Nonglutamate pore residues in ion selection and conduction in voltage-gated Ca2+ channels

Pore mutation N617D in the skeletal muscle DHPR blocks Ca2+ influx due to atypical high-affinity Ca2+ binding

Skeletal muscle excitation-contraction (EC) coupling roots in Ca²⁺-influx-independent inter-channel signaling between the sarcolemmal dihydropyridine receptor (DHPR) and the ryanodine receptor (RyR1) in the sarcoplasmic reticulum. Although DHPR Ca²⁺ influx is irrelevant for EC coupling, its putative role in other muscle-physiological and developmental pathways was recently examined using two distinct genetically engineered mouse models carrying Ca²⁺ non-conducting DHPRs: DHPR(N617D) (Dayal et al., 2017) and DHPR(E1014K) (Lee et al., 2015). Surprisingly, despite complete block of DHPR Ca²⁺-conductance, histological, biochemical, and physiological results obtained from these two models were contradictory. Here, we characterize the permeability and selectivity properties and henceforth the mechanism of Ca²⁺ non-conductance of DHPR(N617). Our results reveal that only mutant DHPR(N617D) with atypical high-affinity Ca²⁺ pore-binding is tight for physiologically relevant monovalent cations like Na⁺ and K⁺. Consequently, we propose a molecular model of cooperativity between two ion selectivity rings formed by negatively charged residues in the DHPR pore region.

Divalent cations permeation in a Ca2+ non-conducting skeletal muscle dihydropyridine receptor mouse model

In response to excitation of skeletal muscle fibers, trains of action potentials induce changes in the configuration of the dihydropyridine receptor (DHPR) anchored in the tubular membrane which opens the Ca²⁺ release channel in the sarcoplasmic reticulum membrane. The DHPR also functions as a voltage-gated Ca²⁺ channel that conducts L-type Ca²⁺ currents routinely recorded in mammalian muscle fibers, which role was debated for more than four decades. Recently, to allow a closer look into the role of DHPR Ca²⁺ influx in mammalian muscle, a knock-in (ki) mouse model (ncDHPR) carrying mutation N617D (adjacent to domain II selectivity filter E) in the DHPRα_1S subunit abolishing Ca²⁺ permeation through the channel was generated [Dayal et al., 2017]. In the present study, the Mn²⁺ quenching technique was initially intended to be used on voltage-clamped muscle fibers from this mouse to determine whether Ca²⁺ influx through a pathway distinct from DHPR may occur to compensate for the absence of DHPR Ca²⁺ influx. Surprisingly, while N617D DHPR muscle fibers of the ki mouse do not conduct Ca²⁺, Mn²⁺ entry and subsequent quenching did occur because Mn²⁺ was able to permeate and produce L-type currents through N617D DHPR. N617D DHPR was also found to conduct Ba²⁺ and Ba²⁺ currents were strongly blocked by external Ca²⁺. Ba²⁺ permeation was smaller, current kinetics slower and Ca²⁺ block more potent than in wild-type DHPR. These results indicate that residue N617 when replaced by the negatively charged residue D is suitably located at entrance of the pore to trap external Ca²⁺ impeding in this way permeation. Because Ba²⁺ binds with lower affinity to D, Ba²⁺ currents occur, but with reduced amplitudes as compared to Ba²⁺ currents through wild-type channels. We conclude that mutations located outside the selectivity filter influence channel permeation and possibly channel gating in a fully differentiated skeletal muscle environment.

