Interactions of monovalent cations with sodium channels in squid axon. I. Modification of physiological inactivation gating

Inactivation of Na channels has been studied in voltage-clamped, internally perfused squid giant axons during changes in the ionic composition of the intracellular solution. Peak Na currents are reduced when tetramethylammonium ions (TMA+) are substituted for Cs ions internally. The reduction reflects a rapid, voltage-dependent block of a site in the channel by TMA+. The estimated fractional electrical distance for the site is 10% of the channel length from the internal surface. Na tail currents are slowed by TMA+ and exhibit kinetics similar to those seen during certain drug treatments. Steady state INa is simultaneously increased by TMA+, resulting in a "cross-over" of current traces with those in Cs+ and in greatly diminished inactivation at positive membrane potentials. Despite the effect on steady state inactivation, the time constants for entry into and exit from the inactivated state are not significantly different in TMA+ and Cs+. Increasing intracellular Na also reduces steady state inactivation in a dose-dependent manner. Ratios of steady state INa to peak INa vary from approximately 0.14 in Cs+- or K+-perfused axons to approximately 0.4 in TMA+- or Na+-perfused axons. These results are consistent with a scheme in which TMA+ or Na+ can interact with a binding site near the inner channel surface that may also be a binding or coordinating site for a natural inactivation particle. A simple competition between the ions and an inactivation particle is, however, not sufficient to account for the increase in steady state INa, and changes in the inactivation process itself must accompany the interaction of TMA+ and Na+ with the channel.     

State-independent intracellular access of quaternary ammonium blockers to the pore of TREK-1

We previously reported that TREK-1 gating by internal pH and pressure occurs close to or within the selectivity filter. These conclusions were based upon kinetic measurements of high-affinity block by quaternary ammonium (QA) ions that appeared to exhibit state-independent accessibility to their binding site within the pore. Intriguingly, recent crystal structures of two related K2P potassium channels were also both found to be open at the helix bundle crossing. However, this did not exclude the possibility of gating at the bundle crossing and it was suggested that side-fenestrations within these structures might allow state-independent access of QA ions to their binding site. In this addendum to our original study we demonstrate that even hydrophobic QA ions do not access the TREK-1 pore via these fenestrations. Furthermore, by using a chemically reactive QA ion immobilized within the pore via covalent cysteine modification we provide additional evidence that the QA binding site remains accessible to the cytoplasm in the closed state. These results support models of K2P channel gating which occur close to or within the selectivity filter and do not involve closure at the helix bundle crossing.     

Pharmacological properties of native CaCCs and TMEM16A

We previously reported that TREK-1 gating by internal pH and pressure occurs close to or within the selectivity filter. These conclusions were based upon kinetic measurements of high-affinity block by quaternary ammonium (QA) ions that appeared to exhibit state-independent accessibility to their binding site within the pore. Intriguingly, recent crystal structures of two related K2P potassium channels were also both found to be open at the helix bundle crossing. However, this did not exclude the possibility of gating at the bundle crossing and it was suggested that side-fenestrations within these structures might allow state-independent access of QA ions to their binding site. In this addendum to our original study we demonstrate that even hydrophobic QA ions do not access the TREK-1 pore via these fenestrations. Furthermore, by using a chemically reactive QA ion immobilized within the pore via covalent cysteine modification we provide additional evidence that the QA binding site remains accessible to the cytoplasm in the closed state. These results support models of K2P channel gating which occur close to or within the selectivity filter and do not involve closure at the helix bundle crossing.     

