An inactivation gate in the selectivity filter of KCNQ1 potassium channels

Inactivation is an inherent property of most voltage-gated K⁺ channels. While fast N-type inactivation has been analyzed in biophysical and structural details, the mechanisms underlying slow inactivation are yet poorly understood. Here, we characterized a slow inactivation mechanism in various KCNQ1 pore mutants, including L273F, which hinders entry of external Ba²⁺ to its deep site in the pore and traps it by slowing its egress. Kinetic studies, molecular modeling, and dynamics simulations suggest that this slow inactivation involves conformational changes that converge to the outer carbonyl ring of the selectivity filter, where the backbone becomes less flexible. This mechanism involves acceleration of inactivation kinetics and enhancement of Ba²⁺ trapping at elevated external K⁺ concentrations. Hence, KCNQ1 slow inactivation considerably differs from C-type inactivation where vacation of K⁺ from the filter was invoked. We suggest that trapping of K⁺ at s₁ due to filter rigidity and hindrance of the dehydration-resolvation transition underlie the slow inactivation of KCNQ1 pore mutants.     

Conformational changes in the selectivity filter of the open-state KcsA channel: an energy minimization study

Potassium channels switch between closed and open conformations and selectively conduct K⁺ ions. There are at least two gates. The TM2 bundle at the intracellular site is the primary gate of KcsA, and rearrangements at the selectivity filter (SF) act as the second gate. The SF blocks ion flow via an inactivation process similar to C-type inactivation of voltage-gated K⁺ channels. We recently generated the open-state conformation of the KcsA channel. We found no major, possibly inactivating, structural changes in the SF associated with this massive inner-pore rearrangement, which suggests that the gates might act independently. Here we energy-minimize the open state of wild-type and mutant KcsA, validating in silico structures of energy-minimized SFs by comparison with crystallographic structures, and use these data to gain insight into how mutation, ion depletion, and K⁺ to Na⁺ substitution influence SF conformation. Both E71 or D80 protonations/mutations and the presence/absence of protein-buried water molecule(s) modify the H-bonding network stabilizing the P-loops, spawning numerous SF conformations. We find that the inactivated state corresponds to conformations with a partially unoccupied or an entirely empty SF. These structures, involving modifications in all four P-loops, are stabilized by H-bonds between amide H and carbonyl O atoms from adjacent P-loops, which block ion passage. The inner portions of the P-loops are more rigid than the outer parts. Changes are localized to the outer binding sites, with innermost site S4 persisting in the inactivated state. Strong binding by Na⁺ locally contracts the SF around Na⁺, releasing ligands that do not participate in Na⁺ coordination, and occluding the permeation pathway. K⁺ selectivity primarily appears to arise from the inability of the SF to completely dehydrate Na⁺ ions due to basic structural differences between liquid water and the “quasi-liquid” SF matrix.     

K+ channel gating: C-type inactivation is enhanced by calcium or lanthanum outside

Many voltage-gated K⁺ channels exhibit C-type inactivation. This typically slow process has been hypothesized to result from dilation of the outer-most ring of the carbonyls in the selectivity filter, destroying this ring’s ability to bind K⁺ with high affinity. We report here strong enhancement of C-type inactivation upon extracellular addition of 10–40 mM Ca²⁺ or 5–50 µM La³⁺. These multivalent cations mildly increase the rate of C-type inactivation during depolarization and markedly promote inactivation and/or suppress recovery when membrane voltage (V_m) is at resting levels (−80 to −100 mV). At −80 mV with 40 mM Ca²⁺ and 0 mM K⁺ externally, ShBΔN channels with the mutation T449A inactivate almost completely within 2 min or less with no pulsing. This behavior is observed only in those mutants that show C-type inactivation on depolarization and is distinct from the effects of Ca²⁺ and La³⁺ on activation (opening and closing of the V_m-controlled gate), i.e., slower activation of K⁺ channels and a positive shift of the mid-voltage of activation. The Ca²⁺/La³⁺ effects on C-type inactivation are antagonized by extracellular K⁺ in the low millimolar range. This, together with the known ability of Ca²⁺ and La³⁺ to block inward current through K⁺ channels at negative voltage, strongly suggests that Ca²⁺/La³⁺ acts at the outer mouth of the selectivity filter. We propose that at −80 mV, Ca²⁺ or La³⁺ ions compete effectively with K⁺ at the channel’s outer mouth and prevent K⁺ from stabilizing the filter’s outer carbonyl ring.     

