Nonselective Conduction in a Mutated NaK Channel with Three Cation-Binding Sites

The NaK channel is a cation-selective protein with similar permeability for K⁺ and Na⁺ ions. Crystallographic structures are available for the wild-type and mutated NaK channels with different numbers of cation-binding sites. We have performed a comparison between the potentials of mean force governing the translocation of K⁺ ions and mixtures of one Na⁺ and three K⁺ ions in a mutated NaK channel with only three cation-binding sites (NaK-CNG). Since NaK-CNG is not selective for K⁺ over Na⁺, analysis of its multi-ion potential energy surfaces can provide clues about how selectivity originates. Comparison of the potentials of mean force of NaK-CNG and K⁺-selective channels yields observations that strongly suggest that the number of contiguous ion binding sites in a single-file mechanism is the key determinant of the channel’s selectivity properties, as already proposed by experimental studies. We conclude that the presence of four binding sites in K⁺-selective channels is essential for highly selective and efficient permeation of K⁺ ions, and that a key difference between K⁺-selective and nonselective channels is the absence/presence of a binding site for Na⁺ ions at the boundary between S2 and S3 in the context of multi-ion permeation events.     

Ion Selectivity of the KcsA Channel: A Perspective from Multi-Ion Free Energy Landscapes

Potassium (K⁺) channels are specialized membrane proteins that are able to facilitate and regulate the conduction of K⁺ through cell membranes. Comprising five specific cation binding sites (S₀-S₄) formed by the backbone carbonyl groups of conserved residues common to all K⁺ channels, the narrow selectivity filter allows fast conduction of K⁺ while being highly selective for K⁺ over Na⁺. To extend our knowledge of the microscopic mechanism underlying selectivity in K⁺ channels, we characterize the free energy landscapes governing the entry and translocation of a Na⁺ or a K⁺ from the extracellular side into the selectivity filter of KcsA. The entry process of an extracellular ion is examined in the presence of two additional K⁺ in the pore, and the three-ion potential of mean force is computed using extensive all-atom umbrella sampling molecular dynamics simulations. A comparison of the potentials of mean force yields a number of important results. First, the free energy minima corresponding to configurations with extracellular K⁺ or Na⁺ in binding site S₀ or S₁ are similar in depth, suggesting that the thermodynamic selectivity governed by the free energy minima for those two binding sites is insignificant. Second, the free energy barriers between stable multi-ion configurations are generally higher for Na⁺ than for K⁺, implying that the kinetics of ion conduction is slower when a Na⁺ enters the pore. Third, the region corresponding to binding site S₂ near the center of the narrow pore emerges as the most selective for K⁺ over Na⁺. In particular, while there is a stable minimum for K⁺ in site S₂, Na⁺ faces a steep free energy increase with no local free energy well in this region. Lastly, analysis shows that selectivity is not correlated with the overall coordination number of the ion entering the pore, but is predominantly affected by changes in the type of coordinating ligands (carbonyls versus water molecules). These results further highlight the importance of the central region near binding site S₂ in the selectivity filter of K⁺ channels.     

Control of ion selectivity in LeuT: two Na+ binding sites with two different mechanisms

The x-ray structure of LeuT, a bacterial homologue of Na⁺/Cl⁻-dependent neurotransmitter transporters, provides a great opportunity to better understand the molecular basis of monovalent cation selectivity in ion-coupled transporters. LeuT possesses two ion binding sites, NA1 and NA2, which are highly selective for Na⁺. Extensive all-atom free-energy molecular dynamics simulations of LeuT embedded in an explicit membrane are performed at different temperatures and various occupancy states of the binding sites to dissect the molecular mechanism of ion selectivity. The results show that the two binding sites display robust selectivity for Na⁺ over K⁺ or Li⁺, the competing ions of most similar radii. Of particular interest, the mechanism primarily responsible for selectivity for each of the two binding sites appears to be different. In NA1, selectivity for Na⁺ over K⁺ arises predominantly from the strong electrostatic field arising from the negatively charged carboxylate group of the leucine substrate coordinating the ion directly. In NA2, which comprises only neutral ligands, selectivity for Na⁺ is enforced by the local structural restraints arising from the hydrogen-bonding network and the covalent connectivity of the polypeptide chain surrounding the ion according to a “snug-fit” mechanism.     