Characterization and localization of two ion-binding sites within the pore of cardiac L-type calcium channels

L-type Ca channels from porcine cardiac sarcolemma were incorporated into planar lipid bilayers. We characterized interactions of permeant and blocking ions with the channel's pore by (a) studying the current-voltage relationships for Ca2+ and Na+ when equal concentrations of the ions were present in both internal and external solutions, (b) testing the dose-dependent block of Ba2+ currents through the channels by internally applied cadmium, and (c) examining the dose and voltage dependence of the block of Na+ currents through the channels by internally and externally applied Ca2+. We found that the I-V relationship for Na+ appears symmetrical through the origin when equal concentrations of Na+ are present on both sides of the channel (gamma = 90 pS in 200 mM NaCl). The conductance for outward Ca2+ currents with 100 mM Ca2+ on both sides of the channel is approximately 8 pS, a value identical to that observed for inward currents when 100 mM Ca2+ was present outside only. This provides evidence that ions pass through the channel equally well regardless of the direction of net flux. In addition, we find that internal Cd2+ is as effective as external Cd2+ in blocking Ba2+ currents through the channels, again suggesting identical interactions of ions with each end of the pore. Finally, we find that micromolar Ca2+, either in the internal or in the external solution, blocks Na+ currents through the channels. The affinity for internally applied Ca2+ appears the same as that for externally applied Ca2+. The voltage dependence of the Ca(2+)-block suggests that the sites to which Ca2+ binds are located approximately 15% and approximately 85% of the electric field into the pore. Taken together, these data provide direct experimental evidence for the existence of at least two ion binding sites with high affinity for Ca2+, and support the idea that the sites are symmetrically located within the electric field across L-type Ca channels.     

Analysis of the effects of cesium ions on potassium channel currents in biological membranes

Cesium ions block potassium channels in biological membranes in a voltage dependent manner. For example, external cesium blocks inward current with little or no effect on outward current. Consequently, it produces a characteristic N-shaped current-voltage relationship. We have modeled this result by single file diffusion of ions in a narrow channel spanning the membrane with a special blocking site in the channel for cesium ions. The model enables us to make detailed comparisons of the effects of cesium on potassium channels in different types of biological membranes.     

Interactions of monovalent cations with sodium channels in squid axon. II. Modification of pharmacological inactivation gating

The time-, frequency-, and voltage-dependent blocking actions of several cationic drug molecules on open Na channels were investigated in voltage-clamped, internally perfused squid giant axons. The relative potencies and time courses of block by the agents (pancuronium [PC], octylguanidinium [C8G], QX-314, and 9-aminoacridine [9-AA]) were compared in different intracellular ionic solutions; specifically, the influences of internal Cs, tetramethylammonium (TMA), and Na ions on block were examined. TMA+ was found to inhibit the steady state block of open Na channels by all of the compounds. The time-dependent, inactivation-like decay of Na currents in pronase-treated axons perfused with either PC, 9-AA, or C8G was retarded by internal TMA+. The apparent dissociation constants (at zero voltage) for interaction between PC and 9-AA with their binding sites were increased when TMA+ was substituted for Cs+ in the internal solution. The steepness of the voltage dependence of 9-AA or PC block found with internal Cs+ solutions was greatly reduced by TMA+, resulting in estimates for the fractional electrical distance of the 9-AA binding site of 0.56 and 0.22 in Cs+ and TMA+, respectively. This change may reflect a shift from predominantly 9-AA block in the presence of Cs+ to predominantly TMA+ block. The depth, but not the rate, of frequency-dependent block by QX-314 and 9-AA is reduced by internal TMA+. In addition, recovery from frequency-dependent block is not altered. Elevation of internal Na produces effects on 9-AA block qualitatively similar to those seen with TMA+. The results are consistent with a scheme in which the open channel blocking drugs, TMA (and Na) ions, and the inactivation gate all compete for a site or for access to a site in the channel from the intracellular surface. In addition, TMA ions decrease the apparent blocking rates of other drugs in a manner analogous to their inhibition of the inactivation process. Multiple occupancy of Na channels and mutual exclusion of drug molecules may play a role in the complex gating behaviors seen under these conditions.     

