The Link between Ion Permeation and Inactivation Gating of Kv4 Potassium Channels

Kv4 potassium channels undergo rapid inactivation but do not seem to exhibit the classical N-type and C-type mechanisms present in other Kv channels. We have previously hypothesized that Kv4 channels preferentially inactivate from the preopen closed state, which involves regions of the channel that contribute to the internal vestibule of the pore. To further test this hypothesis, we have examined the effects of permeant ions on gating of three Kv4 channels (Kv4.1, Kv4.2, and Kv4.3) expressed in Xenopus oocytes. Rb⁺ is an excellent tool for this purpose because its prolonged residency time in the pore delays K⁺ channel closing. The data showed that, only when Rb⁺ carried the current, both channel closing and the development of macroscopic inactivation are slowed (1.5- to 4-fold, relative to the K⁺ current). Furthermore, macroscopic Rb⁺ currents were larger than K⁺ currents (1.2- to 3-fold) as the result of a more stable open state, which increases the maximum open probability. These results demonstrate that pore occupancy can influence inactivation gating in a manner that depends on how channel closing impacts inactivation from the preopen closed state. By examining possible changes in ionic selectivity and the influence of elevating the external K⁺ concentration, additional experiments did not support the presence of C-type inactivation in Kv4 channels.     

Basis for allosteric open-state stabilization of voltage-gated potassium channels by intracellular cations

The open state of voltage-gated potassium (Kv) channels is associated with an increased stability relative to the pre-open closed states and is reflected by a slowing of OFF gating currents after channel opening. The basis for this stabilization is usually assigned to intrinsic structural features of the open pore. We have studied the gating currents of Kv1.2 channels and found that the stabilization of the open state is instead conferred largely by the presence of cations occupying the inner cavity of the channel. Large impermeant intracellular cations such as N-methyl-d-glucamine (NMG⁺) and tetraethylammonium cause severe slowing of channel closure and gating currents, whereas the smaller cation, Cs⁺, displays a more moderate effect on voltage sensor return. A nonconducting mutant also displays significant open state stabilization in the presence of intracellular K⁺, suggesting that K⁺ ions in the intracellular cavity also slow pore closure. A mutation in the S6 segment used previously to enlarge the inner cavity (Kv1.2-I402C) relieves the slowing of OFF gating currents in the presence of the large NMG⁺ ion, suggesting that the interaction site for stabilizing ions resides within the inner cavity and creates an energetic barrier to pore closure. The physiological significance of ionic occupation of the inner cavity is underscored by the threefold slowing of ionic current deactivation in the wild-type channel compared with Kv1.2-I402C. The data suggest that internal ions, including physiological concentrations of K⁺, allosterically regulate the deactivation kinetics of the Kv1.2 channel by impairing pore closure and limiting the return of voltage sensors. This may represent a primary mechanism by which Kv channel deactivation kinetics is linked to ion permeation and reveals a novel role for channel inner cavity residues to indirectly regulate voltage sensor dynamics.     

Modeling squid axon K+ channel by a nucleation and growth kinetic mechanism

A kinetic model accounting for all salient features of the K⁺ channel of the squid giant axon, including the rising phase of the ON gating charge and the Cole-Moore effect, is provided. Upon accounting for a significant feature distinguishing K⁺, Na⁺ and Ca^2 + channels from channel-forming peptides modeled in our previous 2016 BBA paper, the nucleation-and-growth kinetic model developed therein is extended to simulate ON ionic and gating currents of the K⁺ channel of the squid giant axon at different depolarization potentials by the use of only two free parameters. K⁺ channel opening is considered to proceed by progressive aggregation of single subunits, while they are moving their gating charge outward under depolarizing conditions within their tetrameric structure; K⁺ channel closing proceeds in the opposite direction, by repolarization-induced disaggregation of subunits, accompanied by inward movement of their gating charge.     

