Crucial points within the pore as determinants of K⁺ channel conductance and gating

While selective for K⁺, K⁺ channels vary significantly among their rate of ion permeation. Here, we probe the effect of steric hindrance and electrostatics within the ion conduction pathway on K⁺ permeation in the MthK K⁺ channel using structure-based mutagenesis combined with single-channel electrophysiology and X-ray crystallography. We demonstrate that changes in side-chain size and polarity at Ala88, which forms the constriction point of the open MthK pore, have profound effects on single-channel conductance as well as open probability. We also reveal that the negatively charged Glu92s at the intracellular entrance of the open pore form an electrostatic trap, which stabilizes a hydrated K⁺ and facilitates ion permeation. This electrostatic attraction is also responsible for intracellular divalent blockage, which renders the channel inward rectified in the presence of Ca²⁺. In light of the high structural conservation of the selectivity filter, the size and chemical environment differences within the portion of the ion conduction pathway other than the filter are likely the determinants for the conductance variations among K⁺ channels.     

Intersubunit Coupling in the Pore of BK Channels

The structural basis underlying the gating of large conductance Ca²⁺-activated K⁺ (BK) channels remains elusive. We found that substitution of Leu-312 in the S6 transmembrane segment of mSlo1 BK channels with hydrophilic amino acids of smaller side-chain volume favored the open state. The sensitivities of channels to calcium and voltage were modified by some mutations and completely abolished by others. Interpretation of the results in terms of an allosteric model suggests that the calcium-insensitive mutants greatly destabilize the closed relative to the open conformation and may also disrupt the allosteric coupling between Ca²⁺ or voltage sensors and the gate. Some Phe-315 mutations also favor the open state, suggesting that Leu-312 and Phe-315 may interact in the closed state, forming a major energy barrier that the channel has to overcome to open. Homology modeling and molecular dynamic simulations further support that the side chain of Leu-312 can couple strongly with the aromatic ring of Phe-315 in neighboring subunits (L-F coupling) to maintain the channel closed. Additionally, single-channel recordings indicate that the calcium-insensitive mutants, whose kinetics can be approximately characterized by a two-state closed-open (C-O) model, exhibit nearly 100% open probability under physiological conditions without alterations in single-channel conductance. These findings provide a basis for understanding the structure and gating of the BK channel pore.High conductance, “big” K⁺ (BK)⁴ channels encoded by the Slo1 gene are widely expressed in many tissues and respond to both membrane depolarization and submembrane Ca²⁺ concentration ([Ca²⁺]_i) (1–4). Because BK channels have apparently evolved from voltage-dependent K⁺ (K_V) channels, they share many features in common with K_V channels such as a similar K⁺ selectivity filter and conserved ion conduction pore (5). On the other hand, detailed studies indicate that there are significant differences in the permeation and gating properties of K_V and BK channels. First, BK channels have the largest single-channel conductance among K⁺ channels under similar recording conditions (6), partly because of two negatively charged rings at the entrance to the intracellular vestibule of BK channels that are absent from many K_V channels (7). Second, the mouth of the BK pore on the cytoplasmic side appears to be larger than other K⁺ channels because the on-rates for channel block by quaternary ammonium (QA) ions are limited only by diffusion (8), whereas the on-rates for QA block of other K⁺ channels are substantially slower. Additionally, it has been proposed that the pore-lining S6 segment of BK channels may not act as a permeation gate (8) as in Shaker K_V channels (9). Therefore, the BK channel may have an unusual pore, and understanding the structural basis of the above differences could provide important insight into the permeation and gating properties of K⁺ channels.Despite the differences between BK and K_V channels, it is likely that the opening and closing of their pores involve similar conformational changes. Flexing of the inner S6 helix at or near a conserved glycine residue is thought to open the pore, whereas straightening closes it (10, 11). The inner helix of BK channels is potentially more flexible than that of K_V channels because it contains a twin glycine motif (Gly-310–Gly-311). Differences in permeation property, pore geometry, and gating could potentially be accounted for by differences in S6 flexibility as well as the specific side-chain properties and interactions that occur between pore-lining residues. In this study we focused on Leu-312 and Phe-315 because we inferred from sequence analogy with KcsA channels (12) and our previous studies of BK channels (13, 14) that they are two of the five pore-lining residues (the others being Leu-309, Val-319, and Ile-323), and they are near the putative gating hinge. Our results indicate that substitutions of Leu-312 or Phe-315 have profound effects on BK channel gating, consistent with the notion that these residues interact between different subunits to hold the channel closed. The interaction of these residues may also be important for coordinating conformational changes in different subunits to ensure the efficient and cooperative long-range coupling between channel subunits, which is probably a general property of allosterically regulated proteins. Moreover, a surprising loss of Ca²⁺- and voltage sensitivity that accompanies mutations of Leu-312 or Phe-315 raises the possibility that these residues play a broader role in allosteric communication between sensors and gates.     