Access of quaternary ammonium blockers to the internal pore of cyclic nucleotide-gated channels: implications for the location of the gate

Cyclic nucleotide-gated (CNG) channels play important roles in the transduction of visual and olfactory information by sensing changes in the intracellular concentration of cyclic nucleotides. We have investigated the interactions between intracellularly applied quaternary ammonium (QA) ions and the alpha subunit of rod cyclic nucleotide-gated channels. We have used a family of alkyl-triethylammonium derivatives in which the length of one chain is altered. These QA derivatives blocked the permeation pathway of CNG channels in a concentration- and voltage-dependent manner. For QA compounds with tails longer than six methylene groups, increasing the length of the chain resulted in higher apparent affinities of approximately 1.2 RT per methylene group added, which is consistent with the presence of a hydrophobic pocket within the intracellular mouth of the channel that serves as part of the receptor binding site. At the single channel level, decyltriethyl ammonium (C10-TEA) ions did not change the unitary conductance but they did reduce the apparent mean open time, suggesting that the blocker binds to open channels. We provide four lines of evidence suggesting that QA ions can also bind to closed channels: (1) the extent of C10-TEA blockade at subsaturating [cGMP] was larger than at saturating agonist concentration, (2) under saturating concentrations of cGMP, cIMP, or cAMP, blockade levels were inversely correlated with the maximal probability of opening achieved by each agonist, (3) in the closed state, MTS reagents of comparable sizes to QA ions were able to modify V391C in the inner vestibule of the channel, and (4) in the closed state, C10-TEA was able to slow the Cd2+ inhibition observed in V391C channels. These results are in stark contrast to the well-established QA blockade mechanism in Kv channels, where these compounds can only access the inner vestibule in the open state because the gate that opens and closes the channel is located cytoplasmically with respect to the binding site of QA ions. Therefore, in the context of Kv channels, our observations suggest that the regions involved in opening and closing the permeation pathways in these two types of channels are different.     

An ion''s view of the potassium channel. The structure of the permeation pathway as sensed by a variety of blocking ions

We have studied the block of potassium channels in voltage-clamped squid giant axons by nine organic and alkali cations, in order to learn how the channel selects among entering ions. When added to the internal solution, all of the ions blocked the channels, with inside-positive voltages enhancing the block. Cesium blocked the channels from the outside as well, with inside-negative voltages favoring block. We compared the depths to which different ions entered the channel by estimating the "apparent electrical distance" to the blocking site. Simulations with a three-barrier, double-occupancy model showed that the "apparent electrical distance," expressed as a fraction of the total transmembrane voltage, appears to be less than the actual value if the blocking ion can pass completely through the channel. These calculations strengthen our conclusion that sodium and cesium block at sites further into the channel than those occupied by lithium and the organic blockers. Our results, considered together with earlier work, demonstrate that the depth to which an ion can readily penetrate into the potassium channel depends both on its size and on the specific chemical groups on its molecular surface. The addition of hydroxyl groups to alkyl chains on a quaternary ammonium ion can both decrease the strength of binding and allow deeper penetration into the channel. For alkali cations, the degree of hydration is probably crucial in determining how far an ion penetrates. Lithium, the most strongly hydrated, appeared not to penetrate as far as sodium and cesium. Our data suggest that there are, minimally, four ion binding sites in the permeation pathway of the potassium channel, with simultaneous occupancy of at least two.     

Internal cesium and the sodium inactivation gate in Myxicola giant axons.

Internal cesium (CSi), relative to internal potassium (Ki), alters Na current (INa) time course in internally perfused Myxicola giant axons. CSi slows the time to peak INa, slows its decline from peak and increases the steady state to peak current ratio, INainfinity/INapeak. Neither activation nor deactivation kinetics are appreciably affected by CSi. Na current rising phases, times to half maximum and tail current time courses are similar in CSi and Ki. Inactivation time constants determined by both one (tau h) and two (tau c) pulses are also little changed by CSi. The CSi effects are due largely or entirely to an increased INainfinity/INapeak. CSi decreases the steady level of inactivation reached during a step in potential, preventing some fraction of inactivation gates from closing at all, the rest apparently closing normally. Inactivation block in CSi decreases with increasing inward current magnitude and in Ki inactivation block is appreciable only for outward Na channel current, suggesting the site of action is located somewhere in the current pathway. If this site mediates the normal operation of the inactivation gate, then a possible mechanism for gate closure could involve a positively charged structure moving to associate with a negative site near or into the inner channel mouth.     