Coupling of activation and inactivation gate in a K+‐channel: potassium and ligand sensitivity

Potassium (K⁺)‐channel gating is choreographed by a complex interplay between external stimuli, K⁺ concentration and lipidic environment. We combined solid‐state NMR and electrophysiological experiments on a chimeric KcsA–Kv1.3 channel to delineate K⁺, pH and blocker effects on channel structure and function in a membrane setting. Our data show that pH‐induced activation is correlated with protonation of glutamate residues at or near the activation gate. Moreover, K⁺ and channel blockers distinctly affect the open probability of both the inactivation gate comprising the selectivity filter of the channel and the activation gate. The results indicate that the two gates are coupled and that effects of the permeant K⁺ ion on the inactivation gate modulate activation‐gate opening. Our data suggest a mechanism for controlling coordinated and sequential opening and closing of activation and inactivation gates in the K⁺‐channel pore.     

Gating currents from neuronal KV7.4 Channels: General features and correlation with the ionic conductance

The K_V7 (KCNQ) subfamily of voltage-gated K⁺ channels consists of five members (K_V7.1- K_V7.5) giving rise to non-inactivating, and slowly activating/deactivating currents mainly expressed in cardiac (K_V7.1) and neuronal (K_V7.2- K_V7.5) tissue. In the present study, using the cut-open oocyte voltage clamp, we studied the relation of the ionic currents from homomeric neuronal Kv7 channels (K_V7.2-K_V7.5) with the gating currents recorded after K⁺ conductance blockade from the same channels. Increasing the recording temperature from 18{degree sign}C to 28{degree sign}C accelerated activation/deactivation kinetics of the ionic currents in all homomeric K_V7 channels (activation Q10s at 0 mV were 3.8, 4.1, 8.3, and 2.8 for Kv7.2, Kv7.3, Kv7.4 and Kv7.5 channels, respectively), without large changes in currents voltage-dependence; moreover, at 28{degree sign}C, ionic currents carried by K_V7.4 channels also showed a significant increase in their maximal value. Gating currents were only resolved in K_V7.4 and K_V7.5 channels; the size of the ON gating charges at +40 mV was 1.34 ± 0.34 nC for K_V7.4, and 0.79 ± 0.20 nC for K_V7.5. At 28{degree sign}C, K_V7.4 gating currents had the following salient properties: 1) similar time integral of QON and QOFF, indicating no charge immobilization; 2) a left-shift in the V1/2 of the QON/V when compared to the G/V (≈ 50 mV in the presence of 2 mM extracellular Ba²⁺); 3) a QON decay faster than ionic current activation; and 4) a rising phase in the OFF gating charge after depolarizations larger than 0 mV. These observations suggest that, in K_V7.4 channels, VSD movement is followed by a slow and/or low bearing charge step linking to pore opening, a result which may help to clarify the molecular consequence of disease-causing mutations and drugs affecting channel gating.     

Constitutive inactivation of the hKv1.5 mutant channel, H463G, in K+-free solutions at physiological pH

Extracellular acidification and reduction of extracellular K⁺ are known to decrease the currents of some voltage-gated potassium channels. Although the macroscopic conductance of WT hKv1.5 channels is not very sensitive to [K⁺]_o at pH 7.4, it is very sensitive to [K⁺]_o at pH 6.4, and in the mutant, H463G, the removal of K⁺ _o virtually eliminates the current at pH 7.4. We investigated the mechanism of current regulation by K⁺ _o in the Kv1.5 H463G mutant channel at pH 7.4 and the wild-type channel at pH 6.4 by taking advantage of Na⁺ permeation through inactivated channels. Although the H463G currents were abolished in zero [K⁺]_o, robust Na⁺ tail currents through inactivated channels were observed. The appearnnce of H463G Na⁺ currents with a slow rising phase on repolarization after a very brief depolarization (2 ms) suggests that channels could activate directly from closed-inactivated states. In wild-type channels, when intracellular K⁺ was replaced by NMG⁺ and the inward Na⁺ current was recorded, addition of 1 mM K⁺ prevented inactivation, but changing pH from 7.4 to 6.4 reversed this action. The data support the idea that C-type inactivation mediated at R487 in Kv1.5 channels is influenced by H463 in the outer pore. We conclude that both acidification and reduction of [K⁺]_o inhibit Kv1.5 channels through a common mechananism (i.e., by increasing channel inactivation, which occurs in the resting state or develops very rapidly after activation).     