Pore dimensions and the role of occupancy in unitary conductance of Shaker K channels

K channels mediate the selective passage of K⁺ across the plasma membrane by means of intimate interactions with ions at the pore selectivity filter located near the external face. Despite high conservation of the selectivity filter, the K⁺ transport properties of different K channels vary widely, with the unitary conductance spanning a range of over two orders of magnitude. Mutation of Pro475, a residue located at the cytoplasmic entrance of the pore of the small-intermediate conductance K channel Shaker (Pro475Asp (P475D) or Pro475Gln (P475Q)), increases Shaker’s reported ∼20-pS conductance by approximately six- and approximately threefold, respectively, without any detectable effect on its selectivity. These findings suggest that the structural determinants underlying the diversity of K channel conductance are distinct from the selectivity filter, making P475D and P475Q excellent probes to identify key determinants of the K channel unitary conductance. By measuring diffusion-limited unitary outward currents after unilateral addition of 2 M sucrose to the internal solution to increase its viscosity, we estimated a pore internal radius of capture of ∼0.82 Å for all three Shaker variants (wild type, P475D, and P475Q). This estimate is consistent with the internal entrance of the Kv1.2/2.1 structure if the effective radius of hydrated K⁺ is set to ∼4 Å. Unilateral exposure to sucrose allowed us to estimate the internal and external access resistances together with that of the inner pore. We determined that Shaker resistance resides mainly in the inner cavity, whereas only ∼8% resides in the selectivity filter. To reduce the inner resistance, we introduced additional aspartate residues into the internal vestibule to favor ion occupancy. No aspartate addition raised the maximum unitary conductance, measured at saturating [K⁺], beyond that of P475D, suggesting an ∼200-pS conductance ceiling for Shaker. This value is approximately one third of the maximum conductance of the large conductance K (BK) channel (the K channel of highest conductance), reducing the energy gap between their K⁺ transport rates to ∼1 kT. Thus, although Shaker’s pore sustains ion translocation as the BK channel’s does, higher energetic costs of ion stabilization or higher friction with the ion’s rigid hydration cage in its narrower aqueous cavity may entail higher resistance.     

Multi-ion distributions in the cytoplasmic domain of inward rectifier potassium channels

Inward rectifier potassium (Kir) channels act as cellular diodes, allowing unrestricted flow of potassium (K⁺) into the cell while preventing currents of large magnitude in the outward direction. The rectification mechanism by which this occurs involves a coupling between K⁺ and intracellular blockers—magnesium (Mg²⁺) or polyamines—that simultaneously occupy the permeation pathway. In addition to the transmembrane pore, Kirs possess a large cytoplasmic domain (CD) that provides a favorable electronegative environment for cations. Electrophysiological experiments have shown that the CD is a key regulator of both conductance and rectification. In this study, we calculate and compare averaged equilibrium probability densities of K⁺ and Cl⁻ in open-pore models of the CDs of a weak (Kir1.1-ROMK) and a strong (Kir2.1-IRK) rectifier through explicit-solvent molecular-dynamics simulations in ∼1 M KCl. The CD of both channels concentrates K⁺ ions greater than threefold inside the cytoplasmic pore while IRK shows an additional K⁺ accumulation region near the cytoplasmic entrance. Simulations carried out with Mg²⁺ or spermine (SPM⁴⁺) show that these ions interact with pore-lining residues, shielding the surface charge and reducing K⁺ in both channels. The results also show that SPM⁴⁺ behaves differently inside these two channels. Although SPM⁴⁺ remains inside the CD of ROMK, it diffuses around the entire volume of the pore. In contrast, this polyatomic cation finds long-lived conformational states inside the IRK pore, interacting with residues E224, D259, and E299. The strong rectifier CD is also capable of sequestering an additional SPM⁴⁺ at the cytoplasmic entrance near a cluster of negative residues D249, D274, E275, and D276. Although understanding the actual mechanism of rectification blockade will require high-resolution structural information of the blocked state, these simulations provide insight into how sequence variation in the CD can affect the multi-ion distributions that underlie the mechanisms of conduction, rectification affinity, and kinetics.     