Methadone block of K+ current in squid giant fiber lobe neurons

Voltage-dependent ionic currents were recorded from squid giant fiber lobe neurons using the whole-cell patch-clamp technique. When applied to the bathing solution, methadone was found to block IK, I Na and I Ca. Both I Na and I Ca were reduced without apparent change in kinetics and exhibited IC(50)'s of 50-100 and 250-500 mu M, respectively, at +10 mV. In contrast, IK was reduced in a time-dependent manner that is well fit by a simple model of open channel block (K(D)= 32+/- or 2 mu M, +60 mV, 10 degrees Celsius). The mechanism of I(K) block was examined in detail and involves a direct action of methadone, a tertiary amine, on K channels rather than an opioid receptor-mediated pathway. The kinetics of I(K) block resemble those reported for internally applied long chain quaternary ammonium (QA) compounds; and recovery from I(K) block is QA-like in its slow time course and strong dependence on holding potential. A quaternary derivative of methadone (N-methyl- methadone) only reproduced the effects of methadone on I(K) when included in the pipette solution; this compound was without effect when applied externally. I(K) block thus appears to involve diffusion of methadone into the cytoplasm and occlusion of the open K channel at the internal QA blocking site by the protonated form of the drug. This proposed mode of action is supported by the pH and voltage dependence of block as well as by the observation that high external K+ speeds the rate of drug dissociation. In addition, the effect of methadone on I(K) evoked during prolonged (300 ms) depolarizations suggests that methadone block may interfere with endogenous K+ channel inactivation. The effects of temperature, methadone stereoisomers, and the methadone- like drugs propoxyphene and nor-propoxyphene on IK block were examined. Methadone was also found to block I(K) in GH3 cells and in chick myoblasts.     

Blockade of sodium and potassium channels in the node of Ranvier by ajmaline and N-propyl ajmaline

The inhibition of sodium and potassium currents in frog myelinated fibres by ajmaline (AM) and its quaternary derivative, N-propyl ajmaline (NPA), depends on voltage-clamp pulses and the state of channel gating mechanisms. The permanently charged NPA and protonated AM interact only (or mainly) with open channels, while unprotonated AM affects preferently inactivated Na channels. Inhibition of Na currents by NPA and AM does not depend on the current direction and Na ion concentration in external or internal media. In contrast only the outward potassium currents can be blocked by NPA and AM; the inward potassium currents in high K+ ions external media are resistant to the blocking action of these drugs. The voltage dependence of ionic current inhibition by charged drugs suggests the location of their binding sites in the inner mouths of Na and K channels. Judging by the kinetics of current restoration after cessation of pulsing, the drug-binding site complex is much more stable in Na than in potassium channels. Batrachotoxin and aconitine, unlike veratridine and sea anemone toxin, decrease greatly the affinity of Na channel binding sites to NPA and AM. The effects of NPA and AM are compared with those of local anesthetics and other amine blocking drugs.     

Block of tetrodotoxin-resistant Na+ channel pore by multivalent cations: gating modification and Na+ flow dependence