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.     

Anomalous Effect of Permeant Ion Concentration on Peak Open Probability of Cardiac Na+ Channels

Human heart Na⁺ channels were expressed transiently in both mammalian cells and Xenopus oocytes, and Na⁺ currents measured using 150 mM intracellular Na⁺. Decreasing extracellular permeant ion concentration decreases outward Na⁺ current at positive voltages while increasing the driving force for the current. This anomalous effect of permeant ion concentration, especially obvious in a mutant (F1485Q) in which fast inactivation is partially abolished, is due to an alteration of open probability. The effect is only observed when a highly permeant cation (Na⁺, Li⁺, or hydrazinium) is substituted for a relatively impermeant cation (K⁺, Rb⁺, Cs⁺, N -methylglucamine, Tris, choline, or tetramethylammonium). With high concentrations of extracellular permeant cations, the peak open probability of Na⁺ channels increases with depolarization and then saturates at positive voltages. By contrast, with low concentrations of permeant ions, the open probability reaches a maximum at approximately 0 mV and then decreases with further depolarization. There is little effect of permeant ion concentration on activation kinetics at depolarized voltages. Furthermore, the lowered open probability caused by a brief depolarization to +60 mV recovers within 5 ms upon repolarization to −140 mV, indicative of a gating process with rapid kinetics. Tail currents at reduced temperatures reveal the rapid onset of this gating process during a large depolarization. A large depolarization may drive a permeant cation out of a site within the extracellular mouth of the pore, reducing the efficiency with which the channel opens.     

Stabilization of the Conductive Conformation of a Voltage-gated K+ (Kv) Channel: THE LID MECHANISM*

Voltage-gated K⁺ (Kv) channels are molecular switches that sense membrane potential and in response open to allow K⁺ ions to diffuse out of the cell. In these proteins, sensor and pore belong to two distinct structural modules. We previously showed that the pore module alone is a robust yet dynamic structural unit in lipid membranes and that it senses potential and gates open to conduct K⁺ with unchanged fidelity. The implication is that the voltage sensitivity of K⁺ channels is not solely encoded in the sensor. Given that the coupling between sensor and pore remains elusive, we asked whether it is then possible to convert a pore module characterized by brief openings into a conductor with a prolonged lifetime in the open state. The strategy involves selected probes targeted to the filter gate of the channel aiming to modulate the probability of the channel being open assayed by single channel recordings from the sensorless pore module reconstituted in lipid bilayers. Here we show that the premature closing of the pore is bypassed by association of the filter gate with two novel open conformation stabilizers: an antidepressant and a peptide toxin known to act selectively on Kv channels. Such stabilization of the conductive conformation of the channel is faithfully mimicked by the covalent attachment of fluorescein at a cysteine residue selectively introduced near the filter gate. This modulation prolongs the occupancy of permeant ions at the gate. It is this longer embrace between ion and gate that we conjecture underlies the observed stabilization of the conductive conformation. This study provides a new way of thinking about gating.     