Voltage-gated calcium channels: Determinants of channel function and modulation by inorganic cations

Voltage-gated calcium channels (VGCCs) represent a key link between electrical signals and non-electrical processes, such as contraction, secretion and transcription. Evolved to achieve high rates of Ca(2+)-selective flux, they possess an elaborate mechanism for selection of Ca(2+) over foreign ions. It has been convincingly linked to competitive binding in the pore, but the fundamental question of how this is reconcilable with high rates of Ca(2+) transfer remains unanswered. By virtue of their similarity to Ca(2+), polyvalent cations can interfere with the function of VGCCs and have proven instrumental in probing the mechanisms underlying selective permeation. Recent emergence of crystallographic data on a set of Ca(2+)-selective model channels provides a structural framework for permeation in VGCCs, and warrants a reconsideration of their diverse modulation by polyvalent cations, which can be roughly separated into three general mechanisms: (I) long-range interactions with charged regions on the surface, affecting the local potential sensed by the channel or influencing voltage-sensor movement by repulsive forces (electrostatic effects), (II) short-range interactions with sites in the ion-conducting pathway, leading to physical obstruction of the channel (pore block), and in some cases (III) short-range interactions with extracellular binding sites, leading to non-electrostatic modifications of channel gating (allosteric effects). These effects, together with the underlying molecular modifications, provide valuable insights into the function of VGCCs, and have important physiological and pathophysiological implications. Allosteric suppression of some of the pore-forming Cavα1-subunits (Cav2.3, Cav3.2) by Zn(2+) and Cu(2+) may play a major role for the regulation of excitability by endogenous transition metal ions. The fact that these ions can often traverse VGCCs can contribute to the detrimental intracellular accumulation of metal ions following excessive release of endogenous Cu(2+) and Zn(2+) or exposure to non-physiological toxic metal ions.

Structural basis for Ca2+ selectivity of a voltage-gated calcium channel

Voltage-gated calcium (Ca_V) channels catalyze rapid, highly selective influx of Ca²⁺ into cells despite 70-fold higher extracellular concentration of Na⁺. How Ca_V channels solve this fundamental biophysical problem remains unclear. Here we report physiological and crystallographic analyses of a calcium selectivity filter constructed in the homotetrameric bacterial Na_V channel Na_VAb. Our results reveal interactions of hydrated Ca²⁺ with two high-affinity Ca²⁺-binding sites followed by a third lower-affinity site that would coordinate Ca²⁺ as it moves inward. At the selectivity filter entry, Site 1 is formed by four carboxyl side-chains, which play a critical role in determining Ca²⁺ selectivity. Four carboxyls plus four backbone carbonyls form Site 2, which is targeted by the blocking cations, Cd²⁺ and Mn²⁺, with single occupancy. The lower-affinity Site 3 is formed by four backbone carbonyls alone, which mediate exit into the central cavity. This pore architecture suggests a conduction pathway involving transitions between two main states with one or two hydrated Ca²⁺ ions bound in the selectivity filter and supports a “knock-off” mechanism of ion permeation through a stepwise-binding process. The multi-ion selectivity filter of our Ca_VAb model establishes a structural framework for understanding mechanisms of ion selectivity and conductance by vertebrate Ca_V channels.

Sodium leak channels in neuronal excitability and rhythmic behaviors

Extracellular K⁺, Na⁺, and Ca²⁺ ions all influence the resting membrane potential of the neuron. However, the mechanisms by which extracellular Na⁺ and Ca²⁺ regulate basal neuronal excitability are not well understood. Recent findings suggest that NALCN, in association with UNC79 and UNC80, contributes a basal Na⁺ leak conductance in neurons. Mutations in Nalcn, Unc79, or Unc80 lead to severe phenotypes that include neonatal lethality and disruption in rhythmic behaviors. This review discusses the properties of the NALCN complex, its regulation, and its contribution to neuronal function and animal behavior.

A single amino acid change in Ca(v)1.2 channels eliminates the permeation and gating differences between Ca(2+) and Ba(2+)