The ACh-induced whole-cell currents in sheep parotid secretory cells. Do BK channels really carry the ACh-evoked whole-cell K+ current?

As in other salivary glands, the secretory cells of the sheep parotid have a resting K⁺ conductance that is dominated by BK channels, which are activated by acetylcholine (ACh) and are blocked by tetraethylammonium (TEA). Nevertheless, perfusion studies indicate that TEA does not inhibit ACh-evoked fluid secretion or K⁺ efflux from intact sheep parotid glands. In the present study, we have used whole-cell patch clamp techniques to show that ACh activates K⁺ and Cl^– conductances in sheep parotid secretory cells by increasing intracellular free Ca²⁺, and we have compared the blocker sensitivity of the ACh-evoked whole-cell K⁺ current to the previously reported blocker sensitivity of the BK channels seen in these cells.The ACh-induced whole-cell K⁺ current was not blocked by TEA (10 mmol/l) or verapamil (100 mol/l), both of which block the resting K⁺ conductance and inhibit BK channels in these cells. Quinine (1 mmol/l) and quinidine (1 mmol/l), although only weak blockers of the resting K⁺ conductance, inhibited the ACh-evoked current at 0 mV (K⁺ current), by 68% and 78%, respectively. 4-Aminopyridine (10 mmol/l) partially inhibited the ACh-induced K⁺ current and caused it to fluctuate. It also caused the resting membrane currents to fluctuate, possibly by altering cytosolic free Ca²⁺. Ba²⁺ (100 mol/l), a blocker of the inwardly rectifying K⁺ conductance in sheep parotid cells, had no effect on the ACh-induced K⁺ current.We conclude that the ACh-induced K⁺ conductance in sheep parotid cells is pharmacologically distinct from both the outwardly rectifying (BK) K⁺ conductance and the inwardly rectifying K⁺ conductance seen in unstimulated cells. Given that in vitro perfusion and K⁺ efflux studies on other salivary glands in which BK channels dominate the resting conductance (e.g., the rat mandibular, rat parotid and mouse mandibular glands) have revealed an insensitivity to TEA, suggesting that BK channels do not carry the ACh-evoked K⁺ current, we propose that BK channels do not contribute substantially to the K⁺ current evoked by ACh in the secretory cells of most salivary glands.This project was supported by the Australian Research Council. We thank Dr. N. Sangster, Dr. J. Rothwell and Mr. R. Murphy for giving us access to their sheep.     

Single-Channel Characteristics of Wild-Type IKs Channels and Channels formed with Two MinK Mutants that Cause Long QT Syndrome

I_Ks channels are voltage dependent and K⁺ selective. They influence cardiac action potential duration through their contribution to myocyte repolarization. Assembled from minK and KvLQT1 subunits, I_Ks channels are notable for a heteromeric ion conduction pathway in which both subunit types contribute to pore formation. This study was undertaken to assess the effects of minK on pore function. We first characterized the properties of wild-type human I_Ks channels and channels formed only of KvLQT1 subunits. Channels were expressed in Xenopus laevis oocytes or Chinese hamster ovary cells and currents recorded in excised membrane patches or whole-cell mode. Unitary conductance estimates were dependent on bandwidth due to rapid channel “flicker.” At 25 kHz in symmetrical 100-mM KCl, the single-channel conductance of I_Ks channels was ∼16 pS (corresponding to ∼0.8 pA at 50 mV) as judged by noise-variance analysis; this was fourfold greater than the estimated conductance of homomeric KvLQT1 channels. Mutant I_Ks channels formed with D76N and S74L minK subunits are associated with long QT syndrome. When compared with wild type, mutant channels showed lower unitary currents and diminished open probabilities with only minor changes in ion permeabilities. Apparently, the mutations altered single-channel currents at a site in the pore distinct from the ion selectivity apparatus. Patients carrying these mutant minK genes are expected to manifest decreased K⁺ flux through I_Ks channels due to lowered single-channel conductance and altered gating.     