Computational study of non-conductive selectivity filter conformations and C-type inactivation in a voltage-dependent potassium channel

C-type inactivation is a time-dependent process of great physiological significance that is observed in a large class of K⁺ channels. Experimental and computational studies of the pH-activated KcsA channel show that the functional C-type inactivated state, for this channel, is associated with a structural constriction of the selectivity filter at the level of the central glycine residue in the signature sequence, TTV(G)YGD. The structural constriction is allosterically promoted by the wide opening of the intracellular activation gate. However, whether this is a universal mechanism for C-type inactivation has not been established with certainty because similar constricted structures have not been observed for other K⁺ channels. Seeking to ascertain the general plausibility of the constricted filter conformation, molecular dynamics simulations of a homology model of the pore domain of the voltage-gated potassium channel Shaker were performed. Simulations performed with an open intracellular gate spontaneously resulted in a stable constricted-like filter conformation, providing a plausible nonconductive state responsible for C-type inactivation in the Shaker channel. While there are broad similarities with the constricted structure of KcsA, the hypothetical constricted-like conformation of Shaker also displays some subtle differences. Interestingly, those are recapitulated by the Shaker-like E71V KcsA mutant, suggesting that the residue at this position along the pore helix plays a pivotal role in determining the C-type inactivation behavior. Free energy landscape calculations show that the conductive-to-constricted transition in Shaker is allosterically controlled by the degree of opening of the intracellular activation gate, as observed with the KcsA channel. The behavior of the classic inactivating W434F Shaker mutant is also characterized from a 10-μs MD simulation, revealing that the selectivity filter spontaneously adopts a nonconductive conformation that is constricted at the level of the second glycine in the signature sequence, TTVGY(G)D.     

A multipoint hydrogen-bond network underlying KcsA C-type inactivation

In the prokaryotic potassium channel KcsA activation gating at the inner bundle gate is followed by C-type inactivation at the selectivity filter. Entry into the C-type inactivated state has been directly linked to the strength of the H-bond interaction between residues Glu-71 and Asp-80 behind the filter, and is allosterically triggered by the rearrangement of the inner bundle gate. Here, we show that H-bond pairing between residues Trp-67 and Asp-80, conserved in most K⁺ channels, constitutes another critical interaction that determines the rate and extent of KcsA C-type inactivation. Disruption of the equivalent interaction in Shaker (Trp-434-Asp-447) and Kv1.2 (Trp-366-Asp-379) leads also to modulation of the inactivation process, suggesting that these residues also play an analogous role in the inactivation gating of Kv channels. The present results show that in KcsA C-type inactivation gating is governed by a multipoint hydrogen-bond network formed by the triad Trp-67-Glu71-Asp-80. This triad exerts a critical role in the dynamics and conformational stability of the selectivity filter and might serve as a general modulator of selectivity filter gating in other members of the K⁺ channel family.     

An electrostatic interaction between TEA and an introduced pore aromatic drives spring-in-the-door inactivation in Shaker potassium channels

Slow inactivation of Kv1 channels involves conformational changes near the selectivity filter. We examine such changes in Shaker channels lacking fast inactivation by considering the consequences of mutating two residues, T449 just external to the selectivity filter and V438 in the pore helix near the bottom of the selectivity filter. Single mutant T449F channels with the native V438 inactivate very slowly, and the canonical foot-in-the-door effect of extracellular tetraethylammonium (TEA) is not only absent, but the time course of slow inactivation is accelerated by TEA. The V438A mutation dramatically speeds inactivation in T449F channels, and TEA slows inactivation exactly as predicted by the foot-in-the-door model. We propose that TEA has this effect on V438A/T449F channels because the V438A mutation produces allosteric consequences within the selectivity filter and may reorient the aromatic ring at position 449. We investigated the possibility that the blocker promotes the collapse of the outer vestibule (spring-in-the-door) in single mutant T449F channels by an electrostatic attraction between a cationic TEA and the quadrupole moments of the four aromatic rings. To test this idea, we used in vivo nonsense suppression to serially fluorinate the introduced aromatic ring at the 449 position, a manipulation that withdraws electrons from the aromatic face with little effect on the shape, net charge, or hydrophobicity of the aromatic ring. Progressive fluorination causes monotonically enhanced rates of inactivation. In further agreement with our working hypothesis, increasing fluorination of the aromatic gradually transforms the TEA effect from spring-in-the-door to foot-in-the-door. We further substantiate our electrostatic hypothesis by quantum mechanical calculations.     