Glutamate scanning mutagenesis was used to assess the role of the calcicludine binding segment in regulating channel permeation and gating using both Ca(2+) and Ba(2+) as charge carriers. As expected, wild-type Ca(V)1.2 channels had a Ba(2+) conductance ~2x that in Ca(2+) (G(Ba)/G(Ca) = 2) and activation was ~10 mV more positive in Ca(2+) vs. Ba(2+). Of the 11 mutants tested, F1126E was the only one that showed unique permeation and gating properties compared to the wild type. F1126E equalized the Ca(V)1.2 channel conductance (G(Ba)/G(Ca) = 1) and activation voltage dependence between Ca(2+) and Ba(2+). Ba(2+) permeation was reduced because the interactions among multiple Ba(2+) ions and the pore were specifically altered for F1126E, which resulted in Ca(2+)-like ionic conductance and unitary current. However, the high-affinity block of monovalent cation flux was not altered for either Ca(2+) or Ba(2+). The half-activation voltage of F1126E in Ba(2+) was depolarized to match that in Ca(2+), which was unchanged from that in the wild type. As a result, the voltages for half-activation and half-inactivation of F1126E in Ba(2+) and Ca(2+) were similar to those of wild-type in Ca(2+). This effect was specific to F1126E since F1126A did not affect the half-activation voltage in either Ca(2+) or Ba(2+). These results indicate that residues in the outer vestibule of the Ca(V)1.2 channel pore are major determinants of channel gating, selectivity, and permeation.

Molecular determinant for specific Ca/Ba selectivity profiles of low and high threshold Ca2+ channels

Voltage-gated Ca²⁺ channels (VGCC) play a key role in many physiological functions by their high selectivity for Ca²⁺ over other divalent and monovalent cations in physiological situations. Divalent/monovalent selection is shared by all VGCC and is satisfactorily explained by the existence, within the pore, of a set of four conserved glutamate/aspartate residues (EEEE locus) coordinating Ca²⁺ ions. This locus however does not explain either the choice of Ca²⁺ among other divalent cations or the specific conductances encountered in the different VGCC. Our systematic analysis of high- and low-threshold VGCC currents in the presence of Ca²⁺ and Ba²⁺ reveals highly specific selectivity profiles. Sequence analysis, molecular modeling, and mutational studies identify a set of nonconserved charged residues responsible for these profiles. In HVA (high voltage activated) channels, mutations of this set modify divalent cation selectivity and channel conductance without change in divalent/monovalent selection, activation, inactivation, and kinetics properties. The Ca_V2.1 selectivity profile is transferred to Ca_V2.3 when exchanging their residues at this location. Numerical simulations suggest modification in an external Ca²⁺ binding site in the channel pore directly involved in the choice of Ca²⁺, among other divalent physiological cations, as the main permeant cation for VGCC. In LVA (low voltage activated) channels, this locus (called DCS for divalent cation selectivity) also influences divalent cation selection, but our results suggest the existence of additional determinants to fully recapitulate all the differences encountered among LVA channels. These data therefore attribute to the DCS a unique role in the specific shaping of the Ca²⁺ influx between the different HVA channels.

Block of CaV1.2 channels by Gd3+ reveals preopening transitions in the selectivity filter

Using the lanthanide gadolinium (Gd³⁺) as a Ca²⁺ replacing probe, we investigated the voltage dependence of pore blockage of Ca_V1.2 channels. Gd⁺³ reduces peak currents (tonic block) and accelerates decay of ionic current during depolarization (use-dependent block). Because diffusion of Gd³⁺ at concentrations used (<1 μM) is much slower than activation of the channel, the tonic effect is likely to be due to the blockage that occurred in closed channels before depolarization. We found that the dose–response curves for the two blocking effects of Gd³⁺ shifted in parallel for Ba²⁺, Sr²⁺, and Ca²⁺ currents through the wild-type channel, and for Ca²⁺ currents through the selectivity filter mutation EEQE that lowers the blocking potency of Gd³⁺. The correlation indicates that Gd³⁺ binding to the same site causes both tonic and use-dependent blocking effects. The apparent on-rate for the tonic block increases with the prepulse voltage in the range −60 to −45 mV, where significant gating current but no ionic current occurs. When plotted together against voltage, the on-rates of tonic block (−100 to −45 mV) and of use-dependent block (−40 to 40 mV) fall on a single sigmoid that parallels the voltage dependence of the gating charge. The on-rate of tonic block by Gd³⁺ decreases with concentration of Ba²⁺, indicating that the apparent affinity of the site to permeant ions is about 1 mM in closed channels. Therefore, we propose that at submicromolar concentrations, Gd³⁺ binds at the entry to the selectivity locus and that the affinity of the site for permeant ions decreases during preopening transitions of the channel.