K+ Conduction and Mg2+ Blockade in a Shaker Kv-Channel Single Point Mutant with an Unusually High Conductance

Potassium channels exhibit a large diversity of single-channel conductances. Shaker is a low-conductance K-channel in which Pro475→Asp, a single-point mutation near the internal pore entrance, promotes 6- to 8-fold higher unitary current. To assess the mechanism for this higher conductance, we measured Shaker-P475D single-channel current in a wide range of symmetrical K⁺ concentrations and voltages. Below 300 mM K⁺, the current-to-voltage relations (i-V) showed inward rectification that disappeared at 1000 mM K⁺. Single-channel conductance reached a maximum of ～190 pS at saturating [K⁺], a value 4- to 5-fold larger than that estimated for the native channel. Intracellular Mg²⁺ blocked this variant with ～100-fold higher affinity. Near zero voltage, blockade was competitively antagonized by K⁺; however, at voltages >100 mV, it was enhanced by K⁺. This result is consistent with a lock-in effect in a single-file diffusion regime of Mg²⁺ and K⁺ along the pore. Molecular-dynamics simulations revealed higher K⁺ density in the pore, especially near the Asp-475 side chains, as in the high-conductance MthK bacterial channel. The molecular dynamics also showed that K⁺ ions bound distally can coexist with other K⁺ or Mg²⁺ in the cavity, supporting a lock-in mechanism. The maximal K⁺ transport rate and higher occupancy could be due to a decrease in the electrostatic energy profile for K⁺ throughout the pore, reducing the energy wells and barriers differentially by ～0.7 and ～2 kT, respectively.     

Bupivacaine inhibits large conductance,voltage- and Ca2+- activated K+ channels in human umbilical artery smooth muscle cells

Bupivacaine is a local anesthetic compound belonging to the amino amide group. Its anesthetic effect is commonly related to its inhibitory effect on voltage-gated sodium channels. However, several studies have shown that this drug can also inhibit voltage-operated K⁺ channels by a different blocking mechanism. This could explain the observed contractile effects of bupivacaine on blood vessels. Up to now, there were no previous reports in the literature about bupivacaine effects on large conductance voltage- and Ca²⁺-activated K⁺ channels (BK_Ca). Using the patch-clamp technique, it is shown that bupivacaine inhibits single-channel and whole-cell K⁺ currents carried by BK_Ca channels in smooth muscle cells isolated from human umbilical artery (HUA). At the single-channel level bupivacaine produced, in a concentration- and voltage-dependent manner (IC₅₀ 324 µM at +80 mV), a reduction of single-channel current amplitude and induced a flickery mode of the open channel state. Bupivacaine (300 µM) can also block whole-cell K⁺ currents (~45% blockage) in which, under our working conditions, BK_Ca is the main component. This study presents a new inhibitory effect of bupivacaine on an ion channel involved in different cell functions. Hence, the inhibitory effect of bupivacaine on BK_Ca channel activity could affect different physiological functions where these channels are involved. Since bupivacaine is commonly used during labor and delivery, its effects on umbilical arteries, where this channel is highly expressed, should be taken into account.     

The Ach-evoked Ca2+-activated K+ Current in Mouse Mandibular Secretory Cells. Single Channel Studies

Although acetylcholine (ACh) is able to activate voltage- and Ca²⁺-sensitive K⁺ (BK) channels in mouse mandibular secretory cells, our recent whole cell studies have suggested that these channels, like those in sheep parotid secretory cells, do not contribute appreciably to the conductance that carries the ACh-evoked whole cell K⁺ current. In the present study, we have used cell-attached patch clamp methods to identify and characterize the K⁺ channel type responsible for carrying the bulk of this current. When the cells were bathed in a NaCl-rich solution the predominant channel type activated by ACh (1 μmol/l or 50 nmol/l) had a conductance only of 40 pS; it was not blocked by TEA but it was sensitive to quinine and it conducted Rb⁺ to an appreciable extent. BK channels, which could be seen in some but not all patches from resting cells, also showed increased activity when ACh was added to the bath, but they were much less conspicuous during ACh stimulation than the 40-pS channels. When the cells were bathed in a KCl-rich rather than a NaCl-rich solution, a small-conductance K⁺ channel, sensitive to quinine but not to TEA, was still the most conspicuous channel to be activated by ACh although its conductance was reduced to 25 pS. Our studies confirm that the ACh-evoked whole-cell K⁺ current is not carried substantially by BK channels and show that it is carried by a small-conductance K⁺ channel with quite different properties. Received: 28 September 1995/Revised: 26 December 1995     