Tetrodotoxin-resistant (TTX-R) Na(+) channels are much less susceptible to external TTX but more susceptible to external Cd(2+) block than tetrodotoxin-sensitive (TTX-S) Na(+) channels. Both TTX and Cd(2+) seem to block the channel near the "DEKA" ring, which is probably part of a multi-ion single-file region adjacent to the external pore mouth and is involved in the selectivity filter of the channel. In this study we demonstrate that other multivalent transitional metal ions such as La(3+), Zn(2+), Ni(2+), Co(2+), and Mn(2+) also block the TTX-R channels in dorsal root ganglion neurons. Just like Cd(2+), the blocking effect has little intrinsic voltage dependence, but is profoundly influenced by Na(+) flow. The apparent dissociation constants of the blocking ions are always significantly smaller in inward Na(+) currents than those in outward Na(+) current, signaling exit of the blocker along with the Na(+) flow and a high internal energy barrier for "permeation" of these multivalent blocking ions through the pore. Most interestingly, the activation and especially the inactivation kinetics are slowed by the blocking ions. Moreover, the gating changes induced by the same concentration of a blocking ion are evidently different in different directions of Na(+) current flow, but can always be correlated with the extent of pore block. Further quantitative analyses indicate that the apparent slowing of channel activation is chiefly ascribable to Na(+) flow-dependent unblocking of the bound La(3+) from the open Na(+) channel, whereas channel inactivation cannot happen with any discernible speed in the La(3+)-blocked channel. Thus, the selectivity filter of Na(+) channel is probably contiguous to a single-file multi-ion region at the external pore mouth, a region itself being nonselective in terms of significant binding of different multivalent cations. This region is "open" to the external solution even if the channel is "closed" ("deactivated"), but undergoes imperative conformational changes during the gating (especially the inactivation) process of the channel.     

Blockade of GABAA receptor channels by niflumic acid prevents agonist dissociation

The modulation by the nonsteroidal anti-inflammatory drug niflumic acid (NFA) of the GABAA receptor-mediated currents was studied in acutely isolated cerebellar Purkinje cells using the whole-cell recording and fast drug application system. At concentrations of 3–300 μM NFA potentiated GABA (2 μM)-activated currents, and at concentrations of 1–3 mM NFA blocked these responses. The NFA-induced block was strongly voltage-dependent. Analysis of the voltage dependence of the block suggests that the blocking action of NFA is a result of NFA binding at the site located within GABAA channel pore. The termination of GABA and NFA application was followed by a transient increase of the inward current — “tail” current. These data suggest that NFA acts as a sequential open channel blocker, which prevents dissociation of agonist while the channel is blocked. The tail current develops because, prior to dissociation of agonist, the channels that are in the blocked state must return to the close state via the open state. The tail currents were compared in the presence and absence of gabazine, a competitive antagonist that also allosterically inhibits GABA_A receptors. Application of gabazine only during development of tail current did not change neither amplitude nor time course of this current, while noncompetitive antagonists picrotoxin and penicillin blocked it. Protection of tail current from gabazine block indicates that GABA cannot dissociate from the open-blocked state and the agonist was trapped on the receptor while the channel was open. Trapping was specific for the agonist, because the positive allosteric modulator zolpidem (benzodiazepine site agonist) was able to potentiate the tail current in the absence of GABA in the external solution. Our observations provide a model-independent functional support of the hypothesis that open channel block of GABAA channels by NFA prevents an escape of the agonist from its binding sites.     

Interaction of n-alkylguanidines with the sodium channels of squid axon membrane

The effects of n-alkylguanidine derivatives on sodium channel conductance were measured in voltage clamped, internally perfused squid giant axons. After destruction of the sodium inactivation mechanism by internal pronase treatment, internal application of n-amylguanidine (0.5 mM) or n-octylguanidine (0.03 mM) caused a time-dependent block of sodium channels. No time-dependent block was observed with shorter chain derivatives. No change in the rising phase of sodium current was seen and the block of steady-state sodium current was independent of the membrane potential. In axons with intact sodium inactivation, an apparent facilitation of inactivation was observed after application of either n-amylguanidine or n-octylguanidine. These results can be explained by a model in which alkylguanidines enter and occlude open sodium channels from inside the membrane with voltage-independent rate constants. Alkylguanidine block bears a close resemblance to natural sodium inactivation. This might be explained by the fact that alkylguanidines are related to arginine, which has a guanidino group and is thought to be an essential amino acid in the molecular mechanism of sodium inactivation. A strong correlation between alkyl chain length and blocking potency was found, suggesting that a hydrophobic binding site exists near the inner mouth of the sodium channel.     