K/Na Selectivity in Toy Cation Binding Site Models Is Determined by the ‘Host’

The macroscopic ion-selective behavior of K⁺ channels is mediated by a multitude of physiological factors. However, considering the carbonyl-lined binding site of a conductive K⁺ channel as a canonical eightfold coordinated construct can be useful in understanding the principles that correlate the channel's structure with its function. We probe the effects of structure and chemical composition on the K⁺/Na⁺ selectivity provided by a variety of simplified droplet-like ion binding site models. We find that when carbonyl- and water-based models capture the qualitative structural features of the K⁺ channel binding site, a selective preference for K⁺ emerges. Thus our findings suggest that the preference for K⁺ over Na⁺ exhibited by such models is principally built-in, and is not due to a unique K⁺-selective property of carbonyl functional groups. This suggestion is confirmed by a general thermodynamic assessment, which provides a basis for using simplified models to study the design principles underlying the molecular evolution of K⁺ channels.     

Ion behavior in the selectivity filter of HCN1 channels

Hyperpolarization-activated cyclic-nucleotide gated channels (HCNs) are responsible for the generation of pacemaker currents (I_f or I_h) in cardiac and neuronal cells. Despite the overall structural similarity to voltage-gated potassium (Kv) channels, HCNs show much lower selectivity for K⁺ over Na⁺ ions. This increased permeability to Na⁺ is critical to their role in membrane depolarization. HCNs can also select between Na⁺ and Li⁺ ions. Here, we investigate the unique ion selectivity properties of HCNs using molecular-dynamics simulations. Our simulations suggest that the HCN1 pore is flexible and dilated compared with Kv channels with only one stable ion binding site within the selectivity filter. We also observe that ion coordination and hydration differ within the HCN1 selectivity filter compared with those in Kv and cyclic-nucleotide gated channels. Additionally, the C358T mutation further stabilizes the symmetry of the binding site and provides a more fit space for ion coordination, particularly for Li⁺.     

Sodium Ions Do Not Stabilize the Selectivity Filter of a Potassium Channel

Ion conduction is an essential function for electrical activity in all organisms. The non-selective ion channel NaK was previously shown to adopt two stable conformations of the selectivity filter. Here, we present solid-state NMR measurements of NaK demonstrating a population shift between these conformations induced by changing the ions in the sample while the overall structure of NaK is not affected. We show that two K⁺-selective mutants (NaK2K and NaK2K-Y66F) suffer a complete loss of selectivity filter stability under Na⁺ conditions, but do not collapse into a defined structure. Widespread chemical shift perturbations are seen between the Na⁺ and K⁺ states of the K⁺-selective mutants in the region of the pore helix indicating structural changes. We conclude that the stronger link between the selectivity filter and the pore helix in the K⁺-selective mutants, compared to the non-selective wild-type NaK channel, reduces the ion-dependent conformational flexibility of the selectivity filter.     

Free energy simulations of ligand binding to the aspartate transporter Glt(Ph)

Glutamate/Aspartate transporters cotransport three Na⁺ and one H⁺ ions with the substrate and countertransport one K⁺ ion. The binding sites for the substrate and two Na⁺ ions have been observed in the crystal structure of the archeal homolog Glt_Ph, while the binding site for the third Na⁺ ion has been proposed from computational studies and confirmed by experiments. Here we perform detailed free energy simulations of Glt_Ph, giving a comprehensive characterization of the substrate and ion binding sites, and calculating their binding free energies in various configurations. Our results show unequivocally that the substrate binds after the binding of two Na⁺ ions. They also shed light into Asp/Glu selectivity of Glt_Ph, which is not observed in eukaryotic glutamate transporters.     

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.     