Clustered Distribution of Calcium Sensitivities: An Indication of Hetero-tetrameric Gating Components in Ca2+-activated K+ Channels Reconstituted from Avian Nasal Gland Cells

High-conductance, Ca²⁺-activated K⁺ channels from the basolateral membrane of rabbit distal colon epithelial cells were reconstituted into planar phospholipid bilayers to examine the effect of Mg²⁺ on the single-channel properties. Mg²⁺ decreases channel current and conductance in a concentration-dependent manner from both the cytoplasmic and the extracellular side of the channel. In contrast to other K⁺ channels, Mg²⁺ does not cause rectification of current through colonic Ca²⁺-activated K⁺ channels. In addition, cytoplasmic Mg²⁺ decreases the reversal potential of the channel. The Mg²⁺-induced decrease in channel conductance is relieved by high K⁺ concentrations, indicating competitive interaction between K⁺ and Mg²⁺. The monovalent organic cation choline also decreases channel conductance and reversal potential, suggesting that the effect is unspecific. The inhibition of channel current by Mg²⁺ and choline most likely is a result of electrostatic screening of negative charges located superficially in the channel entrance. But in addition to charge, other properties appear to be necessary for channel inhibition, as Na⁺ and Ba²⁺ are no (or only weak) inhibitors. Mg²⁺ and possibly other cations may play a role in the regulation of current through these channels. Received: 25 August 1995/Revised: 16 November 1995     

Quantification and distribution of big conductance Ca-activated K channels in kidney epithelia

Big conductance Ca²⁺ activated K⁺ channels (BK channels) is an abundant channel present in almost all kind of tissue. The accurate quantity and especially the precise distribution of this channel in kidney epithelia are, however, still debated. The aim of the present study has therefore been to examine the presence of BK channels in kidney epithelia and determine the actual number and distribution of these channels. For this purpose, a selective peptidyl ligand for BK channels called iberiotoxin or the radiolabeled double mutant analog ¹²⁵I-IbTX-D19Y/Y36F has been employed. The presence of BK channels were determined by a isotope flux assay where up to 44% of the total K⁺ channel activity could be inhibited by iberiotoxin indicating that BK channels are widely present in kidney epithelia. Consistent with these functional studies, ¹²⁵I-IbTX-D19Y/Y36F binds to membrane vesicles from outer cortex, outer medulla and inner medulla with B_max values (in fmol/mg protein) of 6.8, 2.6 and 21.4, respectively. These studies were performed applying rabbit kidney epithelia tissue. The distinct distribution of BK channels in both rabbit and rat kidney epithelia was confirmed by autoradiography and immunohistochemical studies. In cortical collecting ducts, BK channels were exclusively located in principal cells while no channels could be found in intercalated cells. The abundant and distinct distribution in kidney epithelia talks in favor for BK channels being important contributors in maintaining salt and water homeostasis.     

Oscillating activity of a calcium-activated K+ channel in normal and cancerous mammary cells in culture

Summary Calcium-activated potassium channels were the channels most frequently observed in primary cultured normal mammary cell and in the established mammary tumor cell, MMT060562. In both cells, single-channel and whole-cell clamp recordings sometimes showed slow oscillations of the Ca²⁺-gated K⁺ current. The characteristics of the Ca²⁺-activated K⁺ channels in normal and cancerous mammary cells were quite similar. The slope conductances changed from 8 to 70 pS depending on the mode of recording and the ionic composition in the patch electrode. The open probability of this channel increased between 0.1 to 1 m of the intracellular Ca²⁺, but it was independent of the membrane potential.Charybdotoxin reduced the activity of the Ca²⁺-activated K⁺ channel and the oscillation of the membrane current, but apamin had no apparent effect. The application of tetraethylammonium (TEA) from outside and BaCl₂ from inside of the cell diminished the activity of the channel. The properties of this channel were different from those of both the large conductance (BK or MAXI K) and small conductance (SK) type Ca²⁺-activated K⁺ channels.     