Interaction of barium ions with potassium channels in squid giant axons.

Blocking of potassium channels by internally and externally applied barium ions has been studied in squid giant axons. Internal Ba (3-5 mM) causes rapid decay or "inactivation" of potassium current (IK). The kinetics and degree of block are strongly voltage-dependent. Large positive voltages speed blocking and make it more profound. Raising the external potassium concentration (Ko) from 0 to 250 mM has the opposite effect: block is made slower and less severe. In contrast, for positive voltages block by the tetraethylammonium derivative 3-phenylpropyltriethylammonium ion is almost independent of Ko and voltage. Recovery from block by internal Ba has a rapid phase lasting a few milliseconds and a slow phase lasting approximately 5 min. Internal Ba causes a "hook" in the IK tails recorded on repolarizing the fiber in high potassium external medium. External Ba, on the other hand, blocks without much altering IK time-course. KD (the dissociation constant) for block by external Ba is a few millimolar, and depends on the internal potassium concentration, the holding potential, and other factors. A reaction scheme for Ba and K channels is presented, postulating that internal and external Ba reach the same point in the channel. Once there, Ba blocks and also stabilizes the closed conformation of the channel. The extreme stability of the Ba channel complex implies the existence of negative charge within the channel.     

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

Using the lanthanide gadolinium (Gd(3+)) as a Ca(2+) replacing probe, we investigated the voltage dependence of pore blockage of Ca(V)1.2 channels. Gd(+3) reduces peak currents (tonic block) and accelerates decay of ionic current during depolarization (use-dependent block). Because diffusion of Gd(3+) at concentrations used (<1 microM) 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 Gd(3+) shifted in parallel for Ba(2+), Sr(2+), and Ca(2+) currents through the wild-type channel, and for Ca(2+) currents through the selectivity filter mutation EEQE that lowers the blocking potency of Gd(3+). The correlation indicates that Gd(3+) 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 Gd(3+) decreases with concentration of Ba(2+), 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, Gd(3+) 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.     

Blockage of squid axon potassium conductance by internal tetra-N-alkylammonium ions of various sizes.

We have studied the effects of the tetra-n-alkylammonium (TAA) ions, (CnH2n+1)4N+, n = 1-6, on the potassium conductance of voltage-clamped squid giant axons. Studies using tetrahexylammonium were not quantitatively analyzed as its effect was insufficiently reversible. Each in this series of symmetric ions of graded size blocks the potassium conductance when added to the internal perfusion fluid. There is a general trend for blocking potency to increase with increasing size. We attribute this to stronger interactions of the longer alkyl side chains with hydrophobic regions of the membrane near the channels. Steady-state block by the TAA ions, n = 2-5, showed identical voltage dependence, apparently sensing about 15% of the transmembrane voltage, and kinetics block onset were qualitatively similar. We conclude that the site of action for these ions is the same. Block by TMA is about twice as steeply dependent on voltage. In its action, TMA resembles the alkali cations (French et al., 1979, Biophys, J. 25(2, pt. 2):307a) more than the larger TAA ions. Our results suggest that access to the inner mouth of the K channel is even less restricted than has been previously thought. A calculation indicates that the lumen of the channel cannot be both wide enough to admit the TAA ions and long enough to account for the voltage dependence of block. We consider possible ways to resolve this paradox.     

Temperature dependence of drug blockade of a calcium-dependent potassium channel in cultured hippocampal neurons.

