represent the measured properties of ionic channels in the membrane of the excitable cell. METHODS: The model is based on the generalisation of the notion of a channel with a discrete set of states. Each state has state attributes such as the state conductance, state ionic current and state gating charge. These variables can have quite different waveforms in time, in contrast with a two-state gate channel model, in which all have the same waveforms. RESULTS: The kinetics of all variables are equivalent: gating and ionic currents give equivalent information about channel kinetics; both the equilibrium values of the current and the time constants are functions of membrane potential. The results are in almost perfect concordance with the experimental data regarding the characteristics of nerve impulse. CONCLUSIONS: The expected values of the gating charge and the ionic conductance are weighted sums of the state occupancy probabilities, but the weights differ: for the expected value of the gating charge the weights are the state gating charges and for the expected value of the ionic conductance the weights are the state conductances. Since these weights are different, the expected values of the gating charge and the ionic conductance will differ.     

Internal cesium and the sodium inactivation gate in Myxicola giant axons.

Internal cesium (CSi), relative to internal potassium (Ki), alters Na current (INa) time course in internally perfused Myxicola giant axons. CSi slows the time to peak INa, slows its decline from peak and increases the steady state to peak current ratio, INainfinity/INapeak. Neither activation nor deactivation kinetics are appreciably affected by CSi. Na current rising phases, times to half maximum and tail current time courses are similar in CSi and Ki. Inactivation time constants determined by both one (tau h) and two (tau c) pulses are also little changed by CSi. The CSi effects are due largely or entirely to an increased INainfinity/INapeak. CSi decreases the steady level of inactivation reached during a step in potential, preventing some fraction of inactivation gates from closing at all, the rest apparently closing normally. Inactivation block in CSi decreases with increasing inward current magnitude and in Ki inactivation block is appreciable only for outward Na channel current, suggesting the site of action is located somewhere in the current pathway. If this site mediates the normal operation of the inactivation gate, then a possible mechanism for gate closure could involve a positively charged structure moving to associate with a negative site near or into the inner channel mouth.     

The Na channel voltage sensor associated with inactivation is localized to the external charged residues of domain IV, S4.

Site-3 toxins have been shown to inhibit a component of gating charge (33% of maximum gating charge, Q(max)) in native cardiac Na channels that has been identified with the open-to-inactivated state kinetic transition. To investigate the role of the three outermost arginine amino acid residues in segment 4 domain IV (R1, R2, R3) in gating charge inhibited by site-3 toxins, we recorded ionic and gating currents from human heart Na channels with mutations of the outermost arginines (R1C, R1Q, R2C, and R3C) expressed in fused, mammalian tsA201 cells. All four mutations had ionic currents that activated over the same voltage range with slope factors of their peak conductance-voltage (G-V) relationships similar to those of wild-type channels, although decay of I(Na) was slowest for R1C and R1Q mutant channels and fastest for R3C mutant channels. After Na channel modification by Ap-A toxin, decays of I(Na) were slowed to similar values for all four channel mutants. Toxin modification produced a graded effect on gating charge (Q) of mutant channels, reducing Q(max) by 12% for the R1C and R1Q mutants, by 22% for the R2C mutant, and by 27% for the R3C mutant, only slightly less than the 31% reduction seen for wild-type currents. Consistent with these findings, the relationship of Q(max) to G(max) was significantly shallower for R1 mutants than for R2C and R3C mutant Na channels. These data suggest that site-3 toxins primarily inhibit gating charge associated with movement of the S4 in domain IV, and that the outermost arginine contributes the largest amount to channel gating, with other arginines contributing less.     

Sequence of Gating Charge Movement and Pore Gating in hERG Activation and Deactivation Pathways

K_V11.1 voltage-gated K⁺ channels are noted for unusually slow activation, fast inactivation, and slow deactivation kinetics, which tune channel activity to provide vital repolarizing current during later stages of the cardiac action potential. The bulk of charge movement in human ether-a-go-go-related gene (hERG) is slow, as is return of charge upon repolarization, suggesting that the rates of hERG channel opening and, critically, that of deactivation might be determined by slow voltage sensor movement, and also by a mode-shift after activation. To test these ideas, we compared the kinetics and voltage dependence of ionic activation and deactivation with gating charge movement. At 0 mV, gating charge moved ∼threefold faster than ionic current, which suggests the presence of additional slow transitions downstream of charge movement in the physiological activation pathway. A significant voltage sensor mode-shift was apparent by 24 ms at +60 mV in gating currents, and return of charge closely tracked pore closure after pulses of 100 and 300 ms duration. A deletion of the N-terminus PAS domain, mutation R4AR5A or the LQT2-causing mutation R56Q gave faster-deactivating channels that displayed an attenuated mode-shift of charge. This indicates that charge movement is perturbed by N- and C-terminus interactions, and that these domain interactions stabilize the open state and limit the rate of charge return. We conclude that slow on-gating charge movement can only partly account for slow hERG ionic activation, and that the rate of pore closure has a limiting role in the slow return of gating charges.     

Modulation of gating currents of the Ca(v)3.1 calcium channel by alpha 2 delta 2 and gamma 5 subunits

Modulatory effects of auxiliary alpha(2)delta(2) and gamma(5) subunits on intramembrane charge movement originating from the expressed Ca(v)3.1 calcium channel were investigated. Inward current was blocked by 1mM La(3+). Voltage dependences of Q(on) and Q(off), kinetics of ON- and OFF-charge movement, and I(max)/Q(max) ratio were measured in the absence and the presence of an auxiliary subunit. The alpha(2)delta(2) subunit accelerated significantly both ON- and OFF-charge movement. I(max)/Q(max) ratio and Q(on)-V, Q(off)-V relations were not affected. Coexpression of the alpha(2)delta(2) subunit may accelerate channel transitions between individual closed states, but not the transition from the last closed channel state into an open state. Coexpression of the gamma(5) subunit accelerated the decay of the ON-charge transient and enhanced I(max)/Q(max) ratio. These effects suggest improvement of the coupling between the charge movement and the channel opening due to facilitation of transitions between individual closed states and the transition between the last closed state and an open state.