K binding in the G-loop and water cavity facilitates Ba movement in the Kir2.1 channel

K⁺ are selectively coordinated in the selectivity filter and concerted K⁺ and water movements in this region ensure high conduction rates in K⁺ channels. In channels with long pores many K⁺ binding sites are located intracellular to the selectivity filter (inner vestibule), but their contribution to permeation has not been well studied. We investigated this phenomenon by slowing the ion permeation process via blocking inwardly rectifying Kir2.1 channels with Ba²⁺ in the selectivity filter and observing the effect of K⁺ in the inner vestibule on Ba²⁺ exit. The dose-response effect of the intracellular K⁺ concentration ([K⁺]_i) on Ba²⁺ exit was recorded with and without intracellular polyamines, which compete with K⁺ for binding sites. Ba²⁺ exit was facilitated by the cooperative binding of at least three K⁺. Site-directed mutagenesis studies suggest that K⁺ interacting with Ba²⁺ bound in the selectivity filter were located in the region between selectivity filter and cytoplasmic pore, i.e. the water cavity and G-loop. One of the K⁺ binding sites was located at residue D172 and another was possibly at M301. This study provides functional evidence for the three K⁺ binding sites in the inner vestibule previously identified by crystal structure study.     

Effects of D2O on permeation and gating in the Ca2+-activated potassium channel fromChara

We studied the effects of H₂O/D₂O substitution on the permeation and gating of the large conductance Ca²⁺-activated K⁺ channels inChara gymnophylla droplet membrane using the patchclamp technique. The selectivity sequence of the channel was: K⁺>Rb⁺≫Li⁺, Na⁺, Cs⁺ and Cl⁻. The conductance of this channel in symmetric 100mm KCl was found to be 130 pS. The single channel conductance was decreased by 15% in D₂O as compared to H₂O. The blockade of channel conductance by cytosolic Ca²⁺ weakened in D₂O as a result of a decrease in zero voltage Ca²⁺ binding affinity by a factor of 1.4. Voltage-dependent channel gating was affected by D₂O primarily due to the change in Ca²⁺ binding to the channel during the activation step. The Hill coefficient for Ca²⁺ binding was 3 in D₂O and around 1 in H₂O. The values of the Ca²⁺ binding constant in the open channel conformation were 0.6 and 6 μm in H₂O and D₂O, respectively, while the binding in the closed conformation was much less affected by D₂O. The H₂O/D₂O substitution did not produce a significant change in the slope of channel voltage dependence but caused a shift as large as 60 mV with 1mm internal Ca²⁺.     

The effects of stretch activation on ionic selectivity of the TREK-2 K2P K+ channel

The TREK-2 (KCNK10) K2P potassium channel can be regulated by variety of polymodal stimuli including pressure. In a recent study, we demonstrated that this mechanosensitive K⁺ channel responds to changes in membrane tension by undergoing a major structural change from its ‘down’ state to the more expanded ‘up’ state conformation. These changes are mostly restricted to the lower part of the protein within the bilayer, but are allosterically coupled to the primary gating mechanism located within the selectivity filter. However, any such structural changes within the filter also have the potential to alter ionic selectivity and there are reports that some K2Ps, including TREK channels, exhibit a dynamic ionic selectivity. In this addendum to our previous study we have therefore examined whether the selectivity of TREK-2 is altered by stretch activation. Our results reveal that the filter remains stable and highly selective for K⁺ over Na⁺ during stretch activation, and that permeability to a range of other cations (Rb⁺, Cs⁺ and NH₄⁺) also does not change. The asymmetric structural changes that occur during stretch activation therefore allow the channel to respond to changes in membrane tension without a loss of K⁺ selectivity.     