Calcicludine binding to the outer pore of L-type calcium channels is allosterically coupled to dihydropyridine binding

How dihydropyridines modulate L-type voltage-gated Ca2+ channels is not known. Dihydropyridines bind cooperatively with Ca2+ binding to the selectivity filter, suggesting that they alter channel activity by promoting structural rearrangements in the pore. We used radioligand binding and patch-clamp electrophysiology to demonstrate that calcicludine, a toxin from the venom of the green mamba snake, binds in the outer vestibule of the pore and, like Ca2+, is a positive modulator of dihydropyridine binding. Data were fit using an allosteric scheme where dissociation constants for dihydropyridine and calcicludine binding, KDHP and KCaC, are linked via the coupling factor, alpha. Nine acidic amino acids located within the S5-Pore-helix segment of repeat III were sequentially changed to alanine in groups of three, resulting in the mutant channels, Mut-A, Mut-B, and Mut-C. Mut-A, whose substitutions are proximal to IIIS5, exhibits a 4.5-fold reduction in dihydropyridine binding and is insensitive to calcicludine binding. Block of Mut-A currents by calcicludine is indistinguishable from wild-type, indicating that KCaC is unchanged and that the coupling between dihydropyridine and calcicludine binding (i.e., alpha) is disrupted. Mut-B and Mut-C possess KDHP values that resemble that of the wild type. Mut-C, the most C-terminal of the mutant channels, is insensitive to calcicludine binding and block. KCaC values for the Mut-C single mutants, E1122A, D1127A, and D1129A, increase from 0.3 (wild type) to 1.14, 2.00, and 20.5 microM, respectively. Together, these findings suggest that dihydropyridine antagonist and calcicludine binding to L-type Ca2+ channels promote similar structural changes in the pore that stabilize the channel in a nonconducting, blocked state.

Amino acid substitutions in the pore of the Ca(V)1.2 calcium channel reduce barium currents without affecting calcium currents

Ba(2+) currents through Ca(V)1.2 Ca(2+) channels are typically twice as large as Ca(2+) currents. Replacing Phe-1144 in the pore-loop of domain III with glycine and lysine, and Tyr-1152 with lysine, reduces whole-cell G(Ba)/G(Ca) from 2.2 (wild-type) to 0.95, 1.21, and 0.90, respectively. Whole-cell and single-channel measurements indicate that reductions in G(Ba)/G(Ca) result specifically from a decrease in Ba(2+) conductance and not changes in V(h) or P(O). Half-maximal block of I(Li) is increased by 3.2-, 3.8-, and 1.6-fold in Ca(2+), and 3.8-, 4.2-, and 1.8-fold in Ba(2+) for F1144G, Y1152K, and F1144K, respectively. High affinity interactions of individual divalent cations to the pore are not important for determining G(Ba)/G(Ca), because the fold increases in IC(50) values for Ba(2+) and Ca(2+) are similar. On the contrary, conductance-concentration curves indicate that G(Ba)/G(Ca) is reduced because the interactions of multiple Ba(2+) ions in the mutant pores are altered. The complexity of these interactions is exemplified by the anomalous mole fraction effect, which is flattened for F1144G and FY/GK but accentuated for F1144K. In summary, the physicochemical properties of the amino acid residues at positions 1144 and 1152 are crucial to the pore's ability to distinguish between multiple Ba(2+) ions and Ca(2+) ions.