Modeling squid axon Na+ channel by a nucleation and growth kinetic mechanism

A kinetic model accounting for all salient features of the Na⁺ channel of the squid giant axon is provided. The model furnishes explanations for the Cole-Moore-like effect, the rising phase of the ON gating current and the slow ‘intermediate component’ of its decaying phase, as well as the gating charge immobilization. Experimental ON ionic currents are semi-quantitatively simulated by the use of only three free parameters, upon assuming that the Na⁺ channel opening proceeds along with the stepwise aggregation of its four domains, while they are moving their gating charge outward under depolarizing conditions. The inactivation phase of the ON ionic current is interpreted by a progressive electrostatic attraction between the positively charged ‘hinged lid’ containing the hydrophobic IFM triad and its receptor inside the channel pore, as the stepwise outward movement of the S4 segments of the Na⁺ channel progressively increases the negative charge attracting the triad to its receptor. The Na⁺ channel closing is assumed to proceed by repolarization-induced disaggregation of its domains, accompanied by inward movement of their gating charge. The phenomenon of ‘gating charge immobilization’ can be explained by assuming that gradual structural changes of the receptor over the time course of depolarization strengthen the interaction between the IFM triad and its receptor, causing a slow release of the gating charge during the subsequent repolarization.     

The Permeability of the Sodium Channel to Metal Cations in Myelinated Nerve

The relative permeability of sodium channels to eight metal cations is studied in myelinated nerve fibers. Ionic currents under voltage-clamp conditions are measured in Na-free solutions containing the test ion. Measured reversal potentials and the Goldman equation are used to calculate the permeability sequence: Na⁺ ≈ Li⁺ > Tl⁺ > K⁺. The ratio P_K/P_Na is 1/12. The permeabilities to Rb⁺, Cs⁺, Ca⁺⁺, and Mg⁺⁺ are too small to measure. The permeability ratios agree with observations on the squid giant axon and show that the reversal potential E_Na differs significantly from the Nernst potential for Na⁺ in normal axons. Opening and closing rates for sodium channels are relatively insensitive to the ionic composition of the bathing medium, implying that gating is a structural property of the channel rather than a result of the movement or accumulation of particular ions around the channel. A previously proposed pore model of the channel accommodates the permeant metal cations in a partly hydrated form. The observed sequence of permeabilities follows the order expected for binding to a high field strength anion in Eisenman's theory of ion exchange equilibria.     

The Human Red Cell Voltage-regulated Cation Channel. The Interplay with the Chloride Conductance,the Ca<Superscript>2+</Superscript>-activated K<Superscript>+</Superscript> Channel and the Ca<Superscript>2+</Superscript> Pump

Electrocytes from the electric organ of Electrophorus electricus exhibited sodium action potentials that have been proposed to be repolarized by leak currents and not by outward voltage-gated potassium currents. However, patch-clamp recordings have suggested that electrocytes may contain a very low density of voltage-gated K⁺ channels. We report here the cloning of a K⁺ channel from an eel electric organ cDNA library, which, when expressed in mammalian tissue culture cells, displayed delayed-rectifier K⁺ channel characteristics. The amino-acid sequence of the eel K⁺ channel had the highest identity to Kv1.1 potassium channels. However, different important functional regions of eel Kv1.1 had higher amino-acid identity to other Kv1 members, for example, the eel Kv1.1 S4-S5 region was identical to Kv1.5 and Kv1.6. Northern blot analysis indicated that eel Kv1.1 mRNA was expressed at appreciable levels in the electric organ but it was not detected in eel brain, muscle, or cardiac tissue. Because electrocytes do not express robust outward voltage-gated potassium currents we speculate that eel Kv1.1 channels are chronically inhibited in the electric organ and may be functionally recruited by an unknown mechanism.     

Divalent Cations Slow Activation of EAG Family K Channels through Direct Binding to S4

Voltage-gated K⁺ channels share a common voltage sensor domain (VSD) consisting of four transmembrane helices, including a highly mobile S4 helix that contains the major gating charges. Activation of ether-a-go-go (EAG) family K⁺ channels is sensitive to external divalent cations. We show here that divalent cations slow the activation rate of two EAG family channels (Kv12.1 and Kv10.2) by forming a bridge between a residue in the S4 helix and acidic residues in S2. Histidine 328 in the S4 of Kv12.1 favors binding of Zn²⁺ and Cd²⁺, whereas the homologous residue Serine 321 in Kv10.2 contributes to effects of Mg²⁺ and Ni²⁺. This novel finding provides structural constraints for the position of transmembrane VSD helices in closed, ion-bound EAG family channels. Homology models of Kv12.1 and Kv10.2 VSD structures based on a closed-state model of the Shaker family K⁺ channel Kv1.2 match these constraints. Our results suggest close conformational conservation between closed EAG and Shaker family channels, despite large differences in voltage sensitivity, activation rates, and activation thresholds.     