Three Types of Single Voltage-Dependent Potassium Channels in the Sarcolemma of Frog Skeletal Muscle

Patch-clamp experiments in the sarcolemma of frog skeletal muscle evidenced the presence of three types of voltage-dependent single-channel K⁺ currents. According to their unitary conductance at a membrane voltage of +40 mV, we classified them as 16-, 13-, and 7-pS K⁺ channels. The 16-pS K⁺ channels are active close to a membrane voltage of −80 mV and they do not become inactivated during voltage pulses of 100 ms. Within 10 min after beginning the recording, these channels developed rundown with an exponential time course. The 13-pS K⁺ channels are active near −60 mV; upon a 100-ms depolarization, they exhibited inactivation with an approximate exponential time course. The 7-pS K⁺ channels were recorded at voltages positive to 0 mV. In patches containing all three types of K⁺ channels, the ensemble average currents resemble the kinetic properties of the macroscopic delayed rectifier K⁺ currents recorded in skeletal muscle and other tissues. In conclusion, the biophysical properties of unitary K⁺ currents suggest that these single-channel K⁺ currents may underlie the macroscopic delayed K⁺ currents in frog skeletal muscle fibers. In addition, since the 16- and 13-pS channels were more frequently recorded, both are the main contributors to the delayed K⁺ currents.     

Paxilline inhibits BK channels by an almost exclusively closed-channel block mechanism

Paxilline, a tremorogenic fungal alkaloid, potently inhibits large conductance Ca²⁺- and voltage-activated K⁺ (BK)-type channels, but little is known about the mechanism underlying this inhibition. Here we show that inhibition is inversely dependent on BK channel open probability (Po), and is fully relieved by conditions that increase Po, even in the constant presence of paxilline. Manipulations that shift BK gating to more negative potentials reduce inhibition by paxilline in accordance with the increase in channel Po. Measurements of Po times the number of channels at negative potentials support the idea that paxilline increases occupancy of closed states, effectively reducing the closed–open equilibrium constant, L(0). Gating current measurements exclude an effect of paxilline on voltage sensors. Steady-state inhibition by multiple paxilline concentrations was determined for four distinct equilibration conditions, each with a distinct Po. The IC₅₀ for paxilline shifted from around 10 nM when channels were largely closed to near 10 µM as maximal Po was approached. Model-dependent analysis suggests a mechanism of inhibition in which binding of a single paxilline molecule allosterically alters the intrinsic L(0) favoring occupancy of closed states, with affinity for the closed conformation being >500-fold greater than affinity for the open conformation. The rate of inhibition of closed channels was linear up through 2 µM paxilline, with a slope of 2 × 10⁶ M⁻¹s⁻¹. Paxilline inhibition was hindered by either the bulky cytosolic blocker, bbTBA, or by concentrations of cytosolic sucrose that hinder ion permeation. However, paxilline does not hinder MTSET modification of the inner cavity residue, A313C. We conclude that paxilline binds more tightly to the closed conformation, favoring occupancy of closed-channel conformations, and propose that it binds to a superficial position near the entrance to the central cavity, but does not hinder access of smaller molecules to this cavity.     

Shab K+ channel slow inactivation

Herein, we report the first characterization of Shab slow inactivation. Open Shab channels inactivate within seconds, with two voltage-independent time constants. Additionally, Shab presents significant closed-state inactivation. We found that with short depolarizing pulses, shorter than the slowest inactivation time constant, the resulting inactivation curve has a marked U-shape, but as pulse duration increases, approaching steady-state conditions, the U-shape vanishes, and the resulting inactivation curves converge to the classical Boltzmann h_∞ curve. Regarding the mechanism of inactivation, we found that external K⁺ and TEA facilitate both open- and closed-state inactivation, while the cavity blocker quinidine hinders inactivation. These results together with our previous observations regarding the K⁺-dependent stability of the K⁺ conductance, suggest the novel hypothesis that inactivation of Shab channels, and possibly that of other Kv channels whose inactivation is facilitated by K⁺, does not involve a significant narrowing of the extracellular entry of the pore. Instead, we hypothesize that there is only a rearrangement of a more internal segment of the pore that affects the central cavity and halts K⁺ conduction.     