Electrostatic state of the cytoplasmic domain influences inactivation at the selectivity filter of the KcsA potassium channel

KcsA is a proton-activated K⁺ channel that is regulated at two gates: an activation gate located in the inner entrance of the pore and an inactivation gate at the selectivity filter. Previously, we revealed that the cytoplasmic domain (CPD) of KcsA senses proton and that electrostatic changes of the CPD influences the opening and closing of the activation gate. However, our previous studies did not reveal the effect of CPD on the inactivation gate because we used a non-inactivating mutant (E71A). In the present study, we used mutants that did not harbor the E71A mutation, and showed that the electrostatic state of the CPD influences the inactivation gate. Three novel CPD mutants were generated in which some negatively charged amino acids were replaced with neutral amino acids. These CPD mutants conducted K⁺, but showed various inactivation properties. Mutants carrying the D149N mutation showed high open probability and slow inactivation, whereas those without the D149N mutation showed low open probability and fast inactivation, similar to wild-type KcsA. In addition, mutants with D149N showed poor K⁺ selectivity, and permitted Na⁺ to flow. These results indicated that electrostatic changes in the CPD by D149N mutation triggered the loss of fast inactivation and changes in the conformation of selectivity filter. Additionally, the loss of fast inactivation induced by D149N was reversed by R153A mutation, suggesting that not only the electrostatic state of D149, but also that of R153 affects inactivation.     

Shaker IR T449 Mutants Separate C- from U-Type Inactivation

Previous studies demonstrated that slow inactivation of the Shaker potassium channel can be made ~100-fold faster or slower by point mutations at a site in the outer pore (T449). However, the discovery that two forms of slow inactivation coexist in Shaker raises the question of which inactivation process is affected by mutation. Equivalent mutations in K_V2.1, a channel exhibiting only U-type inactivation, have minimal effects on inactivation, suggesting that mutation of Shaker T449 acts on C-type inactivation alone, a widely held yet untested hypothesis. This study reexamines mutations at Shaker T449, confirming that T449A speeds inactivation and T449Y/V slow it. T449Y and T449V exhibit U-type inactivation that is enhanced by high extracellular potassium, in contrast to C-type inactivation in T449A which is inhibited by high potassium. Automated parameter estimation for a 12-state Markov model suggests that U-type inactivation occurs mainly from closed states upon weak depolarization, but primarily from the open state at positive voltages. The model also suggests that WT channels, which in this study exhibit mostly C-type inactivation, recover from inactivation through closed-inactivated states, producing voltage-dependent recovery. This suggests that both C-type and U-type inactivation involve both open-inactivated and closed-inactivated states.     

Widening the scope of constriction

JGP modeling study suggests that selectivity filter constriction is a plausible mechanism for C-type inactivation of the Shaker voltage-gated potassium channel.