Key roles of Phe1112 and Ser1115 in the pore-forming IIIS5-S6 linker of L-type Ca2+ channel alpha1C subunit (CaV 1.2) in binding of dihydropyridines and action of Ca2+ channel agonists

Voltage-dependent L-type Ca2+ channels are modulated by the binding of Ca2+ channel antagonists and agonists to the pore-forming alpha1c subunit (CaV 1.2). We recently identified Ser1115 in IIIS5-S6 linker of alpha1C subunit as a critical determinant of the action of 1,4-dihydropyridine agonists. In this study, we applied alanine-scanning mutational analysis in IIIS5-S6 linker of rat brain alpha1C subunit (rbCII) to illustrate the role of pore-forming IIIS5-S6 linker in the action of Ca2+ channel modulators. Ca2+ channel currents through wild-type (rbCII) or mutated alpha1C subunits, transiently expressed in BHK6 cells with beta1a and alpha2/delta subunits, were analyzed. The replacement of Phe1112 by Ala (F1112A) significantly impaired the sensitivity to Ca2+ channel agonists (S)-(-)-Bay k 8644 and FPL-64176, and modestly to 1,4-dihydropyridine (DHP) antagonists. The low sensitivity of F1112A and S1115A to DHP antagonists was consistent with the reduced binding affinity for [3H](+)PN200-110. The replacement of Phe1112 by Tyr, but not by Ala, restored the long openings produced by FPL-64176, thus indicating the critical role of aromatic ring of Phe1112 in the Ca2+ channel agonist action. Interestingly, double-mutant Ca2+ channel (F1112A/S1115A) failed to discriminate between Ca2+ channel agonist (S)-(-)-1,4-dihydro-2,6-dimethyl-5-nitro-4-(2-[trifluoromethyl] phenyl)-3-pyridine carboxylic acid methyl ester (Bay k 8644) and antagonist (R)-(+)-Bay k 8644 and was blocked by the two enantiomers in an identical manner. These results indicate that both Phe1112 and Ser1115 in linker IIIS5-S6 are required for the action of Ca2+ channel agonists. A model of the DHP receptor is proposed to visualize possible interactions of Phe1112, Ser1115, and other DHP-sensing residues with a typical DHP ligand nifedipine.

Permeation and selectivity in calcium channels

Recent advances-both experimental and theoretical-provide a tentative image of the structures in Ca channels that make them exceptionally selective. The image is very different from K channels, which obtain high selectivity with a rigid pore that tightly fits K(+) ions and is lined by carbonyl oxygens of the polypeptide backbone. Ca channels rely on four glutamate residues (the EEEE locus), whose carboxyl side chains likely reach into the pore lumen to interact with passing Ca(2+) ions. The structure is thought to be flexible, tightly binding a single Ca(2+) ion in order to block Na(+) flux but rearranging to interact with multiple Ca(2+) ions to allow Ca(2+) flux. The four glutamates are not equivalent, a fact that seems important for Ca(2+) permeation. This review describes the experimental evidence that leads to these conclusions and the attempts by theorists to explain the combination of high selectivity and high flux that characterizes Ca channels.

Control of ion conduction in L-type Ca2+ channels by the concerted action of S5-6 regions

Voltage-gated L-type Ca(2+) channels from cardiac (alpha(1C)) and skeletal (alpha(1S)) muscle differ from one another in ion selectivity and permeation properties, including unitary conductance. In 110 mM Ba(2+), unitary conductance of alpha(1S) is approximately half that of alpha(1C). As a step toward understanding the mechanism of rapid ion flux through these highly selective ion channels, we used chimeras constructed between alpha(1C) and alpha(1S) to identify structural features responsible for the difference in conductance. Combined replacement of the four pore-lining P-loops in alpha(1C) with P-loops from alpha(1S) reduced unitary conductance to a value intermediate between those of the two parent channels. Combined replacement of four larger regions that include sequences flanking the P-loops (S5 and S6 segments along with the P-loop-containing linker between these segments (S5-6)) conferred alpha(1S)-like conductance on alpha(1C). Likewise, substitution of the four S5-6 regions of alpha(1C) into alpha(1S) conferred alpha(1C)-like conductance on alpha(1S). These results indicate that, comparing alpha(1C) with alpha(1S), the differences in structure that are responsible for the difference in ion conduction are housed within the S5-6 regions. Moreover, the pattern of unitary conductance values obtained for chimeras in which a single P-loop or single S5-6 region was replaced suggest a concerted action of pore-lining regions in the control of ion conduction.