The Interaction of Na+ and K+ in Voltage-gated Potassium Channels : Evidence for Cation Binding Sites of Different Affinity

Voltage-gated potassium (K⁺) channels are multi-ion pores. Recent studies suggest that, similar to calcium channels, competition between ionic species for intrapore binding sites may contribute to ionic selectivity in at least some K⁺ channels. Molecular studies suggest that a putative constricted region of the pore, which is presumably the site of selectivity, may be as short as one ionic diameter in length. Taken together, these results suggest that selectivity may occur at just a single binding site in the pore. We are studying a chimeric K⁺ channel that is highly selective for K⁺ over Na⁺ in physiological solutions, but conducts Na⁺ in the absence of K⁺. Na⁺ and K⁺ currents both display slow (C-type) inactivation, but had markedly different inactivation and deactivation kinetics; Na⁺ currents inactivated more rapidly and deactivated more slowly than K⁺ currents. Currents carried by 160 mM Na⁺ were inhibited by external K⁺ with an apparent IC₅₀ <30 μM. K⁺ also altered both inactivation and deactivation kinetics of Na⁺ currents at these low concentrations. In the complementary experiment, currents carried by 3 mM K⁺ were inhibited by external Na⁺, with an apparent IC₅₀ of ∼100 mM. In contrast to the effects of low [K⁺] on Na⁺ current kinetics, Na⁺ did not affect K⁺ current kinetics, even at concentrations that inhibited K⁺ currents by 40–50%. These data suggest that Na⁺ block of K⁺ currents did not involve displacement of K⁺ from the high affinity site involved in gating kinetics. We present a model that describes the permeation pathway as a single high affinity, cation-selective binding site, flanked by low affinity, nonselective sites. This model quantitatively predicts the anomalous mole fraction behavior observed in two different K⁺ channels, differential K⁺ and Na⁺ conductance, and the concentration dependence of K⁺ block of Na⁺ currents and Na⁺ block of K⁺ currents. Based on our results, we hypothesize that the permeation pathway contains a single high affinity binding site, where selectivity and ionic modulation of gating occur.     

Determinants of cation transport selectivity: Equilibrium binding and transport kinetics

ConclusionThe equilibrium ion-binding properties of ion channels and transporters can be difficult to discern from crystal structures alone, as proteins often adopt different lowest energy states depending on the ions bound. In cases where transport is slow, their inherent ion-binding preferences can be used to infer their transport preferences. However, in cases where transport is fast, the transport selectivity can hide their equilibrium preferences by accentuating the kinetics of ions hopping through a channel over its inherent ion-binding preferences. Thus, depending on the arrangement of ion-binding sites in a channel’s selectivity filter, one can achieve either selective or nonselective ion transport.The equilibrium K⁺ selectivity of some nonselective channels suggests a potential mechanism whereby they could evolve into a fast K⁺-selective channel. K⁺ channels and nonselective channels like CNG and HCN are related to one another in both sequence and structure, suggesting an evolutionary link between them. Swap experiments show that only a few mutations separate a nonselective channel from a K⁺-selective channel. One might imagine an evolutionary path between these channels in which the equilibrium preference for a K⁺ ion in a nonselective channel evolves into a K⁺-selective channel through these few mutations to create the selective ion queue. Alternatively, a slow single-ion channel with an equilibrium and transport preference for K⁺ ions could be transformed into a fast multi-ion channel through mutations that create a queue of K⁺-selective ion-binding sites, as is seen in most K⁺ channels studied to date.In the case of multi-ion selectivity filters, such as those found in K⁺ channels, the selectivity filter can be viewed as the active site that interacts with different queues of ions and water molecules. At least three properties emerge from multi-ion queues: (1) high conductance by reducing the affinity of multiple bound ions versus single ions; (2) high selectivity by allowing disfavored ions time to dissociate back into solution; and, consequently, (3) robust selectivity in an environment where ion concentrations can change. For transporters and carriers, the equilibrium preference and slow transport naturally create robust selectivity. In all these cases, equilibrium-based ion selectivity is achieved by slowing transport enough so that the disfavored ion is able to dissociate back into solution before transport takes place.     

Preferential binding of K+ ions in the selectivity filter at equilibrium explains high selectivity of K+ channels

K⁺ channels exhibit strong selectivity for K⁺ ions over Na⁺ ions based on electrophysiology experiments that measure ions competing for passage through the channel. During this conduction process, multiple ions interact within the region of the channel called the selectivity filter. Ion selectivity may arise from an equilibrium preference for K⁺ ions within the selectivity filter or from a kinetic mechanism whereby Na⁺ ions are precluded from entering the selectivity filter. Here, we measure the equilibrium affinity and selectivity of K⁺ and Na⁺ ions binding to two different K⁺ channels, KcsA and MthK, using isothermal titration calorimetry. Both channels exhibit a large preference for K⁺ over Na⁺ ions at equilibrium, in line with electrophysiology recordings of reversal potentials and Ba²⁺ block experiments used to measure the selectivity of the external-most ion-binding sites. These results suggest that the high selectivity observed during ion conduction can originate from a strong equilibrium preference for K⁺ ions in the selectivity filter, and that K⁺ selectivity is an intrinsic property of the filter. We hypothesize that the equilibrium preference for K⁺ ions originates in part through the optimal spacing between sites to accommodate multiple K⁺ ions within the selectivity filter.     