In response to prolonged activation, many K⁺ channels spontaneously reduce the membrane conductance by undergoing C-type inactivation, a kinetic process crucial for the pacing of cardiac action potentials and the modulation of neuronal firing patterns. In the pH-activated bacterial channel KcsA, C-type inactivation appears to involve constriction of the channel’s selectivity filer that prohibits ion conduction, but whether voltage-gated channels like Drosophila Shaker use a similar mechanism is controversial (1). In this issue of JGP, a computational study by Li et al. suggests that filter constriction is indeed a plausible mechanism for the C-type inactivation of Shaker (2).(Left to right) Jing Li, Benoît Roux, and colleagues use computational modeling to show that selectivity filter constriction, allosterically promoted by opening of the intracellular activation gate, is a plausible mechanism for the C-type inactivation of voltage-gated K⁺ channels such as Drosophila Shaker. The selectivity filter is conductive (left) when the intracellular gate is partially open, but adopts a constricted conformation (right) when the gate is open wide.Various structural approaches have shown that C-type inactivation of KcsA channels is associated with the symmetrical constriction of all four channel subunits at the level of the central glycine residue in the selectivity filter. Benoît Roux and colleagues at The University of Chicago used MD simulations to show that the KcsA pore can transition from the conductive to the constricted conformation on an appropriate timescale, and that this transition is allosterically promoted by the wide opening of the pore’s intracellular gate (3). Modeling by Roux and colleagues suggests that C-type inactivation of cardiac hERG channels could also involve selectivity filter constriction, though in this case it appears to be an asymmetric process in which only two of the channel’s subunits move closer together (4).“In view of the high similarity between the pore domains of Shaker and KcsA (almost 40% sequence identity), we wanted to examine if it’s possible for the Shaker selectivity filter to constrict and, if so, how similar it is to KcsA,” Roux explains. Led by first author Jing Li—now an assistant professor at the University of Mississippi—Roux and colleagues developed several homology models of the Shaker pore domain with the intracellular gate open to various degrees (2).MD simulations and free energy calculations revealed that the Shaker selectivity filter can dynamically transition from a conductive to a constricted conformation, and that this transition is allosterically coupled to the intracellular gate; the constricted conformation is stable when the gate is wide open. “Our computations strongly suggest that constriction is a plausible mechanism for the C-type inactivation of Shaker,” Roux says. “There’s no reason based on the currently available information to reject the existence of a constricted state in Shaker channels.”As with KcsA, Shaker channels appear to constrict symmetrically at the level of the selectivity filter’s central glycine. But Li et al.’s simulations revealed some small variations between the two channels, including differences in the number of water molecules bound to each channel subunit and the arrangement of the hydrogen-bond network they form to stabilize the constricted state.Li et al. also modeled the pore domain of the Shaker W434F mutant, which is widely assumed to be trapped in a C-type inactivated state. The simulation suggests that the mutant channel’s filter adopts a stable constricted conformation even when the intracellular gate is only partially open, although the constriction is asymmetric and occurs at the level of a different filter residue (2).Constriction may therefore be a universal mechanism of C-type inactivation, even if the exact conformation varies from channel to channel. But, says Roux, confirming this will require more experimental work using the right conditions and mutations to capture the structure of inactivated channels.     

Role of Outer-pore Residue Y380 in U-type Inactivation of KV2.1 Channels

The interpretation of slow inactivation in potassium channels has been strongly influenced by work on C-type inactivation in Shaker channels. Slow inactivation in Shaker and some other potassium channels can be dramatically modulated by the state of the pore, including mutations at outer pore residue T449, which altered inactivation kinetics up to 100-fold. K_V2.1, another voltage-dependent potassium channel, exhibits a biophysically distinct inactivation mechanism with a U-shaped voltage-dependence and preferential closed-state inactivation, termed U-type inactivation. However, it remains to be demonstrated whether U-type and C-type inactivation have different molecular mechanisms. This study examines mutations at Y380 (homologous to Shaker T449) to investigate whether C-type and U-type inactivation have distinct molecular mechanisms, and whether C-type inactivation can occur at all in K_V2.1. Y380 mutants do not introduce C-type inactivation into K_V2.1 and have little effect on U-type inactivation of K_V2.1. Interestingly, two of the mutants tested exhibit twofold faster recovery from inactivation compared to wild-type channels. The observation that mutations have little effect suggests K_V2.1 lacks C-type inactivation as it exists in Shaker and that C-type and U-type inactivation have different molecular mechanisms. Kinetic modeling predicts that all mutants inactivate preferentially, but not exclusively, from partially activated closed states. Therefore, K_V2.1 exhibits a single U-type inactivation process including some inactivation from open as well as closed states.     

Speeding the Recovery from Ultraslow Inactivation of Voltage-Gated Na+ Channels by Metal Ion Binding to the Selectivity Filter: A Foot-on-the-Door?