Molecular physiology of low-voltage-activated t-type calcium channels

T-type Ca2+ channels were originally called low-voltage-activated (LVA) channels because they can be activated by small depolarizations of the plasma membrane. In many neurons Ca2+ influx through LVA channels triggers low-threshold spikes, which in turn triggers a burst of action potentials mediated by Na+ channels. Burst firing is thought to play an important role in the synchronized activity of the thalamus observed in absence epilepsy, but may also underlie a wider range of thalamocortical dysrhythmias. In addition to a pacemaker role, Ca2+ entry via T-type channels can directly regulate intracellular Ca2+ concentrations, which is an important second messenger for a variety of cellular processes. Molecular cloning revealed the existence of three T-type channel genes. The deduced amino acid sequence shows a similar four-repeat structure to that found in high-voltage-activated (HVA) Ca2+ channels, and Na+ channels, indicating that they are evolutionarily related. Hence, the alpha1-subunits of T-type channels are now designated Cav3. Although mRNAs for all three Cav3 subtypes are expressed in brain, they vary in terms of their peripheral expression, with Cav3.2 showing the widest expression. The electrophysiological activities of recombinant Cav3 channels are very similar to native T-type currents and can be differentiated from HVA channels by their activation at lower voltages, faster inactivation, slower deactivation, and smaller conductance of Ba2+. The Cav3 subtypes can be differentiated by their kinetics and sensitivity to block by Ni2+. The goal of this review is to provide a comprehensive description of T-type currents, their distribution, regulation, pharmacology, and cloning.

Differences in apparent pore sizes of low and high voltage-activated Ca2+ channels

Pore size is of considerable interest in voltage-gated Ca(2+) channels because they exemplify a fundamental ability of certain ion channels: to display large pore diameter, but also great selectivity for their ion of choice. We determined the pore size of several voltage-dependent Ca(2+) channels of known molecular composition with large organic cations as probes. T-type channels supported by the Ca(V)3.1, Ca(V)3.2, and Ca(V)3.3 subunits; L-type channels encoded by the Ca(V)1.2, beta(1), and alpha(2)delta(1) subunits; and R-type channels encoded by the Ca(V)2.3 and beta(3) subunits were each studied using a Xenopus oocyte expression system. The weak permeabilities to organic cations were resolved by looking at inward tails generated upon repolarization after a large depolarizing pulse. Large inward NH(4)(+) currents and sizable methylammonium and dimethylammonium currents were observed in all of the channels tested, whereas trimethylammonium permeated only through L- and R-type channels, and tetramethylammonium currents were observed only in L-type channels. Thus, our experiments revealed an unexpected heterogeneity in pore size among different Ca(2+) channels, with L-type channels having the largest pore (effective diameter = 6.2 A), T-type channels having the tiniest pore (effective diameter = 5.1 A), and R-type channels having a pore size intermediate between these extremes. These findings ran counter to first-order expectations for these channels based simply on their degree of selectivity among inorganic cations or on the bulkiness of their acidic side chains at the locus of selectivity.

Noncontact dipole effects on channel permeation. VI. 5F- and 6F-Trp gramicidin channel currents

Fluorination of peptide side chains has been shown to perturb gramicidin channel conductance without significantly changing the average side chain structure, which, it is hoped, will allow detailed analysis of electrostatic modulation of current flow. Here we report a 1312-point potassium current-voltage-concentration data set for homodimeric channels formed from gramicidin A (gA) or any of eight fluorinated Trp analogs in both lecithin and monoglyceride bilayers. We fit the data with a three-barrier, two-site, two-ion (3B2S) kinetic model. The fluorination-induced changes in the rate constants were constrained by the same factor in both lipids. The rate constant changes were converted to transition-state free-energy differences for comparison with previous electrostatic potential energy differences based on an ab initio force field. The model allowed a reasonably good fit (chi = 8.29 with 1271 degrees of freedom). The measured changes were subtle. Nevertheless, the fitted energy perturbations agree well with electrostatic predictions for five of the eight peptides. For the other three analogs, the fitted changes suggested a reduced translocation barrier rather than the reduced exit barrier as predicted by electrostatics.