Ca2+-activated K+ permeability in human erythrocytes: Modulation of single-channel events

Elevated levels of intracellular Ca²⁺ activate a K⁺-selective permeability in the membrane of human erythrocytes. Currents through single channels were analysed in excised inside-out membrane patches. The effects of several ions that are known to inhibit K⁺ fluxes are described with respect to the single-channel events. The results suggest that the blocking ions can partly move into the channels (but cannot penetrate) and interact with other ions inside the pore. The reduction of single-channel conductance by Cs⁺, tetraethylammonium and Ba²⁺ and of single-channel activity by quinine and Ba²⁺ is referred to different rates of access to the channel. The concentration- and voltage-dependent inhibition by ions with measurable permeability (Na⁺ and Rb⁺) can be explained by their lower permeability, with single-file movement and ionic interactions inside the pore.     

Unique inner pore properties of BK channels revealed by quaternary ammonium block

Potassium channels have a very wide distribution of single-channel conductance, with BK type Ca(2+)-activated K(+) channels having by far the largest. Even though crystallographic views of K(+) channel pores have become available, the structural basis underlying BK channels' large conductance has not been completely understood. In this study we use intracellularly applied quaternary ammonium compounds to probe the pore of BK channels. We show that molecules as large as decyltriethylammonium (C(10)) and tetrabutylammonium (TBA) have much faster block and unblock rates in BK channels when compared with any other tested K(+) channel types. Additionally, our results suggest that at repolarization large QA molecules may be trapped inside blocked BK channels without slowing the overall process of deactivation. Based on these findings we propose that BK channels may differ from other K(+) channels in its geometrical design at the inner mouth, with an enlarged cavity and inner pore providing less spatially restricted access to the cytoplasmic solution. These features could potentially contribute to the large conductance of BK channels.     

Dipole moments of scorpion toxins direct the interaction towards small- or large-conductance Ca2+-activated K+ channels

Summary Ca²⁺-activated K⁺ channels consist of a large family of membrane proteins, among which two groups have been characterized by electrophysiological criteria, the small conductance (SK) and the large conductance (BK) Ca²⁺-activated K⁺ channels. Scorpion toxins that block K⁺ channels exhibit a common three-dimensional structure constituted of a short α-helix connected by disulfide bonds to a β-sheet. The leiurotoxin I (LTX1) related toxins interact specifically with the SK channel via basic residues of their α-helix, while the charybdotoxin (ChTX) family recognizes the BK channel with basic residues of their β-sheet. In an attempt to better understand the structure-activity relationships of these toxins and the characteristics of the electrostatic interactions with the receptor site, we investigated the electrostatic potential supported by natural toxins and a synthetic analogue to find out if it may help in understanding the molecular mechanisms involved in this peptide-protein interaction.     

Lack of negative slope in I-V plots for BK channels at positive potentials in the absence of intracellular blockers

Large-conductance, voltage- and Ca²⁺-activated K⁺ (BK) channels display near linear current–voltage (I-V) plots for voltages between −100 and +100 mV, with an increasing sublinearity for more positive potentials. As is the case for many types of channels, BK channels are blocked at positive potentials by intracellular Ca²⁺ and Mg²⁺. This fast block progressively reduces single-channel conductance with increasing voltage, giving rise to a negative slope in the I-V plots beyond about +120 mV, depending on the concentration of the blockers. In contrast to these observations of pronounced differences in the magnitudes and shapes of I-V plots in the absence and presence of intracellular blockers, Schroeder and Hansen (2007. J. Gen. Physiol. http://dx.doi.org/10.1085/jgp.200709802) have reported identical I-V plots in the absence and presence of blockers for BK channels, with both plots having reduced conductance and negative slopes, as expected for blockers. Schroeder and Hansen included both Ca²⁺ and Mg²⁺ in the intracellular solution rather than a single blocker, and they also studied BK channels expressed from α plus β1 subunits, whereas most previous studies used only α subunits. Although it seems unlikely that these experimental differences would account for the differences in findings between previous studies and those of Schroeder and Hansen, we repeated the experiments using BK channels comprised of α plus β1 subunits with joint application of 2.5 mM Ca²⁺ plus 2.5 mM Mg²⁺, as Schroeder and Hansen did. In contrast to the findings of Schroeder and Hansen of identical I-V plots, we found marked differences in the single-channel I-V plots in the absence and presence of blockers. Consistent with previous studies, we found near linear I-V plots in the absence of blockers and greatly reduced currents and negative slopes in the presence of blockers. Hence, studies of conductance mechanisms for BK channels should exclude intracellular Ca²⁺/Mg²⁺, as they can reduce conductance and induce negative slopes.