Slow inactivated states in voltage-gated ion channels can be modulated by binding molecules both to the outside and to the inside of the pore. Thus, external K⁺ inhibits C-type inactivation in Shaker K⁺ channels by a “foot-in-the-door” mechanism. Here, we explore the modulation of a very long-lived inactivated state, ultraslow inactivation (I_US), by ligand binding to the outer vestibule in voltage-gated Na⁺ channels. Blocking the outer vestibule by a mutant μ-conotoxin GIIIA substantially accelerated recovery from I_US. A similar effect was observed if Cd²⁺ was bound to a cysteine engineered to the selectivity filter (K1237C). In K1237C channels, exposed to 30 μM Cd²⁺, the time constant of recovery from I_US was decreased from 145.0 ± 10.2 s to 32.5 ± 3.3 s (P < 0.001). Recovery from I_US was only accelerated if Cd²⁺ was added to the bath solution during recovery (V = −120 mV) from I_US, but not when the channels were selectively exposed to Cd²⁺ during the development of I_US (−20 mV). These data could be explained by a kinetic model in which Cd²⁺ binds with high affinity to a slow inactivated state (I_S), which is transiently occupied during recovery from I_US. A total of 50 μM Cd²⁺ produced an ∼8 mV hyperpolarizing shift of the steady-state inactivation curve of I_S, supporting this kinetic model. Binding of lidocaine to the internal vestibule significantly reduced the number of channels entering I_US, suggesting that I_US is associated with a conformational change of the internal vestibule of the channel. We propose a molecular model in which slow inactivation (I_S) occurs by a closure of the outer vestibule, whereas I_US arises from a constriction of the internal vestibule produced by a widening of the selectivity filter region. Binding of Cd²⁺ to C1237 promotes the closure of the selectivity filter region, thereby hastening recovery from I_US. Thus, Cd²⁺ ions may act like a foot-on-the-door, kicking the I_S gate to close.     

Models of the structure and gating mechanisms of the pore domain of the NaChBac ion channel

The NaChBac prokaryotic sodium channel appears to be a descendent of an evolutionary link between voltage-gated K_V and Ca_V channels. Like K_V channels, four identical six-transmembrane subunits comprise the NaChBac channel, but its selectivity filter possesses a signature sequence of eukaryotic Ca_V channels. We developed structural models of the NaChBac channel in closed and open conformations, using K⁺-channel crystal structures as initial templates. Our models were also consistent with numerous experimental results and modeling criteria. This study concerns the pore domain. The major differences between our models and K⁺ crystal structures involve the latter portion of the selectivity filter and the bend region in S6 of the open conformation. These NaChBac models may serve as a stepping stone between K⁺ channels of known structure and Na_V, Ca_V, and TRP channels of unknown structure.     

A conducting state with properties of a slow inactivated state in a shaker K(+) channel mutant

In Shaker K(+) channel, the amino terminus deletion Delta6-46 removes fast inactivation (N-type) unmasking a slow inactivation process. In Shaker Delta6-46 (Sh-IR) background, two additional mutations (T449V-I470C) remove slow inactivation, producing a noninactivating channel. However, despite the fact that Sh-IR-T449V-I470C mutant channels remain conductive, prolonged depolarizations (1 min, 0 mV) produce a shift of the QV curve by about -30 mV, suggesting that the channels still undergo the conformational changes typical of slow inactivation. For depolarizations longer than 50 ms, the tail currents measured during repolarization to -90 mV display a slow component that increases in amplitude as the duration of the depolarizing pulse increases. We found that the slow development of the QV shift had a counterpart in the amplitude of the slow component of the ionic tail current that is not present in Sh-IR. During long depolarizations, the time course of both the increase in the slow component of the tail current and the change in voltage dependence of the charge movement could be well fitted by exponential functions with identical time constant of 459 ms. Single channel recordings revealed that after prolonged depolarizations, the channels remain conductive for long periods after membrane repolarization. Nonstationary autocovariance analysis performed on macroscopic current in the T449V-I470C mutant confirmed that a novel open state appears with increasing prepulse depolarization time. These observations suggest that in the mutant studied, a new open state becomes progressively populated during long depolarizations (>50 ms). An appealing interpretation of these results is that the new open state of the mutant channel corresponds to a slow inactivated state of Sh-IR that became conductive.     