Mechanism of the Na,K-ATPase Inhibition by MCS Derivatives

The previously reported class of potent inorganic inhibitors of Na,K-ATPase, named MCS factors, was shown to inhibit not only Na,K-ATPase but several P-type ATPases with high potency in the sub-micromolar range. These MCS factors were found to bind to the intracellular side of the Na, K-ATPase. The inhibition is not competitive with ouabain binding, thus excluding its role as cardiac-steroid-like inhibitor of the Na,K-ATPase. The mechanism of inhibition of Na,K-ATPase was investigated with the fluorescent styryl dye RH421, a dye known to report changes of local electric fields in the membrane dielectric. MCS factors interact with the Na,K-ATPase in the E₁ conformation of the ion pump and induce a conformational rearrangement that causes a change of the equilibrium dissociation constant for one of the first two intracellular cation binding sites. The MCS-inhibited state was found to have bound one cation (H⁺, Na⁺ or K⁺) in one of the two unspecific binding sites, and at high Na⁺ concentrations another Na⁺ ion was bound to the highly Na⁺-selective ion-binding site.     

K+-Dependent Selectivity and External Ca2+ Block of Shab K+ Channels

Potassium channels allow the selective flux of K⁺ excluding the smaller, and more abundant in the extracellular solution, Na⁺ ions. Here we show that Shab is a typical K⁺ channel that excludes Na⁺ under bi-ionic, Na_o/K_i or Na_o/Rb_i, conditions. However, when internal K⁺ is replaced by Cs⁺ (Na_o/Cs_i), stable inward Na⁺ and outward Cs⁺ currents are observed. These currents show that Shab selectivity is not accounted for by protein structural elements alone, as implicit in the snug-fit model of selectivity. Additionally, here we report the block of Shab channels by external Ca²⁺ ions, and compare the effect that internal K⁺ replacement exerts on both Ca²⁺ and TEA block. Our observations indicate that Ca²⁺ blocks the channels at a site located near the external TEA binding site, and that this pore region changes conformation under conditions that allow Na⁺ permeation. In contrast, the latter ion conditions do not significantly affect the binding of quinidine to the pore central cavity. Based on our observations and the structural information derived from the NaK bacterial channel, we hypothesize that Ca²⁺ is probably coordinated by main chain carbonyls of the pore´s first K⁺-binding site.     

Molecular Dynamics Simulations Elucidate the Mechanism of Proton Transport in the Glutamate Transporter EAAT3

The uptake of glutamate in nerve synapses is carried out by the excitatory amino acid transporters (EAATs), involving the cotransport of a proton and three Na⁺ ions and the countertransport of a K⁺ ion. In this study, we use an EAAT3 homology model to calculate the pK_a of several titratable residues around the glutamate binding site to locate the proton carrier site involved in the translocation of the substrate. After identifying E374 as the main candidate for carrying the proton, we calculate the protonation state of this residue in different conformations of EAAT3 and with different ligands bound. We find that E374 is protonated in the fully bound state, but removing the Na2 ion and the substrate reduces the pK_a of this residue and favors the release of the proton to solution. Removing the remaining Na⁺ ions again favors the protonation of E374 in both the outward- and inward-facing states, hence the proton is not released in the empty transporter. By calculating the pK_a of E374 with a K⁺ ion bound in three possible sites, we show that binding of the K⁺ ion is necessary for the release of the proton in the inward-facing state. This suggests a mechanism in which a K⁺ ion replaces one of the ligands bound to the transporter, which may explain the faster transport rates of the EAATs compared to its archaeal homologs.     