Macroscopic Na+ Currents in the “Nonconducting” Shaker Potassium Channel Mutant W434F

C-type inactivation in Shaker potassium channels inhibits K⁺ permeation. The associated structural changes appear to involve the outer region of the pore. Recently, we have shown that C-type inactivation involves a change in the selectivity of the Shaker channel, such that C-type inactivated channels show maintained voltage-sensitive activation and deactivation of Na⁺ and Li⁺ currents in K⁺-free solutions, although they show no measurable ionic currents in physiological solutions. In addition, it appears that the effective block of ion conduction produced by the mutation W434F in the pore region may be associated with permanent C-type inactivation of W434F channels. These conclusions predict that permanently C-type inactivated W434F channels would also show Na⁺ and Li⁺ currents (in K⁺-free solutions) with kinetics similar to those seen in C-type-inactivated Shaker channels. This paper confirms that prediction and demonstrates that activation and deactivation parameters for this mutant can be obtained from macroscopic ionic current measurements. We also show that the prolonged Na⁺ tail currents typical of C-type inactivated channels involve an equivalent prolongation of the return of gating charge, thus demonstrating that the kinetics of gating charge return in W434F channels can be markedly altered by changes in ionic conditions.     

Permeation and Gating of an Inwardly Rectifying Potassium Channel : Evidence for a Variable Energy Well

Permeation, gating, and their interrelationship in an inwardly rectifying potassium (K⁺) channel, ROMK2, were studied using heterologous expression in Xenopus oocytes. Patch-clamp recordings of single channels were obtained in the cell-attached mode. The gating kinetics of ROMK2 were well described by a model having one open and two closed states. One closed state was short lived (∼1 ms) and the other was longer lived (∼40 ms) and less frequent (∼1%). The long closed state was abolished by EDTA, suggesting that it was due to block by divalent cations. These closures exhibit a biphasic voltage dependence, implying that the divalent blockers can permeate the channel. The short closures had a similar biphasic voltage dependence, suggesting that they could be due to block by monovalent, permeating cations. The rate of entering the short closed state varied with the K⁺ concentration and was proportional to current amplitude, suggesting that permeating K⁺ ions may be related to the short closures. To explain the results, we propose a variable intrapore energy well model in which a shallow well may change into a deep one, resulting in a normally permeant K⁺ ion becoming a blocker of its own channel.     

Differential regulation of K+ channels in Arabidopsis epidermal and stelar root cells

The patch clamp technique was applied to protoplasts isolated from the epidermis and pericycle of Arabidopsis roots and their plasma membrane currents investigated. In the whole cell configuration, all protoplasts from the epidermis exhibited depolarization‐activated time‐dependent outwardly rectifying (OR) currents whereas OR currents were present in only 50% of cells from the pericycle. The properties of the OR currents in the epidermis and pericycle were compared with respect to their selectivity, pharmacology and gating. The time‐dependent activation kinetics, selectivity and sensitivity to extracellular tetraethyl ammonium of the OR current in each cell type were not significantly different. The reversal potential (E_rev) of the OR currents indicated that they were primarily due to the movement of K⁺. However, the gating properties of the OR currents from the epidermis differed markedly from those exhibited in the pericycle. Although both cell types displayed OR currents with voltage‐dependent gating modulated in a potassium‐dependent fashion [i.e. the activation threshold (V_0.5) was displaced to more positive voltages as extracellular K⁺ increased], the OR currents in the epidermis also displayed voltage‐independent gating by extracellular K⁺ which dramatically regulated current density. In the present study, reducing extracellular K⁺ activity from 40 to 0.87 mm reduced the OR current density in epidermal cells by approximately 80%. The chord conductance of the OR current saturated as a function of extracellular K⁺ and could be fitted with a Michaelis–Menten function to yield a binding constant (K_m) of 10.5 mm . The ability of other monovalent cations to substitute for K⁺‐gating of the OR currents was also investigated and shown to exhibit a relative sequence of K⁺ ≥ Rb⁺ > Cs⁺ > Na⁺ ≥ Li⁺ (Eisenmann sequence IV) with respect to efficacy of gating. Furthermore, single channel recordings demonstrated that channel activity rather than the single channel conductance was modulated by extracellular K⁺. In contrast, OR current density in the pericycle was largely independent of extracellular K⁺. It is suggested that the contrasting gating properties of the K⁺ channels in the epidermis and pericycle reflect their different physiological roles, particularly with respect to their role in K⁺ (nutrient) transport from the soil solution to the shoot.     