Dynamics, Energetics, and Selectivity of the Low-K KcsA Channel Structure

Potassium channels are a diverse family of integral membrane proteins through which K⁺ can pass selectively. There is ongoing debate about the nature of conformational changes associated with the opening/closing and conductive/nonconductive states of potassium channels. The channels partly exert their function by varying their conductance through a mechanism known as C-type inactivation. Shortly after the activation of K⁺ channels, their selectivity filter stops conducting ions at a rate that depends on various stimuli. The molecular mechanism of C-type inactivation has not been fully understood yet. However, the X-ray structure of the KcsA channel obtained in the presence of low K⁺ concentration is thought to be representative of a K⁺ channel in the C-type inactivated state. Here, extensive, fully atomistic molecular dynamics and free-energy simulations of the low-K⁺ KcsA structure in an explicit lipid bilayer are performed to evaluate the stability of this structure and the selectivity of its binding sites. We find that the low-K⁺ KcsA structure is stable on the timescale of the molecular dynamics simulations performed, and that ions preferably remain in S1 and S4. In the absence of ions, the selectivity filter evolves toward an asymmetric architecture, as already observed in other computations of the high-K⁺ structure of KcsA and KirBac. The low-K⁺ KcsA structure is not permeable by Na⁺, K⁺, or Rb⁺, and the selectivity of its binding sites is different from that of the high-K⁺ structure.     

Changes in apparent water permeability during the moulting cycle in the western rock lobster

The kinetics of water exchange, as measured by ³H₂O fluxes, were examined in the western rock lobster, Panulirus longipes (Milne Edwards) during stages C₄, D₃, D₄, D₄-E and B₁ of the moulting cycle. A series of samples of blood and external water was taken during each experiment and the inward and outward rate constants found using the SAAM 25 computer program, assuming a simple 2-compartment model with reversible exchange. Both inward and outward turnover rates remained constant up to the swelling prior to ecdysis when there was an increase of 203% inwards compared with 133% outwards. The latter increased in stage B₁, so that both rates were comparably high, probably due to the increased permeability of the soft integument.Further analysis showed that the rock lobster does not behave as a single compartment with respect to tritiated water. Two compartments were resolved by graphical analysis, one with fast and the other with slow exchange. It is suggested that blood and tissue ‘free’ water comprise one compartment and chemically ‘bound’ water the other, with fast exchange between the free and bound water and relatively slow exchange between free body water and the external medium.     

The external K+ concentration and mutations in the outer pore mouth affect the inhibition of kv1.5 current by Ni2+

By examining the consequences both of changes of [K⁺]_o and of point mutations in the outer pore mouth, our goal was to determine if the mechanism of the block of Kv1.5 ionic currents by external Ni²⁺ is similar to that for proton block. Ni²⁺ block is inhibited by increasing [K⁺]_o, by mutating a histidine residue in the pore turret (H463Q) or by mutating a residue near the pore mouth (R487V) that is the homolog of Shaker T449. Aside from a slight rightward shift of the Q-V curve, Ni²⁺ had no effect on gating currents. We propose that, as with H_o⁺, Ni²⁺ binding to H463 facilitates an outer pore inactivation process that is antagonized by K_o⁺ and that requires R487. However, whereas H_o⁺ substantially accelerates inactivation of residual currents, Ni²⁺ is much less potent, indicating incomplete overlap of the profiles of these two metal ions. Analyses with Co²⁺ and Mn²⁺, together with previous results, indicate that for the first-row transition metals the rank order for the inhibition of Kv1.5 in 0 mM K_o⁺ is Zn²⁺ (K_D ~ 0.07 mM) ≥ Ni²⁺ (K_D ~ 0.15 mM) > Co²⁺ (K_D ~ 1.4 mM) > Mn²⁺ (K_D > 10 mM).     

Extracellular acidification bySaccharomyces cerevisiae in normal and in heavy water

Titratable acidity of the extracellular medium was compared with that calculated from pH changes in a suspension ofSaccharomyces cerevisiae. After addition of cells to normal water the ratio of titratable acidity to the computed one was about 25, after addition of 50 mmol/Ld-glucose it was about 13, after subsequent addition of K⁺ ions it was only 2. In heavy water the respective values were 30, 9, and 1. Apparently, the principal buffer-generating processes have to do with glucose metabolism but little with the K⁺/H⁺ exchange observed after addition of K⁺. D₂O appears to block processes producing the buffering capacity of the medium, among them possibly extrusion of organic acids.