Modeling of the outer vestibule and selectivity filter of the L-type Ca2+ channel

Using the KcsA bacterial K+ channel crystal structure [Doyle, D. A., et al. (1998) Science 280, 69-74] and the model of the outer vestibule of the Na+ channel [Lipkind, G. M., and Fozzard, H. A. (2000) Biochemistry 39, 8161-8170] as structural templates, we propose a structural model of the outer vestibule and selectivity filter of the pore of the Ca2+ channel (alpha1C or Ca(v)1.2). The Ca2+ channel P loops were modeled by alpha-helix-turn-beta-strand motifs, with the glutamate residues of the EEEE motif located in the turns. P loops were docked in the extracellular part of the inverted teepee structure formed by S5 and S6 alpha-helices with backbone coordinates from the M1 and M2 helices of the KcsA crystal structure. This construction results in a conical outer vestibule that tapers to the selectivity filter at the bottom. The modeled selectivity ring forms a wide open pore ( approximately 6 A) in the absence of Ca2+. When Ca2+ is present ( approximately 1 microM), all four glutamate side chains move to the center and form a cage around the dehydrated Ca2+ ion, blocking the pore. In the millimolar concentration range, Ca2+ also interacts with two low-affinity sites located externally and internally, which were modeled by the same carboxylate groups of the selectivity filter. Calculation of the resulting electrostatic potentials show that the single Ca2+ ion is located in an electrostatic trap. Only when three Ca2+ ions are bound simultaneously in the high- and low-affinity sites of the selectivity filter is Ca2+ able to overcome electrostatic attraction, permitting Ca2+ flux.

Amino acid residues outside of the pore region contribute to N-type calcium channel permeation

It is widely believed that the selectivity of voltage-dependent calcium channels is mainly controlled by amino acid residues contained within four p-loop motifs forming the pore of the channel. An examination of the amino acid sequences of high voltage-activated calcium channels reveals that their domain III S5-H5 regions contain a highly conserved motif with homology to known EF hand calcium binding proteins, hinting that this region may contribute to channel permeation. To test this hypothesis, we used site-directed mutagenesis to replace three conserved negatively charged residues in the N-type calcium channel alpha1B subunit (Glu-1321, Asp-1323, and Glu-1332) with positively charged amino acids (lysine and arginine) and studied their effect on ion selectivity using whole cell and single channel patch clamp recordings. Whereas the wild type channels conducted barium much more effectively than calcium, the mutant displayed nearly equal permeabilities for these two ions. Individual replacement of residue 1332 or a double substitution of residues 1321 and 1323 with lysine and arginine, respectively, were equally effective. Disruption of the putative EF hand motif through replacement of the central glycine residue (1326) with proline resulted in a similar effect, indicating that the responses observed with the triple mutant were not due to changes in the net charge of the channel. Overall, our data indicate that residues outside of the narrow region of the pore have the propensity to contribute to calcium channel permeation. They also raise the possibility that interactions of calcium ions with a putative calcium binding domain at the extracellular side of the channel may underlie the differential permeabilities of the channel for barium and calcium ions.

Identification of an aspartic residue in the P-loop of the vanilloid receptor that modulates pore properties