Molecular Dynamics Simulations Elucidate the Mechanism of Proton Transport in the Glutamate Transporter EAAT3

The uptake of glutamate in nerve synapses is carried out by the excitatory amino acid transporters (EAATs), involving the cotransport of a proton and three Na⁺ ions and the countertransport of a K⁺ ion. In this study, we use an EAAT3 homology model to calculate the pK_a of several titratable residues around the glutamate binding site to locate the proton carrier site involved in the translocation of the substrate. After identifying E374 as the main candidate for carrying the proton, we calculate the protonation state of this residue in different conformations of EAAT3 and with different ligands bound. We find that E374 is protonated in the fully bound state, but removing the Na2 ion and the substrate reduces the pK_a of this residue and favors the release of the proton to solution. Removing the remaining Na⁺ ions again favors the protonation of E374 in both the outward- and inward-facing states, hence the proton is not released in the empty transporter. By calculating the pK_a of E374 with a K⁺ ion bound in three possible sites, we show that binding of the K⁺ ion is necessary for the release of the proton in the inward-facing state. This suggests a mechanism in which a K⁺ ion replaces one of the ligands bound to the transporter, which may explain the faster transport rates of the EAATs compared to its archaeal homologs.     

Route,mechanism, and implications of proton import during Na+/K+ exchange by native Na+/K+-ATPase pumps

A single Na⁺/K⁺-ATPase pumps three Na⁺ outwards and two K⁺ inwards by alternately exposing ion-binding sites to opposite sides of the membrane in a conformational sequence coupled to pump autophosphorylation from ATP and auto-dephosphorylation. The larger flow of Na⁺ than K⁺ generates outward current across the cell membrane. Less well understood is the ability of Na⁺/K⁺ pumps to generate an inward current of protons. Originally noted in pumps deprived of external K⁺ and Na⁺ ions, as inward current at negative membrane potentials that becomes amplified when external pH is lowered, this proton current is generally viewed as an artifact of those unnatural conditions. We demonstrate here that this inward current also flows at physiological K⁺ and Na⁺ concentrations. We show that protons exploit ready reversibility of conformational changes associated with extracellular Na⁺ release from phosphorylated Na⁺/K⁺ pumps. Reversal of a subset of these transitions allows an extracellular proton to bind an acidic side chain and to be subsequently released to the cytoplasm. This back-step of phosphorylated Na⁺/K⁺ pumps that enables proton import is not required for completion of the 3 Na⁺/2 K⁺ transport cycle. However, the back-step occurs readily during Na⁺/K⁺ transport when external K⁺ ion binding and occlusion are delayed, and it occurs more frequently when lowered extracellular pH raises the probability of protonation of the externally accessible carboxylate side chain. The proton route passes through the Na⁺-selective binding site III and is distinct from the principal pathway traversed by the majority of transported Na⁺ and K⁺ ions that passes through binding site II. The inferred occurrence of Na⁺/K⁺ exchange and H⁺ import during the same conformational cycle of a single molecule identifies the Na⁺/K⁺ pump as a hybrid transporter. Whether Na⁺/K⁺ pump–mediated proton inflow may have any physiological or pathophysiological significance remains to be clarified.     

Hydration valve controlled non-selective conduction of Na and K in the NaK channel

The Na⁺ and K⁺ channels are essential to neural signaling, but our current knowledge at the atomic level is mainly limited to the conducting mechanism of K⁺. Unlike a K⁺ channel having four equivalent K⁺-binding sites in its selectivity filter, a NaK channel has a vestibule in the middle part of its selectivity filter, and can conduct both Na⁺ and K⁺ ions. However, the underlying mechanism for non-selective ion conduction in NaK remains elusive. Here we find four small grottos connecting with the vestibule of the NaK selectivity filter, which form a vestibule-grotto complex perpendicular to the filter pore with a few water molecules within it. It is shown that two or more of the water molecules coming to the vestibule to coordinate the cation are necessary for conducting both Na⁺ and K⁺ ions, while only one water molecule in the vestibule will obstruct ion permeation. Thus, the complex with the aid of interior water movement forms a dynamic hydration valve which is flexible in conveying different cations through the vestibule. Similar exquisite hydration valve mechanisms are expected to be utilized by other non-selective cation channels, and the results should shed new light on the importance of water in neural signaling.     