III. Ion Channel Expression in PMA-differentiated Human THP-1 Macrophages

Ion channel expression was studied in THP-1 human monocytic leukemia cells induced to differentiate into macrophage-like cells by exposure to the phorbol ester, phorbol 12-myristate 13-acetate (PMA). Inactivating delayed rectifier K⁺ currents, I _DR, present in almost all undifferentiated THP-1 monocytes, were absent from PMA-differentiated macrophages. Two K⁺ channels were observed in THP-1 cells only after differentiation into macrophages, an inwardly rectifying K⁺ channel (I _IR) and a Ca²⁺-activated maxi-K channel (I _BK). I _IR was a classical inward rectifier, conducting large inward currents negative to E _K and very small outward currents. I _IR was blocked in a voltage-dependent manner by Cs⁺, Na⁺, and Ba²⁺, block increasing with hyperpolarization. Block by Na⁺ and Ba²⁺ was time-dependent, whereas Cs⁺ block was too fast to resolve. Rb⁺ was sparingly permeant. In cell-attached patches with high [K⁺] in the pipette, the single I _IR channel conductance was ∼30 pS and no outward current could be detected. I _BK channels were observed in cell-attached or inside-out patches and in whole-cell configuration. In cell-attached patches the conductance was ∼200–250 pS and at potentials positive to ∼100 mV a negative slope conductance of the unitary current was observed, suggesting block by intracellular Na⁺. I _BK was activated at large positive potentials in cell-attached patches; in inside-out patches the voltage-activation relationship was shifted to more negative potentials by increased [Ca²⁺]. Macroscopic I _BK was blocked by external TEA⁺ with half block at 0.35 mm. THP-1 cells were found to contain mRNA for Kv1.3 and IRK1. Levels of mRNA coding for these K⁺ channels were studied by competitive PCR (polymerase chain reaction), and were found to change upon differentiation in the same direction as did channel expression: IRK1 mRNA increased at least 5-fold, and Kv1.3 mRNA decreased on average 7-fold. Possible functional correlates of the changes in ion channel expression during differentiation of THP-1 cells are discussed. Received: 19 September 1995/Revised: 14 March 1996     

Control of voltage-gated K+ channel permeability to NMDG+ by a residue at the outer pore