The temperature dependence of drug blockade of a calcium-dependent potassium channel K(Ca) has been studied in cultured CA1 hippocampal neurons. Channel openings from a 70-pS K+ channel were recorded when inside-out patches were exposed to a bath solution containing 140 mM K+ and 0.2 mM Ca2+. The mean open times of channel events were not significantly altered when the bath temperature was lowered from 24 degrees to 14 degrees C (Q10 = 1.2). Introduction of the drug RP-62719 into the bath solution (at 5 microM) resulted in the mean open time of the K(Ca) channel to be diminished by 85% (at 24 degrees C) with no change in the amplitudes of the unitary currents. Over the same temperature range of 24 degrees to 14 degrees C, in the presence of RP-62719, the mean open times were significantly prolonged (Q10 = 2.2). A simple open channel block scheme was used to determine the temperature dependence of the onward- (blocking) and off- (unblocking) rate constants. Thermodynamic analysis, using transition rate theory, showed that the blocking rate constant was associated with a large increase in entropy. The relatively high temperature dependence for channel blockade is not consistent with a rate-limiting process established by simple diffusion of the agent to a channel blocking site. Channel block may involve conformational changes in the channel protein as a consequence of hydrophobic interactions between drug and channel sites.     

Ion selectivity and current saturation in inward-rectifier K+ channels

We investigated the features of the inward-rectifier K channel Kir1.1 (ROMK) that underlie the saturation of currents through these channels as a function of permeant ion concentration. We compared values of maximal currents and apparent K(m) for three permeant ions: K(+), Rb(+), and NH(4)(+). Compared with K(+) (i(max) = 4.6 pA and K(m) = 10 mM at -100 mV), Rb(+) had a lower permeability, a lower i(max) (1.8 pA), and a higher K(m) (26 mM). For NH(4)(+), the permeability was reduced more with smaller changes in i(max) (3.7 pA) and K(m) (16 mM). We assessed the role of a site near the outer mouth of channel in the saturation process. This site could be occupied by either permeant ions or low-affinity blocking ions such as Na(+), Li(+), Mg(2+), and Ca(2+) with similar voltage dependence (apparent valence, 0.15-0.20). It prefers Mg(2+) over Ca(2+) and has a monovalent cation selectivity, based on the ability to displace Mg(2+), of K(+) > Li(+) ～ Na(+) > Rb(+) ～ NH(4)(+). Conversely, in the presence of Mg(2+), the K(m) for K(+) conductance was substantially increased. The ability of Mg(2+) to block the channels was reduced when four negatively charged amino acids in the extracellular domain of the channel were mutated to neutral residues. The apparent K(m) for K(+) conduction was unchanged by these mutations under control conditions but became sensitive to the presence of external negative charges when residual divalent cations were chelated with EDTA. The results suggest that a binding site in the outer mouth of the pore controls current saturation. Permeability is more affected by interactions with other sites within the selectivity filter. Most features of permeation (and block) could be simulated by a five-state kinetic model of ion movement through the channel.     

Blockade of current through single calcium channels by trivalent lanthanide cations. Effect of ionic radius on the rates of ion entry and exit

Currents flowing through single dihydropyridine-sensitive Ca2+ channels were recorded from cell-attached patches on C2 myotubes. In the presence of dihydropyridine agonist to prolong the duration of single-channel openings, adding micromolar concentrations of lanthanum (La), cerium (Ce), neodymium (Nd), gadolinium (Gd), dysprosium (Dy), or ytterbium (Yb) to patch electrodes containing 110 mM BaCl2 caused the unitary Ba2+ currents to fluctuate between fully open and shut states. The kinetics of channel blockade followed the predictions of a simple open channel block model in which the fluctuations of the single-channel current arose from the entry and exit of blocking ions from the pore. Entry rates for all the lanthanides tested were relatively insensitive to membrane potential, however, exit rates depended strongly on membrane potential increasing approximately e-fold per 23 mV with hyperpolarization. Individual lanthanide ions differed in both the absolute rates of ion entry and exit: entry rates decreased as cationic radius decreased; exit rates also decreased with cationic radius during the first part of the lanthanide series but then showed little change during the latter part of the series. Overall, the results support the idea that smaller ions enter the channel more slowly, presumably because they dehydrate more slowly; smaller ions also bind more tightly to a site within the channel pore, but lanthanide residence time within the channel approaches a maximum for the smaller cations with radii less than or equal to that of Ca2+.