Molecular mechanism of ion-ion and ion-substrate coupling in the Na+-dependent leucine transporter LeuT

Ion-coupled transport of neurotransmitter molecules by neurotransmitter:sodium symporters (NSS) play an important role in the regulation of neuronal signaling. One of the major events in the transport cycle is ion-substrate coupling and formation of the high-affinity occluded state with bound ions and substrate. Molecular mechanisms of ion-substrate coupling and the corresponding ion-substrate stoichiometry in NSS transporters has yet to be understood. The recent determination of a high-resolution structure for a bacterial homolog of Na⁺/Cl⁻-dependent neurotransmitter transporters, LeuT, offers a unique opportunity to analyze the functional roles of the multi-ion binding sites within the binding pocket. The binding pocket of LeuT contains two metal binding sites. The first ion in site NA1 is directly coupled to the bound substrate (Leu) with the second ion in the neighboring site (NA2) only ∼7 Å away. Extensive, fully atomistic, molecular dynamics, and free energy simulations of LeuT in an explicit lipid bilayer are performed to evaluate substrate-binding affinity as a function of the ion load (single versus double occupancy) and occupancy by specific monovalent cations. It was shown that double ion occupancy of the binding pocket is required to ensure substrate coupling to Na⁺ and not to Li⁺ or K⁺ cations. Furthermore, it was found that presence of the ion in site NA2 is required for structural stability of the binding pocket as well as amplified selectivity for Na⁺ in the case of double ion occupancy.     

Rescue of Na+ Affinity in Aspartate 928 Mutants of Na+,K+-ATPase by Secondary Mutation of Glutamate 314

The Na⁺,K⁺-ATPase binds Na⁺ at three transport sites denoted I, II, and III, of which site III is Na⁺-specific and suggested to be the first occupied in the cooperative binding process activating phosphorylation from ATP. Here we demonstrate that the asparagine substitution of the aspartate associated with site III found in patients with rapid-onset dystonia parkinsonism or alternating hemiplegia of childhood causes a dramatic reduction of Na⁺ affinity in the α1-, α2-, and α3-isoforms of Na⁺,K⁺-ATPase, whereas other substitutions of this aspartate are much less disruptive. This is likely due to interference by the amide function of the asparagine side chain with Na⁺-coordinating residues in site III. Remarkably, the Na⁺ affinity of site III aspartate to asparagine and alanine mutants is rescued by second-site mutation of a glutamate in the extracellular part of the fourth transmembrane helix, distant to site III. This gain-of-function mutation works without recovery of the lost cooperativity and selectivity of Na⁺ binding and does not affect the E₁-E₂ conformational equilibrium or the maximum phosphorylation rate. Hence, the rescue of Na⁺ affinity is likely intrinsic to the Na⁺ binding pocket, and the underlying mechanism could be a tightening of Na⁺ binding at Na⁺ site II, possibly via movement of transmembrane helix four. The second-site mutation also improves Na⁺,K⁺ pump function in intact cells. Rescue of Na⁺ affinity and Na⁺ and K⁺ transport by second-site mutation is unique in the history of Na⁺,K⁺-ATPase and points to new possibilities for treatment of neurological patients carrying Na⁺,K⁺-ATPase mutations.     

Ion binding properties and structure stability of the NaK channel

Ion distribution in the selectivity filter and ion-water and ion-protein interactions of NaK channel are systematically investigated by all-atom molecular dynamics simulations, with the tetramer channel protein being embedded in a solvated phospholipid bilayer. Analysis of the simulation results indicates that K⁺ ions prefer to bind within the sites formed by two adjacent planes of oxygen atoms from the selectivity filter, while Na⁺ ions are inclined to bind to a single plane of four oxygen atoms. At the same time, both K⁺ and Na⁺ ions can diffuse in the vestibule, accompanying with movements of the water molecules confined in a complex formed by the vestibule together with four small grottos connecting to it. As a result, K⁺ ions show a wide range of coordination numbers (6-8), while Na⁺ ions display a constant coordination number of ∼ 6 in the selectivity filter, which may result in the loss of selectivity of NaK. It is also found that a Ca²⁺ can bind at the extracellular site as reported in the crystal structure in a partially hydrated state, or at a higher site in a full hydration state. Furthermore, the carbonyl group of Asp66 can reorient to point towards the center pore when an ion exists in the vestibule, while that of Gly65 always aligns tangentially to the channel axis, as in the crystallographic structures.