Crystal structures of potassium (K⁺) channels reveal that the selectivity filter, the narrow portion of the pore, is only ∼3-Å wide and buttressed from behind, so that its ability to expand is highly constrained, and the permeation of molecules larger than Rb⁺ (2.96 Å in diameter) is prevented. N-methyl-d-glucamine (NMDG⁺), an organic monovalent cation, is thought to be a blocker of Kv channels, as it is much larger (∼7.3 Å in mean diameter) than K⁺ (2.66 Å in diameter). However, in the absence of K⁺, significant NMDG⁺ currents could be recorded from human embryonic kidney cells expressing Kv3.1 or Kv3.2b channels and Kv1.5 R487Y/V, but not wild-type channels. Inward currents were much larger than outward currents due to the presence of intracellular Mg²⁺ (1 mM), which blocked the outward NMDG⁺ current, resulting in a strong inward rectification. The NMDG⁺ current was inhibited by extracellular 4-aminopyridine (5 mM) or tetraethylammonium (10 mM), and largely eliminated in Kv3.2b by an S6 mutation that prevents the channel from opening (P468W) and by a pore helix mutation in Kv1.5 R487Y (W472F) that inactivates the channel at rest. These data indicate that NMDG⁺ passes through the open ion-conducting pore and suggest a very flexible nature of the selectivity filter itself. 0.3 or 1 mM K⁺ added to the external NMDG⁺ solution positively shifted the reversal potential by ∼16 or 31 mV, respectively, giving a permeability ratio for K⁺ over NMDG⁺ (P_K⁺/P_NMDG⁺) of ∼240. Reversal potential shifts in mixtures of K⁺ and NMDG⁺ are in accordance with P_K⁺/P_NMDG⁺, indicating that the ions compete for permeation and suggesting that NMDG⁺ passes through the open state. Comparison of the outer pore regions of Kv3 and Kv1.5 channels identified an Arg residue in Kv1.5 that is replaced by a Tyr in Kv3 channels. Substituting R with Y or V allowed Kv1.5 channels to conduct NMDG⁺, suggesting a regulation by this outer pore residue of Kv channel flexibility and, as a result, permeability.     

Inactivation gating of Kv7.1 channels does not involve concerted cooperative subunit interactions

Inactivation is an intrinsic property of numerous voltage-gated K⁺ (Kv) channels and can occur by N-type or/and C-type mechanisms. N-type inactivation is a fast, voltage independent process, coupled to activation, with each inactivation particle of a tetrameric channel acting independently. In N-type inactivation, a single inactivation particle is necessary and sufficient to occlude the pore. C-type inactivation is a slower process, involving the outermost region of the pore and is mediated by a concerted, highly cooperative interaction between all four subunits. Inactivation of Kv7.1 channels does not exhibit the hallmarks of N- and C-type inactivation. Inactivation of WT Kv7.1 channels can be revealed by hooked tail currents that reflects the recovery from a fast and voltage-independent inactivation process. However, several Kv7.1 mutants such as the pore mutant L273F generate an additional voltage-dependent slow inactivation. The subunit interactions during this slow inactivation gating remain unexplored. The goal of the present study was to study the nature of subunit interactions along Kv7.1 inactivation gating, using concatenated tetrameric Kv7.1 channel and introducing sequentially into each of the four subunits the slow inactivating pore mutation L273F. Incorporating an incremental number of inactivating mutant subunits did not affect the inactivation kinetics but slowed down the recovery kinetics from inactivation. Results indicate that Kv7.1 inactivation gating is not compatible with a concerted cooperative process. Instead, adding an inactivating subunit L273F into the Kv7.1 tetramer incrementally stabilizes the inactivated state, which suggests that like for activation gating, Kv7.1 slow inactivation gating is not a concerted process.     

An Extracellular Ion Pathway Plays a Central Role in the Cooperative Gating of a K2P K+ Channel by Extracellular pH

Proton-gated TASK-3 K⁺ channel belongs to the K_2P family of proteins that underlie the K⁺ leak setting the membrane potential in all cells. TASK-3 is under cooperative gating control by extracellular [H⁺]. Use of recently solved K_2P structures allows us to explore the molecular mechanism of TASK-3 cooperative pH gating. Tunnel-like side portals define an extracellular ion pathway to the selectivity filter. We use a combination of molecular modeling and functional assays to show that pH-sensing histidine residues and K⁺ ions mutually interact electrostatically in the confines of the extracellular ion pathway. K⁺ ions modulate the pK_a of sensing histidine side chains whose charge states in turn determine the open/closed transition of the channel pore. Cooperativity, and therefore steep dependence of TASK-3 K⁺ channel activity on extracellular pH, is dependent on an effect of the permeant ion on the channel pH_o sensors.