Vanilloid receptor subunit 1 (VR1) is a nonselective cation channel that integrates multiple pain-producing stimuli. VR1 channels are blocked with high efficacy by the well established noncompetitive antagonist ruthenium red and exhibit high permeability to divalent cations. The molecular determinants that define these functional properties remain elusive. We have addressed this question and evaluated by site-specific neutralization the contribution on pore properties of acidic residues located in the putative VR1 pore region. Mutant receptors expressed in Xenopus oocytes exhibited capsaicin-operated ionic currents akin to those of wild type channels. Incorporation of glutamine residues at Glu(648) and Glu(651) rendered minor effects on VR1 pore attributes, while Glu(636) slightly modulated pore blockade. In contrast, replacement of Asp(646) by asparagine decreased 10-fold ruthenium red blockade efficacy and reduced 4-fold the relative permeability of the divalent cation Mg(2+) with respect to Na(+) without changing the selectivity of monovalent cations. At variance with wild type channels and E636Q, E648Q, and E651Q mutant receptors, ruthenium red blockade of D646N mutants was weakly sensitive to extracellular pH acidification. Collectively, our results suggest that Asp(646) is a molecular determinant of VR1 pore properties and imply that this residue may form a ring of negative charges that structures a high affinity binding site for cationic molecules at the extracellular entryway.

Side chain orientation in the selectivity filter of a voltage-gated Ca2+ channel

Four glutamate residues (EEEE locus) are essential for ion selectivity in voltage-gated Ca(2+) channels, with ion-specific differences in binding to the locus providing the basis of selectivity. Whether side chain carboxylates or alternatively main chain carbonyls of these glutamates project into the pore to form the ion-binding locus has been uncertain. We have addressed this question by examining effects of sulfhydryl-modifying agents (methanethiosulfonates) on 20 cysteine-substituted mutant forms of an L-type Ca(2+) channel. Sulfhydryl modifiers partially blocked whole oocyte Ba(2+) currents carried by wild type channels, but this block was largely reversed with washout. In contrast, each of the four EEEE locus glutamate --> cysteine mutants (0 position) was persistently blocked by sulfhydryl modifiers, indicating covalent attachment of a modifying group to the side chain of the substituted cysteine. Cysteine substitutions at positions immediately adjacent to the EEEE locus glutamates (+/-1 positions) were also generally susceptible to sulfhydryl modification. Sulfhydryl modifiers had lesser effects on channels substituted one position further from the EEEE locus (+/-2 positions). These results indicate that the carboxylate-bearing side chains of the EEEE locus glutamates and their immediate neighbors project into the water-filled lumen of the pore to form an ion-binding locus. Thus the structure of the Ca(2+) channel selectivity filter differs substantially from that of ancestral K(+) channels.

Ion interactions in the high-affinity binding locus of a voltage-gated Ca(2+) channel

The selectivity filter of voltage-gated Ca(2+) channels is in part composed of four Glu residues, termed the EEEE locus. Ion selectivity in Ca(2+) channels is based on interactions between permeant ions and the EEEE locus: in a mixture of ions, all of which can pass through the pore when present alone, those ions that bind weakly are impermeant, those that bind more strongly are permeant, and those that bind more strongly yet act as pore blockers as a consequence of their low rate of unbinding from the EEEE locus. Thus, competition among ion species is a determining feature of selectivity filter function in Ca(2+) channels. Previous work has shown that Asp and Ala substitutions in the EEEE locus reduce ion selectivity by weakening ion binding affinity. Here we describe for wild-type and EEEE locus mutants an analysis at the single channel level of competition between Cd(2+), which binds very tightly within the EEEE locus, and Ba(2+) or Li(+), which bind less tightly and hence exhibit high flux rates: Cd(2+) binds to the EEEE locus approximately 10(4)x more tightly than does Ba(2+), and approximately 10(8)x more tightly than does Li(+). For wild-type channels, Cd(2+) entry into the EEEE locus was 400x faster when Li(+) rather than Ba(2+) was the current carrier, reflecting the large difference between Ba(2+) and Li(+) in affinity for the EEEE locus. For the substitution mutants, analysis of Cd(2+) block kinetics shows that their weakened ion binding affinity can result from either a reduction in blocker on rate or an enhancement of blocker off rate. Which of these rate effects underlay weakened binding was not specified by the nature of the mutation (Asp vs. Ala), but was instead determined by the valence and affinity of the current-carrying ion (Ba(2+) vs. Li(+)). The dependence of Cd(2+) block kinetics upon properties of the current-carrying ion can be understood by considering the number of EEEE locus oxygen atoms available to interact with the different